PRACTICAL GEOMETRY AND GRAPHICS WORKS BY DAVID ALLAN LOW PRACTICAL GEOMETRY AND GRAPHICS. 'js. 6d. net. TEXT-BOOK ON PRACTICAL SOLID OR DESCRIPTIVE GEOMETRY. Crown 8vo. Part I. With 114 Figures, 2s. Part II. With 64 Figures, 3^. APPLIED MECHANICS : Embracing Strength and Elasticity of Materials, Theory and Design of Structures, Theory of Machines and Hydrau- lics. A Text-Book for Engineering Students. With 850 Illustrations and 780 Exercises. 8vo, "JS. 6d. net. A MANUAL OF MACHINE DRAWING AND DESIGN. By David Allan Low and Alfred William Bevis. With Over 700 Illustrations. 8vo, 7^. 6d. AN INTRODUCTION TO MACHINE DRAW- ING AND DESIGN. With 153 Illustrations and Diagrams. Crown 8vo, 2s. 6d. A POCKET-BOOK FOR MECHANICAL ENGI- NEERS. Fcp. 8vo, ^s. ed. THE DIAGRAM MEASURER. An Instrument for Measuring the Areas of Irregular Figures, and specially useful for determining the Mean Effective Pressure from Indicator Diagrams from Steam, Gas and other Engines. With full instructions, is. IMPROVED DRAWING APPLIANCES. Set-Squares, Adjustable Protractor Set-Squares, Tee-Squares, Protractors, Scales, etc. Particulars will be sent on application. LONGMANS, GREEN, AND CO., LONDON, NEW YORK, BOMBAY, AND CALCUTTA. PRACTICAL GEOMETRY AND GRAPHICS BY DAVID ALLAN LOW (Whitworth Scholar), M.I.Mech.E. Professor of Engineering, East London College (university of london) WITH OVER SOO ILLUSTnA^ld^'S AA^B' OVER 700 e!xerois^^*' >'> vi X\ : : .'. LONGMANS, GREEN, AND CO, 39 PATERNOSTER ROW, LONDON NEW YORK, BOMBAY, AND CALCUTTA 1912 All rights reserved \\ s)^v Ml PREFACE An endeavour has been made to provide in this work a fairly complete course of instruction in practical geometry for technical students. The field covered is a very wide one, but by adopting a concise style and by endeavouring to make the illustrations "talk " the work has been kept of reasonable size. A special feature has been made of the illustrations. These are very numerous, and they have been carefully planned so that even the most complicated of them should be distinct and clearly show the constructions used, notwithstanding that most of them are compara- tively small. Pictorial projections have been freely used in dealing with solid geometry, and these in many cases are just as useful as actual models in illustrating the relative positions of points, lines, and planes in space. Nevertheless teachers are recommended to provide models for class use in teaching solid geometry, and the student should also make small cardboard models for himself in studying many of the problems, especially in the earlier stages of his work. The student cannot hope to master the subject of practical geometry unless he works on the drawing board a large number of examples. Hence, another special feature of this work is the large collection of exercises. These exercises have been prepared and selected with great care, and it will be found that they not only provide ample practice for the student but in many cases they amplify the text. About ninety per cent, of the exercises are original and the remainder have been selected from the examination papers of the Board of Education. To economize space many of the diagrams for the exercises have been placed on a squared ground. It should scarcely be necessary to state that in reproducing these diagrams the squared ground need not be drawn, but by counting the squares the 26083 L vi PREFACE various points and lines may be plotted from two axes at right angles to one another. Great credit is due to Mr. J. W. Barrett for the oare, intelligence, and skill which he has displayed in making the finished drawings for the illustrations from the author's pencil drawings and sketches. D. A. L. East London CoLLEaE (University of London), September, 1912. CONTENTS CHAP. PAGE I. Introductory 1 II. The Circle 16 III. CoKic Sections 30 IV. Tracing Paper Problems 54 V. Approximate Solutions to some Unsolved Problems . . 61 VI. Roulettes and Glissettes 66 VII. Vector Geometry 82 VIII. Graphic Statics . 91 IX. Plane Co-ordinate Geometry 128 X. Periodic Motion 148 XI. Projection 166 XII. Projections of Points and Lines 171 XIII. Projections op Simple Solids in Simple Positions . . . 181 XIV. Changing the Planes of Projection 191 XV. Planes other than the Co-ordinate Planes 198 XVI. Straight Line and Plane 211 XVII. Sections op Solids 241 XVIII. The Sphere, Cylinder, and Cone 249 XIX. Special Projections of Plane Figures and Solids . . . 272 XX. Horizontal Projection 279 XXI. Pictorial Projections 290 XXII. Perspective Projection 300 XXIII. Curved Surfaces and Tangent Planes 313 XXIV. Developments * 349 XXV. Helices and Screws 362 XXVI. Intersection op Surfaces , 888 XXVII. Projection op Shadows 411 XXVIII. Miscellaneous Problems in Solid Geometry 423 Appendix, Mathematical Tables 436 Index 443 CHAPTER I INTRODUCTORY 1. Lines. — Euclid defines a line as " that which has length without breadth." A line, therefore, in the strict mathematical sense has no material existence, and the finest " line " that can be drawn on paper is only a rough approximation to a mathematical line. A straight line is defined by Euclid as " that which lies evenly between its extreme points." An important property of straight lines is that two straight lines cannot coincide at two points without coinciding altogether. This property is made use of in the applications of a " straight-edge." A line is also defined as the locus or path traced by a moving point. If the direction of motion of the point is constant the locus is a straight line. In geometry when the term " line " is used it generally stands for " straight line." 2. The Circle — Definitions. — A circle is a plane figure contained by one line, which is called the circumference, and is such, that all straight lines drawn from a certain point within the figure to the circumference are equal to one another : and this point is called the centre of the circle. The meanings of the terms radius, dia- meter, chord, arc, sector, and segment of a circle are given in Fig. 1 . The term ''circle" is very frequently used when the " circumference " of the circle is meant. Euclid, for example, states that " one circle cannot cut another at more than two points." " A tangent to a circle is a straight line which meets the ference, but, being produced, does not cut it" (see also Art. 13 3. Angles. — " A plane angle is the inclination of two lines to one another, which m^et together, but are not in the same straight line." " When a straight line standing on another straight line makes the adjacent angles equal to one another, each of the angles is called a right angle." If it is required to test whether the angle BAG of a Fig. 1. circum- , p. 12). straight the set-square, which is nominally a right angle, i^ really a right 13 angle, PRACTIOAL GEOMETRY Fig. 2. apply the set-square to a straight-edge DE as shown in Fig. 2, and draw the line AB. Next turn the set-square over into the position AB'C and draw the line AB'. If AB' coin- cides with AB, then the angle BAG is equal to the angle BAG', and therefore by the definition each is a right angle. An angle which is less than a right angle is called an acute angle, and an angle which is greater than a right angle and less than two right angles is called an obtuse angle. If two angles together make up a right angle they are said to be complementary, and one is called the comple- ment of the other. If two angles together make up two right angles they are said to be supplementary, and one is called the supplement of the other. In measuring angles in practical geometry the unit angle is generally the l-90th part of a right angle and is called a degree. The l-60th part of a degree is called a minute, and the l-60th part of a minute is called a second. 47° 35' 23" is to be read 47 degrees, 35 minutes, 23 seconds. The single and double accents which denote minutes and seconds respectively are also used to denote feet and inches respectively, but this double use of these symbols seldom causes any collusion. Angles are also measured in circular measure. AOB (Fig. 3) is an angle, and AB is an arc of a circle whose centre is O. The circular measure of the angle AOB is the ratio = 6. For two right angles the length of the 3-1416, and the circular measure When arc RADIUS A Fig. 3. radius arc is ttt, where tt of two right angles is therefore equal to tt. the arc is equal to the radius the angle is the unit angle in circular measure and is called a radian. If « is the number of degrees in an angle whose circular measure n 6 . is $ radians, then y^Q = -, since each of these is the fraction which the angle is of two right angles. 180<9 Hence n = = 57-2958^, and 6 = 180 = 0-01745W. The instrument most commonly used for measuring angles in degrees is the protractor, portions of two forms of which are shown in Fig. 4. The angle AOB on the paper beneath the protractor is seen to be 55°. The protractor may be made of boxwood, ivory, celluloid, or cardboard. Fig. 4. INTRODUCTORY SCALE OF CHORDS Fig. 5. A scale of chords is a convenient instrument for measuring angles. The way in which the scale is constructed is shown in Fig. 5. ADF is a right angle, and the arc ACF is de- scribed from the centre D. The arc ACF is shown divided into 18 equal parts, each part therefore subtends at D an angle of 5°. On the scale of chords AB, lengths are marked off from A equal to the chords of the arcs of the different angles. For ex- ample, AE is the chord of the arc which subtends an angle ADE of 40"^ at the centre D, and this length is marked off on AB by describing the arc EH from the centre A. It will be found that the length of the chord AC for 60° is equal to the radius of the arc ACF Hence in using the scale of chords the radius of the arc is made equal to the distance between the points marked and 60. The scale shown in Fig. 5 only shows the chords for angles which are multiples of 5° up to 90°, but by making the scale large enough, single degrees, and even fractions of a degree, may be shown. It may also be extended beyond 90°. But when an angle is greater than 90° its supplement, which will be less than 90°, should first be determined. It should be noticed that the divisions on the scale of chords are unequal. By using the ordinary 45° and 60° set-squares separately and together angles which are multiples of 15° may be constructed with i^reat accuracy. Angles may also be measured and constructed by making linear measurements taken from tables of the trigonometrical ratios of angles. 4. Trigonometrical Ratios of Angles. — The angle A in the diagrams, Fig. 6, is contained by the lines OP and OX. The line OP is supposed to start from the position OX and sweep out the angle A by moving round O as centre in the direction opposite to that of the hands of a watch. An angle so described is called a positive angle. If the motion takes place in the opposite direction the angle described is called a negative angle. PN is perpendicular to OX. PN is positive (-f ) when it is above 4 PRACTICAL GEOMETRY OX, and negative (~) when it is below OX. ON is positive when it is to the right of O, and negative when it is to the left of O. OP is always positive. The most important trigonometrical ratios of an angle are, the smcj the cosine^ the tangent^ and the cotangent. The sine of the angle A is the ratio of PN to OP. Thus, sine A = ^. If PN is half of OP, then sine A = i If PN = 2, and OP = 3, then, sine A = |. ' ON A I'N The other important ratios are, cosine A = ^yp , tangent A = qv^> . * ON and cotangent A = pv^. In addition to the above the following ratios are also used : cosecant A = p^, secant A = -^^^ co versed sine A = 1 — sine A, and versed sine A = 1 — cosine A. The names of these ratios are abbreviated as follows : sin, cos, tan, cot, cosec, sec, covers, and vers. The following results are obvious from the definitions : — cot A = r A , tan A = -— — . , cosec A = , — - , sec A = . tan A cot A sm A cos A The complement of A is 90^ — A, and the supplement of A is 180^ - A. The following relations between the trigonometrical ratios of an angle and those of its complement and supplement are easily proved :— sin (90^ - A) = cos A. cos (90° - A) = sin A. tan (90° - A) = cot A. cot (90° - A) = tan A. sin (180° - A) = sin A. cos (180° - A) = - cos A. ■ tan (180° - A) = - tan A. cot (180° - A) = - cot A. It may be noticed that the sine and cosine of an angle can never be greater than 1, but the tangent and cotangent can have any magnitudes. The problem of constructing an angle which has a given trigono- metrical ratio evidently resolves itself into the simple one of con- structing the right-angled triangle OPN (Fig. 6) having given the ratio of one side to another. But in general there are two angles less than 360° which have a given trigonometrical ratio. 5. Accuracy in Drawing. — A good serviceable line by an ordinary draughtsman is about 0*005 inch wide, but an expert draughtsman can work with a line of half that width. A good exercise for the student is to try how many separate parallel lines he can draw between two parallel lines which are 02 inch apart, as shown in Fig. 7, which is twice full size for the sake of clearness. When the lines are drawn as close as possible together, but distinctly separate, it will be found that the distance between them is about equal to the width of the lines. Hence, if the lines and spaces are about 005 inch wide, there will be about 20 lines in a width of 02 inch. The probable error in measuring the distance between two points INTRODUCTORY on a straight line may be as small as the thickness of the division lines on the measuring scale, or say O'OOo inch. The error e in the position of the point of intersection of two straight lines OA and OB (Fig. 8), when the error in the lateral posi- tion of one of them is iT, IS ~. — ;;, where sin 6 is the angle between when 6 = V, e = 0-057 = 10^ Using a radius of 10 inches, an angle may be constructed by marking off the chord from a table of chords with a minimum probable error of from 1-lOth to I- loth of a degree. Great accuracy in drawing can only be obtained by exercising great care, and by having the best instruments kept in the best possible condition. Fig. 8. the lines. If a; = 0*005 inch, e = 0-286 inch inch when = 5°, and e = 0029 inch when inches, an angle Exercises Ta To test accuracy in drawing ayid measuring 1. On a straight line about 7 inches long mark a point near one end. ]\Iark off the following lengths on this line : OA = 1-20 inches, AB = 0-85 inch, BC = 1-35 inches, CD = 1-55 inches, and DE = 0*95 inch, all measured in the same direction along the line. Measure the length OE, which should be 5-90 inches. 2. Take twenty strips of paper about 2J inches long, and number them 1 to 20. On an edge of No. 1 mark off a length of 2 inches. On an edge of No. 2 mark off the length from No. 1. On an edge from No. 3 mark off the length from No. 2, and so on to No. 20. Then compare the length on No. 20 with the length on No. 1. 3. Draw a straight line AB (Fig. 9) and mark two points A and B on it 2 inches apart. Draw BC, making the angle ABC = 60°. Make BC 4 inches long. Draw CD, making the angle BCD = 30°. Make CD = CA. Draw DE parallel to AB. Make DE 4 inches long. Draw EF, making the angle DEF = 30°. Make EF = CA. Let DE cut BC at 0. A circle with centre and radius OB should pass through the points D, F, C, E, and A. Also the chords of the arcs BD, DF, FC, CE, and EA should each be 2 inches long. _ 4. On a straight line AB (Fig. 10) 2 inches long construct an equilateral triangle ABC, using the 60° set-square. Produce the sides of this triangle as shown. Through the angular points of the triangle ABC draw parallels to the opposite sides forming the triangle DEF. Using the 30° and 90° angles of the set-square, draw lines through D, E, and F, to form the hexagon DHEKFL as Fig. 9. PRACTICAL GEOMETRY shown. Join FA, EB, and DC. If these lines are produced, they should pass through the points H, L, and K, respectively. Complete the figure by drawing the circles as shown. 5. Draw two lines OA, OA, each 10 inches long, and containing an angle AOA of 88°. Measure accu- rately and state the distance apart of A, A. What should be the exact distance AA ? State any special precautions you may have taken to ensure accuracy in your construc- tion. [B.E.] 6. Take from the tables the chord and tangent of 22°. Construct an angle of 22° by using the value of the chord, and a second angle of 22° by using the tangent. From each of these angles determine the sine of 22°, and compare the mean of the two values with the true value of sine 22°. [b.e.] 7. By aid of your protractor, and without using the tables, find the value of sin 23° + tan 23° + cos 23°. Now take out the true values of the sine, tangent, and cosine from the tables, add them, and calculate the percentage error in your first answer. [b.e.] 8. In working this question employ a decimal scale of ^ inch to 1 unit. Draw a circular arc, radius 10 units, centre 0. Mark a chord AB of this arc 347 units long, and draw the radii OA, OB. Measure the angle AOB in degrees. From B draw a perpendicular BM on OA, and at A draw a tangent to meet OB produced in N. Measure carefully B]\I, AN and the arc AB (on the above unit scale) and calculate the sine and tangent of the angle, and the angle in radians. Give the correct answers for the degrees, sine, tangent, and radians, the numbers being taken directly from the tables. [b.e.] 9. On the base AB (Fig. 11) construct the polygon ABCDEF to the dimensions given. Then mea- sure the side AF and the angles 6 and ' he cd da way, the similar figures have the same sha^pe but have different dimensions. When the two figures are triangles, they are similar if the angles of the one are equal to the angles of the other, each to each. The equality of the ratios of the sides about the equal angles follows as a consequence of the equality of the angles. It is important to remember that the ratio of the areas of two similar figures is equal to the ratio of the squares on their correspond • ing sides. For example, referring to Fig. 18, area of ABCD : area of ahcd : : AB^ : ah^ 11. Through a given point to draw a straight line which shall be concurrent with two given straight lines when the point of concurrence is inaccessible. — AB and CD (Fig. 19) are the given lines, and P is the given point. Draw a triangle PEF having one angular point at P and the other angular points one on AB and one on CD. Draw HK parallel to EF, meeting AB at H and CD at K. Througji H and K draw parallels to EP and FP respectively, and let them 10 PRACTICAL GEOMETRY meet at Q. A straight line through P and Q will, if produced, meet AB and CD produced at the same point. 12. Graphic Arithmetic. — The solution of ordinary arithmetical problems by geometrical constructions is of some interest when con- sidered as a section of practical geometry, but graphic arithmetic, when regarded as a means to an end, is in general a poor substitute for the ordinary method by calculation. The subject of graphic arithmetic will therefore be treated somewhat briefly here. Bepresentation of niimhers by lines. If the line AB, Fig. 20 (a), be taken to represent the number owe, then a line CD n times the length of AB will represent the number n. Again, if AB represents the number owe, the number represented by the line EF will be the number of times that EF contains AB. In the above examples AB is called the unit. Ordinary drawing scales may be used in marking off or measuring lengths which represent numbers. Scales which are decimally divided are the most convenient for this work. Addition and sidHraction. To add a series of numbers together. Draw a straight line OX, Fig. 20 (b), of indefinite length. Fix upon a unit, that is, decide what length shall represent the number owe. Mark a definite point O on OX. Make OA = the first number, AB = the second number, BC = the third number, and so on. From O to the last point determined in this way will be the answer required. t W^ X — S 1 (aH £ i (J k — ; i' n — s r—^ (d)—^ i i X g 6 X Fig. 20. From one number to subtract another. Make OA, Fig. 20 (c), measured to the right of O, equal to the first number. Make AB, measured to the left of A, equal to the second number which is to be subtracted from the first. From O to B is the answer required. If OB is to the right of the answer is positive ( + ), and if OB is to the left of O, the answer is negative ( — )• To find the value of such an expression as a-\-b — c + d — e., where a, ?>, c, d, and e represent numbers, make (Fig. 20 (d)) OA = a, AB = 5, BC = c, CD = d, and DE = e, then 0Y. = a -^b - c + d - e. Note that in adding the lengths are measured to the right, while in subtracting they are measured to the left. Proportion. In Figs. 21 and 22, OX and OY are two straight lines making any convenient angle with one another. AB and CD are parallel lines meeting OX at A and C, and OY at B and D. The triangles AOB and COD are similar, and therefore OA : OB : : OC : OD, INTRODUCTORY H and if any three of the terms of this proportion are known the fi£?ure can be drawn and the fourth term found. Arithmetical, Geometrical, and Harmonical means of two numbers. Let M and N be two numbers. On a straight line AB (Fig. 23) make AO = M and OB = N. Bisect AB at C. With centre C and radius CA describe the semicircle ADB. Draw OD at right angles to AB. Join CD. Draw OE at right angles to CD. Then CB = arithmetical mean of M and N = i(M + N), OD = geometrical mean of M and N = VM x N, 2M X N DE = harmonic mean of M and N = ^>— r ^t . M + N OD, the geometrical mean of M and N, is also called a mean pro- portional between M and N. If OD = \/M~x^, then OD" = M x N, and M : OD : : OD : N. Multiplication. In Eigs. 21 and 22, since OA : OB : : OC : OD, it follows that OA X OD = OB X OC. Make OB equal to the unit, then OA X OD = 1 X OC = OC. Hence the construction for finding the product of two numbers. Make OA = one of the numbers, OD = the other number, and OB = the unit. Join AB, and draw DC parallel to BA, then OC is the answer. If the given numbers are large, it is better to first divide them by- some power of 10 so as to avoid using a very small unit. For example, let it be required to find 485 X 363. Taking the unit as 1 inch find the product x of 4-85 and 3-63, then 485 x 363 = 4-85 x 3-63 x 10,000 = 10,000a;. After the value of x has been found, 10,000a; is found by simply changing the position of the decimal point. Division. In Figs. 21 and 22, since OA : OB : : OC : OD, it follows that QT^= QTj. Make OB = the unit, then oD~ ^ = ^-^- Hence the construction for finding the quotient of one number divided by another. Make OC = the dividend, OD = the divisor, and OB = the unit. Join CD, and draw BA parallel to DC, then OA is the answer. Square r oot. In Fig. 23, OD^ = OA X OB, therefore OD = VOA X OB. Hence if OB is made equal to the unit, OD = VOA. If the given number is a large one it is better to make OB = « times the unit, and OA = - of the given number, where w is a con- n venient whole number. For example, to find the square root of 48, 12 PRACTICAL GEOMETRY of etc., may be obtained by make O B = 10 times the unit and OA = 4*8 times tiie unit, then 0D=: v/4-8 X I0= Vis, If a be the hypotenuse of a right-angled triangle (Fig. 24) which h and c are the sides, then a- = W + c^ therefore a = V?>M- also c^ = d- - 6^ therefore c = ^/ai' — lr. Involution. The values of a^ d\ «^ multiplication as already explained. For a? =z a X a = h, and a" = a'- x a = ^ X a. The following construction is, however, sometimes more convenient. Draw two axes XOXi and YOY^ (Fig. 25) at right angles to one another. Make OA = the unit, and OAj = «, the given number. Join A^A and draw AjAo at right angles toAjA. Then OA2 = (T. Draw A2A0 at right angles to A^A,. Then OA3 = a'. Draw A3 A 4 at right angles to AgA^. Then OA4 = a^, and so on. If AA'i be drawn at right angles to AAj, and A'^A'a be drawn at right angles to AA\, and so on, then 0A\ = - , OA'o = .; OA'3 = "3 and so on. 13. Definitions relating to CuvweB.— Tangent and Normal. If a straight line PQ (Fig. 26) cuts a curve at two points P and Q. and if the straight line be turned about the point P so as to cause the point Q to approach nearer and nearer to P, then the ultimate position of the straight line is the tangent to the curve at P. The normal to the curve at P is a straight line through P at right angles to the tangent to the curve at P. A good practical method of drawing a tangent to a curve from an external point T (Fig. 26) may be given here. Place a straight-edge on the paper and adjust it until the edge passes through T and touches the curve, then draw the tangent. This method would not be recognized by the mathematician, but as a practical method it is as good as any p other, and much simpler. The exact point of contact must be obtained by some other construction depending on the nature of the curve. Circle of Curvature. If a circle be drawn through three points Q, P, and R in a curve APB (Fig. 27), and if the ^^«' ^'^^ points Q and R be moved so as to approach nearer and nearer to P, then in the limit the circle becomes the circle of curvature of the curve APB at P. The centre of the circle of curvature will evidently lie on INTRODUCTORY 13 curve. Fig. 28. and a curve is an the normal to the curve at P. The centre of the circle of curvature is called the centre of curvature, and the radius of the circle of curvature is called the radius of curvature. Evolute and Involute. The locus of the centre of curvature of a curve is called the evolute of the A curve has only one evolute. The locus of a point on a straight line which rolls Without sliding on a curve is called an involute of the curve. A curve has any number of involutes. In Fig. 28, ABC is a curve and abc is its evolute. Again, abc is a curve and ABC is an involute of ahc. The curves PQR and STU are also involutes of abc. A curve is the evolute of each of its involutes involute of its evolute. The normals to a curve are tangents to its evolute, and the tangents to a curve are normals to its involutes. Envelope. If a curve moves in a definite manner the curve which it always touches is the envelope of the moving curve. Fig. 29 shows the en- velope of a circle which moves so that its centre traces the curve ABC. The evolute of a curve is also the envelope of the normal to the curve. Cusp. If two branches BA and CA of a curve (Fig. 30) terminate at a point A on a common tangent AD, the terminating point A is called a cusp. There are two kinds of cusps ; in the first kind the branches of the curve are on opposite sides of the common tangent, and in the second kind the two branches of the curve are on the same side of the com- mon tangent. Node or Multiple Point. A point branches of a curve pass is called a node or multiple point. The node shown at (a), Fig. 31, is a double point, and the node shown at (6) is a triple point. At the node (a) two tangents can be drawn to the curve. At the node {b) three tangents can be drawn to the curve. Point of Inflexion. If the tangent "^ to a curve at a point also cuts or crosses the curve at that point (Fig. 32), then thtf point is appoint of inflexion. Asymptotes. When a curve approaches nearer and nearer to a through which two or more (I). 14 PRACTICAL GEOMETRY Fig. 32. straight line, but never actually meets the line however far the line and curve be continued, the line and curve are said to be asympioticj and the line is called an asymptote to the curve. Curves which approach nearer and nearer to one another but never actually meet however far they are continued are said to be asymptotic, and each curve is an asymptote to the other. Similar Curves. Two curves, PQ and PjQj (Fig. 33), are said to be similar when any radius vectors (or radii) OP, OQ in the one, drawn from a fixed point O, bear the same ratio to one another that radius vectors O^Pj, OiQi drawn from a fixed point O^, and including the same angle 0, bear to one another. If, in addition to fulfilling the above conditions, OP and OQ are parallel to O^P^ and OjQ^ respectively, then the curves are said to be similar, and similarly situated. The fixed points O and O^ are called centres of similarity, and when these centres coincide the point is called a centre of similitude of the two curves. All conies having the same eccentricity are similar curves. Fig. 33. Draw a straight line Exercises lb X 1. Draw Fig. 34 full size to the dimensions given bisecting the angle between AB and CD, and through the points P and Q draw straight lines concurrent with AB and CD without using the point of concurrence. 2. From the points P and Q (Fig. 34) draw two straight lines to meet on the line passing through A and the middle point of CD and be equally inclined to that line. 3. If a line 3^ inches long represents 26, what does a line 1{^ inches long repre- sent, and what is the unit ? If a line If^ inches long represents If, what is the unit ? 4. Work the following exercises, taking for the unit in each case a line ^ inch PiG. 34. long : - (a) 1^ + 1-^ + 5-11+21. (c) 2-4 + 0-8 - 1-9 - 2 + 4-2 - 1-6. (6) 1-5 - 2 + 3 - 4 + 3-5. (d) ^^ + \l - 1^ + § - 21. 5. Taking a line 1^ inches long to represent the area of a square of 1 inch side, determine a line which shall represent the area of a rectangle 2>J inches long and I inch broad. 6. A is a line 1| inches long, and B is a line 2,'8 inches long. Determine a line which will represent the product of A and B, the unit being a line 1^ inches long. 7. A is a line 2^ inches long, B is a line 1^^, inches long, and C is a line \l inch long. If A represents the product of B and C, draw a line which will represent the product of A and C. INTRODUCTORY 15 8. Find a line representing the volume of a rectangular solid whose dimensions are 3 inches x 1"75 inches x 1*25 inches. Unit = 0*5 inch. 9. The unit being a line 1 inch long, find a line to represent the cube of 1-25. 10. M and N are straight lines 1*25 inches and 1-5 inches long respectively, M 4- N Find a line representing ^ — r;^, the unit being 1 inch. ,__ 20 11. Draw lines representmg V15 and 7/ y^. Unit = 0*25 inch. 12. Find a line to represent cc^ when x = 2V2 - /v/3. Unit one inch. 13. A, B, C, and D are lines 3fg inches, 2^ inches, 2f inches, and 1/g inches A X B long respectively. If ^^ ^ = C, find the unit. I'l /2"3^ 14. Using as unit a length of 1 inch, find a line to represent o.q\/ y^r 32 + 1-42 102" CHAPTER II THE CIRCLE 14. Properties of the Circle— Simple Problems.— (1) In a segment ABGD of a circle (Fig. 35) the angle AOD at the centre is double of the angle ABB at the circumference. (2) Angles ABB and ACD in the same segment of a circle (Fig. 35) are equal to one another. (3) The angle in a semicircle is a right angle. The carpenter, in cutting a semicircular groove in a piece of wood, makes use of this property when he tests it with a square, as shown in Fig. 36. Fig. 35. Fig. 36. Fig. 37. (4) A straight line lohich bisects a chord at right angles passes through the centre of the circle. This suggests a method of finding the centre of a circle to pass through three given points or to circumscribe a given triangle. To describe an arc of a circle through three given points, A, B, and C, when the centre of the circle is inaccessible (Fig. 37). With centres A and C describe arcs CH3 and ASK. Join AB and CB, and produce these lines to meet the arcs at H and K. Mark off short equal arcs HI and Kl. The intersection P of the lines Al, CI, is another point on the arc required. In like manner other points may be found, and a fair curve drawn through all of them is the arc required. The foregoing construction is based on the fact that the three angles of a triangle are together equal to 180°, and that the angles in the same segment of a circle are equal to one another ; also that in equal circles equal arcs subtend equal angles at their centres. The student should have no difficulty in showing that the construction makes the angle APC equal to the angle ABC. For another method see Art. 59, p. 56. THE CIRCLE 17 • (5) A tangent to a circle is at right angles to the radius or diameter drawn to the j)oint of contact. To draw a tangent to a circle from an external point. A good practical method is to place a straight-edge on the paper and adjust it so that the edge passes through the point and touches the circle, then the tangent may be drawn. The point of contact must, however, be obtained by dropping a perpendicular from the centre of the circle to the tangent. The following construction is recommended when the one just given is objected to. With P (Fig. 38), the given external point as centre, describe the arc OSR, passing through O the centre of the given circle. With centre O and radius equal to the diameter of the circle describe an arc to cut the arc OSR at R. Draw OR cutting the circle at T. PT is the tangent required and T is the point of contact. The student should satisfy himself that this construction makes the angle OTP a right angle. ^^^' ^^■ Another method is to describe a semicircle on OP as diameter, to cut the given circje at T, which will be the point of contact of the tangent required. In this case the angle OTP is obviously a right angle because it is the angle in a semicircle. It is obvious that two tangents may be drawn to a circle from an external point, and that they are equal in length. To draw a tangent to two given circles. This may be done very accurately by placing a straight-edge on the paper, adjusting it so that the edge touches the circles, and then drawing the tangent. The points of contact must however be obtained by dropping perpendiculars from the centres of the circles to the tangent. When the preceding construction is objected to, the following may be used : A and B (Figs. 39 and 40) are the centres of the given circles. Join AB cutting the circles at C and D. Make DE equal to BC. Draw / Fig. 39 a circle with centre A and radius AE. Draw BF a tangent to this circle, F being the point of contact. Draw the line AF meeting the given circle, whose centre is A, at H. In Fig. 39, H is on AF produced. Draw BK parallel to AH, meeting the circle whose centre is B, at K. C 18 PRACTICAL GEOMETRY The straight line joining H and K is a tangent to both the given circles, and H and K are the points of contact. If the circles lie outside of one another four common tangents may be drawn to them. (6) The angle ABC (Fig. 41) between the chord AB and the tangent BC to the circle at B is equal to the angle ADB in the alternate segment. To inscribe in a circle ABD (Fig. 41) a triangle equiangular to the triangle EFH. Draw the tangent KBC. Draw the chord AB, making the angle ABC equal to the angle F. Draw the chord DB, making the angle DBK equal to the angle H. Join AD. The triangle ABD is the triangle required. ^^ -' ^- ^ Fig. 43. On a given line ^5 (Figs. 42 and 43) to describe a segment of a circle itlltich shall contain an angle equal to a given angle G. Draw AD, making the angle DAB equal to the angle C. Draw AO at right angles to AD. Bisect AB at E. Draw EO at right angles to AB, meeting AO at O. O is the centre, and OA is the radius of the circle of which the segment AFB contains an angle equal to the angle C. (7) In a quadrilateral ABOD (Fig. 44) inscribed in a circle the opjwsite angles ABC and ADC are together equal to two right angles. Also the other pair of opposite angles are together equal to two right angles. (8) In Fig. 44 AC X BD = AB X CD 4- AD X BC. (9) AC and BD are any two chords of a circle intersecting at F. AF x CF = BF x DF. In Fig. 44 the point F is within the circle, but it may be outside the circle. (10) EH is a tangent to the circle ABCD (Fig. 44), H being the point of contact. EKL is a line cutting the circle at K and L. M^ = EK X EL. To draw a tangent to a given arc of a circle, through a given point, without using the centre of the circle. Fig. 45. The given point P is on the given arc APB but not near Fig. 44. THE CIRCLE 19 either of its extremities. With centre P describe arcs of a circle to cut the given arc at A and B. A line through P parallel to the chord AB is the tangent required. Let C be the middle point of the chord AB. If d is the diameter of the circle of which APB is^n arc, then PC (d - PC) = AC x CB = BC^. ^ BC^-fPC^ PB2 ^, , Hence d = — p^ = p^. The lengths of PB and PC may be measured and d found by arithmetic. t Fig, 45. Fig. 46. Fig. 46. The given point Q is on the given arc and near one of its extremities. Draw chords QP and QB. Join PB. Draw QE making the angle PQE equal to the angle PBQ. QE is the tangent required. Fig. 47. The given point S is outside the given are. Draw the line SAB cutting the arc at A and B Find a length / such Fig. 47. that /•' = SA.SB (see Art. 12, p. 11). With S as centre and radius equal to /, describe an arc of a circle to cut the given arc at T. A line ST is the tangent required and T is the point of contact. 15. To construct a triangle having given the base, the vertical angle, and the length of the bisector of the vertical angle. — First method (Fig. 48). On AB the given base describe a Fig. 48. Fig. 49. segment of a circle ACB containing an angle equal to the given vertical angle. From O the centre of this circle draw OF at right angles to AB and produce it to meet the circle at D. On any straight line make ce equal to the given length of the bisector of the vertical angle. Bisect ce at g. Draw eh at right angles to ce and make eh equal the chord DB. With centre g and radius gh describe an arc of a circle to cut ce produced at d. With centre D and radius equal to 20 PRACTICAL GEOMETRY dc describe an arc of a circle to cut the circle ACB at C. Join AC and BC. ACB is the triangle required. The construction for finding the length of DC is based on the fact that DC X DE = DBl Second method (Fig. 49). Determine the circle ACB and the point D as in the first solution. Through D draw a straight line DQP cutting AB at Q. Make QP equal to the given length of the bisector of the vertical angle. Repeat this construction several times so as to determine a sufficient number of points on the locus of P. The inter- section of the locus of P and the circle ACB determines the vertex of the required triangle. This second method is a very good illustration of the use of a locus. It is quicker and probably more accurate and certainly much easier to discover. 16. To find the locus of a point which moves so that the ratio of its distances from two given points shall be equal to a given ratio. — Let A and B (Fig. 50) be the two given points, and let P be one position of the moving point so that the ratio of AP to BP is equal to a given ratio. In Fig. 50 this ratio is 2 : 1. Draw PD bisecting the angle APB and meeting AB at D. Draw PDi bisecting the angle between AP produced and BP. Bisect DDi at O. A circle with centre O and radius OD will be Fig. 50. the locus required. Draw BE parallel to PD to meet AP produced at E. Draw BEj parallel to PD^ to meet AP at E^. It is easy to show that PE = PE^ = PB. Also, AD : DB : : AP : PE, therefore AD : DB : : AP : PB, and D is a fixed point. Again, AD^ : D,B : : AP : PE„ therefore AD^ : D,B : : AP : PB, and Di is a fixed point. The angle DPD^ is obviously a right angle. Hence a circle described on DDj as diameter will pass through P. If the figure be rotated about ADj as an axis, the circle will describe the surface of a sphere, and the surface of this sphere will evidently be the locus of a point moving in space so that the ratio of its distances from the two fixed points A and B is equal to a given ratio. 17. The Inscribed and Escribed Circles of a Triangle.— The inscribed circle of a triangle is the one which touches each of the three sides. An escribed circle touches one side and tlie other two sides produced. There are three escribed circles to a triangle. The con- structions for drawing the inscribed and escribed circles are based on the fact, that when a circle touches each of two straight lines, its centre THE CIRCLE 21 lies on the line bisecting the angle between them. In Fig. 51, O is the centre of the inscribed circle of the triangle ABC, and Oj is the centre of one of the escribed circles. The following results are not difficult to prove : — (1) The sides of the triangle formed hy joining the centres of the escribed circles pass through the angular points of the original triangle. (2) The line joining the centre of one of the escribed circles and the opposite angle of the triangle passes through the centre of the inscribed circle and is perpen- dicular to the line joining the centres of the other two escribed circles. (3) Referring to Fig. 51, AE = AF = half the perimeter of the triangle ABC. This suggests the construction for the solution of the following problem. Given the perimeter ^ and one angle of a triangle, also the radius of the inscribed circle : to construct the triangle. Make the angle EAF (Fig. 51) equal to the given angle. Draw a circle having a radius equal to the given radius to touch AE and AF. This will be the inscribed circle of the required triangle. Make AE and AF each equal to half the given perimeter. From E and F draw perpendiculars to AE and AF respectively to meet at O^. A circle with O^ as centre and O^E or OjF as radius will be an escribed circle of the triangle. A tangent BC to the two circles now drawn will complete the triangle required. 18. Circles in Contact. — In considering problems on circles in contact with one another two simple facts should be kept in view, viz. (1) J Then two circles touch one another the straight line ichich joins their centres or that line produced passes through the point of contact. (2) When two circles touch one another the distance between their centres is equal to either the sum or difference of their radii. To draw a circle of given radius to touch two given circles. Three cases are shown in Figs. 52, 53, and 54. A and B are the centres of the given Fig. 53. Fig. 54. circles. AB or AB produced cuts the given circles at C and F. Make CD and FE each equal to the given radius. With centre A and radius AD draw the arc DO. With centre B and radius BE draw the arc The perimeter of a triangle is the sum of its sides. 22 PRACTICAL GEOMETRY Fig. 65. EO, cutting the former arc at O. Join O with A and B, and produce these lines if necessary to meet the given circles at H and K. O is the centre of the required circle, and H and K are the points of contact. 19. To draw a series of circles to touch one another and two given lines.- -AB and CD (Fig. 55) are the two given lines. Draw EF, bisecting the angle between AB and CD. Let E be the centre of one circle : its radius is EA, the perpendicular on AB from E. Draw HK perpendicular to EF. Make KL equal to KH. Draw LM perpendicular to AB to meet EF at M. M is the centre and ML is the radius of the next circle. 20. To draw a circle to pass through a given point and touch two given lines. — AB and AC (Fig. 56) are the two given lines and D is the given point. Draw AE bisecting the angle BAC. Join AD. Take any point F in AE. Draw FH perpendicular to AB. With F as centre and FH as radius describe a circle. This circle will touch the lines AB and AC. Let this circle cut AD at K. Draw DO parallel to KF, meeting AE at O. O is the centre and OD the radius of the circle required. 21. To draw a circle to touch two given lines and a given circle. — AB and CD (Fig. 57) are the given ^ lines and EF is the given circle, N being its centre. Draw HK and LM parallel to AB and CD respectively, and at distances from them equal to the radius EN of the given circle. Draw, by preceding problem, a circle to pass through N, and touch the lines HK and LM. O the centre of this circle is the centre of the circle required, and OE is its radius, OEN being a straight line. 22. To draw a circle to touch a through two given points. — AB (Fig. 58) is the given line, and C and D are the given points. Draw CD and produce it to meet AB at E. If the required circle touches AB at K, then EK^ = ED x EC, or EK must be a mean proportional to EC and ED. Hence the following con- struction. Produce CE and make EF equal to ED. On CF describe a semi- circle. Draw EH perpendicular to CF to meet the semicircle at H. Make EK equal to EH. Draw KO perpendicular to AB, and draw LO, bisecting CD at right angles to meet KO at O. O is the centre of the circle re, and r.^ be their radii respec- tively, and let r^ be the radius which is not greater than r.^ or r.j. With centre B and radius equal to ^g — r^ describe the circle DE. With centre C and radius equal to r., 4- 9\ describe the circle FPH. Draw the circle APL which touches the circle DE with internal con- tact, and the circle EPH with external contact and passes through the point A (Art. 30). O, the centre of this circle, is the centre of the required circle, and ON is its radius. The points of contact „ with the given circles are M, K, and N. The construction obviously makes AM, PN, and LK equal to one another. A second solution is obtained in the same way by making the circle APL touch the circle DE with external contact, and the circle FPH with internal contact. Two solutions are obtained by making the radius of the circle DE equal to r.^ -f r^ and the radius of the circle FPH equal to r., — r^. Two solutions are obtained by making the radius of the circle DE equal to r.^ — r^, and the radius of the circle FPH equal to r.^ — 7\ ; but for these solutions the circle APL must have either internal or external contact with both of the circles DE and FPH. The remaining two solutions are obtained in the same way as the previous two except that the radii of the circles DE and FPH are r., + rj and r.^ -f- r^ respectively. Remembering that a straight line is a circle of infinite radius, the method illustrated by Fig. 70 may be easily modified to draw a circle to touch a given line and two given circles, or two given lines and a circle. Exercises II Note. The points of contact of circles which touch one another, and the points of contact of tangents to circles, must he shown distinctly. 1. ABC is a triangle. AC = 1'7 inches. BC = 1 inch. Angle C = 90°. Draw the circle which touches AC at A and passes through B. 2. A line OA, I'b inches long, is a radius of a circle whose centre is 0. AB is a line 2-2 inches long making an angle of 120° with OA. Draw the circle which touches the given circle at A and passes through B. 3. On a straight line 3-5 inches long describe a segment of a circle to contain an angle of 150° without using the centre of the circle. 4. In a circle 3 inches in diameter inscribe a triangle whose angles are to one another as 2 : 3 : 4. 5. Draw an arc of'a circle of 6 inches radius, the chord of the arc being 4 inches long. Then draw the arc of a circle concentric with the first and of 7 inches radius without using the centre. The two arcs are to subtend the same angle at the common centre. 28 PRACTICAL GEOMETRY 6. OA and OL are two straight lines. Angle AOL = 80°. OA = 2-5 inches. OL is of indefinite length. B is a point in OA. OB = 1 inch. Find a point P in OL such that the angle APB is the greatest possible. 7. The centres of two circles are 1-75 inches apart. The radius of one is 1*2 inches, and the radius of the other is 0-9 inch. P is one of the points of intersec- tion of the circles. It is required to draw two straight lines APB and CPD, 3 inches long, and terminated by the circles. [Hmt. If Q is the middle point of AP, and R is the middle point of BP, then QR is half of AB.] 8. From a point 2-2 inches distant from the centre of a circle of 1 inch radius draw a straight line to cut the circle so that the part of it within the circle shall be 1 inch long. 9. Two straight lines include an angle of 60°. Draw a circle 3 inches in diameter, cutting one of the lines at points 1*7 inches apart, and the other at points 2-3 inches apart. 10. The centres of two circles are 3 inches apart. Thh radius of one is 0*6 inch, and the radius of the other is I"! inches. Draw the four common tangents to these circles. 11. In a circle 3 inches in diameter draw a chord dividing the circle into two segments, one of which shall contain an angle of 65°. In the smaller segment inscribe a circle ^ inch in diameter, and in thje larger inscribe a circle which shall pass through the centre of the original circle. 12. ABC is a triangle. AB = 2 inches. BC = 1'75 inches. CA = 1*5 inches. Draw the inscribed and escribed circles of this triangle. 13. Draw a sector of a circle. Radius of circle, 2 inches. Angle of sector, 60°. In this sector inscribe a circle. 14. In a circle 4 inches in diameter draw eight equal circles, each one to touch the original circle and two of the others. 15. Draw an equilateral triangle of 3 inches side and in it place three equal circles, each one touching one side of the triangle and the other two circles. 16. The vertical angle of a triangle is 50°, its altitude is 1*5 inches, and its perimeter is 6*75 inches. Construct the triangle. 17. AB (Fig. 71) is an arc of a circle of 2 inches radius circle of 1-75 inches radius. The centres of these circles are 1*25 inches apart. ADC is an arc of a circle of 0-625 inch radius which touches the arcs AB and BC. Draw the figure ABCD. IS. Draw a triangle ABC. AB = 3 inches. BC = 2-5 inches. CA = 2 inches. Draw a circle of 1 inch radius to touch the side AB and pass thro-ugh the point C. 19. Draw two circles having their centres 3 inches apart, one circle (A) to be 2 inches, and the diameter of the other (B) to be 3 inches. Draw a circle (C), 4 inches in diameter, to touch the circles A and B so that A is inside, and B outside C. 20. Within a circle 3 inches in diameter draw another, 1-8 inches in diameter, touching it. Next draw a third circle, 1 inch in diameter, inside the first circle, outside the second, and touching both. Then draw a circle to pass through the centre of the second circle, touch the first circle internally, and the third externally. 21. The section of a hand-rail is shown in Fig. 72. Draw this figure to the given dimen- sions, which are in millimetres. Show the con- structions by which the centres of the circular arcs are determined and mark the junctions of the arcs. [b.e.] 22. ABC is a triangle. AB = 1*5 inches. BC = 1-4 inches. CA = 1 inch. C is the centre of a circle of 1*6 inches radius. Draw two circles to touch this circle and pass through the points A and B. 23. Draw the locus of the centre of a circle which touches a fixed circle of BC is an arc of a A C -B Fig. 71. The diameter of H 58 ■ • Fig. 72. ^"^ THE CIRCLE 29 dla^ Fig. 73. 1 incli radius and passes through a fixed point 2 inches distant from the centre of the fixed circle. 24. AB, 2 inches long, is a diameter of the circle ACB (Fig. 73). BDE is an arc of a circle of 4 inches radius which touches the circle ACB at B. AE is at right angles to AB. Draw the figure ACBDE and add the circle F which touches the circle ACB, the arc BDE and the straight line AE. 25. Draw a circle 2*5 inches in diameter, and take a point P at a distance of 2*25 inches from its centre. From P draw a tangent to the circle and determine the exact point of contact, using a pencil and straight-edge only. 26. LjNI is a straight line of indefinite length, A and B are two points which are 2 inches apart and are on the same side of LM. The perpendicular distances of A and B from LM are 1 inch and 1-5 inches respectively. B is the centre of a circle of 0*75 inch radius. Draw the two circles which have their centres on LM, pass through A, and touch the circle whose centre is B. 27. The polar of a point P with respect to a circle 2-75 inches in diameter is a straight line at a perpendicular distance of 0*75 inch from its centre. Determine the position of the point P, using a pencil and straight-edge only. 28. Draw three circles and find the centres of similitude of each pair. Then show by using a straight-edge that the line joining any two of the six centres of similitude either passes through a third or through the centres of two of the circles. 29. ABC is a triangle. AB = 3 inches. BC = 4 inches. CA = 3-5 inches. A, B, and C are the centres of three circles whose radii are 1 inch, 1-25 inches, and 2 inches respectively. Find the radical centre of the three circles, and draw the circle which cuts the three circles orthogonally. 30. Draw all the circles which touch each of the three circles given in the preceding exercise. CHAPTEK III CONIC SECTIONS 32. The Conic Sections. — The curves known as the conic sections or conies are, the ellipse^ the hyperbola, and the parabola. They are plane curves, and they may be defined with reference to their properties as plane figures, or they may be defined with reference to the cone of which they are plane sections. 33. Conies defined without Reference to the Cone. — If F (Fig. 74) is a fixed point and XM a fixed straight line, and if a point P move in the plane containing F and XM in such a manner that the distance FP always bears the same ratio to the perpendicular PM to the fixed line, then the curve traced out by the point P is called a conic section or conic. The fixed point F is called the focus, and the fixed straight line XM is called the directrix of the conic. A straight line through the focus at right angles to the directrix is called the axis, and the point A where the axis cuts the curve is called the vertex of Fig. 74. the conic. P being any point on the curve, the constant ratio of FP to PM is called the eccentricity of the conic. AVhen FP is less than PM the conic is an ellipse. When FP is equal to PM the conic is a parabola. When FP is greater than PM the conic is an hyperbola. A conic is therefore an ellipse, a parabola, or an hyperbola according as the eccentricity is less than, equal to, or greater than unity. 34. To construct a Conic having given the Focus, Directrix, and Eccentricity. — In Fig. 75, F is the given focus and XM the given directrix. Take a point D on the axis, and draw DE perpendicular to XD, and of such a length that DE : XT) is equal to the given eccentricity. For example, if the eccentricity is 2 : 3 or jf, make XI) equal to 3 to any scale, and make DE equal to 2 to the same scale. Join XE. Draw any straight line N?i parallel to the given directrix XM, cutting XE at n. With centre F and radius equal to Nn describe arcs of a circle to cut wN and mN produced at P and P. P, P are points on the required conic. In like manner any number of CONIC SECTIONS 31 points may be determined, and a fair curve drawn through them is the conic required. It is obvious that the ratio of Nw to XN is the same as the ratio of DE to XD, and therefore the ratio of FP to PM is the same as the ratio of DE to XD which was made equal to the given eccentricity. The line XE will touch the conic at a point R obtained by drawing FR perpendicular to the axis to meet XE at R. Fig. 75. In Fig. 75, three different cases are shown. In the ellipse the eccentricity is 1:^3, in the parabola the eccentricity is of course 1 : 1, and iri the hyperbola the eccentricity is ^3:1. These eccentricities make the angle DXE equal to 30^ for the ellipse, 45 for the parabola, and 60° for the hyperbola. It is obviouslv unnecessary to draw the line XE in the case of the parabola. The radius for the arc through P may be taken at once from XN in this case, but it is instructive to notice that the construction given applies to all the conies. . If lines FY and FYi be drawn making 45° with the axis and 32 PRACTICAL GEOMETRY meeting XE at Y and Y^, then perpendiculars from Y and Yj to the axis determine the points A and A^ where the conic cuts the axis. In the case of the parabola there is only one such point, or to put it in another way, the point A^ for the parabola is at an infinite distance from A. It will be seen that the ellipse is a closed curve w^ith two vertices, and that the hyperbola has two separate branches each with its own vertex. If AjFi, measured to the left of A^, be made equal to AF, and if AiXi measured to the right of Aj be made equal to AX, and if XiM^ be drawn perpendicular to the axis, then the ellipse may be constructed from the focus F^ and directrix X^Mi, both to the right of the figure, in the same way as from the focus F and directrix XM, using the same eccentricity. Also the hyperbola may be constructed from the focus F^ and directrix X^^Mi, both to the left of the figure, in the same way as from the focus F and directrix XM, using the same eccentricity. Referring to Fig. 75, it will be seen that as the eccentricity increases or diminishes the angle DXE increases or diminishes, and therefore as- the eccentricity of the ellipse increases and approaches to unity the ellipse approaches to the parabola, and as the eccentricity of the hyper- bola diminishes and approaches to unity the hyperbola also approaches to the parabola. A parabola is therefore the limiting form of an ellipse or an hyperbola. Remembering this fact, many of the properties of the parabola may be deduced at once from those of the ellipse or hyperbola. For example, the tangent to an hyperbola at any point P on the curve bisects the angle between the focal distances FP and F^P. Now in the parabola the focus F^ is at an infinite distance from the focus F, therefore F^P is parallel to the axis, and the tangent to a parabola at any point P on the curve bisects the angle between the focal distance FP and the perpendicular PM on the directrix. 35. Conies defined with Reference to the Cone. — In Figs. 76, 77, and 78^ vtu is the projection of a right circular cone on a plane parallel to its axis, vs being the projection of the axis of the cone. In each Fig. xxi represents a plane which cuts the cone and is perpen- dicular to the plane of projection. If xx^ cuts vt and vu below the vertex of the cone (Fig. 76), the section is an ellipse. If xx^ cuts vt above and vu below the vertex (Fig. 78), the section is an hyperbola. If xx^ is parallel to vt (Fig. 77), the section is a parabola. In each Fig. the true shape of the section is shown, and is obtained by the rules of solid geometry. The axis XX^ of the true shape of the section is drawn parallel to .tx'j, and any point P on the curve is determined as follows : — Through any point n within the projection of the cone and on xx^ draw wN perpendicular to xx^ meeting XX^ at N. Through n draw a line perpendicular to vs and terminated by vt and vu. On this line as diameter describe a semicircle. Through n draw np parallel to vs to meet the semicircle at p. On the line wN make NP equal to np. P is a point on the true shape of the section. By repeating this construction any number of points may be obtained, CONIC SECTIONS 33 and a fair curve drawn through them is the curve required. The theory of the above construction will be understood after Art. 226, Chap. XVITI, has been studied. Fig. 78. To determine the positions of the directrices and foci of the conies, draw spheres inscribed in the cone and touching the plane of section. These spheres are represented by the circles whose centres are at s and Si on the projection of the axis of the cone. These spheres will touch the cone in circles whose projections are the chords of contact of the circles which are the projections of the spheres and the lines vt and vu. The planes of these circles of contact intersect the plane of section in lines which are the directrices of the sections, and the projections of these lines are the points x and Xi. (In the case of the parabola the 34 PRACTICAL GEOMETRY point Xi is at an infinite distance from x.) Hence if perpendiculars be drawn from x and x^ to XXi the directrices XM and XiM^ of the true shape of the section are ob- tained. The inscribed spheres touch the plane of section at the foci of the section, and the projections of these points are at / and f^. Hence perpendiculars from / and /^ to xx^^ to meet XX^ determine the foci F and Fj of the true shape of the section. A reference to the sketch shown in Fig. 79 will perhaps make the meaning of the foregoing state- ments a little clearer. As in Art. 34, it is instructive to observe that the parabola is the limiting form of an ellipse or an hyperbola, as the plane of section •^^^- '^^• (Figs. 76 and 78) is turned round so as to come nearer and nearer to a position (Fig. 77) in which it is parallel to vt. Also, when the hyper- bolic section is taken through the vertex of the cone, the hyperbola becomes two straight lines, and when the plane which gives the elliptic section is turned round so as to be perpendicular to the axis of the cone the ellipse becomes a circle. Again, if the plane of the parabolic section be moved parallel to itself nearer and nearer to vt, the ultimate form of the parabola will be a straight line. Studying Figs. 76, 77, and 78 still further, it will be seen that when the hyperbola becomes two (straight lines, the directrices will coincide, and the foci will coincide at the point where the axis of the conic cuts the directrix, and where the two straight lines which form the hyperbola intersect. Again, when the parabola becomes a straight line, that line will be the axis of the conic, and the focus will be on the directrix. Lastly, when the ellipse becomes a circle the foci will coincide at the centre of the circle, and the directrices will move off to infinity. 36. Additional Definitions relating to Conies. — A perpen- dicular PN (Fig. 80) from a point P on a conic to the axis is called the ordinate of the point P, and if PN be produced to cut the conic again at P', the line PP' is called a double ordinate of the conic. RFR', the double ordinate through the focus, is called the latus rectum of the conic. In the ellipse and hyperbola the point which is midway between A and Ai, the points where the conic cuts the axis, is called the centre of the conic, and the ellipse and hyperbola are called central conies. A straight line joining two points on a conic is called a chord of the conic. Fig. 80. CONIC SECTIONS 35 37. General Properties of Conies.— Following from the general definition of a conic (Art. 33), there are many properties possessed by all conies which may be demonstrated. A few of the more important of these general properties will now be given. (1) If a straight line cuts the directrix at D and the conic at P and Q (Figs. 81 and 82), then, F /F \ /\.^^\^ Fig. 81. Fig. 82. the focus, the straight line DF ivill bisect, either the exterior or the interior angle between PF and QF. Only in the case of the hyper- bola, and only when P and Q are on different branches of the curve (Fig. 82) is it the interior angle PFQ which is bisected by DF. If the straight line FP' be drawn bisecting the angle PFQ (Fig. 81) and meeting the conic at 1^', then the angle DFP' is evidently a right angle, and if the line DPQ be turned about D so as to make P and Q approach nearer and nearer to one another, P' will always lie between P and Q, and in the limit when P and Q coincide they will coincide at P' and a straight line through D and P' will be a tangent to the conic at P'. Hence the next general property of conies. (2) The portion of a tangent intercepted between its point of contact and the directrix subtends a right angle at the focus. (3) Tangents at the extremities of a focal chord intersect on the directrix. This follows at once from f>i the preceding property. It is evi- dent, conversely, that if tangents be drawn to a conic from a point on the directrix, the chord of contact passes through the focus. (4) If PFP and QFQ (Fig. 83) be two focal chords, the straight lines P'Q and Q'P intersect at a point on the directrix; also the straight lines PQ and Q'P' intersect at a point on the directrix, and the portion of the directrix DD' between the points of intersection subtends a right angle at the focus. The above follows very easily from the first property given in this article. (5) Tangents TP and TQ (Fig. 84) from any point T subtend equal angles at the focus F. (6) If the normal at P (Fig. 84) meet the axis at G, the ratio of FG to FP is equal to the eccentricity of the conic. (7) PL (Fig. 84) the projection of PG on FP 18 equal to the semi-latus rectum. Fig. 83. Ftg. 84. 36 PRACTICAL GEOMETRY (8) The locus of the middle points of a system of parallel chords is a straight line. This straight line is called a diameter of the conic, and the point where a diameter cuts the conic is called the vertex of the diameter. (9) All diameters of a central conic pass through the centre of the conic, and all diameters of a parabola are parallel to the axis. (10) Tangents at the extremities of a chord PP (Fig. 85) intersect at a point T on the diameter TW which bisects the chord. (11) The tangent at the vertex of a diameter is parallel to the system of chords bisected by that diameter. (12) TVW(Fig. 85) being a diameter, and TP and TP' being tangents to the conic, EE', the portion of the tangent at }^ intercepted between TP and TP, is bisected at V the vertex of the diameter. 38. Properties of the Parabola. — A knowledge of the following properties of the parabola will enable the student to solve a considerable number of problems. (X) If from the ends of a focal chord PPy (Fig. 86) perpendiculars be drawn to the directrix KXK^, then KK^ subtends a right angle at the focus F. (2) The tangent PT (Fig. 87) at any point P bisects the angle between the focal distance FP and the perpendicular PK to the directrix. From this it follows that the tangent is equally inclined to the focal distance of the point of contact and the axis. Also FT = FP Fig. 85. Fig. 86. Fig. 87. Fig. 88. (3) If the tangent at any point P (Fig. 87) meets the axis at T, and PN be the ordinate of P, then AT = AN. This follows easily from the preceding property thus : FT = FP = PK = XN. But AF = AX, therefore AT = AN. (4) Y(Fig. 87), the foot of the perpendicular from the focus F on the tangent at any point P, lies on A Y the tangent at the vertex. (5) PN'^ = 4AF . AN (Fig. 87). (6) Tangents PS and P^S at the ends of a focal chord PP^ intersect at right angles at a point S on the directrix (Fig. 87). CONIC SECTIONS 37 Fig. 89. Definition. If PG (Fig. 87) the normal at P meets the axis at G then NG is called the suhnormal. (7) The suhnormal is constant and equal to 2AF. For, since PT bisects the angle FPK and PG is perpendicular to PT it follows that PG bisects the angle FPL.^ Hence, angle FPG = angle LPG = angle FGP, therefore FG = FP = PK = NX, and NG = FX = 2AF. (8) The angles SFP and SF1\ (Fig. 88) subtended at the focus F hy tangents SP and SF^ are equal to one another and to the angle LSP. • (9) The triangles FPS and FSP^^ (Fig. 88) are similar and FS' = FP.FP,. (10) The focus F (Fig. 89) and the points of intersection S^, S2, and S3 of three tangents to a parabola lie on the same circle. Definition. A straight line YU (Fig. 88) drawn parallel to the axis AF through any point V of a parabola is called a diameter and the point V is called the vertex of the diameter YU. (11) /Sf (Fig. 88), the point of inter- section of two tangents SP and SP^, is equidistant from the diameters through the points of contact P and Pj. ( 1 2) The diameter SVU(Fig. 88) through the point of intersection of tangents SP and SPi bisects the chord, of contact PP^. Also SV = VU, and PP^ is parallel to the tangent at V. (13) A diameter bisects all chords parallel to the tangent at its vertex. Definition. The focal chord parallel to the tangent at the vertex of a diameter is called the parameter of that diameter. (14) The parameter of any diameter is four times the focal distance of the vertex of that diameter. (15) The area enclosed hy the parabola AQP (Fig. 90), the ordinatePN, and the axis AN, is two-thirds of the area of the rectangle ANPL. It follows from this that the area of the figure AQPL is one-third of the area of the rectangle ANPL. 39. To draw the Tangents to a Parabola from an external point.— Let A (Fig. 91) be the vertex and F the focus of the parabola and let S be the external point from which the tan- gents are to be drawn. Join SF and on SF as diameter describe a circle. Draw YYj the tangent at the vertex cutting the circle at Y and Yi. 1 PL is KP produced (Fig. 87). Fig. 90. Fig. 9]. 38 PRACTICAL OEOMETRY Join S to Y and Y^ and produce them. These are the tangents required, Y and Y^ are evidently the feet of the perpendiculars from F on SY and SYj and these are on the tangent at the vertex. Hence by- Art. 38 (4) SY and SYj are tangents from S. 40. To construct a Parabola, having given the Vertex, the Axis, and another point on the Curve.— Let A (Fig, 92) be* the vertex, AN the axis, and P another point on the parabola. This is a problem of very frequent occur- rence and the following construction, is the most convenient. Draw the ordinate VN and complete the rectangle ANPL. Divide AL into any convenient number of equal parts, 1' 2' 3' / /a.^--' r iw \h H and number the points of division 1, -pia 99 2, 3, etc. from A to L. (In Fig. 92, four equal parts have been taken.) Divide LP into the same number of equal parts, and number the points of division, 1', 2', 3', etc. from L to P. From the points 1, 2, 3, etc. on AL draw lines parallel to AN. Join A to the points 1', 2', 3', etc. on LP. The lines having the same numbers at their ends intersect at points on the para- bola. Consider one of these points, Q, where A3' cuts the line through 3 parallel to AN. Draw QM and 3'H perpendicular to AN. The ordinate PN is i of the ordinate QM. Again AN is J of AH and AH is I of AM. Therefore AN = f x |AM = if AM. But [Art. 38, (5)] PN^ = 4AF . AN therefore (iQM)^ = 4AF x ^M^, and QM' = 4AF • AM, which shows that Q is a point on the parabola. 41. Definitions relating to Central Conies. — A central conic cuts the axis at two points A and A^, and there are two foci F and F^. There are also two directrices, one belonging to each focus. In referring to the focus and directrix of a conic it is understood that if the conic is a central conic the focus and directrix belong or correspond the one to the other. In a central conic the line AAj terminated by the two vertices of the curve is called the transverse axis. In the ellipse, Fig. 93, the straight line BCB^ drawn through the centre at right angles to AA^ and terminated by the curve is called the conjugate axis but more generally the minor axisj and the transverse axis is generally called the major axis. In the hyperbola, Fig. 94, there is also a conjugate axis BCBj passing through the centre at right angles to AA^, but it does not meet the curve. The length of the conjugate axis of the hyperbola is obtained by the following construction. With centre A and radius equal to CF describe an arc of a circle to cut the line through C perpendicular to AAj at B and Bj. Then BBi is the length of the conjugate axis. The conjugate axis of the hyperbola is not necessarily CONIC SECTIONS 39 a minor axis, as it may be either less than, equal to, or greater than the transverse axis. Fig. 93. Fig. 94. The circle described with the transverse axis AA^ as a diameter is called the auxiliary circle. The circle described on the minor axis of an ellipse as a diameter is sometimes called the minor auxiliary circle. If an hyperbola be described having BCBj for its transverse axis, and ACAi for its conjugate axis, this hyperbola is called the conjugate hyperbola. Diameters PCPi and QCQi are called conjugate diameters when QQ^ is parallel to the tangents at P and Pj, or when PPj is parallel to the tangents at Q and Q^. 42. General Properties of Central Conies. — The ellipse and hyperbola have many properties in common, and there are other properties possessed by one which when stated in a slightly modified form are also possessed by the other. A number of these properties will now be given. (1) The sum or difference of the focal distances of any point P (Figs. 95 and 96) on the curve is equal to the transverse axis, or PF ± PF^ = AA^. In the ellipse it is the sum and in the hyperbola it is the difference which must be taken. (2) The tangent and normal at any point P (Figs. 95 and 96) on the curve bisect the angles between the focal distances of the point. In the ellipse it is the exterior angle between PF and PFj which is bisected by the tangent, while in the hyperbola it is the interior angle between these lines which is bisected by the tangent. (3) A circle drawn through a point P (Figs. 95 and 96) on the curve and the foci F and F^ cuts the conjugate axis at the points t and g, ivhere the tangent and normal to the curve at P cut that axis. (In Fig. 96 the point g falls outside the limits of the figure.) (4) Perpendiculars FY and F^Y^ (Figs. 95 and 96) on the tangent at any point P meet that tangent on the auxiliary circle, and BC, the semi- conjugate axis, is a mean proportional between them or BO^ = FY . FiY^. (5) Tangents OP and OQ (Figs. 95 and 96) are equally inclined to the focal distances OF and OFi of the point 0. 40 PRACTICAL GEOMETRY (6) The locus of the intersection (Figs, 95 and 96) of pairs of tangents FO and QO, which are at right angles to one another, is a circle ivhose centre is C, and whose radius is equal to ^ AC^ ± BC\ This circle is called the director circle. In determining the radius the plus sign must be taken in the case of the ellipse and the minus sign in the case of the hyperbola. In the case of the hyperbola when EC = AC, the radius of the director circle is zero, and when BC is greater than Fig. 95. Fig. 96. AC there is no director circle, and no pairs of tangents can be drawn which are perpendicular to one another. In Fig. 96 the tangents OP and OQ are shown touching different branches of the hyperbola, but for certain positions of O they will touch one branch only. (7) If the tangent at P meet the transverse axis at T (Figs. 95 and 96) and the conjugate axis at t, and ifN and n he the feet of the perpen- diculars from P on the transverse and conjugate axes respectively, then CN . CT = AC^ and Cn.Ct = BCl (8) PN' : AN . AiN : : BC"^ : ACl (9) CP and CQ (Figs. 93 and 94) being conjugate semi-diameters, CP-^ ± CQ2 = CA^ ± CBl The plus sign is taken for the ellipse and the minus sign for the hyperbola. (10) The area of the parallelogram formed by the tangents at the ends of conjugate diameters is equal to the rectangle contained hy the transverse and conjugate axes. 43. To construct a Central Conic having given the Foci and the Transverse Axis. — F and F^ (Figs. 97 and 98) are the given foci and AAi is the given transverse axis. For the ellipse take any point a in AA^ and for the hyperbola take any point a in AjA produced. With centres F and F^ and radius equal to Aa describe arcs of circles. With centres F and Fj and radius equal to A^a describe arcs of circles to cut the former arcs at P, Q, P^ and Qi. P, Q, P^, and Qi are points on the conic required, and by taking other positions of the point a and repeating the above construction any number of points on the conic may be determined and a fair curve drawn through them will complete the construction. CONIC SECTIONS 41 It will be observed that the property of central conies given in Art. 42 (1; is made use of in the above construction. Fig. 97. Fig. 98. Fig. 99. 44. To construct an Ellipse from the Auxiliary Circles.— It has already been given [Art. 42, (8)J that PN^ ; AN . AjN : : BC^ : AC^ Let the ordinate PN (Fig. 99) be produced to meet the auxiliary circle at a, then by a property of the circle, «N^= AN . A^N, there- fore PN2 : aW : : BC^ : AC^, or PN : aN : : BC : AC. Draw aC cutting the minor auxiliary circle at b, then, since «G = AC and hC = BC, PN: aN:: 6C: aC, therefore Fh is parallel to AC. Hence the following construction for finding points on the ellipse. Draw a radius aC of the auxiliary circle cutting the minor auxiliary circle at h. Through a draw aN parallel to the minor axis, and through h draw 6P parallel to the major axis to meet aN at P. P is a point on the ellipse. In like manner any number of points on the ellipse may be found, and a fair curve drawn through them completes the construction. It may be noted here that the tangent to the auxiliary circle at a, and the tangent to the ellipse at P meet at a point T on the major axis produced. Also the tangent to the minor auxiliary circle at h and the tangent to the ellipse at P meet at a point t on the minor axis pro- duced. 45. The Trammel Method of Drawing an Ellipse.— Re- ferring to Fig. 99, if Fn be drawn parallel to aC, meeting AC at m and BC produced at w, then Pw = aC = AC, and PN : aN : : Pm : aC ; but it has been shown that PN : aN : : BC : AC, therefore P»i : aC : : BC : AC, and consequently Pm = BC. Hence if a straight line be drawn across an ellipse, cutting the curve at P, the major axis at m, and the minor axis at n, and if Tn = AC, then Vm = BC. Conversely it follows that if a straight line Pmw in which Pw = AC and Vm = BC be placed so that n is on the minor axis and m is on the major axis, then P will lie on the ellipse. 42 PRACTICAL GEOMETRY Fig. 100. On the straight edge of a strip of paper, Fig. 100, mark points P, m, and n, such that P?i is equal to the semi-major axis, and Pwi is equal to the semi-minor axis of the ellipse. Place this paper trammel on the paper so that m is on the major axis and n is on the minor axis, a dot made on the paper at P will be on the ellipse. By moving the trammel into a number of different positions a sufficient number of points on the ellipse may be obtained and a fair curve is then drawn through them. Referring again to Fig. 99, if m^Vrii be drawn making the angle Vn^n equal to the angle Pwrii, then Tn^ will be equal to P?i, and Fm^ will be equal to P?». Hence the points m and n on the trammel may be on opposite sides of P as shown on the trammel m^Frii, Fig. 100. The latter form of the trammel should be used when the difference between the major and minor axes of the ellipse is small. The trammel method of drawing an ellipse is most convenient as it keeps the paper free of construction lines other than the axes. 46. Given a Pair of Conjugate Diameters of an Ellipse, to find the Axes.— Let PCPj and QCQ, (Fig. 101) be the given conjugate diameters. Draw PD perpendicular to CQ. Make PH and PHi each equal to CQ. Join CH and CHp The major axis ACAi bisects the angle HCHi, and the minor axis BCB^ is of course perpendicular to ACA^. Join P to the middle point of CH, cutting the major axis at m and the minor axis at 11. P« is the length of the semi- major axis, and Pjh is the length of the semi-minor axis. 47. To construct an Ellipse having given a Pair of Conjugate Diameters.— Let PCP^ and QCQ^ (Figs. 102 and 103) be the given conjugate diameters. First Method. Through P, Q, P„ and Qi (Fig. 102) draw parallels to the given diameters forming the parallelogi'am RT. Divide CP into a number of equal parts, and divide RP into the same number of equal parts. Join Q to 1' the first point of division on RP. A line joining Qi to 1 the first point of division on CP will when produced cut Ql' at a point on the .ellipse required. Repeating this construction Fig. 102. CONIC SECTIONS 43 Fig. 103. with the other points of division on RP and CP other points on the arc PQ are obtained. In like manner points on the arc PQ^ are obtained. Points on the other half of the ellipse may be found by the same method, or by a construction depending on the fact that all diameters are bisected at the centre C, or by making use of the fact that chords parallel to a diameter are bisected by its conjugate. Second Method. Find the axes by the construction described in the preceding article and then use a paper trammel as explained in Art. 45. Third Method. By a triangular trammel. From P, Fig. 103, draw Pm perpendicular to CQ. From Q draw QD perpendicular to CP and make Pw equal to QD. Join mn. If the triangle Pmn be drawn on a strip of paper, mn being on one edge and P on the opposite edge, and if this strip be moved into different positions, m being on QQ^ and n on PPi, then P will be on the ellipse. A second position of the trammel is shown to the right of the figure. Instead of using a strip of ordinary paper, the points m, w, and P may be marked on a piece of tracing paper, a needle hole being made in the tracing paper at P, through which points on the ellipse may be marked by a sharp round-pointed pencil. 48. The Ellipse as the Projection of a Circle.— Many of the properties of the ellipse and many of the constructions connected with it may be readily demonstrated by considering the ellipse as the projec- tion of a circle. A few of these will be considered here, it being assumed that the student has al- ready studied some of the later chapters in this work relating to projection. Referring to Fig. 104, ABAiBi is a circle lying in a hori- zontal plane, AAj and BBi being dia- meters at right an- gles to one another. . ., ., Imagine the circle ABA^B^ to revolve about AA, as an axis until its plane is inclined at an angle to. the horizontal, and let it then be projected on to the horizontal plane containing AA^. ihe point r on Fig. 104. 44 PRACTICAL GEOMETRY the circle in its new position will have the point p for its plan, the point p being determined by the construction shown. Other points on the circle may be treated in the same way, and all points such as p being joined by a fair curve the ellipse ApA-J)^ is determined. On hhi as diameter describe the circle ahaj)^. This circle will have its centre at C, the centre of the other circle. Now imagine the ellipse, which is horizontal, to revolve about hhi as an axis until its plane is inclined at the angle 6 to the horizontal and let it then be projected on to the horizontal plane containing hh^. The point p on the ellipse in its new position will have the point pi for its plan, and it is easy to show that the point p^ is on the circle abaj)i, also that the points P, j?i, and C are in the same straight line. It will be seen that the circles ABAjBi and aba-^^ are the auxiliary circles of the ellipse AfeAjbi and the theory of the construction given in Art. 44 is further ex- plained. It is easy to establish the following theorem in projection : — " The 'projection of the tangent to a curve at any point is the tangent to the projection of the curve at the projection of the point."" Referring again to Fig. 104, TP is a tangent to the circle ABAiBj at P, and when the circle is turned about AA^ as an axis and pro- jected into the ellipse as already described, the point T which is on that axis is stationary and therefore Tp will evidently be the tangent to the ellipse at p. Let Tp produced meet BBj at t. Then when the ellipse is turned about BB^ as an axis and projected into the circle aba^i as already described, the point t which is on that axis is stationary and tp^ will evidently be the tangent to the circle dba^^ at pi. Another theorem in projection which is easily proved is as follows : — The projections on a plane of two intersecting straight lines ivill intersect at a point which is the projection of the point of intersection of the original lines, and the point of intersection of the projections will divide the pro- jections into segments which are to one another as the corresponding segments of the original lines. This enables a simple demonstration to be given of the construction for drawing an ellipse having given a pair of conjugate diameters which has been described in Art. 47 and illustrated by Fig. 102. Referring to Fig. 105, PPi and QQi are two diameters of a circle at right angles to one another. The circle is supposed to be lying on the horizontal plane. A square RSTU is shown circumscribing the circle, the points of contact being P, Qi, Pi, and Q. The radius CP is divided into any number of equal parts, in this case three, at the points 1 and 2, and RP is divided into the same number of equal parts at the points 1' and 2'. If the lines joining Q.^ to the points 1 and 2 be produced it is easy to show that they will intersect the lines joining Q to 1' and 2/ respectively at points on the circle as shown. Now imagine the circle, with all the lines connected with it, to revolve about an axis MN in its plane into an inclined position, and let a projection of the whole be then made on the horizontal plane as shown. The square RSTU projects into the parallelogram rstUj and CONIC SECTIONS 45 the circle projects into an ellipse which touches the sides of the parallelogram at^?, q^, p^, and q. Also pp^ and qq^ will evidently be conjugate diameters of the ellipse. Lastly, the lines through Q^ and Q which intersect on the circle project into lines which intersect on the ellipse and divide cp and rp into three equal parts. Hence the con- struction for drawing the ellipse having given two conjugate diameters. 49. Properties characteristic of the Hyperbola. — It has already been pointed out that the hyperbola has two separate branches and that there is a conjugate hyperbola also having two separate branches. Also the transverse and conjugate axes of the hyperbola are the conjugate and transverse axes respectively of the conjugate hyperbola. Referring to Fig. 106, F and F^ are the foci and AA^ is the trans- verse axis of the hyperbola whose branches are Q and Qi. BB^ is the conjugate axis and Q' and Q', are the branches of the conjugate hyper- bola. A construction has already been given (Art. 41, p. 38) for finding the conjugate axis, and the following construction will evidently give the same result. With centre C, the middle point of AAj, and radius CF describe a circle. Draw the tangent to the hyperbola at A to cut this circle at L and L^. Through C draw BCBj at right angles to AA^. Parallels to AAj through L and L^ will cut BCBj at B and Bi the extremities of the conjugate axis. The circle whose centre is C and radius CF cuts BBj produced at F' and F'l the foci of the conjugate hyperbola. 46 PRACTICAL GEOMETRY The lines CL and CLi produced both ways are the asymptotes of the hyperbola. It will be seen that tlie asymptotes are the diagonals of the rectangle formed by the tangents at the vertices of the hyper- bola and its conjugate. The asymptotes are tangents to the hyperbola and its conjugate at an infinite distance from the centre C. The following properties should be specially noted : — (1) Perpendiculars from the foci to the asymptotes are tangents to one or other of the auxiliary circles. Referring to Fig. 106, FD is a perpen- dicular to the asymptote CL and FD is a tangent to the auxiliary circle described on AA^ as diameter and D is the point of contact. F'D' is a perpendicular to CL and F'D' is a tangent to the auxiliary circle described on BBj as diameter and D' is the point of contact. (2) The auxiliary circles intersect the asymptotes at points on the ^ > ^ t k^x' ^:> P fli-A / /\ /\ V" f] 1 N A / \ "ki^ / \> ^ > \^ < Fig. 106. Fig. 107. directrices. DX (Fig. 106) is a du'ectrix of the hyperbola whose transverse axis is AA^ and D'X' is a directrix of the conjugate hyperbola. (3) The portion HR^ (Fig. 107) of a tangent lying between the asymp- totes is bisected at the point of contact P, and HHi is equal to the diameter EGEy ichich is parallel to HHi. This suggests a method of drawing the tangent to the curve at a point P on it. Draw PM parallel to CL^ to meet CL at M. Make MH equal to CM. Join HP and this will be the tangent required. (4) If from any point P on the curve (Fig. 107) PM and PN be drawn parallel to the asymptotes, meeting them at M and N respectively, then the product PM . PN is constant. This last property may be used to construct an hyperbola when the asymptotes and a point on the curve are given as follows. Referring to Fig. 108, CL and CL^ are the given asymptotes and P is a given point on the hyperbola. Draw PM and PN parallel to CLj and CL respectively and produce PM and PN both ways. Through C draw a number of radial lines to cut PM at points 1, 2, 3, etc., and PN at points r, 2', 3', etc. Parallels to CL through the points 1, 2, 3, etc. CONIC SECTIONS 47 will intersect parallels to CLj points on the hyperbola as shown. through r, 2', 3', etc. respectively at Fig. 108. 50. The Rectangular Hyperbola. — When the transverse and conjugate axes of an hyperbola are equal the asymptotes are at right angles to one another, and the hyperbola is then said to be equilateral or rectangular. In Fig. 109, OX and OY, at right angles to one another, are the asymptotes of a rectangular hyperbola and P is a point on the curve. Other points on the curve are obtained by the construction already given and illustrated by Fig. 108. PM and FN being parallel to OX and OY respec- tively, it will be seen that for the rectangular hyperbola (Fig. 109) PMON is a rectangle. If distances from OY parallel to OX represent to scale the volume «; of a given weight of a gas, and if distances from OX parallel to Y represent to scale the corresponding pressure ;p of the gas, then if the gas is expanded or compressed and the pressure is inversely as the volume, the product pv is constant and the co-ordinates of points on a rectangular hyperbola will show the relation between the pressure and volume of the gas as it is expanded or compressed. The hyperbola is then the expansion curve or the compression curve for the gas. 51. Centre of Curvature of a Conic— The following con- struction is applicable for finding the centre of curvature of any conic. 48 PRACTICAL GEOMETRY P (Fig. 110) is a point on the curve, F the focus, FG the direction of the axis, and PG the normal to the curve at P. Draw GH at right angles to PG meeting PF or PF produced at H. Draw HS at right angles to PH meeting PG pro- duced at S. S is the centre of curvature of the conic at P. In the case of the parabola the point H may be obtained by making FH, on PF produced, equal toPF. The above construction fails when the point P is at A the vertex of the conic. It will be observed that as the point P approaches nearer and nearer to A, the points G, H, and S approach nearer and nearer to one another and in the limit they will coincide at a point on the axis. Now in the parabola FH is equal to PF ; hence the centre of curvature of the parabola at A, its vertex, is on the axis at a distance from A equal to 2AF. In the ellipse and hyperbola PF : PFj : : FG : FjG, and when P coincides with A, this becomes AF : AF^ : : FS : FiS. Hence the following construction for the centre of curvature at A. Draw FjD (Figs. Ill and 112) inclined to ¥,¥. Make F^D equal to AF^, and Fig. 110. Fig. 111. Fig. 112. DE equal to AF. Join EF, and draw DS parallel to EF meeting the axis at S. S is the point required. Another construction which gives the centre of curvature of a central conic at an extremity of the transverse axis, and at the same time gives the centre of curvature at an extremity of the conjugate axis, is shown in Figs. 113 and 114. Referring to the ellipse (Fig. 113) CA is the semi- major axis and CB is the semi- minor axis. Complete the rectangle ACBL. Join AB. Fig. 113. Fig. 114. Draw LSS' at right angles to AB to cut AC at S and BC produced at S' ; then S and S' are the centres of curvature of the ellipse at A and B respectively. CONIC SECTIONS 49 The ellipse may be quickly drawn with sufficient accuracy for many purposes by describing circular arcs through the extremities of the axes from the corresponding centres of curvature and then joining these arcs with fair curves to please the eye Referring to the hyperbola (Fig. 114) CA is the semi-transverse axis and CB is the semi- conjugate axis. Complete the rectangle ACBL. Join CL. Draw SLS' at right angles to CL to cut CA produced at S and CB produced at S'. S is the centre of curvature of the hyperbola at A, and S' is the centre of curvature of the conjugate hyperbola at B. Note that CL is an asymptote of the hyperbola. • 52. Evolute of a Conic. — The evolute being the locus of the centre of curvature, if the construction of the preceding article be applied to a sufficient number of points on the conic, a fair curve drawn through the centres obtained will be the evolute of the conic. Fig. 115 shows the evolute of a parabola, and Fig. 116 shows the Fig. 115, evolute of an ellipse. In the parabola the evolute cuts the conic at two points and if the ordinate PN of one of them be drawn, then AN =8AF. In the ellipse when OB the semi-minor axis is equal to OF the points S^ and §2 will coincide with B^ and B respectively. When OB is greater than OF, Sj and 83 will lie within the ellipse as in Fig. 116, and when OB is less than OF the points Sj and So will lie outside the ellipse. 53. Pole and Polar.— If through a given point P (Figs. 117 and 118) any straight line be drawn to cut a conic at Q and R, tangents to the conic at Q and R will intersect on a fixed straight line LM. Con- versely, the chord of contact of tangents to the conic from any point in LM will pass through P. The fixed line LM is called the ;polar of the point P with respect to the conic, and the point P is called the pole of the line LM with respect to the conic. The point P may be within or without the conic. In the case of a central conic (Fig. 117) if C the centre be joined to P and produced, if necessary, to cut the conic at S, then LM is parallel to the. tangent to the conic at S. In the case of the parabola (Fig. 118) if PS be drawn parallel to the axis to meet the curve at S, then LM is parallel to the tangent to the parabola at S. 50 PRACTICAL GEOMETRY If CP or CP produced cuts the conic at S and LM at T, then CP X CT = CSl If chords QR and KN of a conic (produced if necessary) intersect at P, then the chords QK and NR (produced if necessary) will intersect on LM the polar of P. Also the chords QN and KR (produced if necessary) will intersect on LM the polar of P. This suggests the simplest construction for finding the polar of a given point P. Fro. 117. Fig. 118. A more general way of stating the preceding property is as follows. If a quadrilateral QNRK be inscribed in a conic, the opposite sides and diagonals will (produced if necessary) intersect in three points such that each is the pole of the line joining the other two. Since the circle is a particular form of a conic it follows that all that has been said about the pole and polar with respect to a conic will be true for the pole and polar with respect to a circle. The student should therefore compare this article with Art. 27, p. 24. Exercises III 1. Draw an ellipse, a parabola, and an hyperbola as in Fig. 75, p. 31, having given, FX = 1'5 inches, eccentricity of ellipse = ^, and eccentricity of hyper- bola = |. 2. Using the curves of the preceding exercise, work out on each, the fol- lowing : — (a) P is any point on the conic. PL is the tangent at P, L being on the directrix. G is the point where the normal at P cuts the axis, and F is the focus. PG and LF are joined and produced to meet at p. Construct the locus of p. (&) PQ is a. chord of the conic subtending an angle of say G0° at the focus F. Determine the locus of the intersection of the tangents at P and Q, and also the envelope of the chord PQ. [It will be found that the curves required are conies having the same focus and directrix as the given conic] 3. Using the drawing of exercise 1, take a point T on the directrix XM and 0-5 inch from X, and from T draw all the possible tangents to each of the three conies, by the method given in Art. 13, p. 12 ; then determine the points of con- tact by Art. 37, (2). CONIC SECTIONS 51 4. Construct Figs. 76, 77, and 78, p. 33, as explained in Art. 85, to the follow- ing dimensions : — For Fig. 76, vertical angle of cone tvu = SO"*, va = 2-5 inches, va^ = 1-25 inches. For Fig. 77, vertical angle of cone tva = 60°, va = 1 inch, xXi parallel to vt. For Fig. 78, vertical angle of cone tvtc = 80°, va = 1 inch, va^ = 0*75 inch. The eccentricity of the conic being the ratio of AF to AX, construct each conic separately on another part of the paper by the method of Art. 34 and Fig. 75. Make a tracing of each conic obtained in this way and test whether it agrees with the conic determined as a section of the cone. 5. PTQ is a triangle, PT = 2-75 inches, TQ = 1-75 inches, and PQ = 2 inches. R is a point in PT 1 inch from P. RF is perpendicular to PT, and RF = 1-25 inches. F and Q are on the same side of PT. PT is a tangent to a conic, P being the point of contact. F is the focus, and Q is another point on the curve. Find the directrix and draw the conic. [Art. 87, (1) and (2).] 6. PFNQ is a quadjnlateral. The angles at F and N are right angles. PF = 1-3 inches, FN = NQ = 1*6 inches. P and Q are points on a conic of which F is the focus and FN the direction of the axis. Construct the conic. 7. F is the focus and S is any fixed point on the axis of a conic. From S a perpendicular is drawn to the tangent at a point P on the curve meeting FP at Q. Show by actual drawing that the locus of Q is a circle. 8. A focal chord of a parabola is 2-3 inches long and it is inclined at 30° to the directrix. The middle point of the chord is at a perpendicular distance of 1'2 inches from the directrix. Draw the parabola. 9. AP, a chord of a parabola, is 1-8 inches long and is inclined at 50° to the axis. The point A being the vertex of the parabola, draw the curve. 10. TP, a tangent to a parabola from a point T on the axis, is inclined at 30° to the axis. P is the point of contact, and TP is 3 inches long. Draw as much of the parabola as lies between the vertex and a double ordinate whose distance from the vertex is 2*2 inches. 11. Construct a triangle FPQ. FP = 1*5 inches, PQ = 3-4 inches, and QF = 2-6 inches. Draw a parabola whose focus is F and which passes through P and Q. 12. Make a careful tracing of the parabola of the preceding exercise without any lines other than the carve ; then determine the axis, focus, and directrix of the curve by constructions on the tracing. 13. Draw a line FS 1-3 inches long and a line SP making the angle FSP 45°. SP is a tangent to a parabola of which F is the focus and S a point on the directrix. Find the point of. contact of the tangent and draw the parabola. 14. PNPj, a double ordinate of a parabola, is 3-6 inches long. A being the vertex of the parabola, the area bounded by the curve PAPi and the double ordi- nate PNPj is 4-8 square inches. Draw the curve PAP,. 15. Construct a triangle RST ; RS = 1-7 inches, ST = TR = 2-6 inches. ST and SR, both produced, are tangents to a parabola and TR is parallel to their chord of contact. TR contains the focus. Draw the parabola. 16. ABC is a triangle. AB = 2-2 inches, BC = 2-3 inches, and CA = I'l inches. D is a point in BC 0-9 inch from B. Draw the parabola which touches BC at D and AB and AC produced. 17. The normal PG to a parabola at a point P on the curve is 1-9 inches long, the point G being on the axis. The parameter of the diameter through P is 4-8 inches long. Construct the parabola. 18. The major and minor axes of an ellipse are 4 inches and 3 inches long respectively. Construct the curve by the trammel method and find the foci . 19. The major axis of an ellipse is 3-5 inches long and the distance between the foci is 2*5 inches. Draw the ellipse. 20. ABC is a triangle. AB = 2-3 inches, BC = I'l inches, and CA = 2-2 inches. Draw an ellipse whose foci are A and B and which passes through C. 21. The minor axis of an ellipse is 2-2 inches long and the distance between 52 PRACTICAL GEOMETRY the foci is 2 inches. Draw the ellipse, and construct the locus of the middle points of all the chords through one focus. 22. The major and minor axes of an ellipse are 3 inches and 2 inches long respectively. Draw a half of the ellipse which lies on one side of the major axis. Divide the curve into twelve parts whose chords are equal, and from the points of division draw normals to the ellipse, each normal to project 0*5 inch outside the ellipse. Lastly, draw a fair curve through the outer extremities of the normals. 23. The distance between the foci of an ellipse is 2 inches. A tangent to the ellipse is inclined to the major axis at an angle of 30^^ and cuts that axis produced at a point 2*5 inches from the centre of the ellipse. Draw the ellipse. 24. SABT is a quadrilateral. The angles at A and B are right angles. SA = 0'75 inch, AB = 3 inches, and BT = 2*25 inches. The points S and T are on the same side of AB. ST is a tangent to an ellipse of which AB is the major axis. Construct the ellipse. 25. Two conjugate diameters of an ellipse are 3 inches and 3-5 inches long, and the angle between them is 60°. Draw the ellipse by each of the three methods described in Art. 47, p. 42. 26. CO is a straight link, 2 inches long, which revolves about a fixed axis at C. PON is another straight link, 4 inches long, jointed at its middle point O to the outer end of CO. N is constrained to move in a straight line which passes through C. Draw the loci of the middle points of OP and ON and also the locus of P. 27. Draw a quadrilateral FPOQ. FP = 3-2 inches, angle PFQ = 70°, angle FPO - 56°, FQ = 1-2 inches, and PO - 1-6 inches. Draw an ellipse touching OP at P and OQ at Q, and having F for one focus. 28. The transverse axis of an hyperbola is 2 inches long and the distance between the foci is 2-7 inches. Draw the hyperbola. 29. The transverse and conjugate axes of an hyperbola are 2-2 inches and 1*7 inches long respectively. Draw the hyperbola and the conjugate hyperbola. 30. The foci of an hyperbola are 2-8 inches apart. One point on the curve is 2-9 inches from one focus and 1-1 inches from the other. Draw the hyperbola. 31. The distance between the foci of an hyperbola is 2*9 inches. A tangent to the hyperbola is inclined to the transverse axis at 48° and cuts that axis at a point 0"6 inch from its centre. Draw the hyperbola. 32. The transverse axis of an hyperbola is 2 inches long. A tangent to the hyperbola is inclined at 58° to the transverse axis and cuts that axis at a point 0*8 inch from its centre. Draw the hyperbola. 33. PMMiPj is a quadrilateral. IMM^ = 2-5 inches, the angles at M and Mj are right angles, PM = 0*9 inch, P,Mi = 1'2 inches. P and P^ are points on an hyperbola of which MMj (produced both ways) is a directrix, and whose eccen- tricity is ^. Find the foci and draw the hyperbola. 34. The asymptotes of an hyperbola are at right angles to one another and one point on the curve is 1 inch from each asymptote. Construct the two branches of the curve by the method illustrated by Fig. 108, p. 47. 35. One cubic foot of air at a pressure of 100 lbs. per square inch expands until its volume is 10 cubic feet. The relation between the pressure p and volume V is given by the formula 2>v = 100. Construct the expansion curve. Pressure scale, 1 inch to 20 lbs. per square inch ; volume scale, 1 inch to 2 cubic feet. Draw the tangent and normal to the curve at the point where the volume is 3 cubic feet. 36. AB and CD (Fig. 119) are two straight lines of unlimited length. AB revolves with uniform angular velocity about the centre P, and CD revolves with the same angular ve- locity, but in the opposite direction, about the centre Q. PQ = 2-5 inches. O is the Fig. 119. middle point of PQ. XiOX and YOY, are two lines at right angles to one another, the angle POX being 30°. The initial positions A Y P B /36^ '.-^ X P 6 Y, CONIC SECTIONS 53 of AB and CD are parallel to XjOX. Show by actual drawing that the locus of the point of intersection of AB and CD is a rectangular hyperbola of which X^OX and YOYi are the asymptotes and P and Q points on the curve. 37. Draw the complete e volute of an ellipse whose major and minor axes are 4 inches and 2-75 inches long respectively. 38. The focal distance of the vertex of a parabola is 0-3 inch. Draw that part of the evolute of the parabola which lies between the vertex and a double ordinate whose distance from the vertex is 5 inches. 39. The angle between the asymptotes of an hyperbola is 60° and the vertex is at a distance of 1 inch from their intersection. Draw that part of the evolute of one branch of the hyperbola which lies between the vertex and a double ordi- nate whose distance from the vertex is 5 inches. 40. Draw an ellipse, major axis 3 inches, minor axis 2 inches. Take a point P within the ellipse 0-8 inch from the centre C and lying on a line through C inclined at 30° to the major axis. Through P draw a number of chords of the ellipse and at their extremities draw tangents to the ellipse. Find the pbint of intersection of eadh pair of tangents and see whether the points thus obtained are in one straight line. [By a pair of tangents is meant the tangents at the ends of a chord.] Eepeat the construction for a point Q lying on CP produced, CQ = 2 inches. CHAPTER IV TRACING PAPER PROBLEMS 54. Use of Tracing Paper in Practical Geometry. — Fre- quently draughtsmen have to make geometrical constructions on com- plicated drawings in order to determine some point, line, or figure, and in such cases the fewer the construction lines the better. By using a piece of tracing paper in the manner explained in t .ds chapter the desired result may be obtained very accurately in many cases without making any construction lines whatever on the drawing paper, and some problems can be easily solved by this method whigh would be impossible by ordinary geometrical methods, or which would otherwise involve very complicated constructions. 55. To find the Length of a Given Curved Line. —Let ABCD (Fig. 120) be the given curved line. On a piece of tracing paper TP draw a straight line 1 1, Mark a point A on this line and place the tracing paper on the drawing paper so that this point coincides with one end A of the curved line to be measured. Put a needle point through the tracing paper and into the drawing paper at A. Now turn the tracing paper round until the line 1 1 cuts the curve at a point B not far from A. Remove the needle point from A to B, taking care that the tracing paper does not change its position during the operation. Next turn the tracing paper round until the line on it takes up the position 2 2, cutting the curve at a point C not far from B. The needle point must then be moved to C and the operations continued until a point on the straight line coincides with the last point on the curve. The last point obtained on the straight line must be marked distinctly. The distance between the first and last points marked on the straight line will be approximately equal to the length of the curved line. The approximation will be closer the shorter the steps AB, BC, etc. When the curve has a larger radius of curvature the steps such as AB and BC may be longer than when the radius of curvature is smaller. In Fig. 120 the steps, for the Fig. 120. TRACING PAPER PROBLEMS 55 sake of clearness, are of greater length than would be adopted in practice. The foregoing method is equivalent to stepping off the length of the curve with the dividers, but the tracing paper method has the advantage that the lengths of the different steps may be made to suit the variations of curvature when the curve is not an arc of a circle. It is obvious that this method may also be used to mark off a portion of a given curved line which shall be of a given length. 56. To draw an Involute of a Given Curved Line. — Let ABCD (Fig. 121) be the given curved line. On a piece of tracing paper TP draw a straight line 11. Mark a point A on this line. This point will be called the tracing point. Place the tracing paper on the drawing paper so that the tracing point coincides with the point A on the curve from which the involute is to start. Put a needle point through the tracing paper and into the drawing paper at A. Now turn the tracing paper round until the straight line 1 1 cuts the curve at a point B not far from A. Remove the needle point from A to B, taking care that the tracing paper does not Fig. 121. change its position during the opera- tion. Next turn the tracing paper round until the straight line on it takes up the position 2 2, toucJiing the curve at B, and with a sharp round-pointed pencil make a mark on the drawing paper through the needle hole at the tracing point. If these operations be continued, a number of points are obtained and a fair curve drawn through them will be an approximation to the involute required. The approximation will be closer the shorter the steps AB, BC, etc. 57. To draw a Straight Line to pass through a Given Point and cut two Given Lines so that the Portion inter- cepted between them shall have a Given Length.— Let AB and AC (Fig. 122) be the given lines and D the given point. On a piece of tracing paper TP draw a straight line EF, and mark two points H and K on this line such that HK is equal to the given length. Move the tracing paper into a number of dif- ferent positions on the drawing paper, the point K being on the line AC and the line EF passing through D. A position Fig. 122. will quickly be reached in which the point H is also on the line AB. Now make a mark on the drawmg paper at F ; a line joining this mark with D will be the line required. Instead of using tracing paper for this problem, the points H and 56 PRACTICAL GEOMETRY K may be marked on the straight edge of a strip of paper. This strip of paper may then be moved on the drawing paper until a position is found where H and K lie, one on AB and the other on AC. An ordinary drawing scale may be used in the same way. 58. To draw the Path traced by one Angular Point of a Given Triangle while the other Angular Points move, one on each of two Given Lines.— Let ABC (Fig. 123) be the given triangle. Let A be the tracing point, and let B move on the given line DE while C moves on the given line FH. Draw the triangle ABC on a piece of tracing paper TP. Make a small hole in the tracing paper at A with a needle. Place the tracing paper on the drawing paper so that B is on DE and C on FH. With a sharp round-pointed pencil make a mark on the drawing paper through the needle hole in the tracing paper at A. This will be one point in the path required. By moving the tracing paper into other positions other points may be obtained, and a fair curve KAL drawn through them will be the required path. 59. To draw an Arc of a Circle through Three Given Points without using the Centre of the Circle.— Let A, B, and (Fig. 124) be the given points. Place a piece of tracing paper TP on the draw- ing paper, and draw on the former and AE two straight lines AD passing through B Fig. 124. and C respectively. Make a small hole in the tracing paper at A with a needle. Move the tracing paper round into different positions so that the lines AD and AE always pass through B and C respectively. For each position of the tracing paper make a mark on the drawing paper with a sharp round-pointed pencil through the hole at A. A fair curve drawn through the points obtained in this way will be the arc required. This construction is based on the fact that all angles in the same segment of a circle are of the same magnitude. Another form of this problem is — To describe on a given line BC a segment of a circle which shall contain an angle equal to a given angle BAC. 60. To draw any Roulette.— Let AHB (Fig. 125) be the directing line or base, and let CDE be the rolling curve. (In Fig. 125 the base is a straight line, but it may be any curved line ; and the rolling curve is a circle, but it may also be any curved line.) The base is drawn on the drawing paper and the rolling curve is drawn on a piece of tracing paper. The tracing point P is also marked on the TRACING PAPER PROBLEMS 57 Fig. 125. tracing paper by two lines at right angles, and by a small needle hole. Place the tracing paper on the drawing paper so that the { "^ ^ .j^-j^"^^ P5 rolling curve CDE touches the base, say at C. Make a mark on the drawing paper through the needle hole in the tracing paper at P. Place a needle through the tracing paper and into the drawing paper at C. Turn the tracing paper round about the needle at C until the rolling curve cuts the base at a near point F. Transfer the needle from C to F and turn the tracing paper until the rolling curve touches the base at F. The tracing point will now have moved from P to Pj. Mark the drawing paper at Pj. Again turn the tracing paper until the rolling curve cuts the base at another near point H. Transfer the needle from F to H and turn the tracing paper until the rolling curve touches the base at H. The tracing point will now have moved to Po. Mark the drawing paper at Pg , and continue the process, obtaining the points P3, P4, etc. A fair curve drawn through the points P, Pj , P2, P3, etc., will be the roulette required. In Fig. 125 the roulette is a trochoid. 61. To inscribe in a Given Figure a Figure similar to another Given Figure.— Let ABCD (Fig. 126) be the given figure in which it is required to inscribe a figure similar to a second given figure EFHK. Draw the figure EFHK on a piece of tracing paper. Take a point on the tracing paper as a pole (prefer- ably one angular point of the figure EFHK, say E) and join this point to each of the angular points of the figure on the tracing paper. Graduate these lines, the divisions being proportional to the distances of the pole from the angular points of the figure. In the example illustrated EF, EH, and EK are each divided into two equal parts, and the gradua- tions are extended on these lines produced. Place the tracing paper on the drawing paper and move the former about until the sides of the figure ABCD on the drawing paper cut the lines through the pole on the tracing paper at corresponding points L, M, and N; then prick the drawing paper through the tracing paper at these corre- sponding points and the positions of the angular points of the figure required are obtained. Fig. 126. 58 PRACTICAL GEOMETRY It may happen that the corresponding points mentioned are not at points of graduation on the lines through the pole. In that case the graduations must be made finer in the neighbourhoods where they appear to be required. If the corresponding points required are still not at points of graduation, it may be possible, without further sub- division, to judge by the eye whether the points where the polar lines cut the sides of the first given figure are corresponding points. 62. Drawing Symmetrical Curves. — When a curve is sym- metrical about an axis only the part on one side of that axis need be constructed, the part on the other side may be quickly and accurately drawn by means of a piece of tracing paper as follows. Referring to Fig. 127, at (a) is shown one half of a curve which is symmetrical about the axis YY. A piece of tracing paper TP is Fig. 127. Fig. 128. placed over this figure and the curve and the axis YY are traced in pencil. The tracing paper is then turned over and placed as shown at (h) and the curve on the tracing paper is traced with the pencil. It will then be found that the second half of the curve has appeared on the drawing paper in pencil, the lead for this curve having come from the lead which was put on the tracing paper when it was in the position (a). After removing the tracing paper the curve traced should be lined in to make it more distinct. When a curve is symmetrical about two axes at right angles to one another only one quarter of the curve need be constructed, the other three quarters may be drawn, one quarter at a time, by means of a piece of tracing paper as just described. Fig. 128 shows the method applied to an ellipse. At (1) is shown one quarter of the ellipse constructed, say, by the trammel method. A piece of tracing paper TP is placed over this and on it are traced the semi-axes and the curve lying between them. Turning the tracing paper over and placing it as shown at (2) the second quarter of the curve is transferred to the drawing paper, the lead coming from the first tracing. Turning the tracing paper over again and placing it as shown at (3) the third quarter of the curve is transferred to the draw- ing paper, the lead coming from the second tracing. Turning the TRACING PAPER PROBLEMS 59 traciDg paper over once more and placing it as shown at (4) the last quarter of the curve is obtained. Exercises IV The foUowing exercises are intended to he luorked out by the tracing paper method 1. Find the circumference of a circle 3 inches in diameter, and compare the result with that got by calculation. 2. The sides of a figure ABC are arcs of circles. Radius of AB = li inches, radius ©f BG = 2 inches, radius of CA = 2J inches. The arcs touch one" another in pairs at A, B, and G. Find the perimeter of the figure ABC. 3. Draw the involute of a circle 2 inches in diameter. Also draw a tangent to the circle to meet the involute, the length of this tangent between the involute and the point of contact with the circle to be 5 inches. Find also the length of the involute between the starting point and the point where the forementioned tangent meets it. 4. Draw an ellipse, major axis 2 inches, minor axis 1| inches, and draw that involute of the ellipse which starts from one extremity of the major axis. Find the circumference of the ellipse. 5. ABC is an equilateral triangle of 3 inches side. D is a point in AB 1 inch from A. Draw through D a straight line to cut the side AC at E, and the side CB produced at F, such that EF = 4J inches. 6. Draw an ellipse, major axis 3 inches, minor axis 2 inches. Take a point P, 2 inches from one extremity of the minor axis, and 1^ inches from one extremity of the major axis. Through P draw a straight line to cut the ellipse in two points which shall be 2 inches apart. 7. X'OX and Y'OY are two straight lines intersecting at 0. Angle XOY = 60°. A straight line AB, 3 inches long moves with the end A on X'OX, and the end B on Y'OY. Draw the complete curve traced by a point P in AB which is 1 J inches from A. Draw also the curve traced by the middle point of AB. 8. ABC is an equilateral triangle of 3 inches side. The triangle moves with the point A on the circumference of a circle 2| inches in diameter, and the point B moves on a diameter of that circle produced. Draw the path traced by the point G. Draw also the path traced by the middle point of AB. 9. On a straight line 3 inches long descriljp a segment of a circle containing an angle of 120°, without using the centre of the circle. 10. is the centre and OP a radius of a circle 2 inches in diameter. Q is a point in OP f inch from O, and R is a point in OP produced, and IJ inches from O. Draw the cycloid described by P, also the trochoids described by Q and R, as the circle rolls on a straight line. Draw as much of each curve as is obtained by a little more than one revolution of the circle. 11. Taking the same rolling circle and the same points Q and R as in the pre- ceding exercise, draw the epicycloid described by P, and the epitrochoids described by Q and R as the circle rolls on the outside of a base circle 3 inches in diameter; draw also the hypocycloid described by P, and the hypotrochoids described by Q and R as the circle rolls on the inside of the same base circle. Draw as much of each curve as is obtained by a little more than one revolution of the rolling circle. 12. Draw the roulette described by one extremity of the major axis of an ellipse (major axis, 2^ inches, minor axis, If inches) which rolls on the outside of another ellipse (major axis, 3 inches, minor axis, 2 inches). The roulette to start from one extremity of the minor axis of the fixed ellipse. ^ Draw also, on the same figure, the roulette described by one extremity of the minor axis of the roll- ing ellipse while the first roulette is being described. 13. AB is a straight line 3 inches long. BC is an arc of a circle whose centre 60 PRACTICAL GEOMETRY is in AB and 2i inches from B, and whose chord is 4 inches long. AC is an arc of a circle of 3 inches radius whose centre is on that side of AG which is remote from B. Draw the largest possible equilateral triangle which has its angular points, one on each of the sides of the figure ABC. 14. ABCD is a quadrilateral. AB = 2i inches, BC = If inches, CD = 1^ inches, DA = 2 inches, and AC = 2f inches. In this quadrilateral inscribe a square. CHAPTER V APPROXIMATE SOLUTIONS TO SOME UNSOLVED PROBLEMS 63. Rectification of Circular Arcs. — The ratio of the cir- cumference of a circle to its diameter cannot be expressed exactly, in other words the two are incommensurable. The symbol tt is always used to denote the ratio of the circumference to the diameter and its approximate value is 3-1416 or nearly 3h The best geometrical constructions hitherto given for finding approximately the length of a circular arc, or for marking off an arc of given length, are those due to Rankine,^ and are as follows : — (a) To draw a straight line approximately equal to a given circular arc AB (Fig. 129), Join BA and produce it to D making AD Fig. 130. = iAB. With centre D and radius DB describe the arc BC cutting at C the tangent AC to the arc at A. AC is the straight line requij-ed. Tie error varies as the fourth power of the angle AOB, where O is the centre of the circle of which AB is an arc. When the angle AOB is 30°, AC is less than the arc AB by about -^^ of the length of the arc. (h) To marJc off" on a given circle an arc AB approximately equal to a given length (Fig. 130). Draw a tangent AC to the circle at A, and make AC equal to the given length. Make AD = ^AC. With centre D and radius DO describe the arc CB to cut the circle at B. AB is the arc required. 1 A Manual of Machinery and Millwork. 62 PRACTICAL GEOMETRY The error in (h) as a fraction of the given length is the same as in (a), and follows the same law. If in Fig. 129- the angle AOB is gi-eater than one right angle and less than two right angles the length of one half of the arc AB should be determined by the construction and the result doubled. If the angle AOB is greater than two right angles the length of one quarter of the arc AB should be determined by the construction and the result quadrupled. If in Fig. 130, AC is greater than one and a half times the radius OA the arc equal to one half of AC should be determined by the construction and this arc should then be doubled. If AC is greater than three times OA the arc equal to one quarter of AC should be determined by the construction and this arc should then be quadrupled. The construction in (h) follows easily from that in {a), for if the construction in Fig. 129 be performed and CD be joined (Fig. 131), and the angle CDB be bisected by DE meeting AC at E, a circle with Fig. 131. centre E and radius EC will pass through B. Since CD = DB = 3AD, and since DE bisects the angle CDB, it follows (Euclid VI, 3) that CE'=3AEor AE = iAC. The following slight modification of Rankine's first construction (a) gives a more approximate result, and is to be preferred, especially when the angle AOB is greater than 60°. Instead of making AD equal to half the chord AB make it equal to the chord AF of half the arc AB (Fig. 132) and proceed as before. For the case where the angle AOB is 90° the error in Rankine's construction is about 1 in 170 while in the modified construction the error is only about 1 in 2300. 64. To draw a Straight Line whose Length shall be approximately equal to the Circumference of a Given Circle. — Draw a straight line whose length shall be approximately equal to a quarter of the circumference by the modification of Rankine's con- struction explained in the preceding article ; a line four times this in length will be the line required. The following construction given by the late Mr. T. H. Eagles ^ ^ Constructive Geovietry of Plane Curves, p. 267. APPROXIMATE SOLUTIONS 63 gives a very close approximation. O (Fig. 133) is the centre and AOB a diameter of the given circle. Draw the tangent AC and make AC equal to three times AB. Draw a radius OD making the Fig. 133. angle BOD = 30^. Draw DE at right angles to AB meeting the latter at E. Join EC. The length of EC is very nearly equal to the circumference of the circle. EC is a little longer than the true circumference, the error being about 1 in 21,700. 65. To draw a Straight Line whose Length shall repre- sent approximately the Value of tt. — The circumference of a circle of radius r is 27rr, and therefore a quarter of the circumference is -—. If r = 2, then a quarter of the circumference is equal to tt. 'A Hence if a quarter of a circle be drawn with radius = 2, the length of the arc will be equal to tt, and this length may be determined by one of the constructions of Art. 63. Instead of taking a quarter of a circle with a radius = 2, a sector whose angle is 60° and radius = 3 may be used, or generally a sector whose angle is n°, and radius = may be taken, and the length of its arc will be equal to tt. n The circumference of a circle whose radius is 0*5 is equal to tt and TT may therefore be found by the construction given in the latter part of Art. 64, by making r equal to 0*5. 66. To find the Side of a Square whose Area shall be approximately equal to that of a Given Circle.— Solving this problem is known as " squaring the circle." O is the centre and AB a diameter of the given circle. Fir^t Method (Fig. 134). Draw AC at right angles to AB and Fig. 134. Fig. 135. equal to AO. Draw BC cutting the circle at D. Join BD. BD is the line required. The error in this construction is that BD is too 64 PRACTICAL GEOMETRY long by an amount equal to 0"0164r, where r is the radius of the circle. Second Method (Fig. 135). Produce AB to E, and make BE equal to three times BO. With centre A and radius AO describe the arc OC. With centre E and radius EA describe the arc AC to cut the former arc at C. Draw CE cutting the circle at D. Join BD. BD is the line required. The error in this construction is that BD is too short by an amount equal to O'OOOTr, where r is the radius of the circle. 67. To draw a Straight Line whose Length shall repre- sent approximately the Value of the Square Root of tt.— The area of a circle whose radius is r is 7rr^, and if s is the side of a square whose area is equal to that of the circle, then s^ =7rr'-, or 8 = TaJ TT. Ifr=l, then s = /J tt, and this may be found by one of the constructions in the preceding article. 68. To find the Side of a Square whose Area shall be approximately equal to that of a Given Ellipse.— If a and h are the semi-axes of an ellipse its area is irob.. If r is the radius of a circle equal in area to the ellipse, then -n-r = Trafc, or r^ = ah, and r is a mean proportional between a and h and may be found as in Art. 12, p. 11. The side of a square whose area is approximately equal to that of the circle may then be found by the construction of Art. 66. 69. To inscribe in a Given Circle a Regular Polygon having a Given Number of Sides. — AB (Fig. 136) is a diameter and O the centre of the given circle. With centre A and radius AB describe the arc BC. With centre B and radius BA de- scribe the arc AC cutting the former arc at C. Divide the diameter AB into as many equal parts as there are sides in the polygon. D is the second point of division from A. Draw CD and produce it to cut the circle at E. The chord AE is one side of the polygon, and the others are obtained by stepping the chord AE round the circle. The above construction is exact for an equilateral triangle, a square, and a hexagon. For a pentagon the central angle AOE is Fig. 136. too small, and when the chord AE is stepped round from A five times, the last point will fall short of A by an amount which subtends at an angle of nearly a quarter of a degree. For a heptagon the central angle AOE is too large, and when the chord AE is stepped round from A seven times, the last point will be beyond A by an amount which subtends at an angle of a little more than five-eighths of a degree. APPROXIMATE SOLUTIONS 65 Exercises V 1. Draw an arc of a circle of 2 inches radius subtending an angle of 60° at the centre of the circle ; then draw by Rankine's construction, a straight line equal in length to the arc. 2. From the circumference of a circle of 2 inches radius cut off, by means of Rankine's construction, an arc equal in length to the radius. 3. Find, by construction, and by calculation, the circular measure of an angle of 45°. 4. Construct an angle whose circular measure is 1*2. 5. Find, by construction, and by calculation, the circumference of a circle whose diameter is 2'75 inches. 6. Find, by construction, and by calculation, the diameter of a circle whose circumference is 6 inches. 7. Find, in the simplest possible way, the diameter of a circle whose circum- ference is equal to thei sum of the circumferences of two circles one of which is 1-75 inches, and the other 1*25 inches in diameter. 8. Draw a square whose area shall be equal to that of a circle whose radius is 1*5 inches. 9. Draw a circle having an area equal to that of a square of 2-25 inches side. 10. Construct a square having an area equal to that of an ellipse whose major and minor axes are 3-5 inches and 2-5 inches respectively. 11. In a circle of 2 inches radius inscribe a regular heptagon. CHAPTEE VI ROULETTES AND GLISSETTES 70. Roulettes. — When one curve rolls without sliding on another curve, any point connected with the first curve describes on the plane of the second a curve called a roulette. The curve which rolls is called the rolling curve or generating curve ^ and the curve on which it rolls is called the directing curve or base. The directing curve is generally assumed to be fixed, and is sometimes called t\iQ fixed curve. When the rolling and directing curves are circles the roulette becomes a cycloidal curve. 71. General Construction for Drawing a Roulette. — The best practical method of drawing any roulette is the tracing paper or transparent templet method which is described in Art. 60, p. 56. The following is a general construction which may be used for drawing any roulette. ABCD (Fig. 137) is the base, Abed is the rolling curve, and P is the tracing point. Take a number of points h, c, d, etc. on the rolling curve and determine points B, C, D, etc. on the base such that the arcs AB, BC, CD, etc. are equal to the arcs A?>, 6c, cd, etc. respectively. If the points are sufficiently near to one another the arcs may be assumed equal to their chords. Draw tangents to the base at B, C, D, etc. and tan- gents to the rolling curve at h, c, d, etc. From P draw Pm perpendicular to the tangent at h. On the tangent at B make BM = hm, and draw MP, perpendicular to BM and equal to Pm. Pi will be the position of P when the rolling curve touches the base at B, and will therefore be a point in the roulette described by P. manner other points may be determined. 72. General Construction for the Centre of Curvature of a Roulette. — Three cases are illustrated in Figs. 138, 139, and 140. The description which follows applies to each. Oi is the centre of curvature of the base line AQB at Q. (If AQB Fig. 187. In like ROULETTES AND GLISSETTES 67 is an arc of a circle then Oj is the centre of the circle, and if AQB is a straight line (Fig. 140), then O^ is at an infinite distance from Q in a straight line through Q at right angles to AQB.) Fig. 139. Fig. 140. O.^ is the centre of curvature of the rolling curve CQD at Q. (If CQD is an arc of a circle, then Og is the centre of the circle.) P is the position of the tracing point when the rolling curve is in the position shown. Join PQ. Draw QR at right angles to PQ to meet POg or POg produced at R. Join ROj and produce it if necessary to meet PQ or PQ produced at S. S is the centre of curvature of the roulette at P. When P, O2, and Q are in a straight line the above construction T ^i,- ark QO1XQO2XPQ ^, , . ^. In this case, SQ = ==: ^=—4=—-^^^, the plus sign being fails. QOi X POo^t QO2 xPQ taken when 0^ and O2 are on opposite sides of Q, and the minus sign being taken when O, and O2 are on the same side of Q. PQ = PO2 ± QO2. If AB is a straight line then QO^ is infinite and SQ = If PO2 = QO2, then SQ = QO2 X PQ PO2 * QOi X PQ QOi ±Fq' 73. The Cycloid. — The cycloid is the curve described by a point on the circumference of a circle which rolls on a straight line, the circle and straight line remaining in the same plane. The ordinary geometrical construction for drawing the cycloid is shown in Fig. 141. mo'e' is the straight line upon which the circle "Pho'q rolls and P is the point which describes the cycloid. Tho'q is the rolling circle in its middle position, the diameter POo' being at right angles to mo'e'. Make o'e' equal to half the circumference of the rolling circle. Divide o'e' into a number of equal parts at a', h', c', etc. (preferably six, but for 68 PRACTICAL GEOMETRY the sake of a clearer figure o'e' in Fig. 141 has been divided into five equal parts). Divide the semicircle Pbo' into the same number of equal parts at a, 6, c, etc. Through O draw OE parallel to o'e'. From rt', b', c', etc. draw perpendiculars to o'e' to meet OE at A', B', C, etc. With centres A', B', C, etc. describe arcs of circles touching o'e\ and through a^ 6, c, etc. draw parallels to o'e' to cut these arcs at A, B, C, etc. as shown. The points A, B, C, etc. are points on the half of the cycloid traced by the point P as the circle P6o' makes half a revolution to the right. Points on the other half of the cycloid may be obtained in a similar manner, or, since the curve is sym- metrical about Po' the part to the left of Po' may be copied from the part to the right. If from a point q on the circle Vbo'q a line be drawn parallel to the base line mo' to meet the cycloid at Q then QR parallel to qo' is the normal and QT parallel to qV is the tangent to the cycloid at Q. ■ ' P ► — ^ \B ^^-"^ '^f/ ^ "^'^^s. /^ / \ 6> >v / A/" A 1 B' ] C'/N . E \. I J^^^ 1 v ^ / / ' \c \\/ / // / A ^rS^v,^^ ,y ^^^ / 1// Y ^\::\ ^^v ^ ^ r^^ ^.^ J \ & a! /ycj. L Fig. Ml. Again, if PT be drawn parallel to md to meet at T the tangent to the cycloid at Q, the length of the arc PQ of the cycloid will be twice the length of the tangent QT or twice the length of the chord g-P. Hence the total length of the cycloid is four times the diameter of the rolling circle. If QR be produced to S and RS is made equal to QR then S is the centre of curvature of the cycloid at Q. The locus of S is the evolute of the cycloid. If the rolling circle be drawn below the base line md and touching that line at R it is obvious that this circle will pass through S. Also if the rolling circle be drawn above the base line and touching it at R this circle will pass through Q and since the chord RS is equal to the chord QR the arc RS must be equal to the arc QR. But the arc QR is equal to mR, and md is equal to half the circum- ference of the rolling circle, therefore if RU is a diameter of the circle RSU, the arc S CJ is equal to Ro'. Hence if a line UL be drawn pai'a-Uel to md and the circle RSU be made to roll on this line the ROULETTES AND GLISSETTES 69 The point S will describe a cycloid equal to the original cycloid, evolute of a cycloid is therefore an equal cycloid. 74. The Trochoid.— When a circle rolls on a straight line and remains in the same plane, a point in the plane of the circle, con- nected to the circle but not on its circumference, describes a trochoid. If the describing point is outside the rolling circle the trochoid is called a superior trochoid. If the describing point is inside the rolling circle the trochoid is called an inferior trochoid. A superior trochoid is also called a curtate cycloid and an inferior trochoid is also called a prolate cycloid. The geometrical construction for finding points on a trochoid is similar to that already given for the cycloid and is shown in Fig. 142. mo'^n' is the base line. P is the position of the describing point when it is furthest from the base line and O is the corresponding position of the centre of the rolling circle, o'm' is made equal to half the circum- ference of the rolling circle. The points a', b', c', etc. and A', B', C, etc. are determined as for the cycloid. With centre and radius OP describe a circle, and divide the half of this circle which is to the right of OP into as many equal parts as o'm' is divided into. This determines the points a, h, c, etc. Through a, b, c, etc. draw parallels to the base line and with centres A', B',C',etc. andradius equal to OP describe arcs of circles to cut these parallels at A, B, C, etc. as shown. A, B, C, etc. are points on. the half of the trochoid described by the point P as the rolling circle makes half a revolution to the right. Points on the other half of the trochoid may be obtained in a similar manner, or, since the curve is symmetrical about OP, the part to the left of OP may be copied from the part to the right. If from a point q on the circle qFb a line be drawn parallel to the base line to meet the trochoid at Q, then QR parallel to cjo' is the 70 PRACTICAL GEOMETRY normal and QT perpendicular to QR is the tangent to the trochoid at Q. Draw RV perpendicular to the base line to meet the parallel through to the base line at V. V is the position of the centre of the rolling circle when the describing point is at Q. To find S the centre of curvature of the trochoid at Q, draw RN perpendicular to QR to meet QV produced at N" and draw NS perpendicular to the base line«to meet QR produced at S. The evolute of the trochoid is the locus of the centre of curvature S. The evolute of the superior trochoid is shown in Fig. 142. The evolute of the inferior trochoid is partly on one side and partly on the other side of the curve, and the normals which have the least inclina- tion to the base line are asymptotes of the evolute. 75. The Epicycloid. — When a circle rolls on the outside of a fixed circle, the two circles being in the same plane, a point on the circumference of the rolling circle describes an epicycloid. The ordinary geometrical construction for finding points on an epicycloid is shown in Fig. 143. P is the position of the tracing point Fig. 143. when it is furthest from the fixed or base circle, is the corresponding position of the centre of the rolling circle and o' is the corresponding point of contact of the rolling and base circles. Oj is the centre of the base circle. Make the arc om equal to half the circumference of the rolling circle. Join O^m and produce it to meet at M the circle through O concentric with the base circle. Divide the arc OM into a number of equal parts (preferably six or eight) at A', B', C, etc. and divide the semicircle Pco' into the same number of equal parts at a, h, c, etc. ROULETTES AND GLISSETTES 71 With centre d, describe arcs of circles through a, h, c, etc. and with centres A', B', C, etc. and radius equal to OP describe arcs of circles to cut the former arcs at A, B, 0, etc. as shown. A, B, C, etc. are points on the half of the epicycloid described by P as the rolling circle rolls from o' to m. Points on the other half of the epicycloid may be obtained in a similar manner, or, since the curve is symmetrical about OiP, the part to the left of OiP may be copied from the part to the right. The centre of curvature of the epicycloid at any point Q is found as follows. Draw the rolling circle in the position which it occupies when the tracing point is at Q as shown. V is the centre of the rolling circle in this position and R is its point of contact with the base circle. Join QV and produce it to meet the rolling circle again at N. Join OiN. Join QR and produce it to meet OjN at S. QR is the normal and S is the centre of curvature of the epicycloid at Q. QT at right angles to QR is the tangent to the epicycloid at Q. The locus of S is the evolute of the epicycloid. Join OiR and draw SU perpendicular to QS to meet O^R at U. On UR as diameter describe the circle RSXJ, and with centre Oi and radius OiU describe another circle. If the circle RSU be made to roll on the outside of the circle whose centre is Oi and radius OiU, the point S will describe an epicycloid which will coincide with the evolute of the original epicycloid. This epicycloid which is the evolute of the original epicycloid is similar to it. Two epicycloids are similar when the ratio of the radii of their rolling circles to one another is the same as the ratio of the radii of their base circles. It may be pointed out here that a given epicycloid on a given base circle may be described by a point on the circumference of either of two different rolling circles. Referring to Fig. 144, APB is an Fig. 144. Fig. 145. epicycloid on the base circle LMN. This epicycloid may be described by a point on the circumference of the rolling circle PQN or by a point on the circumference of the rolling circle CPD. The three circles are such that the diameter of the base circle is equal to the difference between the diameters of the two rolling circles. It will 72 PRACTICAL GEOMETRY be observed that while both rolling circles roll on the outside of the base circle the base circle is inside the larger rolling circle. An interesting case of the epicycloid is that in which the rolling circle is equal to the base circle. This is shown in Fig. 145, where OLN is the base circle and OQP the epicycloid. PMN is the position of the rolling circle when the tracing point P is furthest from the base circle. The two ends of the epicycloid meet at forming a cusp at that point. If a straight line OLQ be drawn cutting the base circle at L and the epicycloid at Q then it is not difficult to prove that LQ is equal to ON the diameter of the base circle. This property suggests a simple method of finding points on this particular form of epicycloid. This form of the epicycloid is known as the cardioid. If the angle which OQ makes with OP be denoted by ^ then 0Q = QL + L0 = QL4-0N cos ^ or r = tZ (1 + cos 6) where r = OQ and d is the diameter of the circle OLN". This is the polar equation to the cardioid. The normal to the curve at Q may be found by the construction already given or more simply as follows. Through N draw NRj parallel to OQ to meet the circle again at Rj. QRj is the required normal. The tangent QT at Q is of course perpendicular to QR^. 76. The Epitrochoid. — When a circle rolls on the outside of a fixed circle, the two circles being in the same plane, a point in the plane of the rolling circle, connected to it but not on its circumference describes an epitrochoid. The epitrochoid is called a superior epitrochoid or an inferior epitrochoid according as the describing point is outside or inside the rolling circle. Fig. 146. ROULETTES AND GLISSETTES 73 The geometrical construction for finding points on an epitrochoid is shown in Fig. 146. The construction is so like that already used for the cycloid, the trochoid, and the epicycloid that no detailed description of it need be given here. The centre of curvature of the epitrochoid at any point Q is found as follows. Draw the rolling circle in the position which it occupies when the tracing point is at Q as shown. V is the centre of the rolling circle in this position and R is its point of contact with the base circle. Join QV and produce it. Join QR and produce it. Draw RN at right angles to QR to meet QV produced at N. Join OjN cutting QR produced at S. QR is the normal and S is the centre of curvature of the epitrochoid at Q. 77. The Hypocycloid. — When a circle rolls on the inside of a fixed circle, the two circles being in the same plane, a point on the cir- cumference of the rolling circle describes a hypocycloid. The geometrical construction for finding points on a hypocycloid is shown in Fig. 147. After what has been done in preceding articles no detailed description of this construction is necessary. a .^' — < (I d b to A. Observe that as the Bi * ' Xj — j I I h~^^ sense of A is from left to right C i * • Oa is measured to the right of Di * ' ^^ * 0. Make ah equal to B, Fig. 161. measuring to the right of a because the sense of B is from left to right. Make he equal to C, measuring to the left of h because the sense of C is from right to left. Make cd equal to D, measuring to the right of c because the sense of D is from left to right. Then Od is a vector which is the sum or 84 PRACTICAL GEOMETRY resultant of the vectors A, B, C, and D. If R is the resultant of the vectors A, B, C, and D, then R = A-|-B + C + D. If a vector whose sense is from left to right is said to be posi- tive, then a vector whose sense is from right to left would be said to be negative. Then the result of the above example would be written R = A + B-C + D. Opposite signs represent opposite senses. Subtraction of parallel vectors is converted into addition by changing the signs of the vectors to be subtracted and then pro- ceeding as in addition. It should be observed that in the addition of vectors the order in which they are taken does not aftect the result. For A -h B -f C + D = A + B + D-fC = B-fD4-A + C. 85. Addition of Inclined Vectors. The Vector Polygon. Let A, B, and C (Fig. 162) be three given vectors, it is required to find a single vector which is the sum or re- sultant of the vectors A, B, and C. b > r Take a point o and draw the vector oa C \ > i /\\ /^ parallel and equal to A. The sense of oa is ^ / \ \^' \ from to a the same as that of A. The \ya^ \ f^/'^^ vector A is now represented by oa. From >fX ^v I '/' ' ' a draw the vector ah parallel and equal to B. /^ V ^J/' ' The sense of ah is from a to h the same as ° ^ £, ""/l that of B. The vector B is now represented Fig. 162. by ah. From h draw the vector he parallel and equal to C. The sense of he is from 6 to c the same as that of C. The vector C is now represented by he. Join oc, then the vector oe whose sense is from o to c is the sum or resultant of the vectors A, B, and C. The polygon oahe is called a vector polygon. The vector polygon is of very great importance in vector geometry and it has numerous applications in mechanics. It will be useful to consider the vector polygon as applied (1) to displacements, (2) to velocities, (3) to accelerations, and (4) to forces. (1) Suppose a man to be standing on the deck of a ship which is sailing through water which is itself moving in relation to the earth. Let the man walk across the deck along a straight line whose length and direction in relation to the ship are given by the vector A (Fig. 162). Let the vector B represent the direction and distance which the ship sails through the water in the time that the man walks the distance A. Lastly let the vector C represent the direction and distance which the water moves in the same time. Let the vector polygon oahe (Fig. 162) be drawn. While the man is walking along oa that line is carried parallel to itself by the ship into the position mh. Consequently, neglecting for the moment the motion of the water, the man travels along the imaginary line oh over the water. But while this is happening the imaginary line oh is travelling parallel to itself with the water and reaches the position nc when the man has finished his walk. The actual displacement of the VECTOR GEOMETRY 85 man in relation to the earth is therefore represented by the line oc. That is, oc is the sum or resultant of the three displacements A, B, and C. (2) Since velocity is displacement or distance moved in unit time it follows that if t is the time taken by the man in walking the distance A, t will also be the time of the displacement B of the ship suad of the displacement C of the water, and if each displacement is divided by t the results are the several velocities. Hence the . . oa ah he oc velocities are y, —, — , and —^ and the polygon oahc, measured with a suitable scale, will be a polygon of velocities in which oa represents the velocity of the man's walking on the ship, ah represents the velocity of the ship through the water, he represents the velocity of the water over the earth, and oc is the resultant velocity of the man or his velocity in relation to the earth. (3) Let / denote the uniform acceleration or uniform rate of increase of the velocity of a moving body, then in time t the increase in velocity is ft. If A, B, and (Fig. 162) represent three accelera- tions simultaneously imj^ressed on a body these will also represent three corresponding increases in velocity and the resultant increase in velocity will be represented by oc, and oc will therefore represent the resultant acceleration, oahc is therefore an acceleration polygon. (4) A force acting on a body causes it to move with a uniformly increasing velocity or acceleration and the magnitude of the acceleration is proportional to the magnitude of the force and takes place in the same direction as that of the force. Hence if oahc (Fig. 162) is an acceleration polygon it is also a force polygon. If R is the sum or resultant of the vectors A, B, and C, then R = A -f- B + and the order in which the vectors are taken in performing the summation is immaterial. That is, if R = A + 1^ + CJ, then, also, R = B + A-fC = C + A4-B. The addition is per- formed by drawing the vector polygon, three sides of which are A, B, and C, and the fourth or closing side is R. Observe that if R = A -f B + C, then A + B + C-R = 0, which shows that if the sense of R is reversed the sum of the four vectors A, B, C, and R is zero. When the sum of a number of vectors is zero the vector polygon closes without the use of another vector. / / \C 86. Subtraction of / \ A/fTn) Vectors.— At (/) Fig. 163, V -' v ^^ / three vectors A, B, and C are given, B and C being equal and parallel but the sense of C is opposite to that of B. Hence C = -B. If R = A - B then R = A + C. The solution of R = A + C is shown at (m) and the solution of R = A — B is shown at (n). R=A+C Fig. 163. 86 PRACTICAL GEOMETRY The rule for subtraction is evidently, change the sign of the vector to be subtracted and then proceed as in addition. 87. Example. — A, B, C, and D are four vectors specified as follows. A = 2-460O, B = 1-5 tudes being in inches. It is required to find the value 330O, C = 2-09^0, and D = 2-li8oo, the magm- as ScaLe^ R=A+B-C+D Fig. 164. A + B-C + D = r0. of K = A + B-C + D. The magnitudes and direc- tions of A, B, C, and D are shown to the right in Fig. 164. Take a point 0. Draw oa parallel and equal to OA. From a draw ah parallel and equal to OB, then oh is equal to A + B. From h draw he parallel to DC reversed and equal to 00, then oc is equal to A + B — C. From c draw cd parallel and equal to OD, then od is equal to R R will be found to be equal to 0*79;5oi^. 88. Resolution of Vectors. — If R is the sum or resultant of any number of vectors A, B, C, D, etc., then A, B, C, D, etc., are called the components of the vector R. The operation of finding R when A, B, C, D, etc., are given is called .the summation of vectors or composition of vectors. The converse operation of breaking up a vector into a number of components is called the resolution of a vector. It is evident that a given vector may be resolved into any number of components by constructing a polygon on the given vector. Generally when a vector has to be resolved into components only two components are required the directions of which are given. Let R or ah (Fig. 165) be a given vector and let OX and OY be two given directions ; it is required to resolve R into two components P and Q whose directions shall be parallel to OX and OY respectively. Through a draw ac parallel to OX and through h draw he parallel to OY to meet ac at c, then ac and ch will be the required components P and Q. A common case in practice is that in which the angle XOY is a right angle. 89. Example. — The thick curved line shown in Fig. 166 represents the section of a vane of a water wheel or turbine which revolves about an axis at O. A jet of water impinges on the vane at A with a velocity v-^. The jet is then deflected and flows over the vane leaving it at B. The wheel revolves in the direction of the arrow R. The radius of the wheel at A is r^, and the linear velocity of the vane at A is c^. The radius of the wheel at B is r^ and the linear velocity of the vane at B is c^. Obviously Cg : Ci : : r2 : r^. Fig. 165. VECTOR GEOMETRY 87 C-- .'<-^' Fig. 166. Consider the water in the jet at A where it comes in contact with the vane. This water is beginning to slide along the vane with a velocity s in a direction tangential to the vane at A. This water is also carried round with the wheel with a velocity Cj in the direction of the tangent to the wheel circle at A, and in order that there shall be no shock the resultant of these two velocities s and c, should be Vj^. Of the three velocities v^, c^, and s, if one be known com- pletely and the directions of the other two are given, their magnitudes are readily found. Or if two of the velocities be known completely, the magnitude and direction of the other is readily found. Assume that the water slides along the vane with a constant velocity s relatively to the vane and consider the water in the jet at B. This water has a velocity 8 in the direction of the tangent to the vane at B and also a velocity Cg in the direction of the tangent to the wheel circle at B. Hence BD or v^ the resultant or absolute velocity of the water at B is the resultant of the velocities s and c^. Draw BC parallel and equal to v^ and join CD; then CD is the vector change Vg — v^ in the velocity of the water in passing over the vane. The actual path of a particle of water in passing through the wheel may be found as follows. Make the arc AE equal to a definite fraction of s. With centre O and radius OE describe the arc EF. Make the arc EF equal to the same fraction of c, the velocity of the wheel at E, that the arc AE is of s. Then F is a point in the actual path AFK of a particle of water which enters the wheel at A. Exercises VII 1. Three vectors, A, B,.and G, acting in a horizontal plane are defined in the following table :— See also Fig. 167. Vector. Magnitude. Direction A B C 1-23 units 1-95 „ 2-60 „ Eastwards. 33-2° northwards of east. 112° northwards of east. A + B + C Fig. 167. 88 PRACTICAL GEOMETRY The angles of 33-2° and 112° are to be set off with the protractor, and not by copying the diagram. Determine the resultant or vector sum A + B + C, using a scale of 1 inch to 1 unit. Measure and tabulate the results (thus completing the above table). Theorem : — A vector sum is the same in whatever sequence the vectors are added. Verify this principle by actual drawing in the following case : — Show that A + B + C = A + C + B. [B.E.] 2. Three coplanar vectors A, B, C are given as follows : — Vector. Magnitude. Direction. A B C 37-2 units 59-5 „ 88-0 „ 23-6° 115-5° 238-0° A + B + C A-B + C Fig. 168. In defining direction, the vectors are supposed to act outwards from a point O (Fig. 168), and the angles are measured anti-clockwise from a fixed line OX. These angles must be set of! with a protractor, and not copied from the diagram. Find A + B + C and A — B + C. Measure and record the results (in the form required to complete the foregoing table). Verify by drawing that A - (B - C) = A - B + C. ' Use a scale of J inch to 10 units. [b.e.] 3. Find the vector sum A + B + C + D + E, having given A = 2-15qo l-60„o, C = 2-25,300, B being 1 inch. 4. Four coplanar forces P, Q, follows :— P = 15„o, Q = 9, D = 2-80qo, and E = 5 35,o„o, the unit of magnitude R, and S, acting at a point, are specified as S = 21, --0, the magnitudes of Find the resultant of these forces, and specify it in 0"' "* — "21; the forces being in pounds, the form T = t^o- Use a scale of 1 inch to 10 pounds. 5. A locomotive engine A represented by a point is approaching a level cross- ing C from the south at a speed of 15 miles an hour (22 feet per second), that is velocity of A = 22gQO f.s., directions being measured anti-clockwise from the east. An engine B is approaching from the W.S.W., its velocity being 44.22io f.s. They a,rrive together at C. (a) Show their positions one second before the collision, scale 1 inch to 10 feet. Measure their distance apart and the direction from A to B. (6) What is the relative speed of the two engines when the accident occurs? [b.e.] 6. An aeroplane is headed due west, and is propelled at 50 miles per hour relatively to a steady wind which is blowing at 20 miles per hour from the north- west. Find the actual direction and speed of flight as regards the earth. If the pilot wishes to travel westward, in what direction must he apparently steer, and what will be his speed to the west ? [b.e.] 7. A ship is sailing eastwards at 10 miles an hour. It carries an instrument for recording the apparent velocity of the wind, in both magnitude and direction. (a) If the wind registered by the instrument is apparently one of 20 miles per hour from the north-east, what is the actual wind ? Give the answer in miles per hour and degrees north of east of the quarter from which the wind comes. (6) If a wind of 15 miles per hour from the north-east were actually blowing, what apparent wind would the instrument on the vessel register ? State this answer in miles per hour and degrees north of east as before. Use a scale of J inch to 1 mile per hour, [b.e.] YECTOR GEOMETRY 89 8. A weight of 15 pounds is supported by two cords. One cord is inclined at 40° and the other at 55° to the horizontal. Determine the tensions in the cords. 9. A wheel weighing 100 lb, rolls at a certain speed on a horizontal rail. The wheel is out of balance to the extent that at the speed of rolling there is a radial centrifugal force of 20 lb. On a base 6 inches long, representing one revolution of the wheel, plot, for every 1-1 2th of a revolution, the pressure exerted by the wheel on the rail. Use a force scale of 1 inch to 20 lb. 10. A, B, C, D, E, and F are six forces acting in a plane at a point 0. The magnitudes of the forces are 125, 1*10, 2*25, 1-75, 2-45, and 1-35 pounds re- spectively. The forces act outwards from in lines inclined to a fixed line OX at the following angles, 30°, 60°, 135°, 180°, 225°, and 300° respectively. Find R the resultant of these forces. If these forces are balanced by a force P acting in the line OX and a force Q acting in a line at right angles to OX, determine P and Q. 11. A jet of water having a velocity of 353^0 feet per second passes over a fixed vane as shown in Fig. 169, and is deflected, leaving the vane with a velocity of 35jjjQO feet per second. If w^ denote the change of velocity that has occurred, find u and 6 ; that is, solve the vector equation Un = 35 100° 35 30°' The mass m of water passing per second being 2-5 units {= 2-5 X 32*2 lb.), calcu- late muQ, the magnitude and direction of the change of momentum per second ; find also — mUg, the magnitude and direction of the force acting on the vane, [b.e.] Fig. 170. Fig. 171. 12. A stream of water flowing in the given direction AB (Fig. 170) impinges on a succession of moving vanes, one of' which is shown. BT, CT are tangents to the curve of the vane at its ends. The vector V represents the velocity of the vane to a scale of 1 inch to 20 feet per second. (a) Find and measure the speed of the water along AB in order that the water may come on to the vane at B tangentially, or without shock. (b) Suppose the water to flow over the vane without change of relative speed, represent graphically to scale the absolute velocity of the water as it leaves the vane at C. , i. xu 4. i, (c) Show graphically the vector change U of velocity of the water that Has occurred owing to its passage over the vane. Find and measure tue com- ponent of U in the direction of V. . (d) Determine, either the actual path of the water as it flows over the moving vane, or the line of the resultant force on the vane, due to the change of momentum of the water. [b.e.J 90 PRACTICAL GEOMETRY 13. A jet of water having a velocity Vi of SSg^o feet per second passes over a succession of curved vanes (one of which is given in Fig. 171) moving with a velocity V of 23^,o feet per second. Find Vi - V, the velocity of the water rela- tively to the vane ; that is, find s and o in the vector equation 35, 30° 23oo = Yx-Y, s being the speed along the vane, and a the direction of the vane at entrance, the water coming on tangentially. The water leaves the vane with a velocity relatively to the latter of s^g^o- Find U(= Uq), the change of velocity that has occurred. The mass m of the water flowing per second being 2-5 units (= 2*5 X 32-2 lb.), calculate mU, the magnitude and direc- tion of the change of momentum per second. Find also the power developed, which is equal to the scalar product - mlJV. [B.E.] 14. A jet of water passes over a suc- cession of curved vanes (one of which is shown in Fig. 172), entering tangentially with a velocity Vj of 353QO feet per second, and leaving with a velocity Vg of 8gQ0 feet per second. The vanes have a velocity V of Vqo feet per second, and the speed s of along the vanes is assumed Fig. 172. the water constant. Find V, the speed of the vane. Find also a and j8 the directions of the vane at entrance and exit. The mass m of the water flowing per second being 2'5 units (= 2*5 X 32*2 lb.), and U denoting the vector change of velocity of the water, find wU, the magnitude and direction of the change of momentum per second. Find also the power developed, which is equal to the scalar product - mUV. [B.K.] ( CHAPTER Vlir GRAPHIC STATICS' 90. Coplanar Forces. — Unless otherwise stated when a system of forces is considered it will be assumed that the lines of action of all the forces are in the same plane. In the great majority of problems in statics with which engineers have to deal the forces are in the same plane. The composition and resolution of forces acting at the same point have been considered in Chapter VII. as particular cases of vectors. 91. Specification of Forces in a Plane. — A force is specified when its line of action, its sense, and its magnitude are known. Let OX (Fig. 173) be a fixed line or axis in the plane in which a force A acts, and let O be a fixed point in OX. Let the line of action of the force A cut OX at L, and let x denote the length of the intercept OL. Let tt denote the angle, measured anti-clockwise, which the line F^^ " " '» %; Fig. 173. Fig. 174. of action of the force makes with OX, the force being supposed to act outwards from L. Lastly let a denote the magnitude of the force. Then the force is specified by giving x, a, and a. A convenient way of stating the quantities x, a, and a in speci- fying a force A is, A =,««• For example, if the magnitude of the force A is 19-5 units of force, and the intercept x is 0*7 unit of length and the angle a is 35 degreed, then A = 07^^'^35O' This method of specifying a force fails when the line of action of the force is parallel to OX, but this difficulty may be overcome by giving the intercept OM = y on an axis OY at right angles to OX. To show clearly that it is ij and not x that is given when specifying 92 PRACTICAL GEOMETRY the force, the value of y may be placed above instead of below the level of the value of a. Thus the force C (Fig. 173) whose line of action is parallel to OX would be given by the equation C = %o. The use of the value of y instead of the value of x is also desirable when the intercept x is large because the point L may be practically inac- cessible although the line of action of the force may be at quite a convenient distance from O. The force B (Eig. 173) would therefore be specified by B = ^6/3. The intercept x is positive when it is to the right of O and nega- tive when to the left. Also, the intercept y is positive when it is above O and negative when below. A number of forces are represented in Fig. 174. Without a drawing these forces would be specified as follows, the unit of force being the pound, and the unit of distance the inch. -^ — 0-6 17330 B — i-ilOigoo C = _o.7l 3*5900 D = -vM: E = 1-4300 F = U9,so. H = -"Hi,^ K = -o-^iO, 92. Bow's Notation. — In Fig. 175 the diagram (m) shows the lines of action of a number of forces which are in equilibrium. The diagram (n) is the corresponding polygon of forces. In one system of lettering, each force is denoted by a single letter, as P. In Bow's notation, each force is denoted by two letters, which are placed on opposite sides of the line of action of the force in diagram (?«), and ^ ' ^ at the angular points of the poly- gon in diagram (w). In Bow's notation the force P is referred to as the force AB. In like manner the force Q is referred to as the force BC. The diagram (m), which shows the lines of action of the forces, is called the space diagram or frame diagram, and the diagram (n) which shows the polygon of forces is called the force diagram. 93. The Funicular Polygon or Link Polygon.— Let P, Q, R, and S (Fig. 176) be four forces, acting on a rigid body, but their lines of action do not meet at one point. The forces P, Q, R, and S are balanced by a fifth force T which is at present unknown. Draw the polygon of forces ahcde, that is, draw a polygon whose sides are parallel to the lines of action of the forces and of lengths equal to the magnitudes of the forces as in the case of forces acting at a point. ea the closing side of the polygon will represent in magnitude and direction the fifth force T. It now remains to find a point in the line of action of the force T. Take any point and join it to a, h, c, d, and e. Take any point 2 in the line of action of P and draw the line 2B3 parallel to oh to meet the line of action of Q at 3. Draw 3C4 parallel to oc to meet the line of action of R at 4. Draw 4D5 parallel to od to meet the line of action of S at 5. Draw 5E1 parallel to oe to meet 2A1 GRAPHIC STATICS 93 parallel to oa at 1. Then 1 is a point in the line of action of T which may now be drawn parallel to ea. Conceive that the lines A, B, C, D, and E represent bars jointed to one another at the points 1, 2, 3, 4, and 5. Then these bars may be supposed to take the place of the rigid body upon which the five forces P, Q, R, S, and T are supposed to act. In the case under con- sideration (Fig. 176) it is obvious that the bars A, B, C, D, and £ are subjected to tension. Consider the point 2. Here there are three forces acting which balance one another, namely, the force P and the tensions in the bars A and B, and these three forces are repre- sented in magnitude and direction by the three sides of the triangle abo. Again, the three forces acting at the point 3 are represented by the sides of the triangle hco, also the three forces acting at the point 4 are represented by the sides of the triangle cdo, and the three forces at 5 by the sides of the triangle deo. Now in order that the tensions in the bars E and A may be balanced by the force T, the force T Fig. 176. Fig. 177. must act at the point of intersection of the bars E and A. The point 1 is therefore a point in the line of action of T. The polygon 1 2 3 4 5 is called the funicular polygon or link polygon of the forces P, Q, R, S, and T with reference to the point o, which is called the pole. Since the pole o may have an infinite number of positions, there is an infinite number of link polygons to any system of balanced forces. If the diagrams (F) and (/) (Fig. 176) be compared it will be seen that each line on the one is parallel to a corresponding line on the other. Also, if a system of lines on the one meet at a point the corresponding lines on the other form a closed polygon. From these properties the diagrams (F) and (/) are called reciprocal figures. No reference has yet been made to Fig. 177, but all that has been said with reference to Fig. 176 will also apply to Fig. 177, where the given forces are parallel to one another, except that the bars E and A are in compression, the remaining bars B, C, and D being in tension. 94 PRACTICAL GEOMETRY An examination of Figs. 176 and 177 will show that the simple rule to be remembered in drawing the link polygon is, that any side of that polygon has its extremities on the lines of action of two of the forces, and that that side is parallel to the line which joins the pole to the point of intersection of the lines which represent these two forces on the polygon of forces. Referring to Figs. 176 and 177, it may be noted that the equili- brant of P and Q is represented in magnitude and direction by ca, and that the point of intersection of. the sides A and C of the link polygon is a point in the line of action of this equilibrant. Also the equilibrant of P, Q, and R is represented in magnitude and direction by da, and the point of intersection of the sides A and D of the link polygon is a point in the line of action of this equilibrant. Having shown that the link polygon together with the polygon of forces may be used to determine the equilibrant of any system of forces in a plane, it is obvious that the same construction will also determine the resultant of that system of forces, since the resultant acts along the same line and has the same magnitude as the equilibrant, but acts in the opposite direction or has the opposite sense. Again referring to Figs. 176 and 177, it will be observed that the letters A, B, C, D, and E on the space diagrams are situated in the spaces between the forces P, Q, R, S, and T, and the letters P, Q, R, S, and T may be omitted and the forces referred to as AB, BC, CD, DE, and EA. Also the same forces in the force polygons are lettered ah, he, cd, de, and ea respectively, which is Bow's notation. It will further be noticed that the sides A, B, C, D, and E of the link polygon are parallel to the polar lines oa, oh, oc, od, and oe respectively of the force polygon. 94. Examples. — The following two examples illustrate the application of the link polygon to the solution of problems on forces whose lines of action are either parallel or do not all meet at the same point. (1) Using Bow's notation, AB, BC, and CD (Fig. 178) are three vertical forces acting on a horizontal beam. These forces are balanced by the vertical forces DE and EA whose magnitudes and t 23li. 20W. ZSW. | senses are required. Since the forces are all parallel, the polygon of forces will be a straight line ahcdea, the position of the point e being as yet unknown. Choose a pole o, and join oa, oh, oc, and od. Draw OA, OB, OC, and OD parallel to oa, oh, oc, and od respectively as shown. These lines OA, 01>, OC, and OD will form four sides of the link polygon of which OE will be the closing side. Draw oe parallel to OE to meet ac at e. This completes the solution. It will be found that Fig. 178. GRAPHIC STATICS 95 Also, EA is 18-9 lb. DE is 13*9 lb. and that it acts downwards, and acts upwards. (2) LMN (Fig. 179) is a framed structure supported at M and N, MN being horizontal. There is a vertical load AB of 1100 lb at L and a load BC of 1520 lb. at the middle point of LN and at right angles to LN. The supporting force CD at N is known to be vertical, but its magnitude is un- known. The supporting force DA at M is unknown both as regards magnitude and direction. It is re- quired to complete the de- termination of the forces CD and DA. The triangle of forces ahc determines the direc- tion of the resultant of the given forces AB and BC and a line through R, the point of intersection of AB and BC, parallel to ac is the line of action of that resultant. Replacing AB and BC by their resultant there are now only three external forces acting on the frame and as they are not parallel they must meet at a point which is obviously the point S where the resultant of AB and BC meets CD. This determines the line of action of DA which passes through M and S. The polygon of forces ahcd may now be completed. It will be found that CD = 1380 lb., DA = 1340 lb., and the inclination of DA to the horizontal is 36*5 degrees. This example may be worked without using the point S, as follows. After drawing the sides ah and he of the force polygon choose a pole 0, and join oa, oh, and oc. Next proceed to draw the link polygon starting at the point M which is the only point in the line of action of DA which is known. Draw Ml, across the space A, parallel to oa. Draw 1 2, across the space B, parallel to oh. Draw 2 3, across the space C, parallel to oc. Then M3 is the closing line of the link polygon. Draw od parallel to M3 to meet a vertical through c s.t d which is the remaining angular point of the force polygon. DA may now be drawn parallel to da. 95. The Centre of Parallel Forces. — If a system of parallel forces acts at fixed points, the resultant will act through another fixed point called the centre of the system. This centre is independent of the direction of the forces so long as the sense of each in relation to the sense of one of the forces is unaltered. In Fig. 180, P, Q, R, and S are parallel forces acting at the fixed points A, B, C, and D respectively in a plane. By means of the force and link polygons the line of action LK of the resultant is determined. Let the direction of the forces be changed so that they act as shown by F, Q', R', and S'. The line of action MK of the resultant is 96 PRACTICAL GEOMETRY determined as before. The point K, where LK and MK intersect, is the centre of the parallel forces P, Q, R, and S acting at the fixed points A, B, C, and D respectively. If the construction be repeated with the forces acting in any other direction, it will be found that the new resultant will act through the same point K. In Fig. 180, the forces P, Q, R, and S have all the same sense, and therefore P', Q', R', and S' must have the same sense. But if the sense Fig. 180. of Q, say, were opposite to that of P, then the sense of Q' would be opposite to that of P'. In applying the above method to the determination of the centre of a system of parallel forces, it is usually most convenient to take the two directions of the forces at right angles to one another. 96. Centres of Gravity or Centroids. — The particles of which any body is made up are attracted to the earth by forces which are proportional to the masses of these particles. For all practical purposes these forces may be considered to be parallel, and their resultant will pass through the centre of these parallel forces. In this case the centre of the parallel forces is called the centre of gravity or centroid of the body, and the determination of a centre of gravity resolves into finding the centre of a system of parallel forces. The centre of gravity of a body may also be defined as that point from which if the body is suspended it will balance in any position. When the term centre of gravity is applied to a line, the line is supposed to be an indefinitely thin wire ; and when the centre of gravity of a surface is spoken of the surface is supposed to be an indefinitely thin sheet of material. The following results, which are not difficult to prove, should be noted : — The centroid of a straight line is at its middle point. The centroid of a triangle is at the intersection of its medians. The centroid of a parallelogram is at the intersection of its diagonals. GRAPHIC STATICS 97 If a plane figure is symmetrical about a straight line, the centroid of the figure is in that straight line. To find the centroid of a line made up of a number of straight lines. At the centres of the straight lines apply parallel forces whose magnitudes are proportional to the lengths of these lines. The centre of these parallel forces is the centroid required. To find the centroid of a curved line. Divide the line into a number of parts, preferably of equal length. At the centres of these parts apply parallel forces whose magnitudes are proportional to the lengths of the parts. The centre of these parallel forces is approximately the centroid required. Theoretically the approximation is closer the more numerous the parts into which the curved line is divided, but practically when the parts are very numerous or very short the drawing of the link polygon becomes less accurate. To find the centroid of any irregular figure. Divide the figure into parts whose centroids and areas are known or easily found. At the centroids of these partial areas apply parallel forces whose magnitudes are proportional to these areas. The centre of these parallel forces is the centroid required. If the given figure has an irregular curved boundary line such as is shown in Fig. 181, divide the figure into a number of parallel strips as shown by the full straight lines. Draw the centre lines of these strips, shown dotted. The centroids of these strips may be taken at the middle points of their centre lines, and the areas of the strips may be taken as proportional to the lengths of their centre lines. To find the centroid of a quadrilateral. Let ABCD (Fig. 182) be the quadrilateral. Draw the diagonals AC and BD, intersecting at O. Let OA be less than OC. Make CE equal to AO. Join BE and DE. G, the centroid of the triangle BDE is also the centroid of the quadrilateral ABCD. To find the centroid of an arc of a circle. Let ABC (Fig. 183) be the arc of a circle of which is the centre. Draw OB at right angles Fig. 181. A Fig. 182. to the chord AC. Draw BD at right angles to OB and make BD equal to the arc BC. Join OD. Draw CE parallel to OB to meet OD at E. Draw EG parallel to AC to meet OB at G. G is the centroid of the arc ABC. 98 PRACTICAL GEOMETRY To find the centroid of a sector of a circle. Let OABC (Fig. 184) be the sector of a circle of which O is the centre. Draw OB at right angles to the chord AC. Draw BD at right angles to OB and make BD equal to the arc BC. Join OD. Find a point F in OC such that OF is two-thirds of OC. Draw FH parallel to OB to meet OD at H. Draw HG perpendicular to OB to meet OB at G. G is the centroid of the sector OABC. To find the centroid of a figure considered as part of another figure. Frequently the addition of a simple figure to a given comparatively complicated one will make a simple figure. For example the figure ABCD (Fig. 185) only requires the addition of the triangle OCD to convert it into the sector of a circle whose centre is O. G^ the centroid of the sector O^B is readily found and so 'is G2 the centroid of the triangle OCD. Let G be the centroid of the figure ABCD. Then if at G^ and G parallel ^'^- ^^^• forces P and Q be applied, the magnitudes of P and Q being propor- tional to the areas of OCD and ABCD, the centre of these parallel forces will be at Gj the centroid of the sector OAB. Hence, if parallel forces P and R be applied at Go and G^, hut in opposite directions, the magnitudes of P and R being proportional to the areas of OCD and OAB, the centre of these parallel forces will be at G the centroid of the figure ABCD. The area of a sector of a circle is equal to half the product of the arc and the radius. 97. Centre of Pressure and Centre of Stress. — If a plane figure be subjected to fluid pressure, the point in the plane of the figure at which the resultant of the pressure acts is called the centre of pressure. If the plane figure is a section of a bar or part of a structure which is subjected to stress, the point in the plane of the section at which the resultant of the stress acts is called the centre of stress. In what follows " pressure " will be taken to include " stress." If the pressure be uniform over the figure, then the centre of pressure coincides with the centroid of the figure. A general construction for determining the centre of pressure of any plane figure when the pressure varies uniformly in one direction is illustrated by Fig. 186. ABCD is a plane figure supposed to be vertical, and AB and CD are horizontal. AAj is the altitude of the figure, and the pressure is supposed to vary uniformly from an amount represented by AP at the level AB to an amount represented by A^Q at the level CD. AP and A^Q are horizontal. Join QP and produce it to meet A^A at O. Draw any horizontal SRMN to cut the given figure. Draw the horizontal OF, and the verticals MMj and NNj. Through K, the middle point of MN, draw the vertical KF. Join FMj and FN^ cutting MN at m and n. If this construction be repeated at a sufficient number of levels, and all points GRAPHIC STATICS 99 correspondinrr to m be joined, also all points corresponding to n, a figure abnCDma is obtained and the centroid of this figure will be the centre of pressure of the original figure. The proof is as follows. Suppose that the line MN is the centre line of a very narrmo horizontal strip of the original figure, and let the width of this strip be denoted by w. The magnitude of the resultant pressure on this strip is equal to MN X w; X KS, and it will act at K the middle point of MN. ' Since SRMN is parallel to QA^DC, MiNi : mn:: OAj and, MN : mn : : A^Q therefore, MN X RS = mn x A^Q, and MN XwxUS = mnXwx A^Q, that is, the resultant of the pressure on the strip of length mn when subjected to a pressure A^Q will have the same magnitude as the resultant of the pressure on the strip of length MN when subjected to a pressure RS, and it will act at the same point K which is also the middle point of mn. OR, RS, It follows that the resultant of the pressure on the figure abnCDma when subjected to a uniform pressure A^Q will be the same as the resultant of the varying pressure on the original figure. But when the pressure on a plane figure is uniform, the centre of pressure is at its centroid. Therefore the centroid of the figure abnCDma is the centre of pressure of the original figure. The figure abnCDma is called a modulus figure of the original figure. A common and important practical case is that in which the given figure is a rectangle and the pressure on it varies uniformly in a direction parallel to a side of the rectangle. In Fig. 187, ABCD is a rectangle on which the pressure varies uniformly from nothing at A to an amount DT at D. Applying the 100 PRACTICAL GEOMETRY construction just proved the student will have no difficulty in seeing that the modulus figure for the rectangle ABCD is the, isosceles triangle OCD and that the centre of pressure for the rectangle ABCD is at Ci on the vertical centre line of the rectangle and at a distance from AB equal to |H where H is the height of the rectangle. Also the magnitude of R the resultant of the pressure on ABCD is equal to the area of the rectangle multiplied by the half of DT, where DT is the intensity of the pressure or the pressure per unit area at the level CD. If the rectangle ABCD (Fig. 187) be divided into two rectangles by the line EF, then, Cg, the centre of pressure of the rectangle ABFE is at a distance \h from AB, where h is the height of the rectangle ABFE, and the magnitude of P the resultant of the pressure on ABFE is equal to the area of ABFE multiplied by the half of ES. The centre of pressure of the rectangle CDEF will be at Cg the centroid of the quadrilateral CDe/ and the magnitude of Q the resultant of the pressure on CDEF will be equal to the area of CDEF multiplied by half the sum of DT and ES. Q may however be determined both as regards magnitude and position by considering it as the equilibrant of the parallel forces P and R, the sense of R being opposite to that of P. 98. Masonry Dams. — A masonry dam is a wall for holding back the water at the end of a natural reservoir. One form of dam section is shown in Fig. 188, A V being a vertical line. The principal problems connected with dams are: (1) the de- termination of the line of resistance when the reservoir is empty ; (2) the determination of the line of resistance when the reservoir is full, and (3) the determination of the stresses at various horizontal sections of the dam. Reservoir empty. When the reser- voir is empty the stresses in the dam are those due to its weight. Refer- ring to Fig. 188. Consider a portion of the dam lying between two vertical cross sections one foot apart, then the weight of a part of this between two horizontal section planes will be equal to the area, in square feet, of the cross section between these planes multiplied by the weight of a cubic foot of the. material of the dam. | Let horizontal sections BC, EF, GH, and KL be taken. The resultant M?i of the weight of the top portion ADLK acts vertically through Cj the Fig. 188. centroid of ADLK. w^ cuts KL at Cj which is the centre of pressure or centre of stress for the horizontal section KL. Irmer Face} GRAPHIC STATteS •- ' ^ ' , ' > .|*qi The resultant w.^ of the weight of the portion KLHG acts vertically through Ca the centroid of KLHG. The resultant of the load on GH is Wg which is the resultant of w^ and w^. Wg cuts GH at Co. which is the centre of stress for the horizontal section GH. Continuing in the same way, Wg, the resultant of w^, W2, and w.^, cuts EF at C3 the centre of stress for EF, and W4, the resultant of iDi, W2, Ws, and w;4, cuts BC at c^ the centre of stress for BC. A fair curve drawn through the centres of stress of the various horizontal sections is called the line of resistance for the cross section of the dam. Beservoir full. When the reservoir is full the gravity forces which have just been considered will still act but there will now be in addition the pressure of the water on the inner face. The intensity of the pressure of the water per square foot at any depth h feet from the upper or free surface of the water is equal to h multiplied by the weight of a cubic foot of water or say 62 -SA. Still considering a portion of the dam one foot long. The resultant force on the horizontal section BC is the resultant ofc W^ and P4, where P4 is the resultant of the pressure of the water on the face of the one foot length of dam from A to B. P4 acts at two-thirds of AB from A and at right angles to AB. The magnitude of P4 is the area of the face AB, one foot long, multiplied by half the intensity of the water pressure at B. Let P4 and W4 intersect at O. B4 the resultant of P4 and W4 acts through O in a direction determined by the triangle of forces rpw. The line of action of R4 cuts BC at s^ which is the centre of stress for BC. In a similar manner «3, s^, and s^ the centres of stress for EF, GH, and KL may be determined. A fair curve through these centres of stress of the various horizontal sections determined as above is the line of resistance for the cross section of the dam when the reservoir is full. If each of the horizontal lines BC, EF, etc. be divided into three equal parts then each of the middle parts is called a middle third. If the corresponding extremities of the various middle thirds be joined by fair curves ^ these curves will enclose the middle third of the cross section of the dam, and if a dam is pro- perly designed the lines of resistance should fall within this middle third whether the reservoir is empty or full. If R is the resultant force on any hori- zontal section XXj (Fig. 189) of the dam, then S the vertical component of R causes a normal stress on XX, and the horizontal component T causes a tangential or shear stress on XXj. The normal stress produced by S on XX^ is not uniformly dis- tributed but varies uniformly from 5 - p at X which is furthest from S to 5 -f jp at Xj. 1 If the contour of the cross section of the dam is made up of straight lines these fair curves will become a series of straight lines. 102 FIIACTICAL GEOMETRY Let C be the middle point of XX^. Let XX^ = 2a, and let the distance of S from C be x, then, still considering 1 foot length of the dam, a = ^^» ~ — - _ _ >Ei ^^^^v^^::^^ l'^ \di -\f w. TV c\P, 1050 2100 2100 2100 h 1050 2' L li 40 -HH Fig. 220. GRAPHIC STATICS 117 the roof covering. The other system is at right angles to the left- hand surface of the roof, and is due to wind pressure. All the loads are in pounds. The truss is supposed to be fixed at the right-hand support u but at the left-hand end v it is merely supported ; hence the line of action of the reaction at v must be vertical. The direction of the reaction at u is unknown and the magnitudes of both reactions are unknown. The part abcdefgJik of the polygon of external forces acting on the truss is first drawn. The next step is to determine the reactions KL and LA at the supports. Choose a pole o and draw the link polygon shown by dotted lines on the frame diagram, starting at the point u. By starting at the point u the space K, which is as yet not completely defined, is eliminated. The closing line of the link polygon is wu. A line through the pole o parallel to wu to meet the vertical through a determines the point / and therefore also Ik. This completes the polygon of external forces. Starting at the joint at one of the supports the complete stress diagram may now be drawn as in the preceding example. 107. The Method of Sections. — A little more than one half of a roof truss is shown in Fig. 221. Conceive that this truss is divided into two parts by a plane of section XX which cuts three bars FG, GH, and HA. Next suppose that the part of the structure to the right of XX is removed and that external forces are applied at the sections of the bars cut so as to balance the internal forces in these bars. These external forces will take the place of the forces exerted on the part of the structure to the left of XX through the parts of the cut bars which have been removed. The part of the structure to the left of XX will now be in equilibrium under the action of the given system of loads and the three external forces FG, GH, and HA. It will now be shown how these three applied external forces may be found. The determination of these three forces is evidently the determination of the forces in three of the members of the original structure. Draw the line of loads ahcdef. To complete the polygon of ex- ternal forces on the structure to the left of XX requires the locating of the points g and k Choose a pole o and, starting at the point w, where the lines of action of two of the unknown external forces inter- sect, draw the link polygon of which vu is the closing line. A line through o parallel to vu to meet a line through a parallel to AH determines the point h. The intersection of hg parallel to HG and fg 118 PRACTICAL GEOMETRY parallel to FG determines the point g. The senses of the external forces FG, GH, and HA are found at once by going round the com- pleted polygon of external forces in the direction fixed by the sense of any one of the known external forces. It will be seen that the bar FG is in compression while the bars GH and HA are in tension. This method of sections is extremely useful, for it may be applied to determine directly the forces in three members of a structure with- out drawing the stress diagram for any other part of the structure. In drawing the stress diagram for the truss, a part of which is shown in Fig. 221, the polygon of external forces would be first drawn, then the stress diagram would be built up polygon by polygon com- mencing at one of the supports where there are only two forces whose magnitudes have to be determined. In passing from joint to joint if a joint is arrived at where the magnitudes of three forces have to be determined the polygon of forces for that joint becomes indeterminate. This happens when the joint AMNHA or the joint DEPNMLD is reached. If however a section be taken as shown in Fig. 221 and the force AH determined as explained above the polygon of forces for the joint AMNHA may be completed and the stress diagram may then be proceeded with in the ordinary way. 108. Deflections of Braced Frames. — The bars which make up a braced frame are generally in tension or compression and the forces acting along the bars may be found as described in the preceding articles of this chapter. The bars have then to be proportioned to resist these forces. The pull or push on a bar will cause it to lengthen or shorten by an amount x and will produce a stress / in it. If E is the modulus of elasticity of the material in tension or compression and I is the length of the bar, then E = . = ttz ~ ' *^^ "'- E- For steel E may be taken as 30,000,000 pounds per square inch and if /is, say, 15,000 pounds per square inch, then x = oTT aoo 00 ~ 9000' *^^* ^^ *^® ^^^ ^^^^ lengthen or shorten by an amount which is the l-2000th part of its length. A bar 100 inches long would therefore lengthen or shorten 05 inch under these con- ditions. It is outside the scope of this work to discuss further the design of structures or the determination of the strains produced in their members by given systems of loading, but it will now be shown how the deflections of braced frames may be determined when the alterations in the lengths of the members due to loading are given. • The lower part of Fig. 222 shows the frame diagram of a pent-roof truss loaded at the joints B, C, and D. It is given that the various bars of the truss alter in length by the amounts stated on the lines GRAPHIC STATICS 119 which represent the bars. + denotes increase and - denotes decrease in length. These alterations in length are so small that the change m the form of the truss due to the loads cannot be clearly shown on an ordinary scale drawing of the truss. The displacements of the various joints may however be determined as follows. The joints A and E are supposed to be fixed, that is these joints are not displaced when the truss is loaded. Choose an origin and draw horizontal and vertical axes OX and OY. is the origin and OX and OY are the axes of a displacement diagram which is to be drawn to a large scale. In Fig. 222 the displacement scale is five times full size, but on a drawing board the displacement scale would not be less than ten times full size. Consider the joint B. Through draw Obi parallel to AB and make Obi = 0*08 inch on the displacement scale. Draw Ob.^ parallel to BE and make Ob^ = 0*06 inch on the dis- placement scale. Draw b^b perpen- dicular to 0^1 and ^g^ perpendicular to 0^2 and let these, perpendiculars meet at b. If is the original posi- tion of B then b is its new position when the bar AB has lengthened 008 inch and the bar BE has shortened 0-06 inch. To be strictly accurate b^b should be an arc of a circle whose centre is in h^O produced at a distance from O equal to the length of AB measured on the displacement scale ; but the radius of this arc is so large compared with the length of the arc that the arc is practically a straight line at right angles to ^^O. So also bj) should be an arc of a circle whose centre is in 0^2 produced at a distance from O equal to the length of BE measured on the dis- placement scale. Consider next the joint C. C has a downward displacement whose vertical component is the vertical component of the displacement of B plus the displacement 0*04 inch due to the lengthening of the bar BC. The former is represented by Ocq and the latter by c^Ci. The horizontal component of the displacement is 0*05 inch due to the shortening of the bar CE and this is represented by Oc^. The horizontal c^c to meet the vertical c^c determines c the new position of C on the assumption that was its original position. Lastly consider the joint D. D has a displacement whose com- ponent in the direction BD is made up of the component of the displacement of B in that direction, that is Obj, and the amount 0'04 inch by which the bar BD lengthens and which is represented by b^di. The total component of the displacement of D in the direction Fig. 222. 120 PRACTICAL GEOMETRY BD is therefore Od^. The horizontal component of the displacement of D is made up of the horizontal component of the displacement of C, that is Ocg, and 0*05 inch the amount by which the bar CD shortens and which is represented by Cg^g- ^^^ total horizontal component of the displacement of D is therefore Oc^a- ^i<^ perpendicular to Od^ meeting the vertical through ^2 determines d the new position of D assuming that its original position was 0. The angular deflection of any bar is measured by the ratio y/l where y is the relative displacement of the ends at right angles to the bar and I is the length of the bar. For example, consider the bar BD. The component of B's displacement at right angles to BD is h\ or d^di where bd.^ is parallel to Od^. The component of D's displace- ment at right angles to BD is dd^^. Hence dd^ is the relative displacement of D and B at right angles to BD, and the angular If BD is 14 feet and dd^ is 0-292 = 0-00174. Whether displacement of BD is dd^ -4- BD. 0*292 inch, the angular displacement Ois ^ ^ ,-, this be taken as the circular measure, or the sine, or the tangent of the angle, the angle being very small, the angle is 6 minutes or 1-1 0th of a degree. In the foregoing example one member AE (Fig. 222) was supposed to be fixed and to remain of the same length. An example will now be con- sidered in which all the members are displaced. Fig. 223 shows a roof truss ADF in which the joint A is fixed and the joint F is free to move horizontally. The truss supports dead loads and in addition a wind load on the left-hand side. These loads cause alterations in the lengths of the bars which are stated on the lines which re- present them. Assume in the first place that, say, the bar CD re- mains vertical and that C is fixed in position. Choose an origin and axes OX and OY and determine the dis- placements of the various joints, as in the previous example, the original position of each joint Fig. 223. GRAPHIC STATICS 121 being taken as at O. Then on the assumption that C is fixed and CD remains vertical, A suffers a horizontal displacement 0«i to the left and an upward vertical displacement a^a. Also F suffers a horizontal dis- placement O/i to the right and an upward vertical displacement//. But under the actual conditions A is fixed. Let, therefore, the whole truss be now lowered an amount aa^, or, which is the same thing, let the axis OX be raised to O'X' the level of a. Let, also, the whole truss be moved to the right a distance equal to Oaj, or, which is the same .thing, let the axis OY be moved to the left so as to pass through a. The axes are now O'X' and O'Y' and a which represents the position of the joint A is at the origin 0'. It will be seen that the joint F has now a downward vertical displacement equal to /'/. To bring F to its original level, which is the level of A, the whole truss must now be rotated about A until F rises through a distance equal to ff\ This angular movement will cause the various joints to travel at right angles to the lines joining them to A distances proportional to the lengths of these lines. Consider the joint D. Referred to the origin 0' and the axes O'X' and O'Y', d shows the displacement of D when A is fixed and F is at the distance // below its proper level. It is now required to find the final displacement of D when the truss is turned about A to bring F to its proper level. With A as centre and AD as radius describe the arc DDj to cut the horizontal AF at Dj. Draw the vertical D^HK to cut 0/ at H and 0'/' at K. Then HK is the amount that D will travel at right angles to DA when the truss is turned about A to raise F the distance ff. Draw dd' perpendicular to AD and make dd! equal to HK, then d! shows the final displacement of D referred to the origin 0' and axes O'X' and O'Y'. In like manner the points V, c', and e' are found. 109. The Three-Hinged Arch. — If the ends of a roof or bridge truss are secured to foundations by hinged joints, and there is another hinged joint at an intermediate point, say, at the middle of the truss, such a truss is known as a three-hinged arch, and it is said to be con- structed on the three-hinged system. The determination of the stresses in the various bars of such a truss may be proceeded with as in an ordinary truss as soon as the reactions at the hinges are determined. One method of finding the reactions at the hinges is as follows. Fig. 224 shows a truss hinged at A, B, and C. The resultant load on the part AB is the force P, and the resultant load on the part BC is the force Q. First neglect the load acting on the part BC. The part BC is then under the action of two forces only, namely, the reactions at B and C, and these forces must balance one another, and will therefore act in opposite directions along the straight line BC. The truss as a whole is now under the action of three forces, namely, the force P, the reaction Tj at C, which acts along CB, and the reaction Si at A. Since these three forces are in equilibrium, and since the lines of action of two of them, Ti and P, meet at m, therefore the line of action of the third one, Sj, must be Am. By means of the triangle of forces the magnitudes of Si and Tj can be determined. 122 PRACTICAL GEOMETRY Fig. 224. Next neglect the load on the part AC, and consider the load Q on the part BC. This load Q will cause reactions Sg and Tg at A and B respectively, and these reactions may be found in the same way as Sj and Ti were found. When both loads P and Q act, it is evident that the reaction at A will be the resultant of Si and Sjj, and the re- action at B will be the resultant of Ti and Tg. The reaction of the part AB on the part CB at B will be the force which will balance the force Q and the reaction at C, and the reaction of the part CB on the part AB at B will be the force which will balance the force P and the reaction at A. These two reactions will, of course, be equal and opposite. When the truss is symmetrical about a vertical centre line, and is symmetrically loaded, the reactions at B will be horizontal, and the line of action of the reaction at A will be the line joining A with the point of intersection of the line of action of the resultant load on the half truss AB with the horizontal line through B. The direction of the reaction at C is found in like manner. The two parts of a three-hinged arch may be considered as two girders or two beams loaded ob- liquely. When these beams are solid or built up of plates and angles instead of being open brace work they are called arched ribs. An arched rib of a three-hinged arch is shown in Fig. 225, the joints being at 1 and 4. This rib carries vertical loads AB and BC. The reactions CO and OA at the joints may be deter- mined in the manner already explained, and oafec, the polygon of external forces, may then be drawn. If the link polygon 1 2 3 4 for the external forces be drawn so as to pass through the joints 1 and 4 this polygon Fig. 225. GRAPHIC STATICS 123 is called the linear arch for the rib. The sides of the linear arch are the lines of action of the thrusts which the rib has to support. The magnitudes of these thrusts are given by oa, oh, and oc. It will be observed that each of these thrusts has a horizontal component whose magnitude is given by oh, the perpendicular from o on abc. Consider the normal section LM of the rib. Let G be the centroid of this section. The thrust 11 on LM has the magnitude oh and since R does not pass through G there is a bending moment on the rib at LM whose magnitude is R X GN, where GN is the perpen- dicular from G on 2 3. Draw the vertical GE to meet 2 3 at E. Com- paring the triangles GNE and ohh it will be seen that they are similar, and that GE : GN : : oh : oh, or GE x oh = oh x GN = R x GN. But R X GN is the bending moment at the section LM, therefore GE X oh is also the bending moment at LM. Hence the vertical intercept between the locus of G and the link polygon 1 2 3 4 at any point on that locus is a measure of the bending moment at that point, since oh is constant. The shaded figure is therefore the bending moment diagram for the rib. Let 2 3 meet ML produced at F. Resolve R into components P and Q perpendicular and parallel respectively to LM. It is easily seen that P x GF = R x GN ; therefore the bending moment on the rib at G is equal to P X GF. In addition to the bending moment on the rib at the section LM there is a shear force equal to Q and a normal thrust whose resultant passes through G and is equal to P Exercises VIIIc In working the following exercises on forces in framed structures it is not sufficient to draio the force diagrams. The forces should he scaled off from the force diagrams and the results stated on the lines of the frame diagram. The lines of 4he frame diagram which represent bars which are in compression should be lined in considerably thicker than the others after the forces have been determined. 1. A crane frame is shown at (a) Fig. 226. The external forces are, the load 1^ ~ ~ ■ - -- k+A — — — — — — — I— 20'^ ~~ B ^ w • • 4 -»- N f k J'a] ^, y ^. .- -' ^ 1^ "I 40 / 1 ^ ^C , ^\0> ^ / w .;w ^ X 2000 X X f > / / h \ / 400 ^ X / f< ^ / 1 \ L^ / ^^ / 00 y x* \ 1 / J / t / k 400 X / c / X ^( 'd \ N LI / / c? ( / X y V ^ > », IFT Z / ^ ^ Ss /L 1^ ■^ ^ s 1 ^^1 j^ r ^ y P V. ^ / 151 in — - innn ^ 00 ! ^ M ^ (^ ?m^ ^ m _ _J _ Fig. 226. W of 2 tons, the horizontal force R and the reaction at the footstep at the lower end of the post. The lower end of the post is hemispherical and the reaction there may be assumed to pass through the centre of the sphere, the axis of the 124 PRACTICAL GEOMETRY lower sloping member also passes, when produced, through that point. Draw the frame diagram four times the given size and then determine the reaction at the footstep and the forces in the bars B, C, D, and E, (1), assuming that the load W is hung directly from the joint A, and, (2) assuming that the load W is suspended by a chain which passes over a pulley at A as shown by the dotted lines. [Note that when a chain passes over a pulley the resultant force on the axle of the pulley is the resultant of two forces each equal to the tension in the chain and acting along the straight parts of the chain which proceed from the pulley.] 2. A crane frame is shown at (6) Fig. 226. The load W is 5 tons. Draw the frame diagram, say, three times the given size. Determine the balance weight L so that there shall be no bending action on the lower part of the crane post. Determine the forces in the various members of the frame, (1) assuming that the load W is applied directly at the point of the jib, (2) assuming that the load W is suspended by a chain which passes over two equal pulleys as shown by the dotted lines. [See note to preceding exercise.] 3. A projecting truss for the roof of an open shed is shown at (c) Fig. 226. The truss is loaded as shown, the loads being in pounds. Draw the frame diagram, say, three times the given size and then determine the forces in the various members. 4. A pent roof truss is shown at {d) Fig. 226. The truss is loaded as shown, the loads being in pounds. Draw the frame diagram three times the given size and then determine the forces in the various members. 5. The given roof truss (Fig. 227) is loaded as shown. Find and measure the double this size boolb. Fig. 227. vertical supporting forces at A and B. Determine the thrust in each of the two upper horizontal members of the frame, writing the answers on the bars themselves. [b.e.] 6. A curb roof truss is shown at (a) Fig. 228. The truss is loaded as shown, 1 rS 7 1 ^ 1 — — — — -1 r— |— \' ^ M- r- p p-j ^ A M X ^ ^s 1 1 -- \ o % j> ^ ''N r >* <** \ fl OJ ,.> k' {c > ^»^ 55 i. (d) ^ <^ \ >b ^ y • V, V ^^ t^ - S s u f^ ^ V, s ^^ V s 50 50 B 7i K / . / / / \ \ ' y j^- X w /' / / ib) / \ »^ «^ ^ d i£ / _ ~7 V. , ^ — :^ , ■^ —% ) = 1 . _ I — — =s ^^ Ri -" — ' R: A wmT -- I4i: t — ^ — Fig. 228. the loads being in pounds. Draw the frame diagram three times the given size and then determine the forces in the various members. GRAPHIC STATICS 125 7. The diagram (6) Fig. 228 represents a girder supported and anchored down by vertical forces Rj and Rg respectively. The girder carries loads of 60 tons at each end as shown. Draw the frame diagram three times the given size and then determine the forces Rj and Rg and the forces in the various members. 8. At (c) Fig. 228 is shown the truss for the roof of an island platform of a railway station. The loads (in tons) due to the roof covering and wind pressure are given. Draw the frame diagram double the given size and determine the forces in the members of the frame. The scale of the figure, when drawn double the given size, being J inch to 1 foot, what are the bending moments on the supporting pillar at A and at B ? [B.E.] 9. In the crane shown at (d) Fig. 228 the horizontal member has a pin joint at the left-hand end, and is supported at the other end by an inclined tie bar as shown. The load W of 1 ton is suspended from the middle of the hori- zontal member as shown. Draw the frame diagram to the scale of J inch to 1 foot and then determine, (1) the magnitude and line of action of the resultant shear force on the pin at the left-hand end of the horizontal member, (2) the tension in the tie bar, (3) the thrust in the horizontal member, (4), the total bend- ing moment at the middle of the horizontal member. 10. The diagram. Fig. 229, represents a swivel bridge, its pivot placed at AA. 10 I-2S 1-2$ A w w N b. N \ \ K V / / / Scale 0-75mh=Wfed 10 I 10 A w w Fig. 229. The loads, in tons, are placed as indicated. Draw the diagram double the given size. Determine the equal loads on the counterpoise to the right of AA placed as shown, then find the forces in the various members of the bridge. [b.e.] 11. You are given in Fig. 230 a bowstring truss under the action of wind Loads irv tons Brow double this size Fig. 230. forces, and supported at the ends A and B. Determine the supporting forces at the ends, that at A acting in a vertical line. Also draw the force diagram or reciprocal figure for the truss. [b.e.] 12. Determine the reactions at the supports and draw the stress diagram for the truss of example (2) p. 115 with the same loads except that the wind forces act on the right-hand instead of on the left-hand side of the truss, 13. The given crane (Fig. 231) is set out to a scale of' 1 cm. to 3 feet. A load W causes the bar AD to lengthen, and the three bars radiating from C to shorten, by the amounts written on the bars. Assuming AB to be rigid, find the vertical 126 PRACTICAL GEOMETRY component of the deflection of D. Find also the angular deflection of CD. [B.E.] 14. A crane has the form shown in Fig. 232, A load W causes the bars to alter in length by the amounts written thereon, the minus sign denoting shorten- ing. The joint A being fixed and the joint B being free to move horizontally, find the deflection of D and measure its vertical and horizontal components. What is the angular deflection of the bar CD, if its actual length is 100 inches ? [b.e.] 15. Forces, not shown, acting on the given roof truss (Fig. 233), cause the Fig. 231. Fig. 232. Fig. 233. bars to alter in length by the amounts written thereon, the minus sign denoting shortening. If the end A is fixed, and B is free to move horizontally, find the displacement of B. What is the angular displacement of the horizontal bar CD if its actual length is 110 inches ? [b.e.] 16. The diagram (Fig. 234) shows a simple roof truss, resting on walls and loaded as shown, the span being 15 feet and the inclination of the rafters 39°. (a) Find and measure the horizontal thrust on the walls. (6) Draw diagrams showing the thrust, shearing force and bending moment throughout the length of one of the rafters. Measure the maximum values of these quantities. [b.e.] Fig. 234. Fig. 235. 17. A braced arch, hinged at the crown and at each springing, is loaded as shown in Fig. 235. Determine the horizontal thrust on the abutments. Find the forces in all the members of the structure. What is the shearing force on the pin at the crown ? [b.e.] 18. An arched rib in the form of a circular arc ACB, is hinged at each end A, B, and at the crown C. The span AB is 150 feet, and the rise 30 feet. Draw the curve of the arch to a scale of J inch to 10 feet. A load of 10 tons passes over the arch. Confine your attention to one position only of this load, that for which its horizontal distance from A is 50 feet. Determine and measure the horizontal thrust of the arch in tons. Draw a diagram of bending moment on the rib, and measure the maximum bending m,oment in ton-feet. Determine also and measure the greatest thrust and the GRAPHIC STATICS 127 greatest shear in the rib, and state the horizontal distances from A of the places where these occur [B.E.] 19. The form of an arched rib is a circular arc of 100 feet span and 16 feet rise the supports being at the same level. It is hinged at the ends and loaded with a weight of 12 tons at a horizontal distance of 80 feet from one end. The hori- zontal thrust of the arch is known to be 12-5 tons. Draw a diagram of bending moment for the arch. Indicate the places where the shearing force, thrust, and bending moment on the rib have their maximum values, and give these values. rB.B.l 20. A flying buttress has the form and weight shown in Fig. 236. It is sub- Draiv double this size. t ^»- ' -■^ ^ — — 40'--_ 1 ^ I 20' i Fig. 236. 7-0 6-6 6-3 6-0 76 5*3 5 Loads in tons. Draw double tMs size. Scale ZOFeet to an incfv. Fig, 237. ject to a thrust P as indicated. Show the lines of the forces acting across the several joints. State the magnitude of the force on the bed joint BB. Adopt a force scale of ^ inch to 1 ton. [b.e.] 21. ABDC, Fig. 237, represents the section of a half-arch. The span of the half -arch is 40 feet, rise 20 feet, thickness of key-stone 6 feet, thickness of arch- ring at abutment, AB, 9 feet. The loads on the half-arch are supposed concentrated as shown. The dotted arcs bd and ac represent the limits of safety, and are at one-third of the thickness of the arch-ring from the extrados and intrados respectively. The horizontal thrust at the crown is assumed to be along the line dt, and the curve of thrust is further assumed to pass through the point e where the vertical through the abutment FA meets the dotted arc ac. Determine and draw the curve of thrust between the points d and e, by means of a funicular polygon, and give the value of the horizontal thrust at d. Scale of lengths, 10 feet to an inch. Scale of loads, 10 tons to an inch. [b.e.] CHAPTER IX PLANE CO-ORDINATE GEOMETRY 110. Co-ordinates of a Point. — The position of a point P in a plane (the plane of the paper) may be fixed by giving its distances X and y from two fixed intersecting straight lines OX and OY (Figs. 238 and 239), the distances x and y being measured parallel to OX and OY respectively as shown. The fixed lines OX and OY are called the axes. The axes are of unlimited length and each extends both ways from O. The point O where the axes intersect is called the origin. The distance x is called the abscissa and the distance y the ordinate of the point P, and these two distances together are called the co-ordinates of the point P. A point P whose co-ordinates are x and y may be referred to as the point x,y. Y *-x — ^ P 1 y d X Fig. 238. Fig. 239. Fig. 240. When the axes are at right angles to one another (Fig. 238) x and y are the rectangular co-ordinates of the point P, and when the angle between the axes is not a right angle (Fig. 239) x and y are the oblique co-ordinates of the point P. The abscissa x is positive ( 4- ) or negative ( — ) according as the point P is to the right or left respectively of the axis OY, and the ordinate y is positive or negative according as the point P is above or below the axis OX. The position of a point P in a plane (the plane of the paper) may be fixed in the manner illustrated by Fig. 240. O is a fixed point called the pole, and OX is a fixed straight line called the initial line, or line of reference. The point P is joined to O and the line OP whose length is r is called the radius vector. The angle which OP makes with OX, measured from OX in the anti-clockwise direction is called the vectorial angle, r and 6 are called the polar co-ordinates of PLANE CO-ORDINATE GEOMETRY 129 the point P, and these co-ordinates fix the position* of the point P. As defined above r and are both positive. If is measured in the clockwise direction from OX then it is negative. The angle whether it is positive or negative fixes the position of the positive radius vector OP. If the radius vector is negative then produce PO to F and make OP' equal to OP, then OP being the positive radius vector, OP' is the negative radius vector. A point P whose polar co-ordinates are r and may be referred to as the point r,0. Rectangular co-ordinates are the most common in practical problems and when co-ordinates are referred to, without qualification, rectangular co-ordinates will be understood. 111. The Straight Line.— AB (Figs. 241 and 242) is a straight line which intersects the axis OY at C. Let 00 = c. Take any point P in AB. Draw the ordinate PM and through C draw CL parallel to PL OX to meet PM at L. Then ^^ is a measure of the slope of AB to OX, OL and since the slope of AB is independent of the position of the point P, ~ = constant = m, say. But PL = PM - LM = PM - 00 = y - c, CL and CL = iK. Therefore ^- ^ = w?, or y = mx -\- c, and this is the EiQ. 242. equation to the straight line AB. The meaning of this equation is that, the constants m and c being known, the co-ordinates of every point in the straight line satisfy the equation. The distance OC = c is called the intercept of AB on the axis of y. For the line shown in Fig. 241, m = J and c = 5, hence the equa- tion to AB is ?/= ^ a; -f- 5. It will be found*^that for the point Q, re = 6, and ^ =8. Insertmg these values in the equation, 8 = l X 6 -h 5 = 8, and the equation is satisfied. Again, for the point R, a; = -3, and i/ = SJ. Inserting these values in the equation, 3J = -J X 3 -f 5 = -1^ + o = 3^, and the equation is again satisfied, and so it will be found for every point in AB. , ^ .1 i.- The line AB (Fig. 241) is called the graph of the equation y = \x + b. Conversely if any pair of values of x and y which satisfy the equation y = ^x + b he taken as the co-ordinates of a point, and this point be plotted, all such points will lie in the straight line AB which is the graph of the equation. An equation containing the variables x and y in the first power only is called an equatior, of the first degree. The general form of _the equation of the first degree, with two variables, is Ax + ^y + ^ - ^, where A, B, and C are constants which are finite or zero and may be positive or Negative. It may be proved that the graph of an equation 130 PRACTICAL GEOMETRY of the first degree is a straight line, and since a straight line is fixed by two points in it, the graph of such an equation may be drawn as soon as two values of x and the two corresponding values of y are known. For example, take the equation —2x-\-^y — ^ = 0. Put X = 0, then ^ = 3. Put a; = 10, then ?/ = 9|. Plotting the points a; = 0, 2/ = 3j ^^d ic = 10, 2/ = 9|, and joining them determines the graph of the equation — 2.t; + 3^/ — 9 = 0. If a straight line is pa'rallel to OX and at a distance h from it, then for every point in the line y = h, and this is the equation to the line. The distance h is positive or negative according as the line is Fig. 243. above or below OX. If a straight line is parallel to OY and at a distance a from it, then for every point in the line x = a, and this is the equation to the line. The distance a is positive or negative according as the line is to the right or left of OY. For problems in co-ordinate geometry " squared paper " will be found very convenient. Fig. 243 represents a piece of squared paper on which are drawn eleven straight lines numbered 1 to 11. The equations to the lines shown in Fig. 243 are given below and the student should carefully study these, comparing them with their graphs. The unit used is the length of side of the small squares. 1. y z= ^x -^ 5, or 2y = X -{- 10. 3. y z= ^x — 7, or 2?/ = £c - 14. 2. 2/ = 2^ + 0, or 2y = x, i. y = — 2x -\- 5, or 2x -{- y = 5, PLANE CO-ORDINATE GEOMETRY 131 5. y = — JiT + ^> or a; + 2?/ = 8. 6. 2/ = -^x - 5, or a; + 3?/ + 15 = 0. j^ y = —X — b, or X -{- y -{- 5 = 0. = 5, or -5 = 0. 9. X = 7, or a; - 7 = 0. 10. X = -10, or a; + 10 = 0. 11. y = -7, or 2/ 4- 7 = 0. Comparing the lines 1, 2, and 3 it will be seen that they are parallel, and when their equations are written in the form y = mx + c, the coefficient of x is the same for each line. Line 4 is perpendicular to lines 1, 2, and 3, and the " m" for 4 is the reciprocal of the " m" for 1, 2, and 3, with the sign changed. If the units for x and y are represented by the same length on the graph of the equation y = mx -\- c, then m is the tangent of 6 (Figs. 241 and 242) the inclination of AB to the axis of x, 6 being measured in the anti-clockwise direction. But in many practical problems in co-ordinate geometry the co-ordinates x and y represent different kinds of quantities and even when they represent the same kind of quantity the scales used for measuring them on the graphs may be different, and the slope of the line which is the graph of the equation y = mx-\-c, where wi is a definite number, may be very different in different cases depending on the scales used for measuring x and y. These remarks will be better understood after studying the following two examples. Example 1. — In a certain machine for raising weights the effort Q, in pounds, at the driving point required to raise a load W, in pounds, was found to be given by the equation Q = 0-2W -f- 4. Since Q is much smaller than W a more satisfactory graph of the equation is obtained by using a larger scale for Q than for W. Fig. 244 shows a graph of the equation with the scale for Q five times that for W. Observe that PI to find m or ^ from the graph, PL must be measured on the effort scale and CL on the load scale. On the effort scale PL = 80 and on the load scale CL = 400. Therefore §^ = ^ = ^'^ ^^ ^^ the equation given. . Example 2.— The horse-power, H, of a steam engine was varied by altering the initial steam pressure. The weight of steam, W, in pounds, used by the engine per hour, was measured at different powers and the results were as given in the table. Plotting H horizontally 200 LOAD,W Fig. 244. H ' W 8 150 16 303 26 454 34 548 40 650 132 PRACTICAL GEOMETRY IV\}- - ■ 1 J D ocno- ^ ^-^ S^no- _^ ^ ae -^^ >r^nn- ^z! ^^i" ^300 .-^ 1 1 1 1 1 1 1 1 1 1 ui200 ^^ 55'°°c^^ 1 &; '6 10 20 30 40 HORSE -POWER, H Fig. 245. to a scale of 1 inch to 20 horse-power, and W vertically to a scale of 1 inch to 500 pounds, the results are shown by the dots in Fig. 245. It will be seen that these dots are approximately in a straight line, and that the straight line passing through the points H = 0, W = 50, and H = 40, W = 650, lies evenly amongst the dots. Hence the rela- tion between W and H is given approximately by an equation of the form W = wH + c, where c = 50, PL 600 and m= ^,^= W= ^^- Observe that c and PL are measured on the W scale and that CL is measured on the H scale. Judgment is required in choosing the scales for x and y in plotting. In general the scales should be such that, in the case of a straight line, the line should be inclined to the axis of x at an angle lying between 30° and 60°. In co-ordinate geometry when the part of a line or a figure is being dealt with which is at considerable distances from the axes, a new pair of axes may be drawn nearer to the figure and parallel to the original axes which may now be off the paper. The new origin will however not be the zero point for x or y. For example if the new axis of y is 50 units to the right of the original axis of y the new origin will represent 50 on the axis of x. 112. The Circle.— Referring to Fig. 246, C is the centre of a circle, the co-ordinates of C being a and b. P is any point on the cir- cumference of the circle, the co-ordinates of P being x and y. PM and CN are the perpen- diculars from P and C on OX. CL is parallel to OX and meets PM at L. Let CP, the radius of the circle, be denoted by r. In the right-angled triangle CPL, CL^ + PL^ CF. But CL = NM = OM - OK = a; - a, PL = PM - LM = 2/ - t, and CP = r. Therefore (x - of + (y - hf = r" or x^^f- 2ax - 2ay + a^ + 1'' - 7^ = 0. This is the equation to the circle, r must always be positive, but a and h may be either positive or negative. Conversely the graph of an equation of the form x'-^f + Ax-hBy + C = PLANE CO-ORDINATE GEOMETRY 133 is a circle whose centre has for co-ordinates, a = — and 6 = — , n 2i and whose radius is r = JVa^ + B^ — 40. 113. The Farabola.~OK (Fig. 247) is a fixed straight line, and F is a fixed point. P is a point which moves in the plane of F and OK, so that its distance from F is always equal to its distance from OK. The path of P is a parabola, whose axis is the line through F perpendicular to OK. The line OK is called the directrix, and the point F the focus of the parabola. The curve cuts the axis at A, the vertex of the parabola. FA is equal to AO. Draw PK perpendicular to OK, and PN perpendicular to the axis. Draw the tangent to the parabola at A, and let it meet PK at K'. The tangent at A is obviously perpendicular to the axis of the parabola. Let FA = «, PN = X, and PK' = y. Then PN^ + FN' = PF^ = ON^. That is, x^-i-(ij - of = (y + af. Therefore x^ = iay . , (1) which is the equation to the parabola referred to the axis of the parabola and the tangent at the vertex, the axis being the axis of y, and the tangent the axis of x Fig. 247. Fig. 248. Fig. 249. If the axis of x be moved parallel to itself until it is at a distance h from the vertex (Fig. 248), then ^ in (1) will become y — h, and the new equation will be x'^ = 4 f^ *x-^ ^ V. 6 C y" i^'iQ. 250. 134 PRACTICAL GEOMETRY Fig. 251. Ou IT semi-minor axis by 6, then the equation to the ellipse is -2 + |2= 1j If a = h = r, then a? ^ y^ = r^, which is the equation to the circle when the origin is at its centre. 115. The Hyperbola. — Let a denote the semi-transverse axis and h the semi-conjugate axis of an hyperbola. Let the origin be taken^«* at C (Fig. 251) the centre of - the hyperbola, and let the trans- v^ vK- - X verse and conjugate axes be taken as the axes of x and y respectively. If X and y are the co- ordinates of any point P on the x^ iP- hyperbola, then -^ — p = 1» or h^^ — €?y^ = a^h\ and this is the equation to the hyperbola. If X and y are the co- ordinates of any point Q on the conjugate hyperbola, then V X y 2 ^ = 1, or ay — 6V = a^¥, and this is the equation to the con- jugate hyperbola. If 6 = a, the hyperbola is equilateral or rectangular, then x^ — y^^a^ for the hyperbola and y"^ — x^ = a^ for the conjugate hyperbola. The rectangular hyperbola and its conjugate are identical but differently situated. In the rectangular hyperbola the asymptotes are at right angles to one another. An important equation to the hyperbola is that obtained by taking the asymptotes as the axes of x and y as shown in Figs. 252 and 253, which show one branch only of the curve. OA the semi- transverse axis bisects the angle XOY and the curve is symmetrical about OA pro- duced. In Fig. 252 the asymp- totes are oblique while in Fig. 253 they are at right angles to one another. The hyper- bola in Fig. 253 is therefore Fig. 252. rectangular. Y -xH, i^ ^^^ \t X Fig. 253. For Fig. 252, xy = semi- axes as before. + h' = constant, where a and h are the In Fig. 253, 6 = a and xy = -^ = constant. The curve xy = ^ = constant (Fig. 253) is an important one. In PLANE CO-ORDINATE GEOMETRY 135 the form PV = constant, the co-ordinates of this curve give the relation between the pressure and volume of a gas when it expands or is com- pressed isothermally, that is, at constant temperature. A simple construction for finding any number of points on the curve xy = constant when one point is given is described in Art. 50, p. 47. 116. The Curve y = x^— Whatever be the value of n in the equation y = .x" if x = 0, then y = 0. Therefore the curve whose equation is y = x1 passes through the origin. Let n = 1, then y = x which is the equation to a straight line. Let n = 2, then y = x^ which is the equation to a parabola. Whether x is positive or negative its square is always positive, there- fore ?/ is always positive and the curve lies entirely above the axis of X. Also since x = ± ^/y the two values of x corresponding to any given value of y are numerically equal, but one value is positive and the other negative. The curve is therefore symmetrical about the axis of y. Also if a; = 4-1,?/= +1, and ii x = —l,y= -f 1. Let n = 3, then y = x^. If x is positive x^ is positive, and if x is negative ay^ is negative. Hence the sign of y is the same as that of ic, and the curve lies in the first and third quadrants. If ic = -f-l> 2/ = -f-1, and ii x = —I, y = —1. To plot the curve y = x^ for any given value of n, first select values of X and calculate the corresponding values of y and tabulate as here shown for n = = 2 anc n = 3, then plot. X = 0-0 ±0-4 zkO-8 ±1-0 ±1-2 ±1-4 n = 2,y = 00 +0-16 +0-64 + 1-0 + 1-44 4-1-96 n = S,y = 0-0 ±0-064 ±0-512 ±1-0 ±1-728 ±2-744 Fig. 254 shows the curves (1) y = x, {2) y = x^, and (3) y = a^. The curve y = x^ is known as the cubic parabola. In Fig. 254, the scale for y is the same as that for x and the true forms of the curves are shown. It will be seen that when n is greater than 1 y increases more rapidly than ic, and for comparatively small values of x, y becomes very large when w = -3. To show a sufficient amount of the curve within a reasonable area when n is greater than 1 it is generally necessary to make the scale for y smaller than that for X. This will alter the shape of the curve without altering its character. This will be referred to again when considering the curve y = bx\ Considering further the influence of n on the form of the curve y = x^, it is evident that so long as w is a positive integer, y will have the same sign as x when n is odd, and y will always be positive when n is even whether x is positive or negative. Calling the curves having n odd the odd curves and those having n even the even curves it follows that all the odd curves lie in the first and third quadrants while all the even curves lie in the first and second quadrants. Also, 136 PRACTICAL GEOMETRY (2) as n nearer but for a given ^ ]og y = 1'3 log X. Assume values for X, calculate and tabulate as follows. (3)f IIS ;p -2-4 -2-a H-6 -0-a z 04 Fig. 254. t .'(3) , (I) y=x all the odd curves pass through the points (-f- 1, -f l)and (— 1, —1), that is through the points P and R, Fig. 254, and all the even 'curves pass through the points (+ 1, 4- 1) and (—1, +1)5 that is through the points P and Q, Fig. 254. It will be seen that for a given value of y, greater than ± 1 increases the curve to the axis of y ; value of y less than ± 1 the curve moves further from the axis of y as n increases. Generally in practical problems only positive values of x and y have to be considered, and these relate to the curve in the first quadrant. When n is positive but not a whole number, values of y corre- sponding to assumed values of x in the equation y = x" are found by (D using logarithms as follows. If y = x^ then log y = n log x. For example, to plot the curve y = x^"^ t2 X - 1 2 3 4 5 6 log X = 0-3010 0-4771 0-6021 0-6990 0-7782 log y = 1-3 log X = 0-3913 0-6202 0-7827 0-9037 1-0117 y = 1 2-46 4-17 6 06 8-10 10-27 The curve is shown plotted in Fig. 255, and for comparison the curves y = x, and y = x^ are also shown. 117. The Curve y = bx'^— Let y' = x^, then y — by'. Hence if the curve ?/' = ic'* be plotted, the curve y = by' = bx'' will be obtained by en- larging (or reducing if Z^ is a fraction) the ordinates of the curve y' = x" b times. This is evidently equivalent to drawing the curve y' = x'' with another scale for the ordinates. The factor h may therefore be called a scale factor since it does not alter the character of the curve. tyx^ w ^ -yx PLANE CO-ORDINATE GEOMETRY 137 118. The Curve y = a + bx".— Let y' = hx'\ then y = a + y'. Hence if the curve y' = hx" be plotted, the curve y = a -\- y' = a -{- bx"" will be obtained by raising (lowering if a is negative) the curve bodily- through a height equal to a, or more simply, by lowering (raising if a is negative) the axis of a; a distance equal to a. An important problem of frequent occurrence is to find the equation to a given curve which may have been obtained by plotting a number of observations or the results of an experiment. Let AEF (Fig. 256) be such a curve referred to the axes OX and OY. An inspection of the curve suggests that it may be of the form y = a -\- hx^. The value of a is found at once and is equal to OA which in this case is 80. Take A as a new origin O' and let y denote the ordinate of any point on the curve, measured from O'X' ; then y' =y — a=:y — 80 = hx". m^ Will >F y z z 400 / /. z A. ^ 7 y ^y A^^=^ tf x' it 10 20 30 X JD^ Ao 7 ^ y" - ^^ ^•u- 7 "5^ ; y ^ ^ •^ ^^ 1.0 ^^ 10 ^^ ^ / C? : L X U r 10 l-S logx Fig. 257. Fig. 256. Values of X and y are given in the following table 1 X 5 10 15 20 25 80 y 114 175 255 348 455 574 y' = y - 80 34 95 175 268 375 494 logx 0-6990 1-0000 1-1761 1-3010 1-3979 1-4771 log y' 1-5315 1-9777 2-2430 2-4281 2-5740 2-6937 If the curve is of the form y' = bx"", then log y' = logb + n logx. ^ Let log y' = y", log b = c, and log x = x', then y" = c -\- nx\ which is the equation to a straight line. Values of y' corresponding to the given values of y are inserted m the table, also the values of log x and log y\ taken from a table of logarithms. Plotting the values of log x and log y', as shown in Fig. 257, it is 138 PRACTICAL GEOMETRY PL found that the points lie in a straight line for which n = — - = 1*5, CL PL being measured on the log y' scale and CL on the log x scale. c = OC = 0'477. Hence log b = 0477, and the equation to the curve is, y = 80 -{- 3x^^. * If the points (log x, log y') are not exactly in a straight line, a mean line may be drawn amongst them, from which n and log h may be taken to get an approximate equation to the given curve. 119. The Carve yx^ = c. — The most important application of the equation ^a;"*= c is to the curve whose co-ordinates give the rela- tion between the pressure and volume of a gas which expands or is compressed. If p is the pressure of a gas when its volume is v, then when the gas expands or is compressed the pressure and volume both vary and in general the relation between them is given by an equa- tion o6 the form j9y" = c. In the case where n = I, pv = c, and the curve is a rectangular hyperbola which was considered in Art. 115, p. 134. In studying the curve pv'"- = c only positive values of p, Vj and n need be considered. If y = 0, then >;" = 0, and in order that p X may have the finite value c, p must be infinite. Again, if j? = 0, then v'^ must be infinite, and v must also be infinite if n is finite. Hence the curve j?y" = c approaches nearer and nearer to the axes but never actually meets them, or it meets them at infinite distances from the origin. The axes are therefore asymptotes to the curve. As an example consider the curve py^^ = 292. Taking logarithms of both sides of the equation, logp + 1-3 log V = log 292. Letp = 60, then , log 292 log V = — log 60 2-4654 - 1-778^ '& "^ — 1-3 1-3 = 5286, and V = 3-38. Let V = 4, then logp = log 292 - 1-3 log 4 = 2-4654 - 1-3 x 0-6021 = 1-6827, and p = 48-2. In like manner for any given or assumed value of i; or j? corre- sponding values oi p ov V may be calculated. Various corresponding values of v and p are given in the following table, and these are plotted in Fig. 258, giving the curve ABD. V p 3-38 600 4 48-2 5 36-0 7 23-3 10 14-6 15 8-6 An important practical problem is to determine whether a given curve is of the form pv" = c, and if so to find the values of n and c. If pv'* = c then log p -{- n log v = log c, which is the equation to a straight line. PLANE CO-ORDINATE GEOMETRY 139 Let EFH (Fig. 258) be a given curve which appears to be of the fonn pv"" = c. Corresponding values of v and p for this curve are given in the following table, also the values of log v and log p. "nMuT I 1 1 [■ 1 1 1 1 50 Xa 50- ^ •An 3 ^ L^^ - 30 ^ ^ - \ ^1 a 9n ^F^ > 20- (^ _^^ 10 ^^ ^"*" — .^ — ~. D °'i"" !' 10 IS Volmne v Fig. 258. > 1 Cns- Z^O" s^ B^ "^S - ^ "^^ ^f : ^^ - ^^ i*u- ^. ^SP < __^^_^ logv Fig. 259. 10 V 2-2 3 5 10 15 p 60 40 £0 7-5 4-2 log V 0-3424 0-4771 0-6990 10000 1-1761 log 2) 1-7782 1-G021 1-3010 0-8751 0-6232 The values of log v and log p are plotted in Fig. 259, from which it is seen that the resulting points are in a straight line for which the PL equation is log p = — p-r log v + OC. Measuring PL on the log p PL scale and CL on the log v scale ^.^ = 1-4. Also OC, measured on the OL log p scale, is 2-267. Hence log p = -1'4: log v + 2-267, therefore w = 1-4, log c = 2-267 and c = 185. The equation to the curve is therefore pi;^"^ = 185. In a problem such as the foregoing, if the points (log v, log p) are not exactly in a straight 'line, a mean line may be drawn amongst them, from which n and c may be found to get an approximate equation to the given curve. 120. The Curve y = ae^*.— In the equation y = ae^% e is the base of the Napierian system of logarithms, its numerical value to four places of decimals being 2-7183. a and h are constants. The above equation is called an exponential equation because the variable x occurs as part of the index or exponent of the power of e. The curve which is the graph of y — ae^"" is called an exponential curve. Let X = 0, then e*^ = e" = 1, and y = a. The constant a is there- fore the intercept of the curve on the axis of y. Let y = 0, then e*^ = 0, and a; = - oo . The curve is therefore asymptotic to the axis of x. 140 PRACTICAL GEOMETRY Y \ b / y=0'de^ 3 y-o 8.^ / \ / / \ / / '^N, 2 ^^ / ^ ^ y HiT^ H^ Fig. 260. Taking logarithms of both sides of the equation y = ae*% log y =log a -f hx log e = log a + 0-434'i6a?. From the equation log y = \og a -\- 0-43436a;, y may be calculated if x is given or assumed, or x may be calcu- lated if y is given or assumed. As an exam pie take a = 0*8, and 6 = 2, then y = OSe^, and log y = i-9031 + 0-8686a;. This curve is shown plotted in Fig. 260. The curve y = O'Se'^ is also shown in Fig. 260, and it will be seen that this second curve is the image of the first in a mirror represented by the axis of y. 121. The Curve y = a log« bx. — The curve y = a log, bx is called a logarithmic curve. Referring again to the exponential curve y = ae*"", logg y = logg a -\- bx log^ e, but log^ e = 1, therefore log^ y =loge a + bxj 1 y and X = T loge - , which is of the form x = p log^ qy. The logarithmic curve y = a log, bx is therefore of the same form as the exponential curve y = ae^'' with the variables x and y inter- changed. The logarithmic curve will therefore be asymptotic to the axis of y while the exponential curve is asymptotic to the axis of oa. 122. Spiral Curves. — If a straight line OP revolves in a plane about a fixed point O in a fixed straight line OX in the plane, and if at the same time a point P in OP moves along the line OP, the point P describes a curve called a spiral. The form of the spiral depends on the law connecting the displacement of the point P along OP with the angular displacement of OP. The point O is the pole and the fixed line OX is the initial line. The position of OP at any instant is given by the angle 6 which it makes with OX. 6 is the vectorial angle and r the length of OP is the radius vector. The position of P at any instant is fixed by r and 0. 123. The Archimedean Spiral. — In the Archimedean spiral the displacement of P from O is proportional to 6 and the equation to the curve is, r = a6 where a is a constant. It follows that for equal increments of there are equal increments of r. Stated in another way this means that if successive values of are in arithmetical pro- gression successive values of r are also in arithmetical progression. When ^ = 0, r = 0, and when = 27r, r = 27ra. If 6 be increased by 30° at a time from ^ = 0, then the constant increment of r is 27ra "12* PLANE CO-ORDINATE GEOMETRY 141 The coDstruction for plotting the curve when a is given is shown in Fig. 261. Radii are drawn at intervals of %r 30°. OA is the radius vector when 6 = 27r, or 360°. Hence OA = 27ra. O A is divided into -^^ =12 equal parts. The remainder of the construction is clearly shown in the figure. The tangent PQ at any point P makes an angle with the radius OP whose tangent is equal to — -. Hence if on a radius at right angles to OP, OL be made equal to a, PL will be the normal to the Fkj. 261. spiral at P, and the tangent PQ will be at right angles to PL. 124. The Logarithmic or Equiangular Spiral.— If the suc- cessive values of are in arithmetical progression and the correspond- ing values of r are in geometrical progression the curve traced by P becomes a logarithmic spiral. The equation to the logarithmic spiral is r = a*. Hence log r = log a, and this logarithmic equation may be used to calculate values of r for given or assumed values of 6 when the constant a is known. If ^ = 0, then r = 1 . Fig. 262 shows one and a quarter convolutions of the spiral to a scale of I when a = 1 -2, the unit being 1 inch. If^ =^or 30°, then log r = g log a 3-1416 X 0-0792 D = 0-04147, and r = 1*10. If the increments of ^ be taken equal to ^ then the increments of log r are equal to 0-04147 and successive values of r are quickly calculated. The logarithmic spiral has the property that the angle <^ which the tangent at any point of the curve makes with the radius vector at that point is constant. On account of this property the logarithmic spiral is also known as the equiangular spiral. The tangent of the angle (f> is given by the formula 142 PRACTICAL GEOMETRY tan <^ logio g _ 0-4:343 logi log a ' For the curve shown in Fig. 262, OP logr^ebgd Scale^i *^^^=0W92 = ^'^^- To draw the tangent at the point L, on the radius OL produced make LK = 1 on any scale, and make KH at right angles to OL and equal to 5-48 on the same scale. Join LH, then LH is the tangent to the spiral at L. If OP and OQ are any two radii of the logarithmic spiral, and if OR is a radius bisecting the angle POQ, then OR is a mean proportional between OP and OQ. This property may be used in constructing the curve geometrically when the pole and two points on the curve are known. 125. Graphic Solution of Equations. — Many equa- tions which are difficult or impossible of solution by ordi- nary algebraic methods may be readily solved by graphic methods. On the other hand the graphic method is gene- rally inferior to the algebraic method in the solution of the simpler forms of equations. But in any case a study of the graphic method will lead to a better understanding of the theory of equations. Consider first the simple equation ax -\- h = 0, where a and h are constants. To solve this equation graphically, let y = ax -j- h. This is the equation to a straight line which may readily be drawn. This straight line cuts the axis of x where y — 0, and the distance of this point from the origin is the value of x which satisfies the original equation. In this case the graphic method is obviously inferior to the algebraic. Next consider the pair of simultaneous equations ax -\- hy -{- c = 0^ and a^x -\- h^y + Cj = 0, where a, 6, c, a^, h^, and Ci are constants, The graph of each of these equations is a straight line, and the lines may readily be drawn, and the co-ordinates of their point of inter- section are the values of x and y which satisfy both equations. Ta-ke the equation I'Tx"^ — 0-75a; -1-5 = 0. This is not a difficult equation to solve by the method of algebra but its graphic solution will now be considered in order to illustrate graphic methods. First method. Let y = ITic^ — 0-75a; — 1*5. Choose a number of simple values of x and calculate the corresponding values of y. Plot the points whose co-ordinates are these values of x and y. %^ The Fig. 262. PLANE CO-ORDINATE GEOMETRY 143 curve joining these points will cut the axis of x where y = 0. There will be two such points and their distances from the origin are the values of x which satisfy the original equation. This curve is shown plotted in Fig. 263. The curve cuts the axis of X at A, giving x = 1-18, and at B, giving x = — 0'74, and these are the roots of the equation. The curve should first be sketched to a small scale through a few calculated points in order to see the probable form and position of the curve. The parts of the curve in the neighbourhood of the axis of x should then be plotted carefully to a large scale in order to obtain more accurately the points A and B. Second method. Rewrite the equation in the form 1 -7;?;^ = 0-75a;4- 1 *5. Let y' = l'7x', and let y" = 0-7b x -{- 1-b. Draw the graph of y" = 0*75a; 4-1*5 which is a straight line. Next draw the graph of y' = l'7u;^ which is a parabola. These two graphs are shown in Small sduar es 0-2 unit side lY ni jtx i ^4^ 2 ^^7 •♦. ^ r s ^ > ^ ^*^ • ^ t ^ 1 \ ? %^-.^ t ^ 'sL E^ -T H v^^ 1 ? >^ T "^ \ 7- "^^ ^ J -^-l!^^ r Fig. 263. Fig. 264. Fig. 264, and they intersect at the points E and F. The values of X for the points E and F are the required roots of the given equation. This is evident, for at these points y' = if and there- fore l*7a:^ = 0-7ic -|- 1*5 when for x is substituted the abscissa of E or the abscissa of F. The graph of y' = l'1x^ should first be sketched through a few calculated points and the parts in the neighbourhood of the straight line ?/" = 0'75a; -f- 1'5 should then be drawn carefully to obtain as accurately as possible the points E and F. In general the second method of solution just described will be found preferable to the first as it involves less calculation. As a final example take the equation ic^ — 0*6a; — 0*1 = 0. Re- write the equation in the form x^ = 0'6a; -f O'l. Let y' = x^, and y" = O'Qx -f 0-1. The graph of y" = 0'6x -f 0-1 is a straight line and the graph of y' = x^ is a cubic parabola. A rough sketch of the graphs to a small scale will show that their points of intersection are within the limits x = -\-l and x = —1. The graphs should now be drawn to a large scale between the limits a;= -f-1 and x= —1. They will appear as shown in Fig. 265. 144 PRACTICAL GEOMETRY m I 2E agia Their points of intersection, A, B, and C, give the roots x — 0-85, X = — 0'18, and x = — 0*67. In Fig. 265 the small squares are of O'l unit side. The given equation is of the form x^ ■\- ax -\-'b =i ^^ and is a cubic equation. In the theory of equations it is shown that a cubic equation has three roots but one or more of these roots may be imaginary, that is, there may be three real roots, or two real roots, or one real root, or no real roots. This will be understood by reference to Fig. 265, for a straight line which is the graph of y" = —ax — b may meet the graph of y' = x^ at three points, or two points only, or -pj^ 265 one point only, and the line may not meet the curve at all. When the straight line does not meet the curve there is no real value of x which will satisfy the original equation. Similar remarks apply to the quadratic equation which may have two, but not more than two real roots. Exercises IX 1. The axes being at right angles to one another and the unit of length being 1-lOth of an inch, plot the points whose co-ordinates are given in the following table :— Point A B C D E F G H X 15 20 -17 -23 -18 16 y 20 25 16 - 9 -12 -8 2. Same as exercise 1 except that the co-ordinates are oblique, the angle XOY between the axes being 60°. 3. Plot the points whose polar co-ordinates are given in the following table, the unit of length being 1 inch. Point A B C D E F « H r 2-30 30° 1-25 90° 1-85 105° 2-65 180° 0-95. 200° 1-00 -100° 2-05 320° -1-70 -120° PLANE CO-ORDINATE GEOMETRY 145 4. State in tabular form the polar co-ordinates of the points given in exercise 1, r and d to be positive in each case. 5. The polar or vector co-ordinates of two points A and B are (3 inches, 30°) and (4-2 inches, 100°). That is, it O is the pole, and OX the line of reference, OA = 3 inches, XOA = 30°, OB = 4-2 inches, XOB = 100°. Draw OX and plot the points A and B, Measure AB and the perpendicular from on AB, and calculate the area of the triangle OAB. Verify your answer by calculating the value of |OA.OB sin AOB. [b.e.] 6. Given the equation y = 0-6x + 4 calculate the values of y corresponding to the following values of x, namely, 5, 10, 15, 20, 25, and 30. Taking the unit for X and y as 0*1 inch plot the six points of which the above values of x and the corresponding values of y are the co-ordinates. Show that all these points lie on the same straight line. 7. Draw the straight line (a) passing through the points (10, 15) and ( — 15, —15) and find its equation. Through the point (15, —3) draw a straight line (&) at right angles to (a) and find its equation. Find the co-ordinates of the point of intersection of (a) and (6). 8. Draw the graphs of the equations, x — 2y = 9, and a: -f 3?/ = 24 and determine the co-ordinates of their point of intersection. FiG. 266. 9. In arranging some elementary experiments in . statics, cyclists' trouser clips are used as .spring balances. In order to be able to measure pulls, a series of weights are hung on a clip, and the corresponding openings AA (Fig. 266) are measured. The results are as tabulated. Pull = P ounces . . 1 ^ 8 12 16 20 24 28 32 Opening AA = x inches 0-51 1 1-15 1-83 2-53 3-24 3-89 4-44 4-96 Plot a curve showing the relation between P and x, the scale for P being I inch to 1 ounce. Use this curve to graduate a decimal scale of ounces, which being applied to the spring at A A should measure any pull up to 32 ounces. 10. The co-ordinates of the centre of a circle being a and b, and the radius of the circle being r, draw the circles given in the following table. Dimensions are in inches. \ ' 11 III IV V VI VII VIII a 1 1-5 0-0 00 -1-5 -0-5 1-2 -1-0 0-0 b 20 1 1-5 00 -2-0 1-0 -1-2 0-0 1-3 r 1 1-5 1-5 1-8 2-0 1-6 1-2 0-8 1-7 11. Draw the circles whose equations are — I. a;2 -f ?/2 = 4. III. x'^+y^ -2x = 8. II. ic2 -f- 2/2 - 27/ = 3. IV. x'^ + y-i -2x-y = 2-75. 12. Draw the circle which passes through the three points (9, 8), ( — 16, 13), and (- 5, —12). The unit is to be taken as 0*1 inch. Find the equation to this circle. Draw the straight line joining the points (10, 18), and (— 25, 8), At the points where this line cuts the circumference of the circle draw the tangents and normals to the circle and find their equations. 13. Given the equation x^ = 2y, take the following values of x, namely, 0, ± 0-5, ± 1-0, ± 1-5, zt 2-0, ± 2-5, and ± 3-0, Calculate the corresponding values of y, plot the points, and draw a fair curve through them. Name the curve. Unit = 1 inch. 146 PRACTICAL GEOMETRY 14. Given the equation y^ = 2x — 1, take the following values of y, namely, 0, ±0-5, db 1-0, ±1-5, ±20, ±2-5, and ± 3-0. Calculate the corresponding values of x, plot the points, and draw a fair curve through them. Name the curve. Unit = 1 inch. 15. The equation to an ellipse is 0-49x2 + y^ = 1-96. Take the following values of x, namely, 0, ± 0-4, ± 0-8, ± 1-2, ± 1-6, ± 1-8, and ± 2-0. Calculate the corresponding values of y plot the points and draw a fair curve through them. Unit = 1 inch. 16. Draw the rectangular hyperbola xy = 200 between the limits a; = 5, and X = 40. Unit = 0-1 inch. 17. A cubic foot of gas at a pressure of 100 pounds per square inch expands isothermally until its volume is 5 cubic feet. Draw the expansion curve which shows the relation between the pressure and volume of the gas. Scales, — Pressure, 1 inch to 20 pounds per square inch. Volume, 1 inch to 1 cubic foot. 18. Plot the curves, y = x\ and y = x\ between the limits « = ± 2. Scale for X, 1 inch to 1 unit. Scale for y, 1 inch to 10 units. 19. Plot the curves, y = x-, y = x^'^, and y = x^, between the limits, x = and x = S. Scale for x, 1 inch to 1 unit. Scale for y, 1 inch to 5 units. 20. Plot the points whose co-ordinates are given in the following table, and find the equation to the fair curve joining them. 1 X 00 0-40 0-80 1-20 1-60 2-00 2-40 2-80 y 00 0-10 0-57 1-58 3-24 5-66 8-92 13-13 Take the scale for a; as 1 inch to 1 unit and the scale for y a,sl inch to 5 units. 21. Plot the points whose co-ordinates are given in the following table, and find the equation to the fair curve drawn through them. X 2 4 6 8 10 y 60 78 144 266 448 694 22. Plot the curve y{x + 0-75)' -'^ = 6, between the limits x = 0-75 and cc = 4, X and y being in inches. 23. The volumes {v cubic feet) and corresponding pressures {p pounds per square inch) of a pound weight of steam as it expands are given in the following table. Plot the expan»ion curve and test whether it approximately follows the law pv'^ = c, and if it does, find the values of n and c. V 3K) 3-7 4-7 6-1 7-9 10-6 14-5 20 2 V 153-3 118-3 90-0 67-2 49-3 ^ 35-5 25-0 17-2 24. Draw the first and second convolutions of an Archimedean spiral, having given that a certain radius vector cuts the first convolution at 0*7 inch from the pole and the second at 2 inches from the pole. Draw the tangent to the curve at the point which is 1*5 inches from the pole. 25. The equation to an Archimedean spiral is, r =: J0 inches. Draw two convolutions of the spiral. 26. Draw a triangle POQ. OP = 1-1 inches, OQ = 1-4 inches, and the angle POQ = 45°. P and Q are points on the first convolution of an Archimedean spiral of which is the pole. Find the initial line and draw the first convolution of the curve. 27. The equation to a logarithmic spiral is, r — 1-3^ inches. Draw one con- volution of the spiral and draw a tangent to the curve inclined at 60° to the initial line. PLANE CO-ORDINATE GEOMETRY 147 28. In a logarithmic spiral the common ratio of two radii containing an angle of 30° is 8:9. The longest radius vector in the first convolution is 3 inches. Draw one convolution of the spiral. 29. Plot the curve, y — 6-l"e (^-rs) from cc = to aj = 27r. You may obtain points on the curve by calculation, using mathematical tables ; or by projection from the logarithmic spiral, r = ae~*^'^^^^* Observe that in this spiral the ratio of the lengths of two radii which differ in direction by 360° = e " ""^^^ ^ ^'^ = 2-718 " ^'^^ = 1:3 very nearly. [b.e.] 30. The curve (Fig, 267) representing the curtail of a stone step is constructed of circular arcs, each of 90°. Set out the figure to the given dimensions, which are in centimetres. Scale \. [b.e.) 31. The given volute (Fig. 268) of one convolution is constructed of circular arcs each of 90°. Set out the curve, when the dimensions are as figured, in centimetres. [b.e.] Fig. 267. Fig. 268. Fig. 269. 32. Fig. 268 shows a construction for describing a volute of one convolution. Set out a similar curve of one and a half convolutions, when the dimensions, in centimetres, are as in Fig. 269. [b.e.] 33. Solve, graphically, the equations : — (1) x" - 2-bx + 1-5 = 0. (3) x^ - O'bx + 0-1 = 0. (2) «2 + 3a; + 2 = 0. (4) x^ + 2a;2 - 3a; - 3-375 = 0. 34. Solve, graphically, the simultaneous equations : — (2y^x-l=^0. , (x^+l = 9y. ^"■f \4:X + dy + 1-8 = 0. ^^^ \x^ +x = 6y. 35. Solve, graphically, the equations : — (1) 32=^ + 5x = 6. (2) 15a;2 - 2c2« = 0. CHAPTER X PERIODIC MOTION 126. Periodic Motion. — If any position of a moving body be selected and it is found that after a certain interval of time the body is again moving through that position in the same direction and with the same velocity, the body is said to have periodic motion. The interval of time between two successive appearances of the body in the same position moving in the same direction with the same velocity is called the periodic time or period of the motion. Periodic time is generally measured in seconds and will be denoted by T. The simplest case of periodic motion is that of a body revolving about a fixed axis with uniform velocity. In this case the periodic time is the time taken to make one complete revolution. A swinging pendulum has periodic motion, but it has different velocities in different positions. In general all the parts of a machine have periodic motion although some parts may have very variable velocities and very compli- cated motions during a period. The number of periods in the unit of time is called the frequency and is the reciprocal of the periodic time, or frequency = N = 1/T. 127. Simple Harmonic Motion. — P (Fig. 270) represents a point which is moving with a uniform velocity V along the circum- FiG. 270. ference of the circle XYXjYi whose centre is C. M is another point which is moving backward and forward along the diameter YY^ of the same circle in such a manner that PM is always at right angles to YYi, in other words, M is the projection of P on YYj. Under these circumstances the point M has simple harmonic motion. If XX, is a PERIODIC MOTION 149 diameter at right angles to YYi and if PN is perpendicular to XXj then the point N also has simple harmonic motion. CP is the representative crank of the harmonic motion of the point M or the point N, and the circle XYXiYj is the auxiliary circle or circle of reference. The amplitude of a harmonic motion of a point is the greatest dis- placement of the point from its mean position and is equal to the radius of the representative crank. Denote the angle PCX by 6 and let CP = r, CK = x, and CM = y. Then, x = r cos 6, and y = r sin 6. If the angular velocity of CP be o> = V/r, and if P moves from X to P in the time t, then 6 = lot. Hence, x = r cos wt, and y = r sin o)t. If the time t be plotted along the straight line OL and the corre- sponding displacement y be plotted at right angles to OL as shown in Fig. 270, the harmonic curve OEFGL is obtained. The length OL represents the periodic time and this has been divided into twelve equal parts. The circumference of the circle has been divided into the same number of equal parts to obtain the corresponding values of 6. The distance y is to be taken as positive when measured above XXi and negative when measured below. Also, the distance x is to be taken as positive when measured to the right of YYi and negative when measured to the left. Since 6 is proportional to t, lengths along OL will also represent values of and the curve OEFGL is then called a sine curve. If is in degrees OL represents 360°, but if is in radians OL represents 27r. The tangent to the harmonic or sine curve at any point Q is determined as follows. Draw Qq parallel to OL to meet the circle at q. Draw qn perpendicular to XX,. Make Q/= FO. Draw /S at right angles to OL. Make /S = tt to any convenient scale and make /H = 1 on the same scale. Make fu = Cw. Draw wK parallel to HS to meet /S at K. KQ is the tangent required. 2r The mean height of the curve OEF is — and the mean depth 2r of the curve FGL is also — or 0-637r. In other words, the mean ordi- nate for half a period is 0'637r. If s^ is the mean of the squares of the ordinates for half a period, then s^ = Jr^ and therefore s = 0-707r. These results are of importance in connection with alternating electric currents. Consider the equation y = 2 sin l"2t. This is the equation to a simple harmonic curve for which r = 2 feet, and is the angle which CP makes with CA. The angle a is positive when measured in the anti-clockwise direction and negative when measured in the clockwise direction. PERIODIC MOTION 151 Evidently 9 = (ft -^ a and y = r sin (cf) -\- a). If w is the angular velocity of CP and t is the time taken by P to travel from A to P, then (f> = wt, and y = r sin (wt + a). When a is positive it is called the advance or lead, and when it is negative it is called the lag. The curve which is the graph of the equation y = r sin (^ + «) is the same as the curve which is the graph of the equation y = r sin cf> except that it starts at a different point ; this is clearly shown in Fig. 272. The dotted part of the curve corresponds to the motion Fig. 272. of the crank from the zero position CX to the position CA which is to be taken as the new starting position. Observe that the equal divisions on the circle which correspond to the equal divisions on OL start from the point A. 129. Composition of CoUinear Harmonic Motions. — A simple way of giving a point a motion which is compounded of two or more simple harmonic motions is shown in Fig. 273. A and B are cranks which give simple harmonic motions to the rods C and D which carry pulleys E and F at their upper ends. G and H are sus- pended guide pulleys. A thin cord or line wire is fixed at one end K and passes under or over the different pulleys as shown. The free end of the wire is loaded and guided in a vertical direction and carries a pen or pencil P which traces a ..>.. ^ , curve on a sheet of paper stretched round / (g/g. ' / ^ ' a revolving drum L. The cranks and the '\^ y ^^-...^ drum are driven so that each has a uniform "' Fig. 273. velocity. The vertical components of the motions of the crank pins are communicated to the pencil but the amplitudes of these motions are doubled by the action of the pulleys. If one of the cranks is stopped while the other rotates uniformly, the pencil will have simple harmonic motion of the same period as that of the rod driven by the moving crank but the amplitude of the motion of P will be twice the radius of 152 PRACTICAL GEOMETRY the moving crank. When both cranks rotate the pencil traces on the moving paper a curve whose ordinates are the sum of the ordinates of the harmonic curves due to the separate cranks. Any number of harmonic motions may be compounded in this way by introducing a crank for each. The mechanism illustrated in Fig. 273 is the basis of Lord Kelvin's tide predicting machine. If the crank shafts be at a considerable distance from the guide pulleys G and H compared with the radii of the cranks, the pulleys E and F may be mounted directly on the crank pins and the mechanism is considerably simplified but the motions communicated to the pencil by the separate cranks are not quite simple harmonic motions. When two collinear simple harmonic motions of the same period and therefore of the same frequency are combined the resulting motion is also a simple harmonic motion. Referring to Fig. 274, OApL is the harmonic or sine curve for the crank CP which starts from the zero position CX. The radius of the 'f^ />\n/ X / / < ^x n ,'' ■f .... \ ; .... »N« / // r^y4o \ \, i;^ "■"^3 >- Fig. 274. crank CP is 1-8 inches and the equation to the curve OApL is therefore 2/i = 1-8 sin B in which Q is measured from the zero position of the crank. EFgH is the harmonic or sine curve for the crank CQ which has a lead of 45^. The radius of the crank CQ is 1*2 inches and the equation to the curve EFij'II is therefore 3/2 = 1*2 sin {0 + 45°) in which B is measured from the radius which is 45° in advance of the zero position CX. To combine the two curves the ordinates of the one must be added to the ordinates of the other. For example, rn =pw + 5^- In the addition regard must of course be paid to the signs of the ordinates. The equation to the resulting curve is ?/ = 2/1 + 2/2 = 1*8 sin ^ + 1*2 sin {B + 45°). The resulting curve in this case may be drawn independently as follows. Complete the parallelogram PCQR. Then the diagonal CR is the representative crank whose harmonic curve, having an angle of advance RCP, is the curve which has just been obtained by combining the harmonic curves Oj^L and EF^H. The general construction for determining the representative crank PERIODIC MOTION 153 -Y--- which will give to a point a harmonic motion which is the resultant of the harmonic motions of the same period due to any number of given representative cranks is shown in Fig. 275. CP, CQ, CR, and CS are the relative positions and radii of the given cranks at a given instant. Draw P^ parallel and equal to CQ. Draw qr parallel and equal to CR. Draw rs parallel and equal to CS. Then CS, the closing line of the polygon CP^rs is the crank required. The point whose motion is being considered is supposed to be reciprocating in the line YCYj. The proof of the above construction is as follows. The distance of the moving point from C at any instant is the sum of the projections of the given cranks on the line YCYi at the instant considered, regard being paid to the signs of these pro- jections. But the sum of these projections is evidently equal to the sum of the projections of CP, Vq, qr, and rs on YCYj, and this sum is also equal to the projection of Gs on YCY^. When the simple harmonic motions which have to be combined are not of the same period the resulting motion is not a simple harmonic motion. To construct the resulting displacement curve the separate simple harmonic curves are first drawn and then combined as already explained for motions of the same period (Fig. 274). An example of the compounding of two simple harmonic motions of different periods is illustrated by Fig. 276, where the full curve is the graph of the equation 2/ = 2 sin (^ + 30°) 4- 1-4 sin (W + 50°) 12 3 4 5 The curve (p ) is the graph of the equation 2/i = 2 sin (0 + 30°) and is the harmonic curve for the crank CP which starts with an advance of- 30°. from the zero position CX. 154 PRACTICAL GEOMETRY The curve (q) is the graph of the equation y., = I'i sin {20 + 50°) and is the harmonic curve for the crank CQ which starts with an advance of 50° from the zero position CX. It will be observed that the frequency of the second motion is double that of the first, that is, the crank CQ rotates twice as fast as the crank CP. 130. Composition of Harmonic Motions at Right Angles to one another. — The diagram (a) Fig. 277 shows two slotted bars at right angles to one another and driven by two cranks so that each of the slotted bars has simple harmonic motion. If a pencil P fitting both slots be passed through them where they overlap, then the pencil will have a motion which is compounded of two simple harmonic motions at right angles to one another. The remainder of Fig. 277 shows how the curve traced by the pencil P may be drawn. 26 w 25 l4jLl3 Fig. 277. In the example worked out in Fig. 277 the crank at (6) has a radius of 2 inches while that at (c) has a radius of 1 5 inches. The PERIODIC MOTION 155 first crank makes two revolutions while the second makes three revolu- tions. The frequencies of the two harmonic motions are therefore in the ratio of 2 : 3. When the first crank makes 30^ with the horizontal position CX the second makes 45° with CX. Calling these the initial positions, if the first crank turns through an angle W from its initial position the second crank will turn through an angle Z6 from its initial position, in the same time. The position of the point P is determined, with reference to the axes OX' and OY', {d) Fig. 277, by the two equations x = \'b cos (3^ + 45°) a-nd 2/ = 2 sin {26 + 30°) The circle (h) has been divided into 18 equal parts, starting from tlie initial position of its crank, while the circle (c) has been divided into 12 equal parts, starting from the initial position of its crank. Observe that the. numbers 18 and 12 are in the inverse ratio of the frequencies. The construction for determining points in the path of P is clearly- shown and need not be further described. taking different A great variety of curves may be obtained by A few of the simpler cases The result The result is a frequencies and different angles of lead, may be mentioned here. (i) Equal frequencies and equal cranks. (1) One crank 0° or 180° in advance of the other. is a circle. (2) One crank 90° in advance of the other. straight line. (3) For any other angle between the cranks the result is an ellipse, (ii) Equal frequencies and unequal cranhs. (1) One crank 90° in advance of the other. The result is a straight line. (2) For any other angle between the cranks the result is an ellipse. It is easy to show that when the path of P is a straight line its motion in that straight line is a simple harmonic motion. 131. Composition of Parallel Harmonic Motions. — AB (Fig. 278) is a vibrating link. The vertical component of the motion of A is a simple harmonic motion of which oa is the repre- sentative crank. The vertical component of the motion of B is a simple harmonic motion of which oh is the representative crank. The motions 156 PRACTICAL GEOMETRY of A and B have the same frequency. The advance angles of the cranks oa and oh are a and ^ respectively. C is a poiQt in AB or in AB produced either way. The vertical component of the motion of C is obviously a simple harmonic motion and it is required to find the representative crank for this motion. From a point o' draw o'a' parallel and equal to oa. Draw o'h' parallel and equal to oh. Join a'h' and divide it at c' so that a'c' : c'V : : AC : CB. Then o'c' is the crank required and y is its advance angle. The proof is as follows. Draw c'r parallel to h'o' to meet o'a' at r. Draw cs parallel to a'o' to meet o'h' at 8. Let the vertical motion of B be destroyed, then the vertical motion of C will be to that of A as CB : AB or as c'h' : a'h' or as o'r : o'a'. o'r is therefore the repre- sentative crank for the vertical harmonic motion of C when B has no vertical motion. In like manner when the vertical motion of A is destroyed and B is driven, the representative crank for the vertical motion of C will be o's. Hence, when A and B are both driven the representative crank for the vertical motion of C will be o'c' which is the diagonal of the parallelogram o'rc's as was proved in Art. 129. Denoting the lengths of the cranks oa, oh, and oc by a, h, and c respectively the equations for the vertical displacements of A, B, and C from their mean positions are 7/i = a sin [B -f a), y^^h sin {6 + )S), and 2/3=0 sin {0 + 7) where B is measured from the initial positions oa, oh, and oc. The above problem occurs in connection with reciprocating steam engine valve gears, oa and oh are eccentrics which drive the link AB. The valve is driven from a point C in AB. o'c' is the equivalent eccentric, that is, o'c' is an eccentric which would give the same motion to the valve, driving it directly, as the two eccentrics and the link AB give it. In a vertical engine if the crank is in the vertical position oYj when oa and oh are in the positions shown, then 180 -- a is the angle of advance of the eccentric oa, and /3 is the angle of advance of the eccentric oh. In the actual engine the eccentrics oa and oh are on the same shaft. 132. Velocity and Acceleration in Harmonic Motion. — CP (Fig. 279) is the representative crank for the simple harmonic motions of the points M and N which reciprocate along the vertical and horizontal diameters respectively of the auxiliary circle. Let CP = r and let the position of CP be defined by the angle B which it makes with ex. Let 0) be the angular velocity of CP and let V be the linear velocity of P. Then V = wr. Let the velocities of M and N when in the Fig. 279. positions shown be V^ and V^ respectively. These velocities are the vertical and horizontal components of V respectively. Hence V = V cos ^ = wr cos ^ = wr cos w/, and yx <\ \v^ P V \ ^ X N PERIODIC MOTION 157 V^ = V sin 6 = cor sin = mr sin wf, where t is the time taken by P to travel from X to P. If a scale for velocity be chosen such that CP = V, then PM = V^,, and PN = Y^. The auxiliary circle therefore becomes a velocity diagram on a displacement base for the simple harmonic motion of the point M or the point N. If the angular position of CP be measured from a radius CA which makes an angle a with CX and if the angle ACP = ^ then Vy = V cos (<^ + a) = wr cos ((^ + a) = wr cos {oit + a) and V^ = V sin ( + a) = inr sin (<^ + a) = cur cos (cu< + a) where t is now the time taken by P to travel from A to P. The velocities V^ and V^ may be plotted on a time t or angle B or angle <^ base in exactly the same way as displacements were plotted in Arts. 127 and 128. The radial acceleration of the point P is/= — = wV. Let the acceleration of the points M and N be fy and f^ respectively. These accelerations are the vertical and horizontal components of / respec- tively. Hence (Fig. 280) f^ =fsm 6 = — ^ sin ^ = coV sin 6 = oy^r sin wt, and fx=f cos = — cos = ooV cos 6 = (oh cos wt, where t is the time taken by P to travel from X to P. Since sin 6 = -, and cos $ = - the above equation may be written, and r r^' If a scale for acceleration be chosen such that CP = /, then fy = y and/^ = X. The acceleration of the point M is shown plotted on the vertical diameter YYi as a base. If the angular position of CP be measured from a radius CA making an angle a with CX and if the angle ACP = ^ then for in the above equa- tions substitute ^ -f- a. The accelerations fy and /, may be plotted on a time t or angle B or angle <^ base in exactly the same way as displace- ments were plotted in Arts. 127 and 128. When a point has a motion which is compounded of two or more simple har- monic motions the resultant velocity and resultant acceleration at any f 1 f t4 \*w*^ » M^^ '>^ / /\^ \ fe ArX Y \ ' \x-* 7 ^^^Y. Fig. 280. 158 PRACTICAL GEOMETRY instant are determined from the component velocities and component accelerations exactly as for displacements. 133. Harmonic Analysis. — It has been shown that the displace- ment of a point from its mean position, when it has simple harmonic motion in a straight line, is given by the equation y = r sin (0 -\- a) or hj X = r cos (^ + ct). Again, if a point has periodic motion in a straight line, and if its motion is compounded of a number of simple harmonic motions in which the separate displacements from the mean position are given by. the equations — x-^ = Vi cos (0 + tti), X.2 = rg cos (20 -f og), x^ = r^ cos (3^ -j- ag), and so on, then the resultant displacement is given by the equation — a; = ri cos (0 + aj) + r^ cos (20 -f- a^) + r^ cos (3^ + as) -\- . • • and it has been shown how such a resultant displacement may be found graphically and plotted to obtain a curve of resultant displace- ment on a time t or angle base. If instead of measuring the resultant displacement from the mean position it is measured from a point at a distance c from it, then, X = c -{- r^ COB (0 -^ tti) 4- r.2 cos (20 + o^) + rg cos (30 + a^) + . . . The right hand side of this equation is known as a Fourier series. Any periodic curve of displacement being given it may be resolved into a number of simple harmonic components. The number of these components is greater the greater the complexity of the given periodic curve. The process of breaking up a given periodic curve into a number of simple harmonic curves, or the process of finding the equation to' the curve in the form X = c -{- Ti cos (0 + tti) + **2 COS (20 + ttg) + r. cos (3^ + as) + • • • is called harmonic analysis. The process of harmonic analysis is one of great importance in connection with the study of the periodic motions of machines and of alternating electric currents. A graphic method of harmonic analysis which is comparatively simple and easily applied will now be described. This method is due to Mr. Joseph Harrison and was described by him in Engineering of Feb. 16th, 1906. The procedure will be illustrated by reference to a definite example. The full curve EFGH (Fig. 281) has been plotted on the base line OL. The base represents one complete revolution of a shaft upon which there is an eccentric which drives a slide valve through certain inter- mediate link-work. The ordinates of the curve represent the displace- ments of the valve from a certain fixed position. In order that the student may transfer this curve accurately and of full size to his drawing paper, and work out the example for himself, the ordinates have been dimensioned. Twelve ordinates at equal intervals will be used and these are numbered to 11. PERIODIC MOTION 159 In most engineering problems in harmonic analysis it will be found that not more than three of the harmonic terms are required and in many cases two terms are sufficient. In the example to be worked three terms in addition to the constant will be found. Fig. 281. The equation is i» — c + »'i cos (^ + tti) + r.^ cos (2^ + o.^ + **3 cos (3^ + a.^ and it is required to find c, r^, r<^ , and r.^ , also ai, a^, and a^. Expanding the right hand side, the equation may be written X = c -\- Vi COS tti cos — ri sin a^ sin -\- r2 cos tta cos 20 — r^ sin a^ sin 2^ + r^ cos ttg cos 3^ — rg sin a..^ sin 3^. Let r^ cos a^ = a^, r.^ cos 02 = aa , and r.^ cos a^ = a-^. 160 PRACTICAX GEOMETRY Also, let —Ti sia a^ = 6^, — rg sin 02 = ^2, and —r^ sin ag = 63. Then ic = c + «i cos ^ 4- ^2 cos 20 + % cos 3^ + b^ sin ^ + 62 sin 26 + 63 sin 3(9. Since ri cos aj = a^, and — r^ sin a^ = hi it follows by division that tan ai = \ Also rj^ = a^^ + 61^ and r^ = ± Va^^ + 6i"^. There are similar relations for the other corresponding constants. The constant c is the mean of all the given ordinates and in this case it is 1*63. From an origin O^ beginning with the zero direction draw 12 radial lines at equal angular intervals. Along these radial lines, beginning with the zero line, mark off in succession from Oi the ordinates to 11. Find the horizontal and vertical projections of these radiating vectors as shown. Find the sum of the horizontal projections having regard to their signs. This sum is 4*00 and is equal to Qai^ the coefficient 6 of «! being half the number of ordinates used. Therefore aj = 0'67. Find the sum of the vertical projections, having regard to their signs. This sum is 7*26 and is equal to 66^. Therefore b^ = 1*21. tan ai= = — 1*806 and aj = — 61° to the nearest degree Ti = ± \ ai^ -\- bi^ = ± 1'38. Since r^ cos a, = a^ and cos a^ and a^ are here both positive it follows that rj = + 1 -38. The first harmonic term or the fundamental term is therefore + 1-38 cos (^- 61°). Next, from an origin Oo , beginning with the zero direction, draw, at equal angular intervals, half the number of radial lines that were drawn from O^. On these radial lines, beginning with the zero line, mark off in succession from O2 the ordinates to 1 1, going twice round. Find the sums of the horizontal and vertical projections of these radiating vectors. In this case these sums are —1*09 and — 0*36 respectively. Now, 6a, = — 1*09, therefore a^ = — 0-18. Also, 6^2 = - 0*36, therefore ^2 = - 0-06. tan tta = = — 0*333 and 02= — 18° to the nearest degree. a^ r^ = ± V a2^ + 62^ ~ i 0*19. Since Tq cos ao = a^, and since cos aa is positive and a^ is negative r2 must be negative. Hence rg = —0*19. The second harmonic term or the octave term is therefore -0-19 cos (2(9- 18°). Lastly, from an origin O3 , beginning with the zero direction, draw, at equal angular intervals, one third of the number of radial lines that were drawn from Oj . On these radial lines, which in this case are at right angle intervals, mark off in succession from O3 the ordinates to 11, beginning with the zero line, and going three times round as shown. The sums of the horizontal and vertical projections of these radiating vectors in this case are +0*24 and -f0 04 respectively. PERIODIC MOTION 161 Now, 6a,, = 0-24, therefore a, = 0-04. Also, (jh, = 0-04, therefore 63 = 0-007. tan a.. = — ■' = — 0-175 and a.^ = — 10'^ to the nearest degree. ?••; = ± ^/ a.^^ + 63'^ = ± 0-04. Since r.^ cos ao = a., and since cos a^ and «3 are both positive, r.^ = -\- 0*04. The third harmonic term or the term of the third order is therefore + 0-04 cos (3^ - 10°> The complete equation is now fl!=l-63 + l-38 cos (6l~6rj-0-19 cos (2i9-18°) + 0-04 cos (3(9-10°). The crank circle for the fundamental term x^ = 1-38 cos {0 — 61°) is shown and the curve for this has been projected as explained in Art. 128, and is shown dotted. If the student will work out this example, step by step as described, and also the last four exercises at the end of this chapter, he will find that the method is simpler than it looks from the foregoing somewhat lengthy description. After finding the Fourier equation it is a useful exercise to con- struct the component simple harmonic curves and then construct the resultant curve to see how near it approaches to coincidence with the original curve. If the angular velocity w in the equation 6 = (ot is known, curves of velocity and acceleration for the component harmonic motions may be constructed, and from these the resultant velocity and acceleration curves may be determined. Or the equations for the component velocities and accelerations may be found, and then by addition the equations for the resultant velocity and acceleration may be obtained and then used to calculate the velocity or acceleration for any position of the moving body. Exercises X 1. A point has simple harmonic motion of amplitude 2 inches and periodic time 2 seconds. Construct the curve which shows the relation between displace- ment from mean position and time. Scales. — Displacement, full size ; time 3 inches to one second. Draw the tangents to the curve where the time is 1 second and 1-3 seconds. 2. Taking the equation to a simple harmonic curve, y = r sin oot, cpnstruct the curve for the case where r = 0-75 foot and the frequency is 2 periods per second. Scales. — Displacement, 3 inches to 1 foot; time 10 inches to 1 second. What is the value of u in radians per second ? 3. Construct the sine curve y = 1-75 sin 6, from 6 = 0° to 6 = 360° taking intervals of 30°, y being in inches. Scales. — For y, full size ; for 9, 1*5 inches to 90°. Find the mean of the mid positive ordinates. 4. Given the equation, y = 2 sin 0, fill up the following table, by calculation, taking sin 6 from a table of sines. 162 PRACTICAL GEOMETRY 1 h° 15° 25° 36° 45° 55° 65° 75° 85° j Meau. 1 Sin.e i - 1 y i 1 t Plot e and y and 6 and y^ from = 0° to = 90°. Scales.— 7/ in inches, full size ; Q, 5 inches to 90°. . 5. Given the equations, y^ = 1-7 sin 6, and y^ = 2 sin {6 + 30°), plot the values of 2/i + 2/2 and 6, and y^yo and 6 for values of 6 from 0° to 360° at 30° intervals. 6. A point M has a simple harmonic motion, in which the displacement x from the mid position C is given in inches by x = 2 sin (1-5^ + 0*4), t being time in seconds and the angle being in radians. Draw a horizontal line (along the tee square) for the path of M, on which mark the centre C and the limits.of the swing. Let positive displacements be those to the right of C. Draw the representative crank, its rotation being clockwise. Find the positions of M when ^ = and when t = 2 seconds and measure CM in both cases. [b.e.] 7. A weight hangs by a spring, and has an up and down simple harmonic motion of period T = 2 seconds and amplitude a = 2-25 inches, the advance a being — radians (at the instant when time begins to be reckoned). The dis- placement y from mean position at any time t is thus given by the equation (i^t + a ) = 2-25 sin y = asm (^t + l) to Draw a curve showing the relation between y and t at any time from t t = T = 2 seconds. Adopt as the horizontal scale for time 3 inches to 1 second, and take the ver- tical scale for y full size. Read off the displacement y when t = 025 second, [b.e.] 8. A motion in a straight line, which is compounded of two simple harmonic motions of the same period, is itself a simple harmonic motion of that period. If X is displacement of a point at time t, this theorem is represented by the equation : — jc = «! sin (qt + 61) + a-i sin {qt + e^) = A sin [qt + E). Determine graphically and measure the amplitude or radius A, and the advance E of the resultant motion, having given the corresponding elements of the component motions, viz. : — ai = 2 inches, a^ = S inches ; Ci = 0*25 radian, e, = l"! radians. Find and measure the displacement x when ^ = 0, and also when ^ = 3 seconds, the angular velocity q being J radian per second. [b.e.] 9. Three simple harmonic motions in a straight line are represented by the equations : — 2/, = 1-5 sin O-U, y. = 1-2 sin (0-8^ + 1), and y, = 0-9 sin (1-6^ + 0-5), where y^, y^, and 2/3 are displacements in inches from the mean position, the angles being measured in radians and the time in seconds. These three motions are combined. Plot the separate displacements and the resulting displacements on a time base for a complete cycle. 10. The motion of a point in a straight line is compounded of two simple harmonic motions of nearly equal periods, represented by the following equation : — X = 2-1 sin fdt + ij + sin 8^, where x is displacement in inches from mean position and t is time. PERIODIC MOTION 163 Let the complete period of vibration be divided into nine equal intervals. Taking only the first, fourth, and seventh of these intervals, in each case draw a curve in which abscissae shall represent time, and ordinates the corresponding displacements of the point. Let the time of one of the intervals be re- presented on the paper by a length of 8 inches. In determining successive ordinates the method of projection from the resultant crank may be used with advantage. [b.e.] 11. In the equation y = 2-6 sin [6 + 31^) + 0-33 sin (2a + 112°), which represents a simple vibration with a small superposed octave, the displacement y for any value of 6 is given approximately by the construction defined on the diagram. Fig. 282. By means of this construction, or otherwise, determine y for values of d of 0°, 30°, 60° . . . 360°. Plot a curve with y as ordinate on a 6 base. Scale for 6. — 1 inch to 60°. From your figure measure y when e = 192°, and compare this with the true value of y as calculated from the equation, using the table of sines. [b.e.] 12. A point P in a plane has a compound harmonic motion, whose components parallel to two perpendicular axes OX, OY are given by the equations y = rsln (e+(i)+s sm(za-t 6) Fig. 282. X = a cos {ut + o) = 2*5 cos ( ^ + 7/ = 6 sin {2a>^ + )8) = 1*5 sin i)' inches. inches. Plot the complete locus of P. [b.e.] 13. Referring to Fig. 277, p. 154, draw, full size, the locus of the point P when the frequencies of the component simple harmonic motions are as 3 : 4 instead of 2 : 3. 14. A, B, C are three coUinear points in a vibrating link. AB : BC : AC = 5:1:6. The component motion of A in a certain direction is simple harmonic, with half travel 4 inches, advance —90° ; that is, displacement a?i = 4 sin ( »^ - ^ j = 4 sin (a - 90°). The component motion of B in the same direction is given by x^ = h sin o)t = b sin d. Let the component motion of C be defined by the equation X = a sin {6 -{- a). Find the half travel a and the advance a for the following values of b, and tabulate the results, as indicated ; — ' Values of b in inches. 00 0-5 1-0 1-5 Half travel a Advance o 15. Taking the data of exercise 7 plot the velocities and accelerations of the weight on a time base. Scales. — Time, 3 inches to one second ; velocity, maxi- rnum^ velocity in feet per second = 2-25 inches ; acceleration, maximum accelera- tion in feet per second per second = 2*25 inches. Determine the lengths which represent a \velocity of 1 foot per second and an acceleration of 1 fobt per second per second. 164 PRACTICAL GEOMETRY 16. Taking the data of exercise 9 plot the velocities and accelerations of the component simple harmonic motions also the resultant velocities and accelera- tions, all on the same time base, for a complete cycle. Construct the velocity and acceleration scales. 17. The slide valve of a steam engine is actuated by a Joy gear. Fig. 283 L AS 6 4 I Ll_ 7 30 Copy double this size Fig. 283. I 2 -*- + gives eight positions, 0, 1, 2, ... 7 of the valve, corresponding to the eight crank positions e of 0°, 45°, 90°, . . . 815°. Measuring from the point A, the displacement x of the valve for any crank position Q is given approximately by the Fourier equation — a; = c + a, cos + tto cos 20 + a^ cos 3a + a^ cos 40 + hy sin e + hi sin 20 + 63 sin 30. Determine the eight constants in this equation. If the speed of the crank shaft is 10 radians per second, what is the velocity of the valve when = 0? [b.e.] 18. One cycle of a periodic curve A is given in Fig. 284. Express 2/ as a 360* Fig. 284. function of 0, assuming that all the Fourier vectors of the fourth and higher orders are negligible. 19. The curve B (Fig. 284) shows the displacement ij inches of the block in the link of a Stephenson valve gear, for any crank position degrees, during one revolution of the crank shaft. Express y approximately in terms of by the first three terms of the Fourier series — 2/ = ri sin (0 + Oj) + r^ sin (20 + Uo) + r^ sin 4- a constant Give values of r,, r,, rg, and Oi, a,, 03. . ? IE M Copy double this size + direction Fig. 285. ' + ^3) 20. A point P oscillates in a straight line, the motion being repeated in- definitely. The period of oscillation being divided into twelve equal iuteryjijs, PERIODIC MOTION 165 beginning when t = 0, you are given, in Fig. 285, the twelve corresponding positions of P, numbered to 11. Suppose the displacement from mean position at any time t is given very approximately by the first three terms of the Fourier series— cc = a sin {wt + a) + 6 sin (2a>i + 3) + c sin (3«^ + 7). Find the elements of the motion, that is, find the three half travels a, &, c and the three angles of advance, a, )3, 7 for this case. CHAPTER XI PROJECTION 134. Descriptive Geometry. — Practical Solid Geometry, or Be- 8crij)tive Geometry is that branch of geometry which treats (1) of the representation, on a plane surface, of points, lines, and figures in space, in such a way that the relative positions of the points, lines, and figures, and also the exact forms of the lines and figures are determined, and (2) of the graphic solution of problems connected with points, lines, and figures in space. The problems of descriptive geometry are best solved by means of the method of projections. 135. Projection. — When an object is seen by the eye of a spectator, rays of light come from all the visible parts of the object and converge towards a point within the eye. Now suppose that a flat sheet of glass is placed between the object and the eye of the spectator, and that each ray of light, in passing through the glass from the object to the eye, leaves a mark on the glass of the same colour and tint as the part of the object from which the ray came. In this way a picture would be produced on the surface of the glass, and if the object be removed while the picture and the eye remain stationary, the picture would convey to the mind of the spectator the same knowledge of the object as was conveyed by the presence of the object itself. Again, if instead of the rays of light from all the visible points of the object leaving an impression on the glass, only those which came from the edges of the object were to do so, an outline would be produced on the surface of the glass which, although it would not convey to the mind of the spectator the same impression as the presence of the object itself might still give a good idea of its form. The foregoing remarks are illustrated by Fig. 286, where AB represents an object viewed by an eye at E ; CD is a plane interposed between E and AB ; the thin dotted lines represent a few of the rays of light passing from the edges of the object to the eye, and A'B' is the outline obtained from the intersections of the rays of light with the plane CD. The figure A'B' is called a projection of the object AB on the plane CD. The plane upon which a projection is drawn is called a plane of projection. The rays of light or imaginary lines passing from the different points of the object to the corresponding points of the projection are called projectors. PROJECTION 167 When the projectors converge to a point the projection is called a radial, conical, or jperspective projection. When the point to which the projectors converge is at an infinite distance from the object the projectors become parallel, and the projection is called a parallel projection. If besides being parallel the projectors are also perpendicular to the plane of projection the projection becomes a perpendicular, an orthogonal, or an orthographic projection. For the purposes of descriptive geometry orthographic projections are the most convenient and most commonly used, and when the term projection is used without any qualification orthographic projection is generally understood. In what follows projection will mean ortho- graphic projection. The projection of a point upon a plane is the foot of the perpendicular let fall from the point on to the plane. The projection of a line upon a plane is the line which contains the projections of all the points of the original line. The projecting surface of a line is the surface which contains the Fig. 286. projectors of all the points of that line. When the projecting surface of a line is a plane it is called the projecting plane of the line. The projecting surface of a straight line is always a plane, but a line is not necessarily straight because its projecting surface is a plane. These definitions of projecting surface and projecting plane of a line and the statements which follow them apply to all kinds of projection. One projection alone of a figure is not sufficient for determining its exact form. For example if a triangle ahc drawn on a sheet of paper be taken as the projection on the paper of a triangle ABC somewhere above it, it is clear that the exact form of the triangle ABC will depend on the relative distances of its angular points from the paper, but the projection ahc gives no information about these distances. If, however, another projection a'b'c of the triangle ABC be obtained on a sheet of paper at right angles to the former one, then, as will be shown later, the true form of the triangle ABC may be obtained from these two projections. The representation of an object by means of two projections, one on each of two planes at right angles to one another, and how these 168 PRACTICAL GEOMETRY projections are drawn on a flat sheet of paper will be understood by reference to Figs. 287 and 288. Eig. 287 is to be taken as a pictorial projection of a model. Two planes of projection are shown one being vertical and the other horizontal. These planes, called co-ordinate planes, divide the space surrounding them into four dihedral angles or quadrants which are named, first, second, third, and fourth dihedral angles or first, second, third, and fourth quadrants. If an observer be facing the vertical plane of projection, then the first quadrant is above the horizontal plane of projection and in front of the vertical plane of projection. The second quadrant is behind the first and the others follow in order ELEVATION PLAN Fig. 287. Fig. 288. as shown. The line of intersection of the planes of projection is called the ground line and is lettered XY. An object is shown in the first quadrant and projections o£ it on the horizontal and vertical planes of projection are also shown. The projection on the horizontal plane is called a i^lan and the projection on the vertical plane is called an elevation. Now imagine the vertical plane to turn about XY as an axis, carrying with it the elevation, until it is in a horizontal position. The horizontal and vertical planes of projection will now coincide and the plan and elevation of the object will be on one flat surface and their exact forms may be drawn as shown in Fig. 288. Instead of imagining the vertical plane to turn about XY until it is horizontal, the horizontal plane may be imagined to turn about XY until it is vertical as shown in Fig. 289. PROJECTION 169 In British and European countries the general practice in making working drawings is to conceive the object to be placed in the first quadrant as shown in Fig. 287 and the working plan and elevation are then in the positions shown in Fig. 288, the plan being below and the elevation above XY. In the United States of America the practice of conceiving the object to be placed in the third quadrant as shown in Fig. 289 is now very general and the working plan and elevation are then in the positions shown in Fig. 290, the plan being above and the elevation below XY. Whether the object be placed in the first quadrant or in the third quadrant it is supposed to be viewed from above in obtaining the plan, consequently when the object is in the first quadrant it lies between PLAN ! *. X' |y r — 1 ELEVATION Fig. 289. Fig. 290. the observer and the plane of projection and the projectors from the visible parts have to go through the object to the plan, but when the object is in the third quadrant the plane of projection lies between the observer and the object, hence the projectors from the visible parts to the plan are not obstructed by the object. In like manner for the elevation, the projectors from the visible parts of the object go through the latter when it is in the first quadrant but are clear of it when in the third quadrant; hence the advantage claimed for placing the object in the third quadrant. The practice of placing the object in the first quadrant is however so well established and the advantage claimed for placing it in the third quadrant is so small, being probably more imaginary than real, that it is doubtful whether a change from the older practice should be encouraged. In any case drawings on 170 PRACTICAL GEOMETRY either system can be made with equal facility if the principles are understood. In working problems in descriptive geometry by the method of projections on co-ordinate planes, the given points and lines may be in any one quadrant, but the lines for the solution may extend into any or all of the other quadrants. 136. Notation in Projection. — For the purpose of reference and for clearness, points, lines, and figures may be lettered. In general a point in space is denoted by a capital letter, its plan by a small italic letter, and its elevation by a small italic letter with a dash over it. Thus P denotes a point in space, p its plan and p its elevation. A line AB in space would have its plan lettered ah and its elevation ah'. A point P in space may be referred to as the point P or as the point jip'. In like manner a line AB in space may be referred to as the line AB or as the line ah, a'h'. The horizontal and vertical planes of projection may be referred to by using the abbreviations TI.P. and*V.P. respectively. CHAPTER XII PROJECTIONS OF POINTS AND LINES 137. Rules relating to the Projections of a Point.— Fig. 291 is a pictorial projection of a model showing the horizontal and vertical planes of projection in their natural positions together with four points A, B, C, and D in space, A being in the first quadrant or first dihedral angle, B in the second, C in the third, and D in the fourth. The plans and elevations of these points as obtained by dropping perpendiculars from them on to the horizontal and vertical planes of projection respectively are also shown. The positions of the Fig. 291. Fig. 292. I BP'elevations of the points when the vertical plane of projection is turned about XY until it coincides with the horizontal plane are indi- cated, and in Fig. 292 the various plans and elevations are shown as they appear when the planes of projection are made to coincide and then placed flat on this paper. A careful study of Figs. 291 and 292 should convince the student of the truth of the following rules relating to the projections of a point. 172 PRACTICAL GEOMETRY (1) The plan of a point is beloic or above XY according as the point is in front or hehlnd the vertical plane of projection. (2) The elevation of a point is above or below XY according as the point is above or below the horizontal plane of projection. (3) The distance of the plan of a point from XY is equal to the distance of the point from the vertical plane of projection. (4) The distance of the elevation of a point from XY is equal to the distance of the point from the horizontal plane of projection. (5) The plan and elevation of a point are in a straight line perpendicular to XY. The term projector has already been defined and is the line joining a point and a projection of it, but the line joining the plan and elevation of a point is also called a projector. A plan and elevation are also said to be projected, the one from the other. 138. True Length, Inclinations, and Traces of a Line. — Fig. 293. Pig. 294. The projection of a line on a plane will be shorter than the line itself except when the line is parallel to the plane ; in the latter case the line and its projection have the same length. A line, its projection on one of the co-ordinate planes, and the projectors from its ends to that plane, form a quadrilateral concerning which everything required for constructing it is known if the plan and elevation of the line are given. One method of finding the true length of a line is therefore to construct this quadrilateral. Let the plan ab and elevation a'b' of a line AB be given as in Fig. 294. Referring to the pictorial projection in Fig. 293, it will be seen that the line AB, its plan ab, and the projectors Aa and B?> form a quadrilateral, the base ab of which is given. Also Aa is equal to a'a^ , B6 is equal to b'b^, and the angles Aab and Bba are right an'gles. Hence to find the true length of AB, draw (Fig. 294) oAj at right angles to ab and equal to a^a'. Next draw bV*^ at right angles to ab and equal to bjj'. A/Bi is the true length of AB. PROJECTIONS OF POINTS AND LINES 173 I Note that if the extremities of the line AB are on opposite sides of the horizontal plane, the perpendiculars aAi and hB^ must be drawn on opposite sides of the plan ah. The inclination of a line to a plane is the angle between the line and its projection on that plane. Referring to Figs. 293 and 294, it is evident that the inclination of A]^ to the horizontal plane is the angle between ah and AjBi, so that the construction just given for finding the true length of AB also serves for finding its inclination to the horizontal plane. The inclination of AB to the vertical plane of projection is found by constructing the quadrilateral a'h'B2-^2i ^^ which a'A^ and h'\% are at right angles to a'h' and equal to a^a, and hj) respectively. A2B.2 is the true length of AB and the angle between a'h' and A2B2 is the inclina- tion of AB to the vertical plane of projection. If al)., be drawn parallel to AjB^ (Fig. 294) to meet hB^ at B.(, then aB;5 will also be the true length of AB, and the angle haB.^ will be the inclination of A15 to the horizontal plane. Also the length of ?)B.j is equal to the difference between the distances of B and A from the horizontal plane. Hence the true length of AB and its incli- nation to the horizontal plane may be found by constructing the triangle ahB.^. In like manner the true length and the inclination of Al> to the vertical plane may be found by constructing the triangle a'h'A.f in which a' A3 is equal to the difference between the distances of A and B from the vertical plane. The inclination of a line to the horizontal plane is usually denoted by the Greek letter 6 (theta) and its inclination to the vertical plane by the Greek letter (phi). Notice that 6 is the letter O with a horizontal line through it, while <^ is the same letter with a vertical line through it. The true length of a line AB and its inclinations to the planes of projection may also be found as follows. Referring to Fig. 295, through h draw afih^^ parallel to XY. With centre h and radius ha describe the arc aa^, cutting a^hh^ at a^. Draw «!«/ perpendicular to XY to meet a line through a' parallel to XY at a/, a/// will be the true length of A15 and the angle h'a^'a' will be its inclination 6 to the hori- zontal plane. An inspection of the figure will be sufficient to make clear the corre- sponding construction for finding the incli- nation of the line to the vertical plane. Comparing the constructions shown in Figs. 294 and 295, it will be seen that in both a quadrilateral is drawn having a base equal to one of the projections of the line, and in Fig. 294 this base is made to coincide with that projection while in Fig. 295 the base is made to coincide with XY. When the inclination of a line is mentioned without reference to a^^ 7 a' • : 1 : Y iJ [■ >^' a Fig. 295. 174 PRACTICAL GEOMETRY any particular plane, inclination to the horizontal plane is generally understood. The trace of a line on a surface is a point where the line intersects the surface. When the traces of a straight line are mentioned without reference to any particular surface, the points in which the line or the line produced cuts the planes of projection are understood. The horizontal trace of a line is the point where the line or the line produced cuts the horizontal plane of projection, and the vertical trace of a line is the point where the line or the line produced cuts the vertical plane of projection. After making the construction for finding the true length of a line, shown in Fig. 294, if < B^Ai be produced to meet ba at h then h will be the horizontal trace of the line AB. In like manner if AJi, be produced to meet a'b' at v' then v' will be the vertical trace of AIj. The correctness of these constructions is obvious from an inspection of Fig. 293. If it is only the traces of a line which are required, then it is only necessary to produce the elevation a'b' (Fig. 294) to meet XY at h' iind then draw h'h perpendicular to XY to meet the plan ab pro- duced at h in order to determine the horizontal trace. In like manner, by producing the plan ab to meet XY at v, and drawing vv' perpendicular to XY to meet the elevation a'b' produced at v', the vertical trace is determined. This construction fails however when the projections of the line are perpendicular to XY but the con- struction previously given will apply in this case also, provided that the plans and elevations of two points in the line are definitely marked and lettered. When the projections of a straight line are perpendicular to XY the line itself is perpendicular to XY although it may not meet XY. When a line is parallel to one of the planes of projection it has no trace on that plane. When a line is perpendicular to one of the planes of projection it has no trace on the other plane of projection, and its projec- tion on the plane to which it is perpendicular is a point. 139. True Form of a Plane Figure. — The projection of a plane figure on a plane will not have the same form or dimensions as the figure itself excepting when the plane of the figure is parallel to the plane of pro- jection, in which case the figure and its pro- jection will be exactly alike. To determine the true form of any plane figure, whose pro- jections are given, it is necessary to know the true distances of a sufficient number of points in it from one another ; now these distances may be found by one of the constructions given in the preceding article. Fm. 29G. PROJECTIONS OF POINTS AND LINES 175 An example is shown in Fig. 296, where ale and a'h'o' are the given projections of a triangle. The true lengths of the sides are found by the constructions shown, and the triangle which is the true form of the triangle whose projections are given is then drawn. If the figure given by its projections has more than three sides it should first be divided into triangles ; the true forms of these triangles are then found and assembled to give the true form of the whole figure. In many cases the true form of a plane figure whose projections are given is best determined by the method of rabatment described in Art. 189, p. 221. The traces of the sides of a plane figure whose projections are given may be determined by one of the constructions of the preceding article, and it will be found that all the horizontal traces will lie in one straight line, and all the vertical traces will lie in another straight line, and these two straight lines will intersect on XY, excepting when they are parallel, in which case they will be parallel to XY. This matter will be referred to again in Chapter XVI. 140. To mark off a given Length on a given Line.— Let aJ), a'b' (Fig. 297) be the projections of the line, it is required to find the projections of a point C in this line so that AC shall be a given length. Determine A^Bi the true length of AB. Make A,Cj equal to the given length. Through Cj draw C^c perpen- dicular to ah to meet ah at c. Through c draw cc' perpendicular to XY to meet a!h' at d. c and c' are the projections required. If the given projections of the line are perpendicular to XY (Fig. 298), determine c as before then make the distance of c' from XY equal to C^c. 141. Given the True Length of a Line and the Distances of its Extremities from the Planes of Projection, to draw its Projections, — First determine the projections aa' (Fig. 299) of the end A of the line. On a^a make a^c equal to the distance of the end B of the line from the vertical plane of projection, and on a^a' make a^c' equal to the distance of B from the horizontal plane. Through c and c' draw lines parallel to XY. These parallels to XY will contain the plan and elevation respec- tively of B. With a' as centre and the given true lenojth of the line as radius describe an C, Fig. 297. arc to cut the parallel to XY through c' at Fig. 299. 176 PRACTICAL GEOMETRY Fig. 300. B2. From B2 draw the perpendicular BJ)^ to XY. Then since a'B., is the true length of the line and a^a' and h.^Bo are the distances of its extremities from the horizontal plane it follows (see Fig. 293, p. 172) that a^h^ is the length of the plan of the line. Hence, if with centre a and radius equal to aji^ an arc be described to cut the parallel to XY through c at b then ab is the required plan of the line. A per- pendicular to XY from h to meet the parallel to XY through c' determines b', and a'b' is the required elevation of the line. 142. Given the Projection of a Line on one of the Planes of Projection, its Inclination to that Plane, and the Distance of one end from it, to determine its other Projection. — Let ab (Fig. 300) be the given projection, the inclination to the horizontal plane and let the distance of the end A of the line from the horizontal plane be given. The distance of a' from XY is equal to the given distance of A from the horizontal plane. At a make the angle haB^^ equal to and draw ?>Bi at right angles to ab to meet aB^ at B^. The distance of b' from XY is equal to bBi plus the distance of a' from XY. If the elevation a'b' is given and the incli- nation <^ of the line to the vertical plane of projection and also the distance of A from the vertical plane of projection, the construction is similar to that just given and is shown in Fig. 300. 143. Given the Inclination of a Line to one of the Planes of Projection and the Angle which its Projection on that Plane makes with the Ground Line, to draw its Projections, — Let the line be inclined at an angle to the horizontal plane, and let its plan make an angle a with XY. From a point C in XY (Fig. 301) draw Cb' inclined at an angle ^ to XY. Draw b'b at right angles to XY. Then bC is the length of the plan of the line whose true length is Cb' and whose inclination to the hori- zontal plane is 6. With b as centre and bC as radius describe an arc, and from b draw ba to meet this arc at a and make an angle a with XY. ab is the required plan of the line. A perpendicular from a to XY determines a' and a'b' is the required elevation of the line. « 144. Given the Inclinations of a Line to the Planes Projection, to determine its Projections. — Let the line be in- clined at an angle to the horizontal plane and at an angle <^ to the vertical plane of projection. From a point C in XY (Fig. 302) draw Cb' inclined at an angle to XY. Draw b'b at right angles to XY. Then bC is the length of the plan of the line whose true length is Cb' and whose inclination to the horizontal plane is 0. From b' draw b'T> making the angle C^'D equal to <^. Draw CD of PROJECTIONS OF POINTS AND LINES 177 perpendicular to //D. Then fe'D is the length of the elevation of the line whose true length is C// and whose inclination to the vertical plane of projection is cf). ^^-^-^A' With centre h' and radius h'T> describe an arc D,,,— — -""T'J/ to cut XY at a'. With centre b and radius ^C '^ y/ describe the arc Qa to meet the perpendicular to \\ / / XY from a' at a. ah is the plan and a'b' is the \\ / / elevation required. \/OV/a! Note. The sum of the angles $ and