c. UNIVERSITY OF CALIFORNIA. FROM THE LIBRARY OF DR. JOSEPH LECONTE. GIFT OF MRS. LECONTE. No. / r OUTLINES OP A SYSTEM OP MECHANICAL PHILOSOPHY BEING A RESEARCH INTO THE LAWS OF FORCE. SAMUEL ELLIOTT COUES. " That which we call gravitation and fancy ultimate, is but one fork of a mightier stream for which, as yet, we have no name." BOSTON: CHARLES C. LITTLE AND JAMES BROWN. 1851. Entered according to Act of Congress, in the year 1851, by CHARLES C. LITTLE AND JAMES BROWN, in the Clerk's Office of the District Court of the District of Massachusetts. CAMBRIDGE: PRINTED BY BOLLES AND HOUGHTON. TO THE REV. ANDREW P. PEABODY. MY DEAR SIR! When I first mentioned that I had undertaken a Research into the Laws of Force, you encouraged me to follow up the investigation ; and from that time you have constantly extended to me your sympathy, and have manifested a kind interest in the result of my labors. Thus you are intimately associated in my mind with the work, though it is but just to say that you are in no sense responsible for the correctness of any of my deductions. I dedicate the book to you as an acknowledgment of your kindness, and as a manifestation of my respect for the power of mind which has not only given you your eminent position in your profession, but is conspicuous in every depart- ment of learning to which your attention has been directed. With sincere regard, Your friend, SAMUEL E. COUES. ERRATA. Page 107, line 30th read, descends to a lower level. " 163, line 8th for bury, read buoy. 11 258, line 4th for their, read these. " 263, line 2d for common, read coming. u 272, note omit the quotation marks in the second paragraph. " 280, line 5th insert the before work next line, omit the before law. CONTENTS INTRODUCTION. CHAPTER I. GENERAL PROPOSITIONS RELATING TO FORCE AND MOTION. . 4 CHAPTER II. PLANETARY MOVEMENTS. FORCE FROM THE FALL or BODIES. HEAT. LIGHT. ELECTRICITY. GALVANISM. MAGNETISM. ANIMAL FORCE. IDENTITY OF FORCE. . . . .- . ' 17 CHAPTER III. CAPILLARY ATTRACTION. ELASTICITY. COHESION. FRICTION. SEPARATION OF COHESION. CEMENTS. CHEMICAL AFFINITY. 44 CHAPTER IV. ACTION AND REACTION. REACTION AS A PROPELLING POWER. Yis INERTIA, MECHANICAL POWERS. CENTRIFUGAL FORCE. 60 CHAPTER V. OSCILLATION. MOVEMENT OF THE WAVES. WHIRLPOOLS AND WHIRLWINDS. VORTICAL MOVEMENT. OSCILLATION OF THE SURFACE OF THE EARTH. GEOLOGICAL EPOCH. FORCE OF DE- SCENT. . 85 VI CONTENTS. CHAPTER VI. ATMOSPHERIC DENSITY. GRAVITATION OP THE ATMOSPHERE. ELASTICITY OF AIR. ACTION OF THE BAROMETER. THE BAR- OMETER THE DIRECT MEASURE OF ALTITUDE. . . .113 CHAPTER VII. PRESSURE OF FLUIDS. . . 151 CHAPTER VIII. PRESSURE OF ELUIDS, CONTINUED. GRAVITATION OF FLUIDS. CO- NICAL ADJUTAGES. RELATIVE LEVELS OF AIR AND WATER. 178 CHAPTER IX. THE TIDES. . ,. ^ ^." 225 CHAPTER X. TRADE WINDS. OCEANIC CURRENTS. ERRATIC DRIFT. METEOR- OLOGY. . . . . . . . ... 253 CHAPTER XL THE MATHEMATICAL ARGUMENT FOR GRAVITATION. . . 284 CHAPTER XII. LAW OF THE VELOCITY OF FALLING BODIES. ORIGIN OF THE THE- ORY OF GRAVITATION. MOVEMENTS OF THE SPHERES. HARMONY OF SCIENCE WITH REVELATION. . . . .'' 308 INTRODUCTION. THESE outlines of a System of Mechanical Philosophy are the result of a research made by the author, for his own instruction. In the research he attempted to separate sup- position from fact, the questionable from those things necessarily taken for truth by the laws of the mind. The inquiry took the form of snythetical reasoning, proceeding step by step, deducing the unknown from what appeared self-evident, taking nothing as truth on authority, however great the name which had given currency to the theory ; thus shutting out all sources of error except such as resulted from the weakness of the individual mind. Arriving by this process at conclusions, the very opposite of those taught in the schools of science, these conclusions were tested by an appeal to the phenomena of nature. Both, the reasoning without the phenomena, and the phenomena without the reasoning, pointed to the same general truths. Thus are presented opinions which appear to be sup- ported both by reason and by observation, and presented in the order of their development. The writer feels con- fident, that, however defective may be his logic, however imperfect may be his statement of the facts of science, however crude may be his application of the truth to the i 2 INTRODUCTION. explanation of phenomena, he has unfolded some principles, which, when distinctly evolved from mingled error, will change somewhat the basis on which mechanical philosophy now rests. But, whether or not the opinions here presented are demonstrated to the minds of scientific men, it is admitted that many of the present explanations of philosophy are received as the supposed best possible explanations, rather than as settled truth, on which the mind confidently reposes. The conservatives in science may be successful in pointing out the errors of new theories, but they have other more difficult work, that of the defence of the old theories. A reexamination of principles supposed to be forever set- tled by the authority of a Newton may strike many minds as presumptuous. It will be seen, however, that the splen- did conceptions of Kepler, made distinct and thoroughly demonstrated by Newton, are not assailed. The glorious truth of the harmony of the movements of the spheres, by which the astronomer can track out the orbit of the most eccentric wanderer of the heavens, stands forever, the reflex of the light of creation from the minds of the truly great. It is the school which now determines opinions on philo- sophical subjects. Men are taught to believe rather than to reflect, to receive opinions rather than to evolve them by the process of intense thought. A scientific education is a capital, the value of which is impaired by dissent. It would seem as if nothing further could be attained, as if philosophy had soared its highest flight ; for theories thus pass from mind to mind, from generation to generation, as settled truths, and theories too, somewhat questioned or indistinctly comprehended, even by those who teach them. To induce reflection, therefore, upon admitted theories, INTRODUCTION. 3 cannot fail to do some service to the cause of truth ; for, as it has been observed, " nothing tends more to the corrup- tion of science than to suffer it to stagnate. The waters must be troubled before they can exert their healing virtues. A man who works beyond the surface of things, though he may be wrong himself, yet clears the way for others, and may chance to make his errors subservient to the cause of truth." This work is not intended as an elaborate philosophical treatise, but as a rapid outline ; and only those consider- ations are presented which are necessary to develop the opinions advanced. Much collected material has been laid aside for future use, if it be thought that the opinions set forth are worthy of additional attention. PORTSMOUTH, N.H., Sept. 7, 1850. CHAPTER I. " FOR SINCE THE HUMAN MIND PARTICIPATES AS IT MAY IN THE FRUITFULNESS OF THE CREATIVE NATURE, IT DOTH FOR ITSELF BRING FORTH REASONABLE THOUGHTS." IN all investigations of matter and force, we must divest them of all properties that are boundless, that are without fixed limits, determinate degrees. Thus, matter is not infi- nite in its extent nor in its capacity for motion ; so of force, its action is not infinite ; it has parts, or divisions, each with a fixed rate of power, and as a whole, its aggregate power is fixed, meted out by Him by whose infinite power it was constituted. We need recurrence to this as the point of departure in our course, as that to which we can recur as something fixed, when the ocean on which we speed our way has no guide for our path over its vastness. There is one God, the ultimate Cause of all things, of whom alone can infinity of attributes be affirmed. This truth is here presented, not for its religious bearing, but from the necessity of recurring to it in its relations to the first prin- ciples of philosophy. The admission that His attributes alone are infinite in degree, is essential to distinctness of opinion with regard to matter and force. The human mind cannot comprehend infinity; any proposition, therefore, which involves the boundless, is unintelligible ; decide it affirmatively or negatively, the mind feels no confidence in the result. OUTLINES, ETC. 5 1. Matter has inertness as an essential property ; it has substance and extension ; it exists in atoms or ultimate par- ticles, indestructible and impenetrable, between which atoms there is space ; these atoms aggregated, constitute masses, between which there is space ; these masses constitute worlds, between which there is space. Space is room or freedom for motion, or that in which matter exists and is moved. Motion is the act of the change of place of mat- ter ; it is the passing of matter from one part of space to another. No atom of matter can occupy the same place with another atom. Force is that which produces the motion of matter, or that which causes matter to act. Force cannot act where it is not. These definitions are the usual, commonly received defini- tions of matter and force, and the resultant motion. We express in them all that can be known. An inquiry into their nature or construction embraces the element of the infinity of God who created them, and " plunges us at once into that deep which never yet was fathomed by human intellect." Newton thus speaks of matter. " We believe that God in the beginning formed matter in solid, hard, massy, impenetrable, movable particles, of such sizes, fig- ures, and other properties, and in such proportion to space, as most conduced to the end for which He formed them ; and that these primitive particles being solids, are incom- parably harder than any porous bodies compounded of them, even so very hard as never to wear or to break to pieces ; no ordinary power being able to divide what God himself made one at the first creation." 2. That which is moved and that which moves it, are not identical, not the same thing ; the one, matter, having in- 6 OUTLINES OF A SYSTEM OF ertness as an essential property ; the other, force, having as an essential property power to give motion. Wherever matter is, there is inertness ; wherever force is, there is motion. The belief of the separate and independent existence of cause and effect results from the constitution of the mind. It is what God compels us to believe. It is as inspiration. We think of God as existing separate from his creation, of our minds as separate from thought and perception ; and so of force, as an independent power, as in no sense matter, but as that which gives motion to matter, as that which causes matter to change its place. This separate existence is recognized in the three great laws of motion, which refer to force as the cause of motion. These words of Herschell very distinctly present the idea : " Force may be communicated to inanimate matter, it may be concentrated in the same mass by continuation of animal or muscular force. We thus learn to regard motion in matter as the effect and indication of force, and force may be defined as that which is capable of producing motion in matter, or of stopping and altering its direction when produced." Daniell (Introduction to Chemical Philosophy) says, " A body at rest would remain quiescent unless it were to receive an impulse from without," or objectively, and thus philosophy recognizes the inertness of matter. Growing from this idea is the doctrine of vis inertise. It is a term expressive only of the fact, that matter rests when unmoved, and moves when not at rest, and that time often elapses after the impulse, before motion is apparent. Strictly it asserts the impossibility of self-moving matter. 3. Matter which is in motion must continue in a state of MECHANICAL PHILOSOPHY. 7 uniform motion forever, unless disturbed by the action of an external cause. The same cause produces the same effects. This propo- sition, so far as it goes, is identical with the first of the three great laws of motion, which is, " A body must continue for- ever in a state of rest or of uniform motion, in a straight line, if not disturbed by the action of an external cause." If this be true of bodies both at rest and in motion, the pro- position is true as regards bodies in motion, and as true when considered apart from the direction of the motion as it is when the law defines the line of motion. 4. All motion is in proportion to the force which pro- duces it. The degree of the effect is in proportion to the cause ; in other words, add to or take from the force in action upon given matter, the quantity of motion is changed propor- tionally. The second of the three laws is : " Every change of motion produced by the external (objective) cause is proportional to the force impressed, and in the direction of a straight line in which the force acts." The proposition affirms the first clause of the law, and this is necessarily true independently of the truth of the latter clause. We draw from this proposition the following as corrolla- ries : 1st, that force is divisible, different quantities or degrees of it acting at different times on the same matter ; 2d, force is transferable, for otherwise, that is, without transfer of force, there could be no increase or diminution of motion. 5. The absolute condition of the transfer of force is its presence with matter not susceptible of motion by it. The essential property of force being action, wherever it 8 OUTLINES OF A SYSTEM OF is, it acts, or from its nature it is transferred from matter which cannot be moved to matter having- space for motion. 6. The degree or velocity of the motion of a mass de- pends on the degree of force which acts upon each atom constituting the moving mass. It appears self-evident, that every atom, perhaps in a degree according to its element or kind, requires always the same force to move it with the same velocity, and the motion of the mass depends on the degree of force relative to the number of its atoms. 7. Every atom of the solar system is in continued motion, orbital and rotary. Hence it follows, that it is force which determines the position of every atom, mass, and world, and determines their position positively in space. It also determines the relative position of all things. 8. Matter occupies but one place in space at the same time, and consequently no atom can have motion but in one line of direction at the same time. Hence it follows, that all motion is orbital, rotary, -curvilinear ; for, all atoms being in curvilinear motion, no addition of rectilinear motion can change the curve into the straight line, there will ever remain the element of the curve. The contrary opinion indicates infinity, and is un- intelligible. The foundation principle of geometry is the measure of all angles by arcs of the circle, and the meas- urement of the circle or curve conversely by the inscribed straight lines or angles. Hence the fixed relation between the diameter of the circle and its circumference, and the measure of motion by MECHANICAL PHILOSOPHY. 9 the diameter of the circular orbit. We assume that the harmonic motion of the heavenly bodies bears a certain pro- portion to the orbit, that this velocity has a fixed ratio to the diameter, and that this ratio mathematically determined is proportional to the square of the distance of the circum- ference from the centre. The velocity of bodies moving in free space being in a fixed ratio to the orbit, it is the present force, the* active principle, which determines the orbit. A change of the degree of force would enlarge or diminish the orbit. In all free motion, therefore, the motion is uniform and har- monic. Two atoms moving in the same orbit will move with the same velocity ; in different orbits will preserve that rela- tive position which is determined by the difference of orbit, and the difference of the line of direction ; so that mathe- matically the relative position of any body can be deduced, given as the elements of calculation its orbit and direction of motion. 9. Rectilinear motion, or motion in a straight line, cannot be affirmed of any atom belonging to or in harmony with the solar system, or with the system of worlds. The hori- zontal line on the surface of the globe is curvilinear. So from any one point to another, in, on, and about the earth, the moving body takes the curved line. In the old philo- sophy, circular motion was deemed the natural motion ; but the new philosophy conceives of circular motion as con- strained by the operation of conflicting forces. 10. The supposed perpendicular descent of a falling body is a curvilinear motion. This is not practically admitted, but mathematically deduced ; the fall is termed a " cubical 10 OUTLINES OF A SYSTEM OF parabola." The supposed attraction of the earth does not draw in straight lines, falling bodies preserving ever their rotary motion. 11. Bodies in rotation with the earth, on receiving addi- tional force, must either take a higher level of rotation, or use the force received in additional motion in a new direction. 12. In the act of falling whereby a lower level of rota- tion is assumed, force must be transferred from the falling body when its motion is suspended. The motion of falling is added to the rotary motion, thereby giving action to the present force. This motion being suspended, only rotary motion in a smaller orbit remaining, force will be transferred. Hence arises spare force of descent. The spare force of descent will be mea- sured by the degree of descent. Hence the spare force of falling bodies is measured by the square of the time of descent, equal times giving equal distances of descent. Thus most distinctly is presented the law of falling bodies, or motion begetting motion, which, indistinctly understood, caused the great controversy between the schools of Des Cartes and Leibnitz, and which to this day has obscured mechanical science, by making the occasional abnormal motion of falling bodies the element of calculation of har- monic motion. 13. The motion of the heavenly bodies being harmonic with fixed velocity according to orbit, their velocity is the immediate measure of the velocities of retarded or accele- rated motion ; that is, the abnormal motion is detected and MECHANICAL PHILOSOPHY. 11 measured by the normal, the motion of bodies in confined space being determined by the velocity of bodies in free space. Time is the indirect measure of velocity ; the motion of the earth which measures time, the direct measure of velo- city. Hence all velocity is known by and measured by the rotation of the earth. A body which moves thirty miles in one hour moves over the given space isochronously, or while the earth has moved one twenty-fourth part of her rotary circle. Time, therefore, has no reference to force and motion so as to increase or diminish them, and motion refers to time only as indicating the extent of the motion of the earth. 14. There is beside the consentaneous motion of the atoms of the mass, or the progressive motion of the mass, an atomic or molecular motion of every atom composing the mass. This proposition will receive its most perfect demonstra- tion by the facts and phenomena of nature ; but is believed from analogy, that the same law governs the minute as well as the extended, also from the fact that there is- space between all atoms, that force is primarily in action on the atoms. If force be present with atoms, and there be space for motion, motion is affirmed. We leave this propo*- sition mainly upon these general statements, recurring, ia this place, to one most significant fact : " The expansion of volume of small bodies by dilatation from heat, may be ob* tained without sensible error by trebling the number which expresses its increase in length." Daniell's Introduc- tion to Chemical Philosophy. The trebling of the diameter, it will be perceived, gives nearly the circumference of the* circle of motion. 12 OUTLINES OF A SYSTEM OF 15. Force transfers itself from atom to atom without ap- preciable time. Time being measured by the action of force upon a given quantity of matter, the transfer of force with- out matter is therefore without time ; or with a reduction of the matter, velocity is increased ; annihilate the matter, and time is no longer to be affirmed of its passage. Thus attraction of gravitation is spoken of " as a force which is transmitted instantaneously," and so of light, heat, gal- vanism, &c. So far as they pass in appreciable time it is because they (the forces which move) are connected with the material ; the essential quality of pure force unembodied is change of place without appreciable time. ' 36. Force is diffusible only by contact of the moving atom with another atom. This appears from the fact that force is transferable only when it cannot induce motion, and while space remains there is room for motion. Therefore, the motion of a body must be after a lapse of appreciable time from the contact of the atoms. Consentaneous motion of the mass is from the equal diffusion of motion through its particles. These particles have room for motion before impingement ; therefore, the mass moves in appreciable time from the contact of the atoms. This is finely illustrated by a row of suspended ivory balls through which force is communicated in appreciable time by the measured motion of the balls, according to their distance and the degree of force. It is the foundation of the doctrine of vis inertiae. It is not impossible that the distance of atoms constituting a mass may be relatively determined with regard to the distance of atoms in another mass. It will be found that, the more porous the body, the longer is the lapse of time between the impingement and the MECHANICAL PHILOSOPHY. 13 motion of the atoms as the mass ; we instance equal weights of atmospheric air and of lead. The force is communicated instantly, motion results instantaneously, but time is predi- cable of the passage of atom to atom, to diffuse the motion equally that it may be consentaneous. 17. Force acts independently of direction ; on its trans- fer, its former line of motion does not necessarily imply a con- tinuance of the same line of motion. A body in motion must continue forever in a state of uniform motion, unless disturbed by the action of an objective cause. The force will be transferred upon impact, and the body receiving it will move in the direction in which it is free to move ; or, if the body which obstructs motion be not movable, the force, not being transferred, acts in the opposite direction. The resultant motion of impinging bodies is demonstrated by the mathematical figure, the " polygon of force," and is equally demonstrable by the diagram showing the contact of atoms having surface ; so, too, the angle of incidence and reflection, when a body impinges upon an immovable mass, shows that the resultant motion is determined only by the free space for motion. If two flat surfaces meet, they can be separated only in the opposite direction, if the separating force acts equally on the surface. And so through more complex movements. We refer to facts of common observation ; the rotary motion of the windmill by the horizontal impingement of the wind, the billiard ball, the rise of the wave. On this action of force, independent of direction, depends the appli- cation of force in mechanical combinations, by which the force of falling water is conveyed anywhere, and acts in any direction. Force does not act where it is not ; but the me- 2 14 OUTLINES OF A SYSTEM OF chanic, availing himself of the laws which govern its trans- fer, leads it to the loom and opens for it the desired line of motion only. This doctrine of the transfer of force is one of the found- ations of the supposed action and reaction of force ; every instance of reaction can be directly traced to the transfer of force. 18. Transfer of force, which does not give the body to which it is transferred consentaneous motion of its atoms, gives vibratory motion to the parts of the mass, or increase of molecular motion, the motion induced being of the same degree as the motion that was suspended. The force being transferred, and motion being in proportion to the force, the vibratory or molecular motion must be the same ; or, if the motion of the recipient of the force be retarded, an equal quantity of its force is also turned from the consentaneous motion, so that the resultant motion, internal to the mass, will be doubled ; that is, the internal motion is the aggre- gate of the suspended motion of both impinging masses. Thus, the motion of the tongue of the bell, and of the bell, jointly increase the loudness of its tone ; and other instances of this result present themselves to every mind. Hence the concussion and destruction of two balls in opposite motion, which would not result from the motion of either upon the other at rest. Vibratory motion being the unequal or rather unconsen- taneous motion of the parts of a mass, if there be not a gradual increment of motion from the surface to the centre, there will be nodes or points of rest. Thus musical chords manifest certain points of rest. Vibratory motion being determined by the degree of force, MECHANICAL PHILOSOPHY. 15 if the same quantity of matter be moved the same distance, the times of vibration will be the same ; if the distance be diminished, there will be an increase of velocity. Tone being dependent on time of vibration, an increase or diminution of force changes the range, preserving the tone. Isochronous vibration is, therefore, a branch of the law which induces the same quantity of motion by the same quantity of force. It follows, too, that there can be no vibratory or reciprocal motion in free space. 19. Force is indestructible. This appears from the gen- eral consideration, that what God formed at the beginning no power can destroy. It is imperishable, too, as is evident from its transfer from atom to atom and from mass to mass, and from the state of equable motion, which bodies actuated by a given degree retain. It is also one and identical. That which gives motion is force ; if it have different essen- tial properties, these properties cannot be detected, as force is known only by the motion it gives to matter. There are not differing qualities or kinds of force, which give, this kind, circular motion to bodies, this kind, a straight motion, this kind, motion in a contrary direc- tion ; nor is there a planetary force, and a molecular force, and an oscillatory force, and a directly acting force ; but the one force may act on any element of matter, moving it in any direction, which idea will receive further illustration in the following chapter. In the research made, the general propositions were ex- tended much further ; but up to this point only were they carried with that distinctness which should characterize such propositions. Others remain therefore for further examination. 16 MECHANICAL PHILOSOPHY. It will be observed, that an inquiry like the preceding has reference to force mainly as in action, giving to mat- ter place, position, and motion in reference to space, actual, and not apparent or relative motion. We try to consider relative motion only as indicative of true motion, and this as indicative of the laws of force. Thus the ascent of water in the capillary tube is regarded, not as motion in relation to the tube so much as a new rotatory orbit of the elevated water. The log line which is veered from the ship has apparent motion of its own, but the actual motion is that of the ship. This distinction we would recall to the mind of the general reader. CHAPTER II. "WHEN WE HAVE THE DECREES OF NATURE, AUTHORITY GOES FOR NOTHING." Galileo. THE errors of mechanical philosophy, if there are errors, arise from the assumption of gravitation, or the attractive power of matter ; from the application of the law of the motion of falling bodies, to the uniform motion of bodies remaining in one determined orbit ; from the belief that rectilinear motion is the natural motion, and that the cur- vilinear is a constrained motion induced by conflicting forces ; and from keeping out of sight the intense motion of every atom in its rotation and revolution with the earth, which, from its greater comparative velocity supplies the governing or controlling motion, and by reference to which alone, incidental, retarded, or accelerated motion, is to be understood or to be explained. In the illustration of our views we shall follow no artificial arrangement, but present our thoughts in the order in which they occurred from the natural connection of one class of facts with another class of facts, as this will throw more light on the peculiar views than any predetermined order of investigation. Our first attempt is to illustrate the idea of the identity of force, to prove that the motive power of nature is one, acting under uniform laws ; that force, whether it form the 2* 18 OUTLINES OF A SYSTEM OF dew-drop or marshal the "hosts of heaven," whether it manifest itself in the flow of the tides or of the purple stream of life, whether in the flash of lightning, or in the sweep of the bird with motionless wing, is ever the same principle ; that its divisions and subdivisions, its ever-varying names in science have obscured the law of its action, and thrown a mist over philosophy else apparent, from the ever-changing and conflicting theories. Of the nature of force as well as of the matter it moves, as we have said, we are entirely ignorant, and from the constitution of the -mind we shall forever remain ignorant. But the laws of its action given to it from the beginning, and ever enduring, may perhaps be distinctly traced out and understood. Thus, the force which moves the spheres acts under the intelligible law, that velocity is in proportion to the area of the orbit, that with the diminution of distance from the centre velocity increases, with the increase of dis- tance velocity diminishes ; so that all bodies revolving in free space describe equal areas in equal times. This is a property of orbitual revolution, in other words, it is the property of force. It is a fixed law, subject to no change. Aberrations and perturbations are temporary and oscilla- tory ; the mean time of revolution never changes. The revolution of the heavenly bodies is accompanied by rotation on their axis. This connection of the primary with the secondary movement arises from another law of force, from another property of the power which imparts motion. The two movements appear to have an opposite character. In the one, as we have seen, velocity in- creases by the diminution of the orbit ; in the other, velo- city becomes lessened as the rotating matter approaches the centre of rotation. How slow the rotation of the central MECHANICAL PHILOSOPHY. 19 parts of the earth, while at the equator the velocity of the surface is more than one thousand miles an hour ! From the nature of the rotating sphere there is one fixed ratio of increase of the velocity of its parts. Given the velocity at any distance from the centre of rotation, the velocity at any other distance can be determined. Its ratio of increase is proportional to the increase of the area of the circle described. We have the same measure of increase outward in rotation, that we have inward in revolution. The primary and secondary movements are under the same general law. Besides, there is also a fixed ratio between the velocities of both movements, for such is the far pervading law of nature. If the orbit of any planet were enlarged without additional force of propulsion, it would move, in its new orbit, with de- creased velocity. Its motion would not be harmonic ; it would not describe the equal area of planetary motion. To bring it into harmonic motion it would require additional force, and this additional force needed would be measurable by the increased area of orbit. If, on the other hand, the orbit of any planet were decreased, with the same propelling force its velocity would be increased, and it would be out of harmony with its associated worlds. With equal velo- city it must part with, or transfer, a portion of its force. This degree of spare force would also be measurable by the reduction of the area of the orbit. The degree of force required or imparted is not measured by the increase or dim- inution of the circumference. The orbit does not measure velocity. It is a path of motion, continuous, without be- ginning or end. By a fixed law, the required force is determined by the area described, which increases and diminishes in a higher ratio than the length of the circum- 20 OUTLINES OF A SYSTEM OF ference which encloses the area. Thus, by the enlargement of a planet's orbit, it would need added force to preserve the harmony of planetary motion, and by its diminution it would impart force, and the force added, or given up, would be measurable by the change of area. In the words of Her- schell : " The law of the areas determines the actual velo- city of the revolving body at every point, or the space really run over by it in any given portion of time.' 7 If the velocity be thus determined, so is the present force which determines the velocity. This is equally true of the velocity and force of rotation. If a mass at the surface of the earth be elevated, it gains thereby a superior level of rotation ; its orbit is enlarged, it requires additional force. If the mass fall, thereby decreasing its orbit of rotation, it has the spare force of descent ; it requires less for rotation, and the falling body imparts force. The force received for elevation, the force given out by depression, is measured in one case by the increase, in the other by the decrease, of the area of the circle of rotation. Though in one view it appears as if there were the converse action of force, yet the general kw is apparent, of the increase and diminution of required force for any area of orbit, whether acting outwardly from the centre or inwardly to the centre of revolution. The identity of force, acting in the primary movement of the spheres, and in the secondary movement, is apparent, thus considered, and a general, far-reaching law is most clearly indicated. The force which moves the different parts of the earth in rotation differs much in intensity. How small, compara- tively, in the central masses at the axis of rotation ; how great, on the surface of the earth at the equator ; how MECHANICAL PHILOSOPHY. 21 different the force moving the surface of the earth at the equator from the force moving the surface of the earth at the poles ! Yet, the weight of falling bodies, or their spare force of descent is nearly the same at the equator that it is at the poles. The spare force of descent is most unquestionably greater for an equal change of orbit at the equator than at the poles ; but the change of the area of the orbit is far less by the descent of one foot at the equator than it is at a distance from the equator. As we go from the equator the force of rotation lessens, the area of the orbit lessens 4n that ratio by every foot of descent, so that the increased ratio of the decrease of area compensates for the decreased force of rotation. Thus have we an equal " spare force" of descent on the same parallel of latitude, slightly increasing as we go from the equator, as by the spheroidal form of the earth the decrease of the area is more rapid by equal decreases of diameter, in proportion as the earth changes from the perfect sphere to the oblate spheroid. There is not, then, one law of force for the revolution of the spheres, and another for their rotation, and another for the changes of level of the masses composing the spheres ; and we think that we can show that the law, by which the spheres and masses are moved, also directs and governs the motion of the atoms composing every mass and sphere. The spheres lay spread out before us as distinct objects of conception. From the immense extent of space they occupy, and the almost boundless range of their motion, the law of force indicated by them becomes intelligible, and is the object of precise reasoning and of mathematical calculation. If we would understand the minute, we must throw upon it the light gained from the extended. " There is a certain 22 OUTLINES OF A SYSTEM OF character or style, if I may use the expression, in the opera- tions of Divine Wisdom ; something which everywhere an- nounces amidst an infinite variety of detail, an inimitable unity and harmony of design, in the perception of which philosophical sagacity seems chiefly to exist ; " or, as New- ton expressed the same idea, " Nature will be very con- formable to herself, and very simple." Thus, no less exact, no less fixed by determinate law is the motion of atoms, and, in the examination of the minute, this idea of the extent and universality of primary laws should be ever present to the mind. How unlike the simplicity of nature, her directness of ac- tion, the far-reaching nature of her laws, is the array of op- posing and conflicting forces, by the clashing of which we are taught that the balance or equilibrium of things is preserved ! To return for a moment to the spheres, - there is the im- pelling force, the repulsive or centrifugal force, the attract- ive or centripetal force. Of what use are these ? " I am persuaded," says Plato, " that if the earth is placed in the middle of the heavens, as they say it is, it stands in no need of air or any other support to prevent its fall ; its own equilibrium will keep it up. For whatever is equally poised cannot incline to either side, and consequently stands firm and immovable, this I am convinced of." If the centripetal and centrifugal forces balance each other, they induce no action ; give the earth the force for harmonic motion accord- ing to her orbit, she needs neither to keep her in the track ; there would be no danger of her flying off in a tangent, or of her falling into the central fires of the sun ; evenly balanced with them, she would be equally balanced without them. Why these conflicting forces were created by philosophy MECHANICAL PHILOSOPHY. 23 is very apparent. They follow from the strange assumption that nature abhors the orbitual or curvilinear motion ; that, in the words of Herschell, " A straight line, dynamically speaking, is the only path which can be pursued by a body absolutely free, and under the action of no external" cor- rective "force." Centrifugal force is therefore not exactly a force, but the tendency of nature to escape from the con- fined curvilinear motion, and to get back the sphere into the straight line of motion. Philosophy looks upon the myriads of rolling spheres as in unnatural, constrained movement, and there must needs be conflicting forces, to form the grooves and channels which hedge in the planets, and keep them to their orbits, when they would so rejoice in free straight motion to the bounds of space. Whewell says that, " In cosmical phenomena, every thing in proportion as it is referred tojpechanical prin- ciples tends to simplicity, to permanent and uniform forces, to one common property. In magnetical and chemical appearances, the application of mechanical principles leads only to a new complexity which requires a new explanation, and this explanation involves changeable and variable forces, gradation and opposition of qualities." That is, plain, simple, mechanical laws apply only to the enlarged action of nature ; in her recesses there is confusion, unintelligibility. For the want, therefore, of fixed general laws in the minor mechanism of nature, or for the lack of comprehension of those laws, the department of " mechanico-chemical " sciences is cut off from general philosophy, and managed by a great array of conflicting forces, such as heterogeneous attraction, homogeneous attraction, capillary attraction, various forms of repulsion, elasticity, cohesion, chemical affinity, current affinity, and the forces of the imponderables. Every judg- 24 OUTLINES OF A SYSTEM OF ment in this department is particular. " There is no en- largement of view to general propositions." We see deep thinking, " but the conclusions arrived at, even though clearly expressed, are intricate and obscure." There is not in the teachings of mechanico-chemical science the prominence, the boldness, the exactness; the simplicity, which characterize the works of nature, whether her force be exerted on the atom or on the world. Imponderables are so called because they are not the subject of weight. They impart no force by the act of descent, but for this reason they are not proved to be imma- terial, without matter. We read, {London EncyclopcedicC) that " a stream of electric fluid issuing from points, possesses force sufficient to counteract the power of gravitation in light bodies" ; ofcourse the imponderables could counteract the gravity of any matter which was their vehicle, or rather which they moved. Gravity being the unused force of rotation, given out on the arrestation of the motion of the falling body, they have none of this spare force ; they can- not be arrested ; they consume all their inherent force in their rapid flight. It is only by the stopping of the descend- ing motion of falling bodies that they give out force or indi- cate weight. We know not of pure disembodied force, and believe that the imponderables are the combination of force and matter, the force in intense degree compared with the matter ; that the element of matter, and its quantity in the possession of force, makes the distinctive character of the imponderables, and that force is thus fitted for especial func- tions in the economy of nature. This view does no violence to any system of philosophy, and appears demonstrable by the views we have taken in the preceding propositions. MECHANICAL PHILOSOPHY. 25 First, of heat. Heat has been regarded as the repulsive force, as the diluent of force, keeping it in due bounds. The same philosophers who would set aside mechanical action with reference to the mechanico-chemical sciences, at the very outset bring back the discharged mechanical laws. They need a pendulum or balance spring, something by which to regulate and control the mixture of forces. Heat is elected to this office of antagonism. The perfect law of force needs not this restraint. But there is a peculiarity of the action of force under the condition of heat, which has- been generally referred not to its nature, but to its con- nected matter. It seems fitted thereby more especially to induce corpuscular motion, and the heat acts plainly and distinctly in giving consentaneous motion to masses ; yet most usually its effects are traced in an internal action. We notice in this place the difference between solar and radiant, or reflected heat. The passage of solar heat through a lens shows that force then has under its control matter, the atoms of which have extent of surface, as will be explained when we refer to light. Radiant or reflected heat is not reflected or bent by the passage of its ray& through a glass lens, but is absorbed by the glass, which becomes heated, and continues so until by conduction the heat is equally diffused. It appears, then, as if by the impact it deposited a portion, at least, of its accompanying matter, and, the matter being deposited, the heat in passing, through the lens is absorbed. The force has taken its con- nection with other matter. Radiant heat is then force par- tially divested of its matter ; partially, we say, because in. its passage through a lens of rock salt, it again obeys the law of the passage of light and heat through a transparent media. A secondary radiation of heat still further deprives 3 26 OUTLINES OF A SYSTEM OF it of its matter. Thus we come to the conclusion that these differences are caused by the deposit of matter at the im- pingement of its rajs. It shakes off, as it were, its imped- ing embodiment, that with unimpaired energy it may give its strength to the corpuscular movements. The action of heat is readily explained. Every species of matter has that quantity or degree of force necessary to maintain its atomic structure. This is called latent heat, and is latent force. Now with the normal degree of force in molecular action, another degree of heat or force can be received and made latent in the corpuscular action without apparent change of structure. This is specific heat ; another added quantity becomes sensible or diffusible heat. It is beyond the normal heat which its structure can bear, and it swells or enlarges. Increase the heat still fur- ther, the molecular action increases, the orbit of circula- tion enlarges, and the solid becomes fluid and the fluid aeri- form. Hence heat acts repulsively by the very law which fixes the orbits of rolling spheres, that of increasing cir- cles with increasing force. "We have already referred to the fact, that the volume of the dilating body increases three times in small bodies for its length of increase, indi- cating the ever circular orbit of force. Latent heat is therefore normal molecular action, capacity for heat, that which a body can bear, and use internally without change of condition ; sensible heat shows itself by dilatation and expansion, by the increase of the circular motion of its atoms, and by its transfer. Daniell says that the polarity of heat is as certainly demonstrated as the polarity of light, though the experi- ments which demonstrate it are of a more delicate nature. Polarity is circular motion, or rather the indication of circu- MECHANICAL PHILOSOPHY. 27 lar motion. It is the direction of the orbit, and, applied to matter through which force circulates, the poles are the anode and the cathode, 'the direction of the current which passes ; or as Whewell describes it : " Polarization indicates opposite properties in opposite directions, so exactly equal as to be capable of accurately neutralizing each other ; that is, the same force passes and repasses circularly with an even power." Heat is always accompanied with a greater or less degree of light. This is certain with reference to free current heat. Latent heat and conducted heat are not the subject of exam- ination ; but yet as the breaking up of cohesion manifests light with the evolved heat, it appears almost certain that light is the essential condition of force manifesting itself as heat. What is light ? Not inert sluggish matter, not the disembodied force instantaneously diffusing itself, but the combination of the two. This is the reason of the endless disputes about the materiality and immateriality of light ; both views are partially right, both are wrong. There are indications that will support either side of the ques- tion, but the phenomena collected together result in the union of the two. It is force which gives it its transit, its dynamical laws ; it is matter which strikes the eye and forms the picture there. It is what force transports by which the world is painted in all its glory. It is not " a propagated quality of motion, extending in right lines in all directions from the point from which it emanates ; " but something is borne along on the wings of force so subtile as to be felt only by the most delicate tissue of the animal system, the retina. The materiality of light has the support of Newton and the great philosophers of his clay, and of many subsequently. 28 OUTLINES OF A SYSTEM OF Its materiality seems demonstrable from its being absorbed bj the vegetable tissues, giving them color and strength of fibre which no " propagated quality of motion " can give. It is inherent in the diamond ; it can be collected from the sun's rays by solar phosphori, and when emanated, the supply can be again received by a fresh exposure to the sun ; it is evolved from decaying bodies and from the liv- ing animal organization ; it obeys the laws of motion, of known moving matter, its line of motion is bent, and when not absorbed by the body on which it impinges, as the pon- derous missile on the ice or water, the angle of reflection is equal to the angle of incidence. Light also changes its line of motion in passing through a denser medium. This change of direction is only at its ingress and egress. It is a surface change, determined not by the medium, but by its transit within and without. May not this be the theory of the change ? The atoms of light, being matter, have extension of surface ; they strike the concave or convex lens on their edges as they enter, at an angle, not with their surfaces parallel to the glass ; on the egress one edge escapes while the opposite is yet resisted by the denser medium ; to use a popularly technical word, they are canted by the convex towards a centre, by the con- cave from a centre or focus, both on entering and leaving the glass. It appears, too, as if light were composed of atoms of different extensions, as by the prism these atoms are separated by their greater or less impinging surfaces. The fall of a flat piece of wood angularly on the water which would be turned, illustrates the idea ; in the case of the atom of light, the concave or convex glass would make the angle. Does not this also explain the angle of reflection ? It is remarkable, too, that the refractive powers of media are MECHANICAL PHILOSOPHY. 29 in proportion to their densities ; water acts more powerfully than air, and the power of water is increased by its having salt in solution. Bring to the mind, too, that the change of direction is at the surface only, and we must impute it to the manner of its entrance by surface change. A wave of ether or a " propagated quality " of motion by act of im- pingement would accommodate itself to the angle of im- pingement, as do the waters of the ocean to the projecting cliffs of the shore. The theory illustrates the phenomena, even if it be drawn from the imagination only. But it will be thought that our view is too mechanical and rough to be affirmed of light ; for how exceedingly minute must be those particles which in myriads cross and recross without impingement ! Space is indeed incompre- hensible in its minute divisions, as in its most extended bounds. It seems to flow out on either side, in wave- like undulations, upon the confines of infinity, with which it blends without distinctness of separation. Obscure as it is to us there is about the atom room, fixed laws, accu- racy of motion, and to higher beings the laws of God, operating in a mere point, may be as palpably distinct, as to us is the waving of the branches of the tree that bends before us in the summer's wind ; and because the motion of the atom is obscure to us, must we throw upon it the reflected light from the phenomena which nature, in her enlarged sphere, places before the eye. We understand the minute only as we comprehend the extended ; for they both have the one God over them, whose law is universal, unchangeable in reference to the atom and to the sphere. We advert but to one more of the phenomena of light, its polarity or the circular motion of its atoms. This is the stamp of force, its great characteristic, ever denoting its 3* 30 OUTLINES OF A SYSTEM OF presence. We will describe polarization in the words of Daniell. " It may assist our comprehension of the pheno- mena to illustrate them by a rough analogy ; a ray of com- mon light as it is emitted from a self-luminous body, we may conceive to revolve upon an axis coincident with its own direction, as a cylindrical rod may be made to turn, or which comes to the same thing, the reflecting or refracting surface may be made actually to revolve around the ray as an axis preserving the same relation to it, and no change in the phenomena will be perceived." We add, that the rolling earth flying in her orbit would be an illustration perhaps more apposite. We proceed to the examination of electricity. Franklin, with the sound discrimination which characterized his mind, expressed the truth in relation to it. We will quote his language, substituting the word " force " for " electrical fluid." " The opposite states of electrical excitement depend upon the increase or diminution of force relatively to the two bodies." These two states have been called the positive and negative. When two substances are rubbed together, sometimes the one and sometimes the other is excited. All substances have been divided into electrics and dialectrics, the one the conductors, the other the non-conductors of elec- tricity ; but subsequently it has been ascertained that all substances are conductors, their conducting powers differing only in degree. Hence we have not conductors and non- conductors, but substances differing in being good or bad conductors ; the metals, water, animal and vegetable bodies on the one hand, and oil, glass, dry air on the other. There is in the extremes a striking difference of atomic structure, as for instance, in iron and spermaceti. Any dissimilar substances rubbed together with proper MECHANICAL PHILOSOPHY. 31 precautions are capable of exerting the power, one of them becoming excited. The effect is produced by the applica- tion of force, nor does it change its nature. When confined, it is force ; when again set free, it is force. Electricity is thus described : " It is freely evolved by the mechanical action of heterogeneous substances ; still more abundantly by chemical action ; it is a product of animal organization ; it is capable of evolving heat, and heat is capable of evolv- ing electricity. It is capable of acting on bodies in oppo- sition to gravity, and is capable of the most energetic action on its own constituent atoms. Every form of matter may be excited to its action, and it may be transferred from one portion of matter in which it has been called forth, to another previously in its natural state." We could not more distinctly describe force. Electricity is force existing under some peculiar conditions. Its polarity is one of its most prominent phenomena. It can be insulated, or a channel formed for its circulation ; it can be kept a pris- oner, or its path opened that it may return to the earth, and add the strength of its feeble stream to swell the torrent of force which ' bears along the mighty orb in her rolling path. Differing from galvanism, which appears as a continuous stream of force, electricity is, as it were, a collected mass, a sphere revolving on the surface of the glass. It does not seem to affect the molecular action, but to pass through the aggregated atoms as free, revolving in its own orbit ; for, if you break the cylinder which contains it, the electrical spark is found in one of the parts only. Electricity, too, gives another striking demonstration of its nature. We quote : " If the electricity collected be distributed between balls of different diameters, it will be found that, the smaller 32 OUTLINES OF A SYSTEM OF the sphere, the more intense the action." Such is the law of force, wherever it exists ; there is circular motion, equal- ity of diffusion, the velocity increasing with the decrease of the diameter of the orbit. In the excited rod, too, the action is more intense at the ends than at the centre ; for the law is that of increased speed with the narrowing diameter of the elliptical orbit. Electricity gives to matter no attractive power, as it partially escapes from its receptacle, it draws or repels other bodies towards or from its receptacle ; and whether attracted or repelled, the moving body determines its motion by its own state of excitement. If equally ex- cited, it adds to the circulating force ; if less excited, it absorbs a part of the circulating force. No attraction of matter can be affirmed of this fitful, spasmodic action of bodies floating in the vortices of revolving force. How beautiful the provision by which the unexcited body advances to the excited, then in contact receives its burthen to be conveyed to other bodies, so that the resultant motion of vertical force is the equal distribution of that force, an equilibrium preserved not by opposing forces, but by the very nature and laws which govern the action of force. Galvanism is the result of the breaking up of existing structures, thereby freeing the force which bound their atoms together. Would any one ask what is the cement of the building when, by its destruction, the earth is covered and the air filled with lime? It is the force of cohesion made current, which constitutes galvanism. The condition of its being " current affinity" is decomposition, and a conduct- ing circuit or orbit in which it is to move. " Now," says Daniell, " it is curious to observe how chemical affinity in all these experiments waits upon the conducting and col- lecting power ; the strong attraction of zinc for oxsulphion MECHANICAL PHILOSOPHY. 33 is held in complete check till a passage is open for the circu- lation of the force ; the force which circulates must be equal in all parts of its circuit, it stops with the slightest break in the continuity of its conductor." Urged sometimes by the intensity of the charge, it leaps through a short space of air, and then with its flame arched upward, proclaims the tendency of force to assume the circle, whose circum- ference is proportional to the degree of the force which revolves. Dr. Farraday has proved that the contact of dissimilar metals is not necessary to the generation of the current, and that the force is always in exact proportion to the amount of chemical affinity. With a knowledge of the laws of force, this fact needed not the demonstration of experiment ; for the force of cohesion liberated must measure the current force ready to act in new combination, or to pass for exam- ination along the conducting wire to the matter it is to bring together in newly built structures. How beautiful, too, the analogy between the chemist and the mechanic ; the former, commanding for his work the force once used for cohesion, and again directing its strength for a similar purpose ; the latter, using as his property the force of a moving world, directing it in the circuit of his machinery, that it may destroy structure and build other structures that min- ister to human wants. This very analogy has been thus traced out. " The analogy of the transmission and direction of mechanical force, may perhaps assist in the formation of a clear idea of this influence of bodies," [current affinity.] " Every one is familiar with the modes by which the mus- cular force of animals, the elastic force of steam, &c., is led by the solid matter of levers, cords, and wheels to distant points from its source arid there set to work, somewhat in 34 OUTLINES OF A SYSTEM OF the same way we may conceive that the force of affinity may be directed to distant points through appropriate conductors. But its journey ings must be in a circle, and the arrange- ment must be made in such a way that the impulse may return to the point from which it set out ; it must circulate." " In no case," says Farraday, " is there a pure creation of force, a production of power without the exhaustion of something to supply it." Of course it has excited the won- der of chemists, that two pieces of metal, producing no change in their states, should be an inexhaustible source of power. The wonder ceases when the distinction is made between current affinity brought into action, and continuing in action in its orbit, and the current affinity from broken cohesion, returning after its circuit to rebuild from the ele- ments which had been torn asunder, at the broken orbit between the positive and negative pole. The one is seen in the action of the magnet, the other in the passage of the galvanic current, passing from the work of destruction through the wire to the work of re-creation, or at once passing through bodies in chemical affinity. Before we proceed to the examination of the union of the magnetical and electrical phenomena and the action of the magnet, we will explain our views more fully of the effect of the galvanic current in changing the condition of bodies on which it acts. Polarity is the positive and negative pole, or the direction of the current force. The wire is the con- ducting circuit, between the poles of which is the substance acted upon. " Now the idea of polarity," says Whewell, " involves the conception of opposite properties in contrary directions ; for example, attraction and repulsion, darkness and light, synthesis and analysis." That is, force revolves, the current in its passage one way repels, in the other MECHANICAL PHILOSOPHY. 35 attracts ; in one way gives darkness, in another way light ; it breaks down structure or rebuilds structure, for in one way force is taken from the body and from the other pole it returns. In the one case, for instance, it resolves water into its constituent gases, in the other combines the ele- ments of water into that fluid. This proves that our idea of polarity is right, and opens the mystery of chemical action generally ; for the same result is had without the wire, the transfer of force. Farraday expresses the idea in almost the same language. " Chemical synthesis and analysis must be conceived as taking place by virtue of equal and opposite forces, by which the particles are sepa- rated or united," that is, by the transmission of force. We continue to quote : " These forces, by the very con- sideration of their being polar, may be transferred from point to point, and thus we have a positive force active at one extremity of a line of particles corresponding to a nega- tive force at the other extremity ; all the intermediate par- ticles neutralize each other's action.'' This idea was introduced by Prout, confirmed by Davy, and fully illus- trated by Farraday ; and for its full comprehension it needs only that we discharge the unmeaning expression, ' negative force,' and consider the phenomena as indicating the transfer of force in its circulating orbit. In our view of magnetism, we have the labor lessened by the acknowledged fact, that current affinity, or galvanism, or electricity, is identical with magnetism. It is so decided by competent authority. This was first announced by (Ersted in 1820, and proved by a series of experiments. Franklin long before this had induced magnetical polarity in fine needles by passing through them a current of elec- tricity. The disturbance of the polarity of the ship's com- pass is also a well known fact. 36 OUTLINES OF A SYSTEM OF We call attention to this phenomenon : place the needle over the conducting wire ; it lies across the path of the rushing force ; beneath, it lies again across the marked pole in the contrary direction. Dr. Farraday succeeded in pro- ducing a revolution of the needle about the wire, and of the wire around the needle. The principal effects of terrestrial magnetism " may be imitated by distributing a wire around the surface of an artificial globe, in a spiral direction from the equator to the poles, the two extremities being turned inwards, brought out at the two axes, by which the connec- tion may be made with the battery. A magnetic needle properly suspended in different situations near the globe, will arrange itself in positions perfectly analogous to those assumed by the dipping needle in the corresponding regions of the earth." The action of conducting wires rolled in the form of the flat spiral, produces on one side the action of the marked (north) pole, and on the other of the unmarked pole of the magnet. As it has been remarked, this is the fundamental fact, (the rotary movement accompanying the orbitual,) to which other facts of eZe9 the wave was raised, force was supplied for its higher rotation. It appears, therefore, that what is called the resistance of the water to the propelled vessel, comes not from reaction, but is the loss of force in establishing the current by which her path is opened. In the preceding statements the word momentum has been employed in conformity to the usual language. As was before observed, momentum is the degree of force present in action upon the body. It is the energy or strength of the motion. The intensity of force is measurable by the velocity it im- parts ; but as it requires more or less force according to the weight of the body, to move a body with a given velocity, in ascertaining the present force of a body in motion, its weight is one of the elements of the calculation. Momentum is therefore the force which moves the body, that which it will impart when the motion is arrested. It is simply force, and the use of the word momentum is not only unnecessary, but it leads to a confusion of ideas to employ two words to express the same thing. If a bullet be discharged from a gun through a door left ajar, it will pass through the wood, giving no motion to thOj door. In gunnery, cannon balls, to do the most injury to a ship, should be fired with small charges of powder, that they may not pass through the ship, but transfer their mo- tion to it. In these cases, reaction increases with the les- sening of the force, that is, if the ball pass through the ship, it does not injure the ship so much as if the motion of the ball be arrested, and its force transferred to the work of destruction. The gun recoils proportionally to the force of the explosion, of course j for explosive mixtures act in all directions, 70 OUTLINES OF A SYSTEM OF The doctrine of vis inertias asks a passing comment. It is inferred from the first law of motion. Bodies in motion continue in motion from the inertia of motion ; bodies at rest continue at rest from the inertia of rest ; that is, bodies which move do move, bodies at rest are at rest. This is all. The idea receives some coloring from two facts. First, the progressive motion of a mass is in proportion to the force impressed, and takes place after a lapse of time from the application of the force to the atoms of the body. There is needed time for the force to be diffused among the atoms by atomic motion, before consentaneous or progressive motion is induced. The other fact is, that in most cases force in moving bodies is gradually applied. Thus a bullet slowly moving will enter the water; for it can, as it were, await the tardy resolution of the atoms of the water into progressive motion to give it place. But the bullet from the gun is deflected. Its velocity is so great that it cannot transfer its force ; for it would take many instants for the particles of water, moving with the same velocity with the bullet, to travel through their atomic space, and to induce progressive motion of the column necessary io be moved for the passage of the bullet through the water. We now come to the consideration of another principle, which is often referred to in the explanation of the mechan- ical powers. It is this : The loss of time is the gain of power ; and, conversely, the gain of time is the loss of power. It is not so. Why, let us ask, are there in the text-books of mechanical philosophy assertions like this : " Time is an important element of force " ? Time has no reference whatever to force, or to motion consequent upon the force applied. It can neither make nor destroy it. It can- not increase or diminish it. A body with the same present MECHANICAL PHILOSOPHY. 71 force moves on forever with an uniform motion. Time can never change the quantity, quality, or direction of motion. Time is a succession of events. It is itself measured by motion, by the harmonic uniform motion of the spheres. We measure motion by time indirectly ; its direct measure is the motion of the earth. Velocity is more conveniently applied to the artificial divisions of time than to the earth's motion. It is, perhaps, better for common purposes to say that a body moves so many miles an hour, than to say that it moves so many miles while the earth moves one twenty- fourth of a rotation. But the doctrine like that of action and reaction, and of vis inertioe, has a coloring or semblance of truth from the misconception of facts. In two ways time has an apparent connection with force, as if time increased force. First ; animal or muscular force is produced by the ani- mal by a succession of efforts. It is generated gradually, and of course imparted gradually. By time the force is increased or added to. Time does not increase power ; but the muscles can supply more force in five minutes than in one minute. This idea is fully illustrated by the inclined plane. A horse, in dragging up a weight, has more time to produce the required force ; but when the load is ele- vated, he has imparted just that degree of force which is required to elevate the weight directly, at once, verti- cally. The mechanical power of the inclined plane enables the animal to do by successive efforts what he could not do at once. He cannot raise the weight at once ; he can raise the weight in time. A man cannot raise by one effort a ton of iron ten feet, but in an hour he can furnish the necessary force. Yet, it is said in a work on mechanics, that it requires no force to move a body horizontally, full 72 OUTLINES OF A SYSTEM OF force to raise it vertically, and that the gain of power by the inclined plane is in simple proportion to the angle it makes with the horizon ! Secondly ; another misconception is of the law of falling bodies. The force of the falling stone, it is commonly said, increases according to the square of the time of descent. The force increases not with time, but with every line of descent. The descending body has, proportionally to its change of level, an increase of spare force, of force unused at its lower level of rotation. The greater the fall, the more the force. Thus in the use of animal strength, and in the use of the force of the falling body there is, not an increase of force by time, but an addition to the force received in time. A man's power of labor is measured by time ; the power of the waterfall is measured by the space of descent, or for con- venience' sake, by the time it falls, as the space and time are in one fixed ratio. So simple is the explanation of the philosophy of the me- chanical powers, that it is surprising that the subject should ever have been deemed intricate, or that so much mathe- matical labor should have been wasted on it. To under- stand the lever, and, that understood, all the mechanical powers are understood, does not require one to read Archimedes' mathematical demonstration, nor to understand the laws of statics, dynamics, virtual velocities, equilibrium of forces, and centres of gravity. Let one idea be present to the mind, and there can be no misconception. The force applied is the force that produces the result ; time will not increase or diminish it, it ever remains of one intensity, capable of producing only one degree of motion ; no lapse of time, no mechanical skill can change its nature or degree. MECHANICAL PHILOSOPHY. 73 Without reference to loss by friction, it may be transferred through pulleys, levers, wheels, over inclined planes, when- ever needed, and when used at the end of the line there is only, and just that force which was at first applied. It will there produce the same quantity of motion, neither more nor less, that its direct use would have produced without the intervention of the machinery. If by the lever one pound raises two pounds, the two pounds will be moved half as far ; if a man raise a ton by means of a pully, he has put forth just the strength that would be required to raise a ton to the same height without the pully. His gain has been the time given for him to produce and apply the strength. He could not lift a cord of wood at once, but log by log he can supply the needed force for piling it. If a smaller wheel . turn a larger one more slowly, there is still the same degree of motion in the larger wheel that was in the smaller ; if the larger turn the smaller, there is still the same motion in proportion to the quantity of matter. It requires one degree of force to give one quantity of motion ; a given force can do neither more nor less. This is rigorously true, and, if it be understood, there is no mystery about the me- chanical powers. If there be a gain of power, it is distinctly traceable to the gradual addition of force from animal strength, or from the increasing force of a descending body. The measurement of these by time has led to the confusion thrown over the subject by the doctrine, that there is a gain or loss of force by time. It will not be necessary to remark particularly on either class of the mechanical powers, as it is believed that this general statement covers the whole ground. The next supposed force to be examined is the centrifugal force, or the tendency of bodies moving in curved lines to 7 74 OUTLINES OF A SYSTEM OF assume a rectilinear motion. It is not exactly a force, but a tendency of the moving mass not to move as it is moving. In the Philosophy of the Inductive Sciences , we find the following explanation of the character of this ten- dency. " The centrifugal force is not a distinct force in a strict sense, but only a certain result of the first law of motion, and is measured by the portion of centripetal force which counteracts it." " The projectile force is a hypo- thetical impulse, which may at some former period have caused the motion to begin, while the central force, gravita- tion, is an actual force which must act continuously, and during the whole time of motion, in order that the motion may go on in the curve." If we had no doubt of the truth of the theories which relate to the motions of the spheres, the reading of such passages would suggest a doubt. There is an obscurity of language, not arising from the want of power of expression, for no man has more power than this author, but because there was no distinct idea to be conveyed. In the first place, centrifugal force is not a force, but a result ; not being a force, it is still measured by another force. Then, the force which is not a force is counteracted, of course it is destroyed, it no longer acts. This verbal criticism is made only for the argument, that doctrines feebly expressed by strong men are of doubtful soundness. It is supposed that the moon, for instance, received originally an impulse of motion in a straight line, but that, being constantly acted upon by the attraction of the earth, the straight line is changed into the curve ; that the attrac- tion of the earth which would, unchecked, draw her to the earth, is opposed by the centrifugal force ; and that the moon, under the influence of forces acting in opposite direc- MECHANICAL PHILOSOPHY. 75 tions, is held in her orbitual course, the original impulse giving the motion. But as the moon's orbit is elliptical, she is at times com- paratively nearer to, and at times further from the earth. Of course, in her changing distance, the centripetal and centrifugal forces vary in intensity. The earth attracts less or more according to distance, and the counteracting force changes relatively ; they preserve an equilibrium. It cannot be that the force of opposition can remain with an equal intensity, when the force of attraction is continually changing. They therefore change proportionally, or to the same degree, so that the moon is guided in her course by forces perfectly elastic. Again ; if the original impulse of the moon's motion were an impulse of rectilinear motion, and the attraction of the earth acts in a straight line to her centre, how from two forces acting at right angles is the curved line of motion produced ? An original impulse in a straight line of direct- ion, and another impulse in a straight line at a right angle with it, would ever and invariably produce a straight line of motion at the mean distance, half way between the two lines of impulse. If gravitation changed the moon's motion, the moon must necessarily be brought thereby nearer to the earth ; if it act on the moon impelled in a straight line, the resulting motion would be a mean direction, lessening the distance between the attracting and attracted bodies. Even Newton, at an early period of his speculations, held the opinion that the result of attraction on the impelling force would be motion in a kind of spiral. That the orbit of the moon could be formed by the action of the two forces, has been nominally proved from the case of the cannon ball, which under the joint force of projection 76 OUTLINES OF A SYSTEM OF and gravitation describes a curve. But the case is not an analogous one. The curve of the projectile is occasioned by the regular decrease of the force of impulse. Its onward force is gradually lost by the resistance of the atmosphere, and thus "gravitation" brings the path described into a curve. In order for the attraction of the earth to give a curve to the orbit of the moon, the impulse of the moon must be gradually lessened by some retarding medium, as the can- non ball is retarded by its passage through the air, whence would result a spiral curve gradually bringing the moon to the earth. But never can the impulse in two directions of the rectilinear force result in a curve. We know that the re- verse is mathematically proved, and that the nature of the curve which would be produced is pointed out ; but the mathematics by which this is done, is of a peculiar kind introduced with the theory of gravitation, being rendered necessary by this theory. What gives the elliptical form of orbit, for instance, of the comet, which, at one time widens its path in the broad expanse of almost limitless space, and then narrowing its orbit, almost brushes in its rapid flight the face of the sun ? It is not force of motion ; for this force acts according to the law of the area described in every part of the orbit. It is not attraction ; for attraction merely holds its own, increas- ing or diminishing according to distance. Nor yet is it centrifugal force ; for this follows, and is measured by, gravi- tation. It is not space ; for there is no grooved channel or marked track through its vastness. A sphere, perfectly a sphere, each atom of which was moved with equal force, would necessarily describe a circle. May it not be that it is the shape of the revolving body ; that, if the shape of this world, for instance, is given, the ellipsis of her orbit may be MECHANICAL PHILOSOPHY. 77 determined ; and that, if we knew the form of the comet, its eccentricity of path could be understood. The idea of centrifugal force grows out of a trivial, and perhaps misunderstood fact, and is invariably illustrated by it. We allude, of course, to the action of the sling. From the hand proceeds the impulse of motion, the string is the gravitating power, or that which by its tension measures this power, and the tendency of the stone to fly off in a tangent represents the centrifugal force. It is unquestionably the tendency of the stone to escape, and, if the string were to break or be let slip, the stone would no longer continue to move in the same circle, but the impressed force would give it another direction of motion. The force of motion of the stone is from the centre. There is nothing to give the stone its circular movement except the string ; that broken, the impressed force gives the stone a curved motion in another direction. So far is this action from being analogous to the motion of the nioon, that it is the very reverse. The stone from the sling receives force acting in a line of direction from the centre ; the moon receives from the centre of her orbit an impulse toward the centre. It is not a fortunate illustra- tion to compare the effect of an impulse away from the centre, to an impulse affecting the body and drawing it toward the centre. Centrifugal force, too, is often illustrated by the neces- sity which a man finds in running round a small circle, of leaning inwards toward the centre, "to counteract the cen- trifugal force." But we will quote a contrary opinion : c< Let any man move in a circular or elliptical line described or marked out to him, and he will find no tendency in him- self either to the centre or from the centre. If he attempt 7* 78 OUTLINES OF A SYSTEM OF the motion with great velocity, or if he do it carelessly and inattentively, he may go out of the line either from the centre or towards it ; but this is to be ascribed not to the nature of the motion but to our infirmity, or perhaps to the animal form, which is more fitted for progressive motion in a right line than for any kind of curvilinear motion." Thus says Lord Monboddo, and proves that philosophers are not agreed among themselves concerning a fact, which is assumed as a " standard example " of their mechanical doctrines. However it may be with a man running round in a circle, we feel quite sure that a revolving sphere would not have to lean inward to prevent its falling outward, or to lean outward to prevent its falling inward. The action of the governor of the steam engine has also been referred to, in order to illustrate centrifugal force. The two heavy balls are so suspended that when not revolv- ing they hang motionless ; endued with activity in propor- tion to the velocity of their revolution, they rise, and describe wider and wider revolutions. The reason of the rise of these balls is the force communicated to them, from which they take a higher level of rotation, a beautiful illustra- tion of the views we present. They could not thus rise from the action of centrifugal force, were there any centrifu- gal force ; it impels, if it impel at all, from the centre. How could the moon be held in her orbit, if centrifugal force acted in any* : other direction than the direction oppo- site to the force of gravitation, which is to counteract it ? The breaking of the too swiftly revolving wheel is another illustration of the centrifugal force, which keeps the planets from responding to the attraction of gravitation. But the application of force to turn the wheel is at the centre, as in the sling it is from within outward. The central part MECHANICAL PHILOSOPHY. 79 of the wheel as truly impels the circumference, as the crank or rod impels the centre. There is motion induced under the condition, that the cohesion of all the matter in motion will bear the force applied at the centre. If too much force be applied, the crank or the wheel may break. The greatest force required is at the circumference, while the force is applied at the point the furthest removed. Every practical mechanic knows that there is no danger of a wheel's breaking if the motive force be applied to the cir- cumference. But nature does not so unskilfully apply her motive power. Her force for revolution or rotation is present with every atom. It is equally diffused through the whole mass, every particle retaining its proportional motive power according to the orbit to be described ; each moves of itself, and from its own energy ; one does not push, draw, or impel another. There is for this reason harmony of motion, all things moving according to the order of nature. Those who require a balance of forces, conflicting powers, those who compare the motion of the spheres to a school- boy's sling, or to the dizzying whirl of a man running in a circle, seem to degrade the mechanism of the heavens below the results of human ingenuity. We pass from centrifugal force to its opposite, centripetal or attractive force, gravitation. It may be well to give an outline of the theory as pre- sented by those who have the most unshaken confidence in its truth. The theory of universal gravitation asserts, that the force, by which the different planets are attracted to the sun, is in the inverse proportion of the squares of their distances, and that the force, by which the same planet is attracted to the sun in different parts of its orbit, is also in the inverse proportion of the squares of its distances ; 80 OUTLINES OF A SYSTEM OP that the earth also exerts a similar force on the moon, and that this force is identical with the force of gravity ; that bodies thus act on other bodies besides those which revolve round them ; that thus the sun exerts such a force on the moon, and that the planets exert such forces on one another ; further, that this force, thus generally exerted by the entire masses of the sun, earth, and planets, results from the attraction of each particle of these masses, which attraction follows the above law, and belongs to all matter alike ; also, that this attraction, operating on the " hypothetical impulse of motion," gives its spheroidal form to the earth, and their elliptical form to the orbits of the heavenly bodies. This theory has been a settled doctrine of philosophy for nearly two centuries, and generally, if not universally, it is deemed an established truth. It seems to have passed away from examination, to be laid aside as that which need never again be the subject of thought. It is spoken of as ascer- tained ; and its discovery and extended application are considered as among the most glorious achievements of the human intellect. Thus it will be almost impossible, even if the theory be not founded in truth, to bring the minds of men to its re- examination. It has become associated with the universe from its most enlarged to its most attenuated parts. The attempt to substitute other theories, to assign other laws of force, may be deemed the wandering of an erratic mind, or the presumption of an ignorant man. But this research was commenced without reference to the public, and the results are presented, not presumptuously, but firmly, not with the belief that we have fully developed the truth, that all our views are sound, that no mistakes are made, but with the conviction that our speculations are founded MECHANICAL PHILOSOPHY. 81 upon principles that fully deserve attention and examination. We appeal to those who believe that there is yet hope of progress in philosophy. Attraction, as coming under human observation, is mainly believed on considerations derived from the fall of bodies to the earth, and from their supposed weight or pressure when at rest. This is the foundation of the theory. All else is assumption or deduction. The mutual attraction of different masses at the surface of the earth is supposed to corroborate the theory ; but from the utter impossibility of measuring this slight action, or even of ascertaining if there be any, the mutual attraction of the minor masses being overwhelmed by the immense comparative mass of the earth, it is a proof about as conclusive as that the sun shines because a fixed star twinkles. The doctrine of at- traction, therefore, rests on the observed fact that bodies unsupported fall to the earth. If, therefore, the descent of a body can be fully accounted for by the spare force of rotation at a lower level, and its weight or pressure by the fact that it requires force to lift it up to a higher level, the reason on which the theory of gravitation stands is taken away. The law of gravitation is not needed for the motion of the heavenly bodies. There is more truth to nature, there is more simplicity and beauty in the idea that the force of the revolving body is within itself ; that its curvilinear motion is its natural motion ; that it goes round in its orbit without needing the guidance and direction of central and tangential forces ; that it can be trusted to the unerring energy imparted to it from the beginning. It needs no great pre- sumption thus to affirm ; for by ancient philosophers, and in more recent times by Copernicus, Galileo, Kepler, Des 82 OUTLINES "OF A SYSTEM OF Cartes, it was believed that circular motion was the natural motion. Nor is the general acceptation of a theory any proof that it is the most true and most perfect theory that will ever be presented. How long endured the Ptolemaic system of astronomy, how firm was the belief of men in its truth ! Those who first questioned it, those who first doubted that the sun revolved around the earth, were not only deemed unsound in reason, but " diabolical and wicked," and were visited by the vengeance of the offended good sense of man. Extensive, too, was the sway of the theory of Des Cartes, which preceded the theory of gravitation. The Cartesian hypothesis, representing the worlds as moved by vortices of revolving matter, and the fall of bodies as motion downward by the decrease of the range of the vor- tex, they sinking to the lowest part of the whirlpool, held for a while an even contest with the hypothesis of gravita- tion, the battle hanging long with doubtful issue. Because it was decided at last in favor of the Newtonian school, is it to be supposed that the speculations of that truly great man, Des Cartes, were all absurd, that he affirmed no truth, that Newton was right in all his affirmations, and that the power of progress expired with his life ? How great were Galileo, Copernicus, Leibnitz, Kepler ! Yet who takes for granted all that they asserted ? To see truth fitfully, through the obscurity of error, is the most that can be hoped for by any man. or can be claimed as the result of the labors of any philosopher. Among the minds distinguished as far surpassing in power the range of ordinary intellects, was that of Kepler. He seemed, on some points at least, to have an intuitive per- ception of truth, and his discoveries have led to extended MECHANICAL PHILOSOPHY. 83 practical results. His determinations of the laws of plan- etary motion are, and must ever continue to be, the basis of knowledge in astronomy. Yet even he believed that the earth was an animal, and many of his other ideas create a smile, they appear so fanciful and absurd ; but fanciful and absurd because time and further observation have refuted them. It is no evidence of a want of reverence for the great, that we believe and assert that no individual is without error or has attained the whole truth ; that no authority, however great, should determine and settle every principle in philosophy. " There were giants in those days ;" but so long as the race of man exists there will be strength. " Why," said a very great man, far back in the ages of time, u why is it that neither very small nor very large bodies go far when we throw them, but in order that this may happen the thing thrown must have a certain propor- tion to the agent which throws it ? Is it that the thing which is thrown must react against the thing which pushes it ; and that a body so large as not to yield at all, or so small as to yield entirely and not to react, produces no throw or push?" Should the human mind have rested upon philosophy like this ? By no means. The theories of philosophy are not truth, but monuments set up to mark the progress of man in his search for truth, guides in the path which leads to the truth. We should read with rever- ence for the great minds of olden times, while rejoicing in the advance which present opinions indicate ; we should read present opinions in the belief that they also will serve future generations to mark a continued and accelerated progress ; we should read with respect for those who have 84 OUTLINES OP A SYSTEM OF faithfully discharged their trusts, and with confidence that those who are yet to do work upon the earth, will do it even more successfully, for having the vantage ground of former attainments, the highest reach of the minds of the greatest men of one century furnishing the elements of thought to the succeeding age. Those who reverence Newton should show their reverence by imitating him in his unwearied and eager search for new truth. He was not satisfied with philosophy as he found it ; but, taking the floating theories of his time, he employed his immense intellect in giving them system, character, definite- ness, so that his philosophy, partaking of the vigor of his mind, has so long held dominion over the world. Though his name is most intimately associated in the general mind with the theory of gravitation, his labors in this depart- ment used but a small portion of his energy. Every sub- ject in the vast range of subjects to which he directed his attention retains the marks of his strength. He is often thought of as a mere mathematician, verifying the ideas of others. Far from it. His originality of mind equalled his mathematical exactness of conception. How eagerly did he seize upon every new truth, how ready was his mind for progress ! The contemplation of such a char- acter should prevent us from ever remaining satisfied with ideas to which the least doubt can be attached. CHAPTER V. " IN THE CONSTANT OSCILLATION OP THE HUMAN MIND BETWEEN IDEAS AND FACTS, AFTER HAVING FOR A MOMENT TOUCHED THE LATTER, IT SEEMS TO SWING BACK MORE IMPETUOUSLY TO THE FORMER." Whewell WE pass from the examination of the very minute and of the far-extended, to the common facts of our daily observa- tion ; gladly throwing down the telescope and microscope, we will look with the naked eye at nature in the ordinary range of vision. Were we to select one class of facts to illustrate the ideas we present, and to disprove the attraction of matter, it would be that which relates to oscillatory motion, the action of the pendulum and kindred movements. The swing of a pendulum, increasing in velocity in pro- portion to the decrease of distance from the centre of oscil- lation, the force of its motion being measurable by the area of the circle of which it describes a segment, shows that the nature of force is the same, however its energies may operate. It brings to the mind the relative speed of the planets, increasing as the diameter of their orbits diminishes. Its regular beats mark time with the same precision as does the harmonic motion of the heavenly bodies. It is, therefore, a free, unrestrained movement, showing the laws of force, and had it been rightly understood, the laws which 8 86 OULTINES OF A SYSTEM OF regulate the planetary movements might have been distinctly inferred from it. " We feel," says Bailly, in his History of Astronomy, " that nature is very simple in her operations ; the positions and motions of the planets offer at first sight the appearance of intricacy, but the principle which impels them has a naturalness and simplicity like the character of truth ; " and this principle has application not only to them, but to all natural and unrestrained motion. Thus in the pendulum, its orbit prescribed and a uniform force of impulse given, motion ensues, invariable, equal, measured by the area described. A pendulum beating seconds does not change as to time of vibration with the addition or subtraction of weight, nor with a stronger or weaker impulse given to it ; the weight of the mass moved and the length of the sweep do not change the time, if the same length of rod is retained. The force of motion is ever in proportion to the mass, and the stronger impulse only increases the range of motion with an increase of velocity that gives the equal time. The impulse lifts it higher and it falls with greater rapidity, and the fall both in distance and velocity determines the succeeding rise. It is evident, therefore, that this result is produced by the same principle which occasions the fall of bodies to the earth ; for the downward force is just the force of a body falling vertically the same distance, and the rise is also the same both in relation to distance and velocity. It is the same principle which causes the rise and fall of a stone thrown into the air, to be in equal times. How can this equal rise and fall of the pendulum be explained on the theory of gravitation ? Where is the reference to the centre of attraction, where the gravitating power ? How is it that the power drawing to the earth draws and repels MECHANICAL PHILOSOPHY. equally ? The rise is unquestionably a continuation of the same motion as the fall, proving that the force has no more reference to a downward than to an upward attraction. Galileo first called attention to the fact that in the case of a stone swung by a string, the time of its rise was equal to the time of its fall without reference to the path or orbit of its rise ; thus pointing to the truth that oscillation is but the transfer and retransfer of the force of rotation, and that, consequently, the force disengaged by the fall is the force which occasions the rise. The force is produced by the descent, and is absorbed by the ascent ; it is in proportion to the degree of descent, and is necessary for the same de- gree of ascent ; the degree of force is proportional to the change of level, one mean level being ever preserved in all oscillation. Therefore, the cause of oscillation is to be referred to the moving body and not to the earth. We repeat the idea ; the force by which the oscillating body moves is the force disengaged from rotation by the decrease of the level of rotation. It is the unseen force by which all things move in their diurnal round, for a moment becoming visible in the curve of the pendulum, as the un- seen motes floating in the air show themselves for an instant in passing through the beams of the sun. From the view we have taken it will be perceived, that as the pendulum preserves one mean level, and as its force of descent is, as it were, annihilated by its ascent, it can neither communicate force, nor be the source of any motive power. We can also understand the manner in which the force of impulse acts ; it gives the elevation by the descent from which force is produced. Practically, to continue the oscil- lation of the pendulum, force of impulse, as by the weight of the clock, must be added continually ; for a single impulse of 88 OUTLINES OF A SYSTEM OP elevation is soon lost by friction, and by the force taken to move away the air from the path of the vibrating mass. In a vacuum and without friction, the pendulum would continue to act without a renewal of the impulse. To understand oscillation, we should separate in our minds the cause of oscillation, the transfer of rotative force to other motion and its reapplication to rotation, from the impulse which first elevates the mass to the position from which it falls, and which is only the condition of oscillation. This view of the subject takes away many of the abstrac- tions which have been connected with the action of the lever, and with the motions of bodies in equilibrio. It throws over all connected subjects a plain and intelligible law. The mind escapes from embarrassment. What more simple idea can we have in relation to the action of a lever of unequal arms, where a smaller weight balances a larger weight and oscillates with it, than to know that one in proportion to the mass ascends in the degree in which the other descends, the greater descent of the smaller weight affording sufficient force for the less ascent of the larger weight, and the con- verse ? How difficult to conceive that the earth, with an attractive force in propotion to its mass, could draw down five pounds so as to elevate ten pounds, merely because the two unequal weights are at different distances from a certain fixed point, though at the same distance from her centre ! In a scale-beam balanced by two equal weights, how could oscillation take place under the law of gravitation ? Yet if you give one of these weights an impulse, they will oscil- late, oscillate forever in a vacuum without friction. Gravitation has no power to give alternate motion, at- tracting both weights with equal force, it cannot first make one heavier and then the other. If both were held with MECHANICAL PHILOSOPHY. 89 equal strength, it would be absolutely impossible for this vibration to take place ; there is an absence of all cause, or tendency, or capacity for oscillation. " Vis inertias of mo- tion" gives no aid ; for the motion is suspended and renewed at every vibration. Nor does " action and reaction;" for the difficulty is to account for the action. The earth might as reasonably be supposed to attract only one side of an evenly balanced wheel, and thus give it continuous rotation, as first to attract one weight and then another, when both weights are equally heavy. The motion is unquestionably from the transfer and retransfer of rotative force. The balance rotates as one mass with one degree of force, but this force flows from one part to the other of the mass. So far from being able to induce oscillation, the law of gravitation would immediately overcome the motion. The power of attraction, it is said, mcreases with the decrease, and decreases with the increase of the distance from the centre of attraction. The weight going down is therefore more forcibly attracted, the weight going up is more feebly attracted, and this in an increasing ratio, both for the de- pression and for the elevation. The difference, it may be said, is so slight, that its results can never be detected by observation. But slight as may be this want of equilibrium, it actually exists. Balances have been made so perfect and so nicely adjusted, as to turn by the impulse of the thou- sandth part of a grain. Suppose a perfect balance without friction at the fulcrum, and acting in a vacuum. Here this want of equilibrium would be felt; the descending weight, being more attracted, could not rise ; the ascending weight, less attracted, could not fall. There could be no oscillation under the law of gravitation. Thus nature in the vast range of her adjustments would feel 8* 90 OUTLINES OF A SYSTEM OP and respond to this difference of attractive power at the differing distances from the centre of attraction. Through- out extended space there could be no oscillatory movement. The spheres, according to theory, evenly balanced in their orbits by the central and tangential forces, would, by mu- tual attraction, have erratic movements. There would be perturbations, actual perturbations, wanderings, actual wanderings, from their path under the increasing power of the lessening distance. Their changes could not be com- pensatory and periodic ; the mean time of revolution and mean extent of axis of orbit could not be preserved ; they would aberrate, but never oscillate, for the force causing aberration would be increased by the act of aberration. On this earth too, under the law of gravitation, the order of nature would be broken up. Off the Cape of Good Hope, there are at times waves more than a half mile in breadth, and very many miles in length. Millions and millions of tons of water are thus heaped up in one volume ; the increase and diminution of attraction in this case would be felt and responded to, for there are out of balance thou- sands of tons. It must be that the ascending water would continue to rise, and the valley of depression to sink lower. What too would be the result of the great tidal wave raising and depressing the waters of an ocean ? Quietly to sink the less attracted elevation, and abruptly to lift the more strongly attracted depression ? Impossible ; under the law of gravitation there can be no bound or limit, no oscillation whatever. Perturbation, swerving motion, is without check. There is no voice of command, Thus far and no farther shalt thou rise, and here shall thy proud waves be stayed. But on the other hand, in the hypothesis we offer, oscilla- tion is measured in its extent by the impulse. The force of MECHANICAL PHILOSOPHY. the undulation is neither an increasing nor a diminishing force. It is not acquired from other bodies, nor imparted. It exists in the mass moved, and is transferred from part to part. It is a current of force flowing by an impulse. This idea will be further elucidated as we proceed, and a prin- ciple will be unfolded by which the oscillation of all fluids is limited within a definite range, so that the equipoised and freely moving element, water, has a fixed bound to its oscillations. We would rest the truth of the hypothesis on this nice adjustment, this beautiful equipoise of motion by which is secured the permanence and harmony of creation ; and with these ideas, the rise of the wave reflects from its spray not only the light of the sun, but its motion reflects to the mind a more beautiful light, light revealing the law of nature, by which movements as free as the breath of the breeze are held in subjection with a chain so strong, that He only who forged it can rend it asunder. We will now recur more particularly to the phenomena of the waves. To show that they are not distinctly under- stood, we will cite the following description from a standard work on Natural Philosophy: " Certain particles of water are first forced down, and the surrounding particles are forced up above their level ; their circular ridge subsides, and not only fills up the original depression, but from its momentum forces up another ridge exterior to it ; this sub- siding forces up another ridge, and so on." This descrip- tion calls to mind the following passage from an ancient philosopher : " His whole performance seemed to reach no further than if a man should say, ' Socrates does all by intellect,' and after proposing to give a reason for my action 92 OUTLINES OF A SYSTEM OF should say, * I am sitting on my bed, because my body is composed of bones and nerves ; the bones are hard, solid, and separated by joints, and the nerves being able to bend and unbend themselves tie the bones to the flesh, &c., and that is the reason forsooth that I sit in this position.' ' But we need an explanation of the phenomena of the waves more distinct than comes from the mere recital of the phases of their rise and fall. It is expressly mentioned by Plutarch, and by Pliny, that the seamen of their day used to still the waves by pouring oil into the sea. A letter writ- ten in 1707, speaks of a storm at sea " which had nothing particular about it, except that the captain found himself obliged to pour oil in the sea, which had an excellent effect, and succeeded in preserving us." Franklin, in his paper on this subject, says : "A small quantity of oil, for in- stance, a quarter of an ounce, will spread itself quickly on the water in a pond to the extent of an acre, and if poured on the windward side, the water will thereby be rendered quite smooth as far as the film of oil extends Its prin- cipal operation is to prevent the rising of new waves, and to prevent the wind from driving those already raised with as much force as it would if their surface was not oiled." This idea of stilling the waves by means of oil is omitted in recent works on the subject, and is considered by many as a popular superstition ; but when was Franklin mistaken in facts which he investigated ? and what popular belief is there thus extensive which has no foundation in truth ? Why is it, as before stated, that a thin stratum of oil spread over the surface of water, will prevent its freezing when exposed to a degree of cold much below the point of conge- lation ? Why does oil prevent the adhesion of substances pressed together ? All these results are from the non-con- MECHANICAL PHILOSOPHY. 93 ducting properties of oil. Force as heat does not escape through it ; force of cohesion does not pass this barrier ; force to give the impulse which occasions the undulation of the waves, is repelled from the water. The theory of the identity of force a priori, without experiment, would have indicated these results. A fact analogous to the rise of the wave, is the rise of the air in a ventilating tube ; over the upper orifice passes the horizontal wind, particles of which, by their friction or attrition on the air in the tube, are arrested in their course ; the force by which they were impelled is imparted to the air in the ventilating tube, and consequently the air is raised to a higher level of rotation. Wherever there is a passage of a current of matter, any part of which is arrested in its course, that which arrests it is moved. With this idea fixed in the mind we are able, not only to give a satis- factory explanation of the rise of the wave, but also of many common facts coming under our daily observation. When the wind passes over the surface of the sea, parti- cles of this aerial current are arrested in their course by any projecting inequality, or in the absence of already formed waves, by friction or attrition, as already explained. The water has additional force transferred to it by the passing wind. It acquires force for rotation at a higher level. It therefore rises. The elevation of the first wave, however slight, offers a greater impinging surface ; it there- fore continues to rise, and its rise is proportional to the strength of the wind which causes it. This undulation of the water arises from the same principle as the oscillation of the pendulum, the motion of which is the reception and transfer of the force of rotation at its different levels ; the descent liberates force for the ascent, and one mean level 94 OUTLINES OF A SYSTEM OF of rotation is ever preserved. Thus rises the wave, its motion the reception and transfer of force, its impulse of oscillation the force robbed from the passing wind. Thus, and thus only, can we explain a fact which is rather indefinitely expressed in the following language from high authority : " Momentum may be accumulated to an enor- mous degree in very large suspended masses, by forces, which, at their first application, appear to be totally inade- quate to move them." The impulse ^s " totally inade- quate " to cause the motion ; a child's hand cannot move a thousand pounds, but the child's hand can destroy a balance, and the force of nature transferred according to the level of rotation is the cause of motion. In the case of the wave, the wind destroys the equilibrium ; but the action of a more intense force moves the mountain of waters. The motion of the wave is deeply interesting in all its aspects. The crests of the surge rise vertically, though they are apparently progressive. It is not until the water shoals toward the beach that they acquire a progressive motion, progressive because near the shore there is not depth for the vertical movement. It requires double the generally supposed depth to form the vertical wave ; for the uplifted water falls as much below the valley of depres- sion as it rises above it. There is a descending wave, a current under water, which as a wedge forces up the suc- ceeding wave, an opposite wave under the water. Hence on the shoaling water is the undertow, a retreat of the water at a certain depth with advancing water at the sur- face. The extent of this reciprocal wave is in exact pro- portion to the extent of the visible wave. Besides, the surface of the atmosphere is also to a degree in oscillation with the water over which it is spread. The MECHANICAL PHILOSOPHY. 95 wind conforms to the surface, it oscillates with the water ; the sails of a boat, or the lower sails of a ship, are not becalmed with a steady wind, though surrounded by a wall of water. Says an experienced navigator, " the lower sails in scudding are at times becalmed, from the rise of the stern of the ship, but never becalmed on the wind, though the waves rise higher than the sails, a fact which I have often tried to account for." For this reason, the undulating motion of the wind over the undulating surface of the sea, is it that the wind off shore, not having acquired the cor- responding undulation, however strong it may blow, smooths the sea. A most interesting scene was described by a friend, who stood on a small rocky island in the midst of the ocean, looking with intense delight on the forces of nature as displayed in a storm. The mountain waves were dark, almost black, the intensity of their gloom being heightened by the circle of white foam which surged upon the rocks. A sudden veering of the wind, this wind being without the conforming undulation, prostrated the billows as it were at once ; the ocean became as smooth as in a summer's breeze. There was no surge on the rock ; but the surface of the sea was white with foam and curling in wreaths of vapor as far as the eye could reach. Gradually, however, the new wind acquired the sympathetic undulating move- ment, the waves again began to rise, and soon the surf dashed with its former fury against the island. Only because the rise and fall of the wave are from the reception and transfer of force, the mean level of the ocean ever remaining the same, could this result have been produced. If there had been " accumulation of mo- mentum to an enormous degree," > if the attracting earth 96 OUTLINES OF A SYSTEM OF had drawn down the depressed waters with more strength than the elevated waters, the ocean could never have been thus smoothed into the quiet of one level ; the new wind would have increased the surging waves, so that they would have lifted their crests still higher in confused and broken masses, resulting in a conflict of motion which the strength of no vessel that ever floated could withstand. There is something fascinating in the contemplation of the intensity of the force of the elements so perfectly under the control of law, as is witnessed on the barren rocks in the midst of the ocean's storm. Before passing to other instances of oscillatory move- ment, we will notice some analogous phenomena. The whirl- pool and the whirlwind are illustrative of the action of force. We will copy first a description of these phenomena which contains their usual explanation. " When gusts of wind come from different quarters, and meet in a certain place, there the air acquires a circular, or rotatory, or screw-like motion, either ascending or descending, as it were, around an axis ; and this axis is sometimes stationary, and at other times moves in a particular direction. This phenomenon, which is called a whirlwind, gives a whirling motion to dust, sand, water, a part of a cloud, and sometimes to bodies of great weight and bulk, carrying them upwards and down- wards, and at last scattering them in every direction. The water-spout is formed by the centrifugal force of the wind, creating a vacuum in the centre through which the water ascends." These are the common ideas ; for circular motion is usually considered as the result of conflicting forces. The action of two currents of water, in the formation of the whirlpool, and of two winds in the formation of the whirlwind, is precisely the same. The onward motion of the MECHANICAL PHILOSOPHY. 97 particles of water or air is arrested by the impingement of the two currents, but the force which impelled them is not annihilated ; the onward motion only is ended, and the force from its nature must produce motion. The circular is the only open range of action ; for no separate particle of either stream can be accelerated in the stream by a sudden impulse. Therefore, the arrested water or air moves in a vortex until its force is gradually imparted to the current in which it floats. In the water-spout a part of the force of the revolving wind is conveyed to the water ; the water, having force for rotation at the higher level thus communicated to it, rises. The water on which the whirlwind rests becomes violently agitated with the additional force received, and is elevated as foam, vapor, and water and air mingled together. Of one an observer said, " the water at the base seemed to boil and go up in detached masses mingled with the air." The raising of heavy bodies on the land and of the water of the sea by whirlwinds, in fact, the elevation of matter gen- erally, is ever on the condition that the due degree of rota- tive force is supplied. It may be supplied from below, as in the act of pushing up ; it may be supplied from above in the act of drawing up. All the phenomena of change of level are explained on this principle ; the falling body imparts its no longer needed force, the rising body demands an increased supply. This idea is finely illustrated in the fall of water from a great height into a basin of stone, as in the "Pool" at the White Mountains. The water received in the basin de- scends from a great elevation ; it has great spare force of rotation, which force, not transferred to the rock on which it falls, impels the water in a vertical movement, and thus 9 98 OUTLINES OF A SYSTEM OF forms for itself a circular receptacle. If the water had barely flowed into this receptacle without force, or from a moderate elevation, the issuing water would have used this force, a current between the inlet and outlet would have been established, and no vertical movement been induced. Water arrested between two currents makes the whirl- pool. Arrested water from a great fall only, can make a permanent whirlpool, which will scoop out for itself the vortex mould from the solid rock. A fact which has strayed somewhat from all theories, and which the books on Hydrodynamics that we have examined do not even notice, a trivial fact, coming under our daily observation, is fully illustrative of the principle ; we refer to the vortex in the body of a tunnel full of water, which is formed on the issue of the water from the pipe below. Fill a tunnel with water ; when it is stationary allow it to flow out from the pipe ; the water in the tunnel immediately assumes a vortical movement, and whirls faster and faster as it descends. We have inquired of many who were well read in the usual explanations of philosophy, and their answer has been that the cause of this vortex is the conflict of two forces. How is this ? By theory, there is only one force present, the force of gravitation, the downward drawing force of the attraction of the earth. One suggested that the vortex was formed by reason of the conical shape of the tunnel ; that he was wrong is evident from the fact, that a tunnel of any form gives the same result. The explanation of the fact is very simple on the principle which we present. The water issuing from the tube uses, in its downward motion, all the spare force of its own descent to a lower level. But the water remaining in the MECHANICAL PHILOSOPHY. tunnel has also descended to a lower level of rotation. It has therefore spare force, and this force has no other range than to confer circular motion to the water. The water therefore revolves. Thus is it, that facts, common, trivial facts, declare the general law. We return from this digression to oscillatory movements, and affirm that the surface or crust of the globe, as it has been called, has undulatory motion. We think that we shall be able, as we proceed, to establish the fact, that the barometer indicates, not the density of the atmosphere and consequently the level of rotation, but that it indicates this level positively and directly. For the present, however, take the barometer as it is commonly understood, as indicating by the oscillations of the mercury the density of the atmosphere. There are oscillations of the mercury entirely unac- counted for by this theory. At the same apparent level the barometer has a range of about three inches. This well known fact cannot be explained by any supposed varia- tion in the density of the incumbent atmosphere. Philosophy acknowledges her ignorance of the cause of these changes. The dryness or the humidity of the air will not account for them ; this is admitted. Winds cannot give the reason ; for it would require the passage of a current of air two thousand eight hundred and eighty miles, at the rate of sixty miles an hour, to account for a variation of one half inch of the mercury. Besides, these changes often precede the change in the atmosphere ; they may take place when there is a dead calm, or during the blowing of a steady gale, thus foretelling atmospheric changes rather than being produced by them. Do not these facts indicate that the same cause which changes the level of the barometer pro- 100 OUTLINES OF A SYSTEM OF duces the change in the atmosphere, not that the atmos- pheric change affects the barometer ? These oscillations of the mercury are not without cause, and there is one cause to which we would assign them, the rise and depression of the earth's surface on which the barometer stands. We believe that the earth is to a degree elastic, yielding ; that it is susceptible of undulatory move- ment, periodic, or occasional, so extensive in range, yet so slight in amount as to produce no convulsion, no apparent change ; yet to be traced by the oscillations of the barom- eter, and by the winds and storms which indicate a new distribution of the force of rotation. A scientific writer says, that the surface of the globe is no more stable or firm comparatively than is a heap of saw- dust which is floating on the surface of the water. This is a strong metaphor, but he drew his inference from a suppo- sition which we are far from believing, from hidden fires shut up in the bosom of the earth. For, as he says, if in the same proportion the heat continues into the interior of the earth, which is evidenced by the fact of its increase so far as we have penetrated, at one hundred miles from the surface it would be greater than any artificial heat ever produced. The most refractory substances would be reduced to a fluid state ; therefore, the solid crust is of small com- parative depth, and the internal fires by their intensity may well be supposed to give motion to it. But there are many well known facts which prove that there are fluctuations of the surface of the globe. An ele- vation of the coast of Chili of eighty-five feet has been proved by geologists, and a recent elevation of four feet, extending along a thousand miles of the South American coast, was produced in a single night. Earthquakes have been felt MECHANICAL PHILOSOPHY. 101 throughout an entire hemisphere. During the great earth- quake near Lisbon, the waters rose with the upheaving earth one hundred feet, and the motion was propagated across the Atlantic Ocean, vessels feeling the surge according to their distance from the centre of motion. We would also refer to the " periodic although irregularly alter- nating rise and fall of the waters of the Caspian sea," and to the fact that harbors in the Mediterranean sea have been suddenly left dry for many hours. It is stated by an emi- nent geologist, that the strata of the earth, her ridges, her mountains and valleys take the general form that would be induced by continuous undulations ; and geologists generally assert the same fact, referring it to various causes. If there be changes which result in convulsion, and which thus leave a permanent record, why may there not be gentler changes, fluctuations unattended with severe catastrophes or abiding results ? We have the authority of Humboldt for the assertion, that without earthquakes the surface of the earth is capable- of gentle and progressive oscillations; and he also remarks that " the opinion so implicitly entertained regarding the force of gravity at any given point of the earth's surface, has in some degree been controverted by the gradual rise of large portions of the earth's surface." The sudden changes of level in the waters of our great lakes have long excited attention, and have never been sat- isfactorily accounted for. We copy from the Annual of Scientific Discovery a condensed account of the facts so far as they are known, and the hypotheses which are offered for their solution. " The results of recent observations prove that these waters do not rise and fall at stated periods, cor- responding to the ebb and flow of the tide, but are subject to extraordinary risings, which are independent of the 9* 102 OUTLINES OF A SYSTEM OF influence of the -sun and moon. These risings attracted the attention of the earliest voyageurs in these regions. Char- levoix, who traversed the lakes nearly a century ago, says in reference to Lake Ontario : ' I observed that in this lake there is a sort of reflux and flux, almost instantaneous ; the rocks near the banks being covered with water and un- covered again several times in the space of a quarter of an hour, even if the surface of the lake was very calm, with scarce a breath of air. After reflecting for some time on this appearance, I imagined it was owing to springs at the bottom of the lake, and to the shock of their currents with those of the rivers which fall into them from all sides, and thus produce those intermitting motions.' The same move- ments were noticed by Mackenzie, in 1787 ; by an expedi- tion under Colonel Bradstreet, in 1764 ; on Lake Erie, in 1823 ; and at various later periods. In the summer of 1834, an extraordinary retrocession of the waters of Lake Superior took place at the outlet of Sault Sainte Marie. The river at this place is nearly a mile wide, and in the dis- tance of a mile falls 18.5 feet. The phenomena occurred about noon. The day was calm, but cloudy. The water retired suddenly, leaving the bed of the river bare, except for a distance of thirty rods, and it remained so nearly an hour. Persons went out and caught fish in pools formed in the depressions of the rocks. The return of the waters is represented as having been very grand. They came down like an immense surge. In the summer of 1847, on one occasion the waters rose and fell at intervals of about fifteen minutes, during an entire afternoon. The variation was from ten to twenty inches, the day being calm and clear ; but the barometer was falling. Before the. expiration of forty-eight hours a violent gale set in. At Copper Harbor, MECHANICAL PHILOSOPHY. 103 the ebb and flow of the water through narrow inlets and estuaries have been repeatedly noticed when there was not a breath of wind on the lake. Similar phenomena occur on several of the Swiss lakes. Professor Mather, who observed the barometer at Copper Harbor during one of these fluctua- tions, remarks : c As a general thing, fluctuations in the barometer accompanied fluctuations in the level of the water ; but sometimes the water-level varied rapidly in the harbor, while no such variations occurred in the barometer at the place of observation.' " As a general rule, these variations in the water-level indicate the approach of a storm, or a disturbed state of the atmosphere. We are therefore led to infer that these phe- nomena result, not from the prevalence of the winds acting on the water, accumulating it at one point and depressing it at others, but from sudden and local changes in the pres- sure of the atmosphere giving rise to a series of barometric waves." How could there be these " sudden and local changes" in the pressure of the atmosphere, with a calm day, and of course an equable temperature ? Or how could they exist at all in a fluid so elastic as the air, the very nature of elasticity being such as to correct at once any difference of density in the same volume ? Our views lead us to regard these changes in the level of the water as indicative of changes of the level of those portions of the earth on which the water rests. And as a proof that vibration of the earth's surface does occasion barometrical change, we need only refer to the well-known fact that at the time of the great Lisbon earthquake, the mercury fell so far in the barometer even in Great Britain, " as to disappear from that portion of the top usually left uncovered for examination." Hum- 104 OUTLINES OF A SYSTEM OF boldt also remarks that " the connection between the erup- tion of a small volcano with the state of the barometer is generally recognized, although our present knowledge of volcanic phenomena, and the slight changes of atmospheric pressure accompanying our winds, do not enable us to offer any satisfactory explanation of the fact." But we need not accumulate facts. Science generally indicates a change of level of different portions of the crust of this globe, taking place either periodically, or as it were incidentally. Nor are we limited to science for our proofs of mutation. Science may point to the barometer as indica- tive of these changes ; she may show the earthquake and the storm ; she may declare, from the upraised strata, from the mountain ridges, from the depressed valleys, from the confused commingling of the primitive, the transition, and the recent formation, that the earth is not an unyielding mass, bound together by a law which gives increased density according to the approach to its centre. The world, now permanent as the home of man, has passed through at least one great and sudden change. The upturned strata, the drift from the poles so enormous in quantity, that were it again collected and restored it would change the form of the earth, abundantly prove this. We know that this great change has been accounted for by natural causes, by the accumulation of the present changes in foregone times, by the condensation, as it were, of present events in the lapse of past ages, by the volcano, the earthquake, the storm, the drift of rivers, the gradual deposit of floods ; glaciers have been launched, and ice- bergs freighted with diluvium and boulders. We are not pre- pared to seek a solution of the great changes of the earth from natural causes, from the intensification of the present MECHANICAL PHILOSOPHY. 105 action of force, condensed to stronger action in the youth of the world. There has been one change at least, which came not from a natural cause, from the e very-day phenomena of nature. We refer to the time when the earth was without form and void, and darkness was on the face of the deep, when the spirit of God moved on the face of the water, and it was said, Let there be light, and the rays of the sun created " in the beginning" for the first time penetrated the mist that went up from the surface of the earth ; when " the firmaments rose " and " divided the waters from the waters." How great the change which thus converted a chaotic world into a bright and beautiful home for man ! The intensity of the force is written down on the broken strata, the torn and ragged mountain ridges, and in the smoothing and furrowing of the stubborn rocks. The form of the earth was changed, and with this change came necessarily a change of its rotation, and it may be of the form of its orbit ; for a change in one condition of a sphere, must change its every phase. And that this change did take place proves that there can be no reference to any supposed centre as the radiating point of its motive force ; for the globe is self-poised, asking of no other leave to be, borrowing of no other the power to move, connected, as a part of a system of worlds, yet speeding on in a path of her own in perfect balance, in ac- curate equilibrium, as if buoyed up by the right arm of God. As there is a perfect equipoise in the earth as a sphere, as a whole, so is there the same perfect equipoise in her parts, in her elements, in her constituting masses. From this perfect equipoise come the slight aberrations and per- turbations, the oscillations of the surface. As the pendulum swings on the condition of equilibrium ever preserving one 106 OUTLINES OF A SYSTEM OF mean level, so may the surface vibrate of the even-balanced earth. Therefore is there freedom, ease, elasticity of mo- tion, nothing stationary, yet nothing wandering to an extent that can mar the designs of creative wisdom ; all things flowing gently as if without rule, yet bound together by laws as sure and as unchangeable as is the power of Him who formed the earth in the beginning, as the home of his children, whose security and happiness were the objects of creative skill. An idea given in a sermon by the Rev. A. P. Peabody has fastened itself in our thoughts ; we quote from memory : " In the Ptolemaic system, this earth was considered as the centre of the system to which all the wandering hosts of heaven were tributary, aids, accompanying circumstances. The better lights of astronomy dispelled this error, and the earth is looked upon now as a part, a minute part of a uni- verse without a conceivable limit. But the earth from this is not degraded, but exalted, not decreased, but increased in interest. The part of such a whole far transcends in sublimity the centre of a system so narrow that all refers to its own limited bounds." The idea extended to man imparts to the individual a dignity proportional to the extent of the universe of which he is a participant, -- little in himself, yet how great considered as an intregral part of the whole crea- tion ! And this intimate connection, too, not merely apper* tains to his physical nature, but he has yet greater dignity of position from the view that, connected as he is with God's material universe, there is also for him a connection with the Sustaining Spirit, the Life of the Universe, that indeed he is the child of God, We return from this " oscillation " of thought, In a MECHANICAL PHILOSOPHY. 10T still night, at a hotel of great extent, built of massive granite, a vibratory motion was distinctly perceptible. This great stone building, the adjacent buildings of brick, and the intervening ground to a great extent were perceptibly moved by the passing of a carriage over the paved street. Did the muscular force of the horse thus produce motion of the enormous mass of stone, brick, earth, and the solid ledge ? The impulse only was given, and this impulse, slight as it was, so nicely adjusted is the balance of force, resulted in oscillation. The vibration called forth by the motion of the carriage, was the bringing into action the weight of the mass, the transfer and retransfer of the force of rotation as the oscillating matter rose and sunk in level. Had gravitation bound down the enormous mass, drawn it with the force of thousands of thousands tons, it would have stood firm and unyielding. How much safer for a ship to float on the free moving water, than to re- ceive the shock of the storm when stranded on the solid rock ! As we write, we raise our eyes to a range of lofty moun- tains, the top of one of which rises some four thousand feet, with a summit of bald rock, the granite reaching from this height to the broad base, and extending for many long miles below, ledge upon ledge, stratum upon stratum, all bound together by the circulation of force through every particle, fragment, mass. But there is no weight. The granite crystals touch each other no more closely at the lowest base than at the summit, nor press more heavily on each other. There is no weight, except on the condition that the mountain descends to a level of rotation. It is self-poised, as is the whole earth. Practical men, who know only what they have seen, and 108 OUTLINES OP A SYSTEM OF believe in what takes place, without being troubled by theory, work on the faith that there is no force of gravita- tion in the mass which preserves one line of rotation. In taking away 'the foundation of a brick wall which had been undermined, to rebuild it, the owner expressed his fears that too much had been removed of the support at once, and that the building would fall. The reply of the mechanic was, " I used to fear, but now I know that it is safe until it begins to move, and I shall work without any jar ; if it should begin to move, twice the present support would not keep it up." In taking away the support of the arch of a stone bridge, after the keystone was put in, a slight, sudden sag of the bridge crushed the keystone, a stone, the cohesion of which, if standing firm at one level, would have borne all the granite that could have been piled miles high upon it. This principle is evidenced by the superior security of the arch for bridges and similar structures. In the arch, there can be no descent without crushing the material of which it is formed. Thus too has the passing of a body of troops over a bridge, with measured step by beat of drum, often given the vibration which calls into action the weight or force of descent. In the Britannia tubular iron bridge of immense weight, some of the spans of which are four hundred and seventy-two feet in length, care has been taken to secure the bridge against vibration ; the upper portions of the tube are made thicker, operating as an arch, the particles of which are compressed by any descent. Heavy as it is, it will undoubtedly stand if it has no vibration to call forth the force of descent. The moon floating around the earth will not fall because she possesses force for rotation, in proportion to her distance MECHANICAL PHILOSOPHY. 109 from the earth. So the crust of the earth cannot fall, as it ever has the due force for rotation ; there may be oscilla- tion in the orbit of the moon, the mean distance being pre- served ; there may be a movement of the earth's surface, but it is an oscillatory movement ; there is both the rise and the fall, one mean of rotation being preserved. Masses and frag- ments of the earth fall, when unsupported they take a lower level of rotation, and as they fall yield up to other bodies the force of their former superior level. Hence every movement is oscillatory, the transfer of force, the force remaining of fixed quantity in all its transfers, preserving the perfect equilibrium of creation. After the assertion of the law of falling bodies by Galileo, there was found a great difficulty in applying it to the commencement of the motion ; for this beginning of motion clearly shows that they do not fall by attraction. Great disputes took place in regard to the velocity with which bodies begin to fall. It led to the consideration of the infinite divisibility of space ; for the motion at its commencement is so slight that the body hardly appears to move, or, as it has been expressed, " when a body begins to fall from rest, it begins to fall with no velocity. In one thousandth part of a second it has only acquired one thousandth part of the velocity which it has at the end of one second." If gravi- tation act with its supposed force upon a body at rest, how great would be its instantaneous velocity when the support was taken away ! Its fall would be as sudden as the recoil of a bent spring. Nor could it be understood why bodies which had fallen by the force of gravity should be able to rise again to the same level against the force 'of gravity ; or why on the inclined plane the velocity of a body should be measured by 10 110 OUTLINES OF A SYSTEM OP the vertical height from which it falls ; nor why the fall should be with uniformly accelerated velocity. Even Gal- ileo, vigorous as were his powers of thought, could not mas- ter the subject. And the obscurity has continued to this day. The theory of gravitation acknowledges a difference be- tween the weight of a body, that is, its tendency to fall, and the force of the fall, weight being an invariable quality, while the force of descent is in proportion to the time of the fall. We rega'rd the cause of the fall, and the force given out by the fall as essentially different, and we hope that we shall be able, in the process of this inquiry, to explain the cause as well as the results. But whatever it may be, the stone unsupported will not remain at rest. We have just read in an account of a recent ascent of Mont Blanc, that " spots have to be passed where no word can be spoken lest thou- sands of tons of snow should be set in motion ; " for it has been known, that the mere vibration of the air, caused by the human voice, has brought down the avalanche. The intensity of molecular action, the pulse of nature, the very throb of force, the vibration and oscillation of all things would account for the fact that the suspended body has motion, has the beginning of its downward course. The impulse given, the most minute line of descent induced, there is the spare force of rotation, there is force for the motion of the mass in a new direction. It has commenced its fall, it has unused force. It cannot rotate more rapidly at the lower level ; for it is a part of a current of matter passing round the earth in an equable stream. * Downward, then, it must take its way. Its very appearance in the act of falling indicates the law of its motion. It is not at- tracted ; for it does not rush at once to the earth, as do the MECHANICAL PHILOSOPHY. Ill particles of steel to the magnet ; but, for an instant, as if in suspense, like " A long-swept wave about to break, It on the curl hangs pausing ; " then, gathering force for its downward career, it falls ; " Still gathering force it smokes, and urged amain, Whirls, leaps, and thunders down, impetuous to the plain." The force obtained by the change of the level of the falling mass, of water for instance, cannot come from the at- tracting earth ; for the attractive force is force to draw the mass toward her centre, and having acted according to this, the essential principle of attraction, it would cease to act, or merely hold the water at its new level. But the force of the fall of bodies remains ; it is a living principle. It was in them at their higher level, there acting in rotation. If water falls, it transfers this force to other bodies, inducing motion in them. If not imparted, it is sufficient in intensity to raise the water again to its former level. It is not a mere gravitating, or downward force, but force giving motion irrespective of direction. Thus, the fall of water over an artificial dam is not from the downward attraction of the earth. That force can only exert its essential property of bringing the particles of mat- ter nearer to each other. In doing this, it has discharged its only conceivable function. But the particles of water by the act of descent impart the spare force of their lower level of rotation; and this force, diverted from the majestic stream of rotative power, can have given to it by mechanical appliances the line of direction which crushes the grain, or on the revolving spindle twirls the fibre of cotton, the mechanic using the force of nature for the comforts and 112 luxuries of life. Thus is imparted to the practical mechanic a dignity arising from his position. He is not a mere cun- ning workman in wood and brass ; but he bears in his hand the sceptre of power over nature, he controls her ener- gies, he borrows her force, from water, wind, and steam, and through the lever and the wheel, he directs the action of this force for the well-being of man. When engaged in the examination of facts, the thoughts will oscillate from them to abstract principles, from material things to that which they represent. Does not this law of the mind prove that the connection of the intel- lect with material objects is not its only tie to the universe ? We have considered the artisan as borrowing the power of nature for his purposes, considered him as not confined to that degree of strength only which flows through his own frame ; he goes out of himself to the great fountains of energy for his purposes. So, he who would comprehend the things around him, he who is the artisan in philosophy, is he confined to his own feeble strength, limited to his own power of thought ? Is there not a communion between him and truth more direct than comes from the contemplation of external objects merely ? Is he never allowed to borrow wisdom from the Fountain of Wisdom ? " Now all the knowledge and wisdom that is in creatures, whether angels or men, is nothing else but a participation of that one eternal, immutable, and uncreated wisdom of God, or several signatures of that one archetypal seal, or like so many multiplied reflections of one and the same face, made in several glasses, whereof some are clearer, some obscurer, some standing nearer, some further off." CHAPTER VI. " SURELY IT IS A WORK WELL DESERVING OUR PAINS, TO MAKE A STRICT INQUIRY CONCERNING THE FIRST PRINCIPLES OF HUMAN KNOWLEDGE, TO SIFT AND EXAMINE THEM ON ALL SIDES ; ESPECIALLY SINCE THERE MAY BE SOME GROUNDS TO SUSPECT, THAT THESE LETS AND DIFFI- CULTIES, WHICH STAY AND EMBARRASS THE MIND IN ITS SEARCH AFTER TRUTH, DO NOT SPRING FROM ANY DARKNESS AND INTRICACY IN THE OBJECTS, OR NATURAL DEFECT IN THE UNDERSTANDING, SO MUCH AS FROM FALSE PRINCIPLES WHICH HAVE BEEN INSISTED ON, AND MIGHT HAVE BEEN AVOIDED. " HOW DIFFICULT AND DISCOURAGING SOEVER THIS STEP MAY SEEM, WHEN I CONSIDER HOW MANY GREAT AND EXTRAORDINARY MEN HAVE GONE BEFORE ME IN THE SAME DESIGN, YET I AM NOT WITHOUT SOME HOPES, UPON THE CONSIDERATION THAT THE LARGEST VIEWS ARE NOT ALWAYS THE CLEAREST, AND THAT HE WHO IS SHORT-SIGHTED WILL BE OBLIGED TO DRAW THE OBJECT NEARER, AND MAY PERHAPS, BY A CLOSE AND NARROW SURVEY, DISCERN THAT WHICH HAD ESCAPED FAR BETTER EYES." Bishop Berkeley. THERE are, unquestionably, two different casts of mind, one giving greater, the other less attention to facts ; the one the more rigid and exact in observation, the other the more prone to speculation. Hence the perpetual con- flict between what are called the practical and the theoret- ical. But the dispute concerning the values of the two methods in philosophy is in words merely. The man who only knows facts, and the man who, ignorant of the doings of nature, dreams rather than judges, are both unfit for philosophy. Theories unsupported by facts are worthless, and an accumulation of facts without reference to the laws of their combination is also worthless. 10* 114 OUTLINES OF A SYSTEM OF But every man is in some degree a theorist, and he is a theorist because he is a man. The animal alone rests contented with the facts presented to the senses. In proportion to the strength of a mind is its tendency to go beneath the surface of things, to be dissatisfied with- out hypothesis to connect the facts that are observed, and therefore to seek some principle of unity. Thus every philosopher is necessarily a theorist. Even Bacon, the father of the Inductive Method, was a theorist, and at times a wild and fanciful theorist. " Some noises," says he, " help sleep, as the blowing of the wind and the trickling of the water ; they move a gentle attention, and whatever moveth attention without too much labor, stilleth the natural and discursive motion of the spirits." " What indeed," asks a profound and accurate thinker, " are Newton's Que- ries but so many hypotheses which are proposed to philoso- phers as subjects of examination ? " " And," he continues, " did not even the great doctrine of gravitation take its first rise from a fortunate conjecture ? " It is remarked by Sir David Brewster that " the influ- ence of the imagination as an instrument of research has been much overlooked by those who have ventured to give laws to philosophy. This faculty is of the greatest value in physical inquiries ; if we use it as a guide and confide in its indications, it will infallibly deceive us ; but if we employ it as an auxiliary, it will afford us the most invaluable aid." After an hypothesis has been suggested by the imagination, it should become the subject of rigorous examination, and be retained or discharged, as it may or may not give the desired explanation ; for the proof of the truth of a theory is its har- mony with facts. True philosophy, therefore, uses both reason and observation in making progress. MECHANICAL PHILOSOPHY. 115 And while philosophy demands that no theory shall be admitted as proved any further than it is supported by facts, and that science should be guarded from wayward fancies and day-dreams, equal care should be taken to reexamine the theories that are current, so that the errors that must necessarily be handed down in the regular transmission of science, from the education of one generation by the pre- ceding, may be expelled. There is far less danger that new errors be received than that old ones be suffered to re- main ; for against new theories the educated contend most strenuously, if they conflict with a system to the full com- prehension of which a lifetime has been devoted. Errors once established therefore become permanent ; they are incorporated into a system. Common sense, which might detect them, defers to the authority of science, and science to the wisdom of former times. However, all things on the whole are wisely determined so that progress shall be made, though it be by a succession of waves surging at long inter- vals, rather than by the steady advance of the tide. But we have been drawn from our path. We return to the exam- ination of the theories relating to the differing densities of the atmosphere, as indicated by the rise and fall of the mercury in the barometer. It is generally supposed that the atmosphere increases in density from its upper surface to its line of contact with the globe. In the language of Sir John Herschell, " when we have ascended to the height of one thousand feet, we have have left below us about one-thirtieth of the atmosphere ; at ten thousand six hundred feet of elevation, rather less than that of JEtna, we have ascended through about one third ; at eighteen thousand feet, which is nearly that of Cotopaxi, through one half of the material, or at least of the pondera- 116 OUTLINES OF A SYSTEM OF ble body of air incumbent on the earth's surface." This lessening density as we go up from the surface, is supposed to be proved by the depression of the mercury in the barometrical tube. Before the experiments of Torricelli, the ascent and sup- port of fluids by a vacuum were accounted for by the abhor- rence of nature for a vacuum. When it was discovered that this "abhorrence" was limited for water to about thirty-three feet, for mercury to about thirty inches, and for other fluids in proportion to their density, some new theory became necessary, and the weight or pressure of the atmosphere was substituted. Galileo, Torricelli, Pascal, seem jointly to have formed the new theory, and Pascal fully established it by experiments, which gave the fact that at different altitudes the level of the mercury varied, that it rose higher in the vacuum as the level of the instrument decreased, and that it fell as the barometer was elevated. Thus the "fuga vacui" being abandoned, the support of the fluid being attributed to the pressure of the atmosphere, and the degree of support being found to lessen upon ascent, the hypothesis that the weight or pressure of the atmosphere decreases according to elevation was established, and re- mains unquestioned to this day. This theory, however, though it has been useful for many practical purposes, does not give a complete explanation of the facts connected with the barometer. How is the air supposed to be packed according to baro- metrical indications ? We will quote from one who very distinctly gives the commonly received opinions. " The first stratum of air gravitates with its own share of the earth's attraction, the second with its own share, and with the weight of the stratum over it, and so on ; the lower MECHANICAL PHILOSOPHY. 117 stratum bearing in addition to its own weight all the weight of the air over it." The atmosphere has also been com- pared to a series of fleeces of wool, the lower the most compressed. Gravitation of the atmosphere, if the air be attracted at all, would appear at first sight as if threads were attached to each particle, drawing every one with equal tension. No particle could rise relatively to another particle, if all were drawn down with equal force. The particle going down must be more strongly drawn, the particle going up must be drawn with less comparative force. With equal attract- ion there could be no relative change of place. The only difference in weight of the different strata would arise from the increase or diminution of the force of attraction, accord- ing to the distance of each stratum from the centre of attraction. If this force acted on the whole atmosphere as one volume, the whole volume would be of as uniform den- sity as a mass of granite. If the force of attraction operated on each particle according to its distance from the centre of attraction, the difference in the weight qf different strata would be far less, than that apparently indicated by the barometer. Such a condensation of the atmosphere as is supposed could not result from the law of gravitation ; for that law assumes a decrease of force proportional to the square of the distance. A volume of one hundred cubic inches of air weighs but thirty-one grains, is attracted by a force the value of which is only thirty-one grains. How large must be the volume of air which weighs a ton, is attracted by a force measured by one ton ? It would cover the whole of a large and high mountain. This ton of air would weigh but one ounce less, a mile from the surface of the globe, than it 118 OUTLINES OF A SYSTEM OF would at its very surface. This is the only ratio in which gravitation could change the weight of the different strata of air. The earth can have no favoritism. She holds in place or draws down every particle of air equally, or, more accurately, in proportion to its distance from the centre. But, admitting that each stratum of air bears not only its own share of the earth's attraction, but also the weight of all the strata over it, still this could not condense the atmo- sphere to the degree that is supposed. No one doubts that the temperature of the atmosphere changes with its level. At the summit of a mountain, where by theory the air has lost one half of its density, the cold compared with that at the surface of the earth below is most intense. Heat, it is said, always rarefies the air, cold condenses it ; and of course there would, from this cause, be a greater density in proportion to the elevation. It is also settled, that the force of the elasticity of air increases with its density. Of course elasticity acts against the rarer strata, and this elasticity would of itself pre- serve throughout the whole atmosphere an equilibrium of density. If a quantity of air be artificially condensed, how quickly will it return to its normal state when the force which compresses it is removed ! If the air be an elastic fluid, no volume of it can exist without an equal pressure in every direction, be the volume large or small, a few cubic inches or the whole atmosphere. If any portion of it be rarefied by heat, this will give to its particles greater < c force of repulsion," so as to equalize its pressure with that of the surrounding denser air. Moreover, if gravitation could press down the different strata of the air in the ratio supposed, it could not maintain MECHANICAL PHILOSOPHY. 119 the pressure, it could not preserve this difference of den- sity. There is a perfect intermobility of the particles of fluids, and every wind that blows would tend to bring back the equilibrium. It is supposed that winds are caused by the rushing of air from the colder and more condensed portions of the atmosphere to those comparatively more rarefied. An upward current would at once be established to restore an equilibrium, to undo what gravitation had done. But the law by which the atmosphere is packed ac- cording to barometrical indications, is not the law which regulates the gravitation of fluids. It is a law which acts in this case only. The law, by which one stratum of the atmosphere bears not only its own weight, but that of all the strata over it, is assumed for special purposes. Having dis- charged its function, it is, ever after, a dead letter. We hear no more of this vertical gravitation, no more of the bearing down of one stratum upon another. Fluids press equally in all directions. This is acknowledged as a general law. The very action of the atmosphere on the barometer must ofcen be by an upward gravitating power, pressing against the leather at the bottom of the cistern containing the mercury. The acknowledged principle that the pressure of fluids is equal in all directions, " upwards, downwards, and side- ways," would prevent such a compression of the atmosphere as the barometer is supposed to indicate. If a cubic foot of air presses equally by its six sides, it presses the cubic foot above it with the same force as the cubic foot below it. In no way whatever can it be shown, without contradicting all the present theories, that there is a difference of density among the different strata of air. If this difference actually exists, we must give up gravitation with force according to dis- 120 OUTLINES OF A SYSTEM OF tance, the action of heat in the rarefaction of the air, the elasticity of air in proportion to its density , the diffusiveness of air, the intermobility of the particles of air, and the prin- ciple that the pressure of fluids is equal in every direction. But in fact the varying density of the air has no proof whatever. It may be, or may not be. If it be, it is caused by a principle not embraced in any of the present theories, and it cannot be proved from the range of the mercurial column. We wish to express this idea distinctly. If the air be more dense at the surface of the earth than a mile above it, the increase of density does not arise from gravitation ; and, if there is a difference of density at differ- ent levels, the barometer cannot indicate it. We referred, in the preceding chapter, to the oscillations of the mercury at one supposed level ; we have occasion to use again the same facts, and to add to them others of the same character. These oscillations, of which the range is about three inches, while the barometer remains at the same place on the earth's surface, are not accounted for by the present philosophy. Scientific men confess their inability to explain them. Professor Daniell says, " The cause of these oscilla- tions has long been the subject of investigation with philos- ophers, and the problem in all its generalities is difficult and complicated." " The difficulty," says an article in the London Encyclopedia, " consists in explaining why these oscillations are greater in high latitudes than between the tropics, as well as why they should exceed in all cases the quantities which calculation of different densities of atmo- sphere might assign." Again : " It is hard to say what can be the cause of the changes of the height of the mercury at the same level, changes which would be equal to a change of level of two or three thousand feet." MECHANICAL PHILOSOPHY. 121 Ifc is supposed by some that different degrees of hu- midity in the atmosphere might account for these changes. Professor Leslie inclines to this belief, " because all other assigned causes are insufficient." But the barometer usually falls in a damp atmosphere, and vapor of itself has weight, nor does it necessarily rarefy air which contains it. The winds passing over the surface of the earth cannot be the cause ; for, as we have already shown, it would require a wind passing over nearly three thousand miles at the rate of sixty miles an hour, to change the height of the mercury half an inch. Attempts have also been made to trace the cause in the vacua occasioned by conflicting winds. In vain ; for winds by theory restore equilibrium, they do not create inequalities, nor could a vacuum exist for days and weeks if it could be formed. The maximum of oscillation is near the parallel of 45 latitude. The oscillations vary with the time of the year, (being greater in one month, less in another month,) and also with the hour of the day. They also vary with sudden changes of the level of the water, with the height of the tides, and with the position of the moon in relation to the earth. All these periodic and other changes cannot be traced to the state of the atmosphere as the cause. There- fore, if the barometer indicates varying density of the atmos- phere, it also indicates some other fact, the oscillations have some other cause. If it do not indicate the density of the air in one position on the earth, it may not in any, espe- cially as the corresponding variation of density has no proof independent of the change in the mercurial column. But it may be thought that we have forgotten the fact that, " if a man ascends a high mountain, he will feel an incon- venience in his ears, and other cavities of the body from the 11 122 OUTLINES A SYSTEM OP dilatation of the enclosed air adjusting itself to the dimin- ished outside pressure." This /act, if it be true, is insuffi- cient to bear the burden of proof of the great principle under discussion. If uncomfortable bodily sensations are experi- enced, it does not follow that the reason for them is the " dilatation of the inclosed air," or the rarefaction of that outside. There may be other reasons for painful sensations on the ascent of high mountains. The effect on the animal structure of the air at great heights, we think, proves distinctly that it is not so rarefied as is supposed. The bird soars as lightly from the top of the high mountain as from the plain. The condor, the heaviest of birds, flies without effort at a height of fifteen thousand feet, though supported by air of only half the density of that below. And man, after recovering from the fatigue of ascent, is not always distressed for breath ; he does not require lungs of double capacity, nor does he breathe twice as fast to obtain his usual supply of vital air. No one could live comfortably in air of only half its usual density ; yet in the highest ascents in balloons we read that " the aeronauts suffered no inconvenience in their respir- ation or other animal functions." We shall again recur to this part of the subject. It may also be alleged that the boiling point of water varies according to elevation, because the pressure upon the surface of the water is diminished by the rarefaction of the air ; or that, as water boils in vacuo at a very low tempera- ture, so as we ascend and the air is rarefied, water boils with a less degree of heat. The reason why water boils more easily the greater its elevation, is simply its possession of a rotative force proportional to its level of rotation. Beyond a certain elevation water would at once pass into vapor. MECHANICAL PHILOSOPHY. We do not expect the minds of others, at this period of the investigation, to accept pur explanation of the vaporiza- tion of water at different levels. We will, therefore, for the present, admit that the atmosphere is more or less rare- fied according to the altitude of its strata, that the mean weight of the air, from the action of heat or other causes, varies, so as to make a column of it bear on the earth some- times with a greater, sometimes with a lesser pressure. But even if we admit the gravitation of air, and the varying weight of a given quantity of air, it does not follow that either its normal pressure or its variation of pressure is measured by the stationary or varying weight of the sus- pended column of mercury. In other words, there is no proof that the weight of the column of mercury is the measure of the weight of the air. In the first place, when the barometer is constructed, the mercury in the tube does not owe its elevation to the press- ure of the air. Let a tube closed at the top be immersed in mercury, and when filled let it be withdrawn upward by the hand ; the mercury is raised with the tube above the level of the mercury from which it is taken. The force re- quired to lift it is just the weight of the mercury and tube together. The pressure of the atmosphere on the lower surface of mercury does not in tae least degree aid in the elevation, does not diminish the weight, because the sus- taining mercury is pressed by the air, not one iota less of force is required to give the sustained mercury its eleva- tion. The fact is admitted, and is accounted for in this manner : " The force used in lifting the mercury is needed to elevate the air over the tube ; that being done by the applied force, it is the weight of the atmosphere which elevates the mercury in the tube." But this reason is 124 OUTLINES OF A SYSTEM OF given without reflection ; for the air is no heavier over the tube when the tube is filled with mercury than when it is filled with water or air, yet the force applied measures the weight of the fluid within, and the contained weight does not increase or diminish the weight of the column of air over the tube. It is certain, therefore, that when the column of mercury is lifted with the tube, it is the applied force that lifts it, and not the weight of the atmosphere bearing on the surface of the mercury from which it is withdrawn. Of course, the weight of the atmosphere, not capable in the least of aiding the process of elevation, has no efficacy in sustaining the column w r hen raised. One would almost suppose that an air-supported column of mer- cury would be like the air-supported balloon, and would not press with any weight upon the instrument. When the tube is elevated beyond what may be termed the limit of extension, the mercury is no longer lifted with it. However high the tube be drawn, the surface of the mercury in it remains at a certain distance from the surface of the lower mercury. This distance, at the mean level of the earth's surface, is about thirty inches. It varies accord- ing to altitude. In the usual process of constructing barometers, the tube is filled with mercury, and its lower end immersed in a basin of the same fluid, technically called the cistern. The mercury falls from the top of the tube to the limit of its suspension ; and as much as falls from the tube is raised in the cistern. As much mercury is elevated in the cistern as is depressed in the tube ; the descent and ascent are exactly equal. In all subsequent changes the fall of mercury is equal to the rise, particle for particle ; the flow of mercury back and forth makes the same relative change in the MECHANICAL PHILOSOPHY. 125 volumes of the tube and cistern mercury. A perfect equi- librium was at first established by the ascent of a quantity of mercury in the cistern exactly equal in amount to that which descended in the tube, and the equilibrium is ever sustained by the same process, without reference to atmo- spheric pressure. With this perfectly balanced instrument the atmosphere is supposed to be weighed. It is in one scale, but no test weight is put in the other scale. The air is weighed against nothing. All the ponderable matter hangs on one arm of an evenly balanced lever, and its weight is to be ascertained by the degree of the ascent of the other arm. Place on the outer mercury an additional pound of the fluid, the mercury in the tube will not rise so as to weigh a pound more ; add to the density of the air over the outer mercury, the rise in the tube will not correspond to the increased weight of air on or over the cistern. When we added mercury to that in the cistern, the mercury in the tube rose just enough to maintain its former distance from the lower surface. When the tube was first plunged in the cistern, it made no difference how great or how little was the quantity of mercury in the cistern ; it makes no difference afterwards whether mercury be added or taken away ; the same distance will be preserved between the two surfaces. The rise of the fluid in the tube will not, therefore, measure the weight in and on the cistern. It will be said, however, that though, when an additional pound of mercury is placed in the cistern, an equivalent pound does not rise in the tube, enough rises inside to cor- respond with the increased height outside, and therefore it weighs a column of mercury resting on the surface of the outside mercury, which is of the same area as itself, and 126 OUTLINES OF A SYSTEM OP consequently, in weighing the air over the cistern, it weighs a column of air of its own area only. This idea is a mere statement of facts. The result empirically obtained is exalted into a principle, and one which is at variance with all other principles of the action of fluids. Fill a cylinder with mercury, and from the cylin- der let a long tube ascend; subject the mercury in the cylinder to the pressure of a piston, and the rise of the mer- cury in this tube, that is, the weight of the mercury sup- ported by the pressure of the piston will be measured by the whole pressure of the piston, not by its pressure on a sur- face of mercury in the cylinder, equal merely to the area of the tube in which the mercury is supported. So if the rise and fall of the mercury in the barometer are proportional to the weight of the air, they are so to the weight of all the air over the cistern ; but, as it makes no difference in the ac- tion of the barometer whether the surface of the cistern is of two inches area, bearing a column of air of two inches area, or is an ocean of mercury, bearing the atmosphere of a hemi- sphere, we are compelled to look for some reason besides the weight of the air to account for the fact, that the two surfaces of fluid in the barometer preserve a fixed distance between them. In other words, the variation in the length of the column of mercury is not determined by a correspond- ing variation in the density of the air. In the use of mercury to indicate the pressure of steam, or of the condensed air of blowing cylinders, the extent of its rise in the indicating tube corresponds to the extent of the surface of mercury exposed to it. In a steam gauge the area of mercury exposed to the pressure of the steam bears such a proportion to the area of mercury in the indicating tube, that the usual range of force is measured by its rise and fall. MECHANICAL PHILOSOPHY. 127 Now, enlarge the surface exposed to the action of the steam, give it an area equal to the area of the piston, the gauge would burst by the increased pressure, and the mercury be thrown with violence in all directions. Take out the baro- metrical tube from its cistern, and place it in an ocean of mercury, its range would not change, the two surfaces would still remain at the same distance apart. Why does the mercury select one column of air of its own area and answer to its pressure, regardless of the pressure of a hundred other columns of the same size and weight which bear upon the cistern ? It cannot be from the uni- form bore of the tube ; for the tube may be unequal, either contracted or enlarged ; it may be a cone with its base downward, or a cone with its base upward ; the aperture or opening between the tube and cistern may be larger or smaller than the bore of the tube ; the relative quantity of the mercury in the cistern may be such, that on bringing the instrument to a lower level it will nearly all be drawn into the tube, and yet will remain suspended, so that in this case, if the mercury is sustained at all by the atmosphere, it is by a column of less area than the bore of the tube pressing on the small orifice between the tube and cistern. There is indeed nothing in the action of the barometer which proves that the mercury in the tube is sustained by a column of air of its own area. Further ; if it were possible that the sustained mercury under any circumstances could select a column of air of its own area, out of a volume of air pressing by elasticity in every direction, and disregard the pressure, weight and elasticity of other columns which act on the surface of the cistern, yet it would be impossible as the barometer is usually con- structed. The cistern is closed at top ; its bottom is a piece 128 OUTLINES OF A SYSTEM OF of leather ; the instrument is inclosed in a wooden case and suspended perhaps in a close room. It then receives the pressure or weight of its selected column of air forty-five miles high, one quarter of an inch in diameter, which may be twisted and beat about by the winds of heaven, and reaches the instrument through doors or windows, passing through the air in the room, which is subject to expansion and condensation by artificial changes of heat. Yet, not affected by these changes, it penetrates through the openings of the wooden case, acts on the bottom of the leathern support, and still gives exactly the degree of pressure belonging to its area, to the mercury in the tube through an aperture of any size ! Is it possible that any thing can be measured by such an instrument, except, perhaps, the elasticity of the air in the apartment in which it stands, which would affect the whole extent of the surface of the mercury on which it acts? But if this last and only possible action of the air by its elasticity be the cause of the oscillation, why is it that two upper surfaces of mercury, one in the cistern and one in the tube, are an essential condition of the oscillation ? A tube in a conoidal form with a piece of leather over its base, would as well indicate the pressure of the atmosphere. The leather would act as well thus placed. It would have the same elasticity. The air pressing on it would act as truly without an upper surface of mercury as with it. The fact that two upper surfaces of the fluid are necessary, abun- dantly proves that another cause for the action of the barometer is yet to be discovered. In our examination of the action of the pump and of the syphon, we hope to throw more light on the subject of the elevation and support of fluids by means of a vacuum. MECHANICAL PHILOSOPHY. 129 Surely enough has been already said to throw a strong sus- picion over the theory which explains barometric action by atmospheric pressure. Indeed, the explanation has often been received with some distrust. A friend, whose strength of mind was never questioned, said, " I have believed the explanation, relying on the authority which gives it, rather than because it satisfies my mind ; there is something about the action of the barometer which is not yet understood." If both the construction of the barometer and the quali- ties of the atmosphere are such as to throw great doubts over the supposed action of the weight of the air on the mercury, how much are these doubts increased when it is known that the mercury changes its level in the tube, under circumstances which forbid the idea that there have been equivalent changes in the density of the air ? To place this matter in a strong light, we will give the following state- ment from Humboldt's Cosmos : " The horary oscilla- tions of the barometer between the tropics present two maxima, namely, at 9 or 9 A. M., and 10J or lOf P. M. ; and two minima, at 4 or 4|, P. M., and 4 A. M., occurring, therefore, in almost the hottest and coldest hours. Their regularity is so great that, in the daytime especially, the hour may be ascertained from the height of the mercurial column without an error, on the average, of more than fif- teen or seventeen minutes. In the torrid zones of the New Continent, on the coasts, as well as at elevations of nearly thirteen thousand feet above the level of the sea, where the mean temperature falls to 44 6', I have found the regular- ity of the ebb and flow of the aerial ocean undisturbed by storms, hurricanes, rain, and earthquakes." Can we receive the idea conveyed in the latter clause of this quotation ? If there is an ebb and flow of the aerial 130 OUTLINES OF A SYSTEM OP ocean, is it possible that its regularity should remain undis- turbed by storms and hurricanes ? If the oscillations of the barometer day after day, month after month, are as regular and uniform as the beating of the pendulum of the clock, these changes come not from the capricious, fitful alterations of the state of the air. The action of the most unrestrained element in nature gives not results the most exact and most regularly continued. If, as Humboldt expressly states, the horary oscillations of the barometer are not affected by changes of atmospheric tem- perature, neither by heat nor by cold, by snow nor by rain, by storm nor by calm, by the peace of nature nor by the throe of the elements, if the changes go on regularly and periodically on the plains and on the tops of high mountains, surely it is vain to seek in the variations of atmospheric pressure the cause of these oscillations. Geologists have often noticed that the changes of the level of different portions of the earth are complementary. There is a rise in one place corresponding to the fall in another place ; for instance, an elevation taking place in Sweden is responded to by a depression in Iceland. Be Beaumont calls this the " mouvement de bascule." Besides these occasional movements resulting in permanent change, we believe that there are periodical fluctuations of the surface of the earth of this compensatory nature, occasioned by the varying distribution of the force by which she moves in her orbit. This fluctuation would enlarge the earth in one diameter, and contract the diameter at right angles with this. Thus there are two daily elevations and depressions corres- ponding with each other. This gives the two maxima and minima of the barometer. The elliptical form of the earth's circumference is depend- MECHANICAL PHILOSOPHY. 131 ent on her position as being nearer to, or further from the centre of revolution ; and the shrinking or expansion is regu. larly propagated by her rotation. The movement being oscillatory, the maxima will, of course, be somewhat after noon and midnight, corresponding with the minima of the barometer. The extreme would also be greatest within the tropics. Connected with this subject are the horary changes of the horizontal magnetic intensity, to which we shall here- after allude. To one other fact only will we at this time advert. It is stated, on good authority, that the barometer is more to be depended on for determining heights, than trigonometrical observations are. The reason given is, that " the refraction of the air prevents accurate measurements of the angle." If we are correct, the reason is obvious ; but it is impossible that the density of the atmosphere should, under all disturbing influences, always correspond to elevation with a greater accuracy than the results of geometric calculation. In our attempt to explain the cause of the action of the barometer, we can, in this place, but imperfectly advance the views that have presented themselves. These views involve peculiar ideas, not only in regard to the force of rotation and revolution, but to the vacuum, to the action of fluids in relation to their own particles, and to their action in relation to other matter ; and the ideas, to be presented with any distinctness, must be gradually unfolded as we proceed. The changes of the mercury result in a longer or shorter column of the fluid in rotation as one mass. In the rotation of any one mass, the force of rotation is unequally diffused through it ; the parts, say the upper and the lower, rotate with greater and less force. This inequality of present force increases with the distance of the two surfaces. It 132 OUTLINES OF A SYSTEM OF increases also with the density of the mass, the distance be- tween the surfaces remaining the same ; it increases by a greater degree of rotative velocity, in a mass of the same density and same distance of the two surfaces. In other words, while the ratio of difference remains the same between the different parts of the same body, the actual inequality is increased by increased extension, or density, or velocity. "We have, then, an unequally distributed rotative force present in every mass, and the extent of the inequality is in direct proportion to the difference of the orbit of the upper and lower extremities, to the density of the body, and to the velocity of its rotation. In solids bound together by cohesion, in fluids so placed that the upper and lower surfaces cannot approach or draw apart, this inequality must and will continue, whatever be their depth, density, or velocity of rotation. But from the law of the diffusion of force, there is a normal difference of diffusion to which all fluid bodies conform when free to adjust their volume in relation to it. From this principle comes what we term the limit of ex- tension of fluids, a distance between the upper and lower surfaces, which measures the normal inequality of the pre- sent force, an idea which we hope fully to illustrate as we proceed. At present we merely state the fact. The limit is perceived only in fluids so placed that a change can be made in the length of the column. This is the case with the mercury in the barometer. It can shorten or lengthen its column, and it must have the upper and lower surfaces to effect this. It keeps the normal inequality the same under any force of rotation, by extending or lessening the distance between the two surfaces. It rotates with a column which corresponds in length to the force of rotation. If the MECHANICAL PHILOSOPHY. 133 barometer is made with a fluid of less density than mercury, there is the " limit " for the same cause, but it admits of a greater distance between the two surfaces, under the same force of rotation. We dismiss the special consideration of the barometer, with a most unhesitating belief that its action is caused by the increase or diminution of the force of rotation, that in its changes it denotes its level, that it indicates directly the altitude. We believe so from the fact that such would be its action as deduced from principles established in our mind on other grounds. We also believe so, because we find the oscillations always to be such as could be occasioned by changes of level, and often such as could never be produced by varying densities of the atmosphere ; and because, if the atmosphere be of varying density, the construction of the barometer is such that it could not be affected by the varia- tion. We solicit a thorough examination of this subject ; for, if we are correct, it gives a value to the instrument far greater than it now possesses, its readings being at present confined to atmospheric pressure. We pass from the barometer, hoping further to elucidate its action by examining the limit of extension in relation to water. The principle is the same in every fluid ; but water, for many obvious reasons, most distinctly illustrates the opinions that we would present. Water, in a tube closed at the top and open at the bot- tom, on being immersed in water will remain suspended at any height within the limit. But if the top of the tube be opened and air be allowed to enter it, the inclosed water will sink to the level of the water in which the tube is im- mersed. The exclusion of air from the tube is, therefore, 12 134 OUTLINES OF A SYSTEM OF the condition requisite for the water in it to remain above the level of the water in which it stands. This appears of easy explanation. When a volume of water is in contact with air, the surface of this volume of water, if at rest, will be of uniform level. In the two elements, air and water, there is a difference of capacity for force, so that the one, when in contact with the other, invariably retains a fixed degree of force relative to the other. This principle gives uniformity of level to the surface ef any volume of water in contact with air ; but, if any part of its upper surface is with- out this contact, its level of rotation does not depend on that which gives level to the parts of the surface of the water which are in contact with the air. Under the theory of gravitation it is supposed that it is the weight- of the atmosphere on the water outside of the tube, and its absence within it, which create the inequality of pressure, resulting in the elevation and support of the water in the tube. This is supposed to be shown by the action of the atmospheric pump, by the syphon, and in fact by all the cases of the elevation of w r ater which exhibit the law of extension. It is considered as occasioned by the vacuum, fluids being suspended because of a vacuum, or because there would be a vacuum if the fluid did not ascend. The idea is not distinctly advanced at the present day that the action of the fluid is from an attractive power of the va- cuum ; but the inference necessarily drawn from the facts in connection with present theories is, that nature so abhors a vacuum that action is immediately induced, not only to fill the vacuum formed, but to prevent it from being formed. There is always a supposition of aid from the weight of an outside column of air, of the same area as the column of heavier fluid to be acted upon ; but in no case can the action MECHANICAL PHILOSOPHY. 135 of this external counterpoise be proved, and in many cases it is certain that it does not exist or act. In a succeeding chapter, when speaking of the properties of air, we shall endeavor to illustrate the principle, by which a vacuum arti- ficially created, as it were, draws in matter to fill the void space. In our present view of the subject, we confine our- selves to the illustration of the idea, that the support of a column of fluid within the limit of extension does not and cannot depend on the pressure of a column of air of its own area. We will suppose a common atmospheric pump, working with perfect nicety, and with the least possible friction. The piston is in contact with the surface of the water to be raised, and on being lifted the water is raised with it. There is no vacuum here ; the atmosphere rests on the piston, and the piston on the water, and this mutual relation of atmo- sphere, piston, and water continues. The piston and the water below it are not in the least relieved of the weight of the aerial column over them ; if it pressed on the piston be- fore it was moved, it equally presses when it is moving upward. If the pressure of an equal column of air on the water of the cistern raises the water in the pump, its action prevents a vacuum from being formed. We make for the present the simple statement, that force applied to the water gives it power to rise to a higher level, and the elevation of the piston gives it space, room, freedom to ascend, the needed force for ascent is supplied, and a channel opened for the action of the force. In all similar cases we shall ever find, that when fluids rise in pipes, it is because of the application of force, with space for the action of the force. That, in the case of the pump to which we have just alluded, a column of air of the area of the ascending column 136 OULTINES OF A SYSTEM OF of water, in other words, atmospheric pressure on the water in the cistern, does not lift up the water in the pump, can be most distinctly proved. We will suppose the piston, which touches the surface of the water, and the elevation of which gives space for the rise of the water, to be securely fastened to the tube, and that the pump, tube, and piston together, be lifted as high as the piston was previously lifted in the pump. The same quantity of water will be raised as before. In the one case, space has been given for the water to rise by elevating the piston ; in the other, by elevating the tube with the stationary piston. The force required to raise the tube, valve and water is just the weight of the tube, valve and water. In either case there needs to be supplied the same degree of force, which would be required to raise a stone of the same weight. How then can it be said, that in working the pump, the pressure of the atmosphere is the elevating power, when for every pound of water raised the force necessary to raise a pound is required ? It is said in Ewbank's Hydraulics that the pump will work " if the well be covered with slabs of stone, and coated all over with the best hydraulic cement," thus cut- ting off from the water of the well all pressure of the atmo- sphere, except such as is drawn by the action of the piston " through the minute pores." The only necessary con- nection with the atmosphere is limited to that orifice, which will admit into the well a volume of air equal to the volume of water withdrawn, otherwise there would certainly be a vacuum formed in the well. No connection whatever be- tween the atmosphere and well is needed, if the water ele- vated runs back through another pipe into the well. The act of pumping is the establishment of a current of water. It has no connection whatever with atmospheric pressure. MECHANICAL PHILOSOPHY. 137 A pump would work completely immersed under water, there establishing a connected current, and after the cur- rent was formed the upper surface of the water would not be even ruffled, the atmosphere pressing equally on all the parts of the current below. It is said that the atmosphere presses on the body of every man with a force of some fifteen tons, but because it bears equally in every direction, because it is so exactly equipoised, it is not an object of sensation. We do not feel it. Its force is neutralized, destroyed, so far at least that it induces no perceptible results. This is true, not only in relation to the human body, but to every mass of matter immersed in air. The cistern and the water that it contains, the valves, the water in the tube, and the jet of water issuing from the tube, are as one body ; the enfolding atmosphere is wrapped around the whole with equal strain. If the pressure of the air has power to cause the water to ascend through the tube, it has the same power to act in the opposite direction. If it press water in at the bottom of the tube, why does it not press it back with equal force ? When the upward current is established in the pump, all the force to create the current must be supplied ; the force needed is exactly equivalent to the weight of water elevated. Therefore, the doctrine of equal areas of atmosphere sup- porting the denser fluid in vacuo has no more application to the raising of water by the pump, than it has to the drawing of water from a well by the pole and bucket. By both mechanical means strength is put forth proportional to the quantity of water to be raised, and to the distance of eleva- tion, the weight of the atmosphere, so far as any practical result is concerned, being neutralized, destroyed, by the affirmed law of its equal pressure in every direction. 12* 138 OUTLINES OF A SYSTEM OF But for the skeptical we will mention a fact which per- fectly demonstrates that the action of the pump has no reference to the pressure of the atmosphere. By accident, in Seville, in 1766, it was discovered that water could be raised by the pump fifty feet and more, if a small opening was made for the admission of air into the tube of the pump. This circumstance excited great attention at the time, and was supposed to prove that water could be raised by atmo- spheric pressure much higher than thirty-three feet. In the Journal of the Franklin Institute for May, 1837, it is stated with reference to the action of pumps worked by steam, that a little air is sometimes admitted into the pump pipes, which " makes the pump work more lively in conse- quence of the spring it gives to the column of water." And in the same paper, Mr. Perkins states, that " forty years before an attempt was made to impose upon him a pump which raised water by atmospheric pressure one hundred feet ; but he detected a small pin hole in the pipe through which the air was admitted." These facts are fatal to the theory that atmospheric press- ure causes the elevation of water in pumps ; for there may be the pressure on the ascending as well as on the impelling column. No matter how little this pressure is, though the fact was shown in Ewbank's well, closed by hydraulic cement, that the pressure through small apertures is as strong as through large, if the pressure within was but an hundredth part of that without, what there was of it would balance pro- portionally the external pressure, and to this extent too it would impair the vacuum ; but instead of this it gives new power of ascent to the water, more than doubling the possi- ble extent of its elevation. To account for this we are told, " It was ascertained, on investigation of these facts, that the MECHANICAL PHILOSOPHY. 139 air on entering the pipe mixed with the water, which there- fore, instead of being carried up in an unbroken column, was raised in disjointed portions or in the form of thick rain. This mixture being much lighter than water could be sup- ported by the atmosphere, and by proportioning the quantity of air to be admitted, a column of the compound fluid may be elevated one or two hundred feet by the atmosphere." In this explanation the fact seems to be forgotten, that it is not the weight of the column of water which determines the altitude to which it can be raised. Increase the force, and ten thousand pounds may be lifted as readily as ten pounds. It is the height of water, not the weight, which attained, it will no longer rise ; and the main fact was quite forgotten, that atmospheric pressure was at work as well within as without the tube. Our views can be presented more distinctly by reference to the action of the syphon. In the pump the current is established by animal force, or by the power of wind, steam, &c. applied to the piston ; in the syphon the same end is obtained by the presence of a longer column of water in one leg than in the other. To use the common language, gravi- tation acting on the longer column with greater force than on the shorter, the equipoise is destroyed, and the water falls in the one, rises in the other, thus establishing a con- tinuous flow. It is the force of descent of one body drawing up another body with which it is connected, as by a rope passing over a wheel. The strength of the flow is therefore determined by the difference in height of the two columns, the force gained by the descent of one being more than sufficient for the elevation of the other. The flow has no reference to the attraction of gravitation ; for by different diameters of the two columns, the quantity or weight of water may be greatest in the shorter leg. 140 OUTLINES OF A SYSTEM OF We will suppose a syphon, the shorter leg of which shall be ten feet high, containing a hundred pounds of water, its longer leg of eleven feet containing five pounds of water. The water from the longer leg is discharging itself into the air in a continuous stream. What supports the one hundred pounds of water, which, by theory, is drawn towards the earth by a force equal to its weight, while the water in the longer leg is drawn down by a force of only five pounds ? Certainly it cannot be atmospheric pressure on the larger tube ; for there is also atmospheric pressure at the discharging orifice of the smaller tube. The attraction of the hundred pounds of water, if it be attracted at all, should be suffi- cient to draw up the five pounds and to draw in the air after it. Of course the one hundred pounds does not feel the force of attraction. The action of the syphon is therefore but the fall of water through a tube arched upward, and the force of the fall is measured by the difference of altitude between the two levels, that from which it is drawn and that into which it issues. In the pump it appears as if a vacuum were created, as if the current were established by the weight of the air pressing on the water in the well, and not on that in the tube. In the syphon there is not the most remote indication that a vacuum is formed, and the pressure of the atmosphere is exactly the same on the water which enters the pipe, and on that which leaves it. There is no vacuum ; for the syphon is kept full of water, and this creates a plenum as much as if it were filled with lead ; and with the shorter leg immersed in water, the surface of which is at a higher level than that in which the longer leg is immersed, if there be any difference, the atmosphere presses more heavily at the discharging than at the receiving orifice. There can be no MECHANICAL PHILOSOPHY. 141 pretence of atmospheric action on a current of water flowing from a higher to a lower level, through a tube arched up- wards. The air in this case has no more to do with the current than if it flowed through a pipe bent downward, or curved laterally, no more than if the water ran down through a straight tube, or without any tube through an orifice in the side of the containing vessel. The action of the syphon is imputed to atmospheric pressure, because the limit to which water can rise in it is the limit, beyond which water cannot be raised in the cases in which atmospheric pressure is supposed to be the cause of the elevation. It is true that if the water at the top of the syphon should part, and it should descend in each column, there would be a vacuum ; but, there being no gravitation, it will not part till beyond the limit of extension. It then parts through the action of the law which regulates the limit. But because, if the syphon does not establish its current, and the water falls in both the legs, there is a vacuum, it does not follow that a vacuum or the dread of one establishes the current when it flows. While the current is flowing there is, if any, an equal pressure at both ends, and from them up through the whole length of the pipe. The vacuum is formed, if the syphon be raised above the limit. If the instrument be extended higher, the water does not rise ; but remains elevated at an equal height in both legs, measuring from the respective levels of the surfaces of the water in which they are immersed. It is supposed, that each suspended column is counterpoised by an equal weight of atmosphere, that is, by a column of air of the same area as the suspended column of water. Of course, this being the case, any variation of the limit marks an equivalent change in atmospheric weight. 142 OUTLINES OF A SYSTEM OF Without going into the question at this time, of the pos- sible efficacy of the air in sustaining water in such cases, which may well be doubted, as we have seen that it has not the most remote agency in giving it its elevation, we feel confident that the weight of the suspended column does not weigh a column of air of its own area. If water be subjected to pressure in a cylinder by a pis- ton acting on its upper surface, the rise of water issuing or sustained by the pressure is measured by the whole amount of the force of the piston, as in the case of a forcing-pump. If the atmosphere presses on the surface of water in a pond, or in a small vessel, the pressure is measurable by the force acting on the whole surface. A pond a mile in area bears the pressure of a column of air a mile in area ; and the water in a small vessel bears the pressure of the column over it. On this principle only can water be acted on by the air, and any variations of pressure arising from atmo- spheric changes would express the variations of the weight of the whole volume of air over the pressed surface. Thus far we have considered the limit of extension of fluids, and appear to find that this limit is not determined by the gravitation of the fluid, since the quantity sustained under the same circumstances may be one pound, or one thousand pounds ; nor by the gravitation of the air on the exposed surface of the fluid, since this may be one inch or a thousand miles in area ; nor by any virtue or efficacy of the vacuum, since it may be equally filled, saturated, and thus destroyed by matter of its own volume, whether the matter drawn to fill it is light as air or dense as mercury. The limit is therefore not caused or determined by the gravitat- ing power. We advance to a farther consideration, to create the MECHANICAL PHILOSOPHY. 143 limit, it is not necessary that the fluid be confined in pipes or vessels. Water out of pipes, unconfined, in the free air, obeys the law. The waters of the ocean respond to this limit. Water-spouts, with mingled air, may raise a broken column to a higher range ; the waves may dash themselves farther up on a rocky coast. Wave may be formed on wave, a new limit of extension may perhaps be formed upon the original limit, an ocean wave upon a tidal wave ; but recorded events always give a height of the rise of floods, which denotes the bound assigned by nature to the heaping up of the waters. It is difficult to measure the height of a wave, and impos- sible to separate exactly the unbroken water from the crest which is mingled with air. We know, however, that the rise of waves is less than thirty-four feet in the most violent storm. One measurement taken in a long-continued heavy gale gave thirty-two and a half feet from elevation to de- pression ; on striking a wall of rock, the unbroken column ascended sixty-five feet from the level of the ocean, dashing its spray much higher. The extent of the rise of the tide in the bays of Fundy and of St. Malo is said to be sixty feet, and the reference to heights of which the simple limit forms the root or multiple, in the statements of the rise of floods, is so frequent as to indicate some principle. It is certain, however^that the waves of the ocean have a fixed limit corresponding to the limit of the extension of water in tubes. The isolated fact of the limit is thus advanced to an uni- versal principle; 'for it has never been imagined that an unequal atmospheric pressure causes the rise of the waves. Whenever a fluid is so placed that its degree of extension upwards and downwards can be changed or modified, when 144 OUTLINES OF A SYSTEM OF it is free to assume its own position, it obeys the law of limit. To give it a greater extension as one mass, it must be re- strained or confined. Its spread or dilation in breadth must be prevented, either artificially as in tubes, or naturally as in a containing basin. Its base must be cut off, it must be separated from other volumes of the same fluid. Water can be elevated to any height by the lifting pump, or by the application in any manner of force beneath the volume of water to be raised. But if the force be applied from above, as in the atmospheric pump, or in any manner to a body of water remaining in connection with other water, the force applied is conveyed away from the special volume to the whole volume ; a portion therefore cannot be elevated. It must first be separated, that the force applied may act upon it. It will then rise ; but before the separation the force applied is communicated to the whole volume. It is thus that separated volumes may be lifted to any height, if suffi- cient force be used ; and this explains the fact before alluded to, that, when air was admitted into the pump by a perfora- tion in the tube, water was lifted beyond the limit, since the air separated the one volume into detached portions. The limit of extension is therefore the degree to which fluids can be drawn upward in an unbroken column. It is the limit of the inequality in the distribution of the force of rotation, which will remain when the e^ess can be trans- ferred to another portion of the same volume. It is the limit of elasticity of form ; for while a solid body ever retains one extension, no one part of it being susceptible of ele- vation independently of the other parts of the mass, to raise one part requiring force sufficient to raise the whole, por- tions of fluids can be drawn up, force, to a limited degree, confining itself to the part. Thus, a column of water can MECHANICAL PHILOSOPHY. 145 be extended from the volume ; but beyond this limit force no longer confines itself to the part to which it is applied, but diffuses itself through the whole volume. Therefore, the sea knows its place ; the level of the waters composing so large a relative portion of the globe is preserved, not with a dead uniformity, not with a rigid flatness of sur- face, but with constant changes, limited undulations ; and the ocean, free to move, yet under the law of extension, is as securely bound, as are the rocky cliffs against which its rolling surface strikes. The more our attention is directed to the unfathomable deep, the more wonderful appears the action of the laws which control it. We are taught to regard the vaporization of the surface of the ocean as a means by which the equili- brium of heat is preserved, and by which the waters circu- late from the sea to the clouds, from the clouds to the thirsty earth, and again collecting in swelling streams return back to the ocean in a never-ceasing flow. How great the quantity of fluid thus in constant change, hundreds of millions of tons rising in one day from the comparatively small extent of the Mediterranean Sea, the quantity ever rising from the entire surface of the waters of the globe, from the frozen polar seas, as well as from the tepid oceans of the torrid zones, being beyond all estimate ! This vaporization not only waters the earth, not only restores the equilibrium of temperature, these effects being as it were the incidental mercy of the law of nature ; but it is the preservation of an equilibrium si force. The ocean exhausts itself of the strength not necessary for its level of motion, the vapor draws off the excess of energy, and the waters preserve their equable flow. The risen vapor, again condensing, slowly imparts a quickening impulse to the slug- is 146 OUTLINES OF A SYSTEM OF gishly moving air, or rapidly throws out the force in the light- ning's flash, giving to some portion of the earth the needed impulse. For this reason is there greater condensation, more copious rain, in high lands and mountainous regions, which from their elevation require the added force. No one can contemplate the extent of the oceans of the globe, their vast surface compared with the land, without being assured that this unequal distribution is not from acci- dent, without the belief that there is connected with it the furtherance of some great design. And when we consider its relations to force, its strong conducting power, we see a reason for the ocean's vastness, and comprehend its action in the economy of nature. There is a reason too for the pre- ponderance of water in the southern over the northern hemisphere, which may yet be discovered by man ; for, though land and water seem confusedly mingled as if with- out law, not by accident came the position of the smallest island, nor the bounds of the paltriest lake. Then again, the waters of the ocean have a molecular action, increasing in intensity as they deepen. The experi- ments of Scoresby, the well-known fact of the breaking of a vessel containing air when let down to a certain depth, the bursting of a tight, full cask, by the insertion of a long slender tube filled with water, the "spring" of water, of which mechanics take advantage in their management of water-power, by narrowing the aperture through which the water flows, the eflect of conical ajutages, by which the flow of water from a discharging orifice is greatly increased from the transfer of the molecular action into the progressive motion of the moving jet, all these facts together prove that there is an increase of the atomic action of water pro- portional to the distance from the surface, and that this MECHANICAL PHILOSOPHY. 147 change is not in the least dependent on a force of gravita- tion ; for water is almost incompressible, and, were it com- pressed, the increase of molecular action is altogether too rapid for the rate of increase of gravitation, according to the distance from the centre. Thus the waters receive and retain a greater force than is needed for rotation, resolving it into molecular action, the ocean becoming, as it were, the storehouse of force, from which it may be gradually imparted according as it is needed for the motions of the various parts of the earth. It is by this provision that force divides or diffuses itself equally throughout the volume of the fluid ; for, as stratum after stratum requires the less for rotation, the unused force is employed in molecular motion. It is by this equal diffu- sion that the movable element preserves its continuity ; and, without the bonds of cohesion to hold its particles together, it moves with the earth as one mass, no portion ever raising itself beyond the limit, or floating in the atmosphere in detached masses. Without this provision, the air would not be divided from the waters, element would not be separated from element, the waters could not be gathered together into one place. It appears evident, then, that there is in water and other fluids a molecular action, which increases in intensity accord- ing to the depth, or distance from the surface. On the other hand, the rotative force increases as it ascends from the depths, being greatest at the surface. One therefore is the complement of the other, each being capable of resolution into the other. Therefore, force is ever equally diffused through the same volume, the aggregate of force being evenly distributed through each body of water, whatever its depth or extent. It is therefore equal throughout the space occupied by the water. 148 OUTLINES OF A SYSTEM OF How far extends this principle of the equal distribution of force relative to space ? Is it universal, in solids and fluids, from the densest matter to that which makes the nearest approach to a vacuum ? Do accelerated and retarded motion take place from the adjustments of force, as in different degrees it acts in the atoms and in the mass, in the mole- cular and the progressive motion ? Is it a normal adjust- ment which gives harmony of movement to the spheres ? Is motion irrespective of mass ? Has the rarer medium of the atmosphere, for instance, an increase of molecular action to compensate, as it were, for its less quantity of progressive motion in a given space ? This indeed opens a wide range of thought ; but we pause in the inquiry. May we not hope that in time to come the intellect of man may be able to penetrate these mysteries, and to find in the now complicated phenomena of motion that simplicity and comprehensibility, which belong to every domain of nature ? If force be equally diffused through space, and we extend the idea of the equality of its diffusion to limitless space, the human mind almost shrinks back at the contemplation of this expanse of energy. There is but one step farther which it can take, going on from boundless force to Him from whom it is the emanation. To return : there is then by fixed laws a permanence given to the free-moving elements. There is a defined limit of extension, measured by the density of the fluid, and by the velocity of its motion. This is determined by the degree of the inequality of force which will be retained by any volume of fluid, so placed that it can transfer the added force. Broken columns of water may be elevated to any range of rotation ; but water resting on water as its base, refuses to extend itself, or to be drawn out above its normal MECHANICAL PHILOSOPHY. 149 range. Beyond this, force -will not so adjust itself as to keep it one mass ; if you apply force, the water receives it, but will not retain it. The raging storm passing over the wide ocean, ever imparting force, gives to the water a defi- nite range of altitude only, while the excess is silently trans- ferred to the deeps below. Urge it further and further, it still refuses to rise, and, if saturated, if it can retain no more in the intensity of molecular action, the water at the surface changes into vapor and floats upward in harmless cloud- wreaths. " And God said, I will establish my covenant with you, neither shall all flesh be cut off any more by the waters of a flood, neither shall there any more be a flood to destroy the earth. I do set my bow in the clouds, and it shall be for a token of a covenant between me and the earth." The bow in the cloud has been by many looked upon as a figure of speech only, as a beautiful metaphor, possessing no more significance than the clear sunshine after the falling rain. It has not been connected in men's minds with any law of nature, which determines the limit of the rise of the waters. Yet it is the expression of the law by which the floods keep their place. It connects science with the writ- ten Word. Understood, the rainbow shows the harmony of the creation with the voice of God. It practically as well as spiritually records the covenant. The water ascends from its immense ocean bed only as the vapor of the clouds. It cannot rise to deluge the earth. The flowing stands firm, the free moving element is bound in chains ; for though intense force, in its might, may rush across the rolling waves, it will not impart to them the power to rise above a fixed limit, except as vapor, and on the 13* 150 clouds the covenant is written in the vivid colors of the rays of the sun. Devoutly thankful should we be when reason thus re- echoes the voice of God, when science, in her feeble utterance, repeats the declarations of Scripture. We cannot, with the thought of this connection, look upon the bow in the clouds but with increased delight, and with a strengthened reverence for the written Word, with some- what of the feeling which prompted the exclamation of Cole- ridge, " What a mine of undiscovered treasures, what a new world of power and truth, does the Bible promise to our future meditation, when in some gracious moment, one solitary text of all its inspired contents dawns upon us in the pure un- troubled brightness of an idea, which even as the light, its material symbol, reflects itself from a thousand surfaces! " CHAPTER VII. "THERE ARE INDEED MANY THINGS IN THE FRAME OF NATURE, WHICH WE CANNOT REACH TO THE REASONS OF, THEY BEING MADE BY A KNOWLEDGE FAR SUPERIOR AND TRANSCENDENT TO THAT OF OURS, AND OUR EXPERIENCE AND RATIOCINATION BUT SLOWLY DISCOVER- ING THE CONTRIVANCES OF PROVIDENCE THEREIN. "NO MAN EVER WAS OR CAN BE DECEIVED IN TAKING THAT FOR A TRUTH WHICH HE CLEARLY AND DISTINCTLY APPREHENDS, BUT ONLY IN ASSENTING TO THINGS NOT CLEARLY APPREHENDED BY HIM." Cudworth. WE continue our examination of the action of force upon fluids. Our views bring us to the conclusion that there is no weight or pressure of the particles of water against each other, against a containing vessel, or against a foreign body immersed, other than arises from the force of molecular action, which manifests itself under certain circumstances. We do not believe that gravitation presses together the particles of water, or presses them against an immersed body. This proposition at first sight appears to contradict the generally received opinions on the subject. It is not so. Though expressed in different language, our proposition is in harmony with established views. The law of gravitation is modified in its application to fluids. It is said, u the par- ticles of fluids gravitate independently of each other, not only downwards, but upwards and sideways." " The press- ure of fluids is equal in all directions, being founded on the 152 OUTLINES OF A SYSTEM OF complete intermobility of the particles of the fluid, and on the equal propagation of pressure in every direction." " When a fluid is at rest the pressure will be nothing, be- cause the opposite dead pressures will be equal." These quotations are from the highest authority, and completely prove the proposition with which this chapter commences, so far at least as relates to any result from the pressure. Admitting, however, the theory that the atoms of water do press against each other, and against an immersed body, the pressure, if it is equal in every direction, cannot proceed from an attraction of gravitation drawing towards the centre of the earth. Why this equal pressure, of the existence of which there can be no proof, is attributed to a force acting downward only, does not appear. A consideration of the weight of a mass of matter rigidly at one level, or of the pressure of one mass against another, or of the mutual pressure of their atoms when relatively at perfect rest, involves what may be called transcendental dynamics. It treats of a tendency to fall, a tendency of the particles of matter to move against each other, which is followed by no action. The tendency to fall, of a body secured so rigidly that it cannot be moved, can never be the subject of experiment. We can measure force only by resultant motion. There is no force of descent unless there is a descent. A body secured at one level at perfect rest, would feel heavy only by the upward pressure of the hand against it. Suppose a body which by its fall presses a spiral spring, the weight of the body is its force of descent upon the spring, which, if it have not force of elasticity enough to throw it back, will remain compressed. The compression is a change in the position and arrangement of the atoms com- posing the spring. This comparison will indicate the reason MECHANICAL PHILOSOPHY. 153 of the feeling of pressure in the hand supporting any mass of matter. We will suppose a vessel ten feet high containing water. From an aperture near the upper surface the water will run with but little force, falling down almost perpendic- ularly ; from an aperture in the middle it spouts with con- siderable power ; and from one at the bottom the flow is with greatly increased energy. The jet is horizontal in proportion to the distance of the orifice from the upper sur- face ; its force is in proportion to the descent of the water inside the vessel. There is little or no force of descent in the water flowing from the upper orifice, the whole force of descent is in that flowing from the lower opening. It is the force of descent which impels the water, not abstract weight or tendency to descend ; for a pound of water at the surface has as much desire to go down, is as much attracted, as a pound at the bottom of the vessel, that is, neither is at- tracted to the earth. Matter itself is inert, without power to move or tendency to move. It obeys the law of force, and if absolutely at rest it is without force ; nothing can be affirmed of it, but that it is, the fact that it exists in space. We proceed to more practical illustrations of the pressure and equilibrium of fluids. We will describe from nature. We were leaning on the rail of a bridge, a few rods above which rose a dam about ten feet in height, which held back a pond of water extend- ing beyond the dam for at least a mile. The dam was per- haps two hundred feet long, it was old and dilapidated, and from between the logs there were at every height countless jets of water. On the top of the dam was a flash board. a plank placed edgewise, slightly secured, to in- crease the height of the dam. At one place this flash board 154 OUTLINES OF A SYSTEM OF had given way, and there the water poured over the dam in an unbroken sheet. We will look at this dam with its many jets of water, the broad sheet tumbling over a part of it, to understand the nature of the pressure of water. It will give us the truth, if observed with minds free'from all predeter- mined theories. In the first place, we see that the water does not press equally in all directions, upward, downward and sideways ; for the lower jets of water issue with much more force than the upper jets. There is a gradual diminution of pressure from the lowest to the highest ; the top of the water falling over the dam does not press at all, for the sur- face retreats, forming a curve. The pressure increases from the surface to the bottom. Fluids do not gravitate equally in every direction, or the force of gravitation would have thrown out equal jets from the top to the bottom. Perhaps the water gravitates downward only. That cannot be the case ; for then there would be no lateral pressure, but at each jet the water would flow nearly without force. One other thing is certain, that this great volume of water, two hundred feet broad and a mile long, does not press laterally with a weight in proportion to the mass of the heaped up water. So weak an inclosure could hardly bear a ton's weight. There is lateral force then only in that water which runs over the dam, or escapes through the apertures. That which is at rest can have no pressure ; for, if it had, the weak barrier would be overthrown. Suppose a stone weighing one hundred pounds, pressed equally one very side by springs. With the pressure of these springs it weighs just one hundre.d pounds as it did without them ; for the action of one spring neutralizes the pressure of the opposite spring, so that the "gravity" of MECHANICAL PHILOSOPHY". 155 the stone is not changed. We will take away the springs and weigh this stone under water, which by theory presses on it as did the springs, equally in every direction. It has lost weight, therefore water does not press equally in all directions on the stone. Nor does the water press down- ward only ; for in this case the stone would weigh more in water, " having to bear not only its own share of attractive force, but the weight of all the strata (of water) over it." How, then, can we ascertain the specific gravity of the stone on both or either of the two laws of the gravitation of fluids ? An equal pressure on all sides would be " dead pressure," and the stone would weigh the same in water as in air. A vertical pressure would increase its weight. "We once heard two men disputing on this subject, one affirming that a stone did weigh less in water, because he had often tried it ; the other affirming that it could not weigh less, " for you see," said he, " the stone is as much drawn down by gravity in the water as out of it, and the water cannot lift any, when there is more water over it bearing clown than under it lifting up." In fact, on either or all of the principles affirmed to ac- count for the pressure, the change in the gravity of the stone cannot be explained. It is true that the stone dis- places a quantity of water equal to its bulk, but this fact neither increases nor diminishes the force with which the earth attracts it. What is the action of the surrounding water ? How does it press on the stone ? Downward only ? Surely not ; " fluids press equally in every direct- ion." Equally on all sides? Then the "opposite dead pressures" must entirely neutralize each other, and have no effect whatever. The decreased weight of the stone can be accounted for only on some new principle. 156 OUTLINES OF A SYSTEM OF We will bring the pressure of water to an infallible test, that of our sense of touch, our honest perceptions which favor no theory whatever. Immerse the hand in water ; in the act of immersion pressure is felt, for the water is moved by the introduction of the hand, but when it is at rest in the water not the least pressure is experienced. Place the hand near a small orifice from which water is issuing, and pressure will be felt because there is a motion of the water. Stop the orifice with the palm of the hand, and there is no pressure ; for the water has ceased to flow. We now pass to the consideration of that action of fluids which is called the hydrostatic paradox, an increase of pressure which is not in proportion to the force applied, but is in proportion to the surface of the pressing fluid. A multiplication of pressure is apparently produced, an effect greater than the cause, by some supposed myste- rious " principle of fluidity " applied force in some cases increases its power according to the extent of the surface against which it acts. It is said that " the true laws of the equilibrium of fluids were discovered by Archimedes, and rediscovered by Galileo and Stevinus, the intermediate time having been occupied by a vagueness and confusion of thought on physical sub- jects." The doctrine is that, as a fluid is a body, the par- ticles of which have a perfect intermobility, " therefore all pressure exerted on one part is transferred to all other parts." Stevinus deduced from this principle, that the pressure on the bottom of a vessel filled with fluid, may be greater than the whole weight of the fluid. And it is also deduced, that the pressure may diverge, and may be multi- plied in every direction. Pascal shows, in his Treatise on the Equilibrium of Fluids, " that a fluid inclosed in a vessel MECHANICAL PHILOSOPHY. 157 necessarily presses equally in all directions by imagining two pistons, or sliding plugs, applied at different parts, the surface of one being a hundred times greater than the other ; it is clear that the force of one man acting at the first piston, will balance the force of one hundred men act- ing at the other." And therefore he concludes that, " a vessel full of water is a machine which will multiply force to any degree we choose." The apparent multiplication of pressure is indeed a diffi- cult subject to grasp or comprehend. The explanations given of the facts are far from being clear. This seems to be admitted ; for, as Whewell remarks, " there is a difficulty of holding fast this idea of fluidity. Even at this day, men of great talents not unfamiliar with the subject, sometimes admit in their reasonings an oversight or fallacy with regard to this point. The importance of the idea when clearly apprehended and securely held may be judged of from this, that the whole science of hydrostatics, in its most modern form, is only the development of this idea." But has all " vagueness and confusion of thought " on this subject passed away ? Is it now clearly understood how there can be an equal pressure in every direction, and at the same time the pressure be increased according to depth, and again multiplied according to surface ? The facts which are supposed to prove the multiplication of pressure in fluids are, the elevation of a great weight by a less weight of water, as in the hydrostatic -paradox, the bursting of a full cask by the pressure of a very small quan- tity of water poured into a long tube inserted in it, and the floating of bodies in water of less weight than the mass that is buoyed up. The hydrostatic paradox, as it is called, may be exhibited 14 158 OUTLINES OF A SYSTEM OF in the following manner : Insert a long slender tube into a cylinder with a movable piston ; pour water into the tube, and the piston will be elevated by it ; if the tube holds only a pound of water, and has an area only one hundredth part as great as that of the piston, the pound of water poured into the tube will elevate a hundred pounds placed on the piston. The same action is shown in the Bramah press, by which a great pressure is produced by gradual increments of force, from water driven into a large cylinder by a small forcing-pump. The explanation which is usually given of these facts is, " that as the pressure of the particles of fluid is equally dis- tributed among themselves, so external force or pressure is distributed in the same way." . . "In the hydrostatic press an immense accumulation of force is brought to bear upon a particular point, by pressure applied by a small column of water reacting upon a large mass placed on the surface of the piston." This explanation is hardly more than a recital of the facts ; how or why the small column of water should react with a force proportional to the surface against which it is applied is not in the least explained. The fact that the weight or pressure of one pound of water may be made to produce a pressure equal to that of a hun- dred or a thousand pounds, is in reality no more paradoxical than that one pound on the long arm of a lever should balance a greater weight on the short arm. Its action is similar to that 'of other mechanical powers. There is no increase or multiplication of the applied force. The descent of every pound of water gives a spare force of descent suffi- cient for the elevation of a pound weight. It will raise a pound to the same height from which it fell, or one hundred pounds T