This is a table of type quadgram and their frequencies. Use it to search & browse the list to learn more about your study carrel.
quadgram | frequency |
---|---|
on the other hand | 80 |
that is to say | 72 |
it is necessary to | 53 |
at the same time | 49 |
it would be necessary | 32 |
the principle of the | 31 |
the conservation of energy | 30 |
the motion of the | 29 |
would be necessary to | 29 |
of the conservation of | 27 |
it is clear that | 26 |
in the same way | 26 |
on the one hand | 23 |
a great number of | 23 |
at the instant alpha | 23 |
the calculus of probabilities | 23 |
the principle of relativity | 22 |
of the principle of | 22 |
the velocity of light | 22 |
at the instant beta | 22 |
the same point of | 22 |
would no longer be | 21 |
of action and reaction | 20 |
principle of the conservation | 20 |
this is not all | 20 |
we do not know | 19 |
but it is not | 19 |
but this is not | 19 |
of the equality of | 19 |
the study of the | 18 |
the kinetic theory of | 18 |
and this is why | 18 |
it is easy to | 18 |
equality of action and | 18 |
in the case of | 18 |
kinetic theory of gases | 18 |
of the second order | 17 |
the velocity of the | 17 |
of the milky way | 17 |
one to the other | 17 |
the theory of lorentz | 17 |
it is a question | 16 |
a finite number of | 16 |
is equal to the | 16 |
series of muscular sensations | 16 |
at the end of | 16 |
a certain number of | 16 |
the notion of space | 16 |
the principle of least | 15 |
the principle of induction | 15 |
principle of least action | 15 |
the equality of action | 15 |
at the instant t | 15 |
at the beginning of | 15 |
it is impossible to | 15 |
it will be said | 15 |
by the aid of | 15 |
the square root of | 15 |
square root of two | 15 |
it is true that | 14 |
as i have said | 14 |
of the straight line | 14 |
there would be no | 14 |
is not the same | 14 |
it would not be | 14 |
motion of the earth | 14 |
it is proper to | 14 |
the action of the | 14 |
one of the most | 13 |
of which we have | 13 |
it is evident that | 13 |
in so far as | 13 |
this it is which | 13 |
it is true of | 13 |
however that may be | 13 |
have the right to | 13 |
i know not what | 13 |
the work of the | 13 |
this point of view | 13 |
it may happen that | 13 |
is a question of | 13 |
to say that the | 13 |
the state of the | 12 |
principle of complete induction | 12 |
the rotation of the | 12 |
of the laws of | 12 |
velocity of the earth | 12 |
the laws of chance | 12 |
to the action of | 12 |
of the first order | 12 |
in such a way | 12 |
we have just seen | 12 |
the existence of the | 12 |
space has three dimensions | 12 |
the direction of the | 12 |
the action of a | 12 |
of the physical continuum | 12 |
it will not be | 12 |
the sense of the | 12 |
and that of the | 12 |
of the motion of | 11 |
the earth turns round | 11 |
the history of science | 11 |
the laws of the | 11 |
fact in the rough | 11 |
this is why i | 11 |
that it would be | 11 |
to the theory of | 11 |
the notion of the | 11 |
it is necessary that | 11 |
to suppose that the | 11 |
may be regarded as | 11 |
it is not a | 11 |
have been able to | 11 |
the square of the | 11 |
the center of gravity | 11 |
with reference to the | 11 |
the aid of the | 11 |
we have seen that | 11 |
what is the probability | 11 |
action of a closed | 11 |
which i shall call | 11 |
the point occupied by | 11 |
of the theory of | 11 |
have no means of | 11 |
point of the retina | 11 |
the point of view | 11 |
it is the same | 11 |
point of view of | 10 |
continuum of several dimensions | 10 |
same point of space | 10 |
a at the instant | 10 |
we represent to ourselves | 10 |
an element of current | 10 |
i have said above | 10 |
same point of the | 10 |
is easy to see | 10 |
the nature of the | 10 |
the ratio of the | 10 |
since it would be | 10 |
we are led to | 10 |
in the theory of | 10 |
the principle of complete | 10 |
i have just said | 10 |
of which i have | 10 |
to be able to | 10 |
the history of the | 10 |
for its own sake | 10 |
in conformity with the | 10 |
this is not the | 10 |
that they are not | 10 |
of the notion of | 10 |
the law of acceleration | 10 |
rotation of the earth | 10 |
it can not be | 10 |
under the form of | 9 |
than all the others | 9 |
in a certain measure | 9 |
from this point of | 9 |
the complexity of the | 9 |
such a way that | 9 |
will no longer be | 9 |
no longer the same | 9 |
have nothing in common | 9 |
that space has three | 9 |
if we do not | 9 |
as we have seen | 9 |
one point to another | 9 |
space of three dimensions | 9 |
than that of the | 9 |
a and b are | 9 |
which i have just | 9 |
of the center of | 9 |
the sum of the | 9 |
accompanied by the same | 9 |
it is no longer | 9 |
a point of space | 9 |
sense of the word | 9 |
the physical continuum of | 9 |
the same for all | 9 |
the principles of mechanics | 9 |
is the probability that | 9 |
the motion of a | 9 |
have been led to | 9 |
principle of the equality | 9 |
b at the instant | 9 |
from one point to | 9 |
such and such a | 9 |
that it is necessary | 9 |
with respect to the | 9 |
of the mathematical continuum | 9 |
of a closed current | 9 |
it will be true | 9 |
the same time the | 8 |
we have just said | 8 |
the relativity of space | 8 |
of the parameters q | 8 |
the fact in the | 8 |
to which we are | 8 |
from the particular to | 8 |
it is needful to | 8 |
there is no longer | 8 |
principle of sufficient reason | 8 |
the absolute velocity of | 8 |
it is probable that | 8 |
the movements of the | 8 |
as if it were | 8 |
it is because we | 8 |
by the motion of | 8 |
the definition of the | 8 |
at the same point | 8 |
in the sense of | 8 |
be equal to the | 8 |
the principle of relative | 8 |
the eclipse happened at | 8 |
the same laws as | 8 |
it is not the | 8 |
is one of the | 8 |
is no longer a | 8 |
would have to be | 8 |
the principle of inertia | 8 |
differential equations of the | 8 |
the equality of two | 8 |
that there is no | 8 |
in the first place | 8 |
the center of the | 8 |
a function of the | 8 |
is at the same | 8 |
is the same as | 8 |
the law of the | 8 |
this is what we | 8 |
we shall say that | 8 |
be regarded as an | 8 |
be regarded as the | 8 |
to the principle of | 8 |
the part of the | 8 |
with the principle of | 8 |
the probability of causes | 8 |
the case of the | 8 |
from the point of | 8 |
the enunciation of the | 8 |
principle of relative motion | 8 |
the motions of the | 8 |
the laws of nature | 8 |
what we have just | 8 |
from one to the | 8 |
depend only on the | 8 |
the elements of the | 8 |
particular to the general | 8 |
a very great number | 8 |
is proportional to the | 8 |
the principle of sufficient | 8 |
it seems to me | 8 |
one or the other | 8 |
correspond to the same | 8 |
the particular to the | 8 |
represent to ourselves a | 8 |
the same muscular sensations | 8 |
when we say that | 8 |
but we do not | 8 |
the form of a | 7 |
the mind of the | 7 |
the mathematical continuum of | 7 |
it may be said | 7 |
the radius of the | 7 |
equations of the second | 7 |
more than three dimensions | 7 |
the number of dimensions | 7 |
of the law of | 7 |
to the same point | 7 |
in the second case | 7 |
one of the other | 7 |
accompanied by muscular sensations | 7 |
it is that the | 7 |
what does that mean | 7 |
the position of the | 7 |
i say that a | 7 |
the theory of lesage | 7 |
to the same thing | 7 |
shall be able to | 7 |
the principle of contradiction | 7 |
of the calculus of | 7 |
that there is a | 7 |
is what is called | 7 |
parts of the universe | 7 |
if it is true | 7 |
to represent to ourselves | 7 |
that it is a | 7 |
the different parts of | 7 |
this would be to | 7 |
the equations of lagrange | 7 |
is no longer the | 7 |
center of gravity of | 7 |
with regard to the | 7 |
in the physical sciences | 7 |
in the same sense | 7 |
the rest of the | 7 |
operate at a distance | 7 |
the acceleration of a | 7 |
that the principle of | 7 |
under the name of | 7 |
a weight of grams | 7 |
this is what is | 7 |
one of the elements | 7 |
in contact with the | 7 |
i have just spoken | 7 |
the beginning of the | 7 |
mutual action of two | 7 |
continuum of three dimensions | 7 |
on an element of | 7 |
of one of the | 7 |
an area of two | 7 |
from time to time | 7 |
the parts of the | 7 |
is true of n | 7 |
will be true for | 7 |
i do not know | 7 |
and it is not | 7 |
under the influence of | 7 |
according to the same | 7 |
the relative position of | 7 |
very great number of | 7 |
it is not so | 7 |
the dimensions of the | 7 |
the first of these | 7 |
of the elements of | 7 |
an infinity of ways | 7 |
of the minor planets | 6 |
at the initial instant | 6 |
the end of the | 6 |
instants alpha and beta | 6 |
the place of the | 6 |
science for its own | 6 |
in an infinity of | 6 |
carried along by the | 6 |
there can be no | 6 |
and this it is | 6 |
the inertia of the | 6 |
we should be led | 6 |
we can not represent | 6 |
how do we know | 6 |
by means of the | 6 |
a part of the | 6 |
we are forced to | 6 |
is none the less | 6 |
in what concerns the | 6 |
do not wish to | 6 |
it is true for | 6 |
of the existence of | 6 |
is clear that the | 6 |
to speak of the | 6 |
there is no absolute | 6 |
the hypothesis of lorentz | 6 |
it enables us to | 6 |
it was necessary to | 6 |
the same relative position | 6 |
if they do not | 6 |
what i have just | 6 |
and the scientific fact | 6 |
that i do not | 6 |
law of great numbers | 6 |
there is no need | 6 |
on a portion of | 6 |
can be divided by | 6 |
appear to us as | 6 |
the unity of the | 6 |
we know that the | 6 |
the probability that the | 6 |
when it is a | 6 |
the course of the | 6 |
that is not all | 6 |
number of possible cases | 6 |
in the first case | 6 |
hypothesis of central forces | 6 |
in the genesis of | 6 |
in accordance with the | 6 |
of the movements of | 6 |
the instants alpha and | 6 |
shall confine myself to | 6 |
does not mean that | 6 |
it is possible to | 6 |
a question of the | 6 |
needless to add that | 6 |
the intensity of the | 6 |
to the number of | 6 |
which enable us to | 6 |
to the square of | 6 |
depends only on the | 6 |
absolute velocity of the | 6 |
law according to which | 6 |
do not hesitate to | 6 |
and on the other | 6 |
the totality of impressions | 6 |
in a straight line | 6 |
it would be a | 6 |
in the course of | 6 |
series sigma and sigma | 6 |
to the rules of | 6 |
in the same proportion | 6 |
at the moment of | 6 |
of the logic of | 6 |
but that is not | 6 |
the hypothesis of central | 6 |
it is not enough | 6 |
which enables us to | 6 |
is the principle of | 6 |
of the heavenly bodies | 6 |
between a and b | 6 |
no longer be the | 6 |
we shall have to | 6 |
the origin of the | 6 |
the various parts of | 6 |
of a great number | 6 |
to the laws of | 6 |
of each of these | 6 |
at the center of | 6 |
and their mutual distances | 6 |
should be led to | 6 |
the existence of a | 6 |
can represent to ourselves | 6 |
is not the only | 6 |
a closed current on | 6 |
by so much the | 6 |
is due to the | 6 |
we should not have | 6 |
the law of great | 6 |
a physical continuum of | 6 |
in relation to the | 6 |
should be regarded as | 6 |
the hypothesis of the | 6 |
it is difficult to | 6 |
to the law of | 6 |
not be regarded as | 6 |
by a at the | 6 |
is not a question | 6 |
as we have said | 6 |
is to say that | 6 |
is the study of | 6 |
physical continuum of several | 6 |
the milky way is | 6 |
at the moment when | 6 |
and we can not | 6 |
what is called the | 6 |
the end of a | 6 |
motion of the center | 6 |
one of the series | 6 |
motion of a rigid | 6 |
to the study of | 6 |
one of the two | 6 |
we can represent to | 6 |
the nature of mathematical | 6 |
to the same laws | 6 |
it can only be | 6 |
the rules of the | 6 |
we have seen above | 6 |
sigma and sigma sigma | 6 |
the axis of the | 6 |
the duration of the | 6 |
that it does not | 6 |
is to say the | 6 |
the laws of motion | 6 |
it seems to us | 6 |
it would be the | 5 |
the acceleration of the | 5 |
to the same displacement | 5 |
is not to be | 5 |
a certain point of | 5 |
in such a world | 5 |
it will be the | 5 |
bound to our body | 5 |
may be replaced by | 5 |
the law of relativity | 5 |
of the various parts | 5 |
of the whole number | 5 |
represent to ourselves the | 5 |
and then it is | 5 |
that the action of | 5 |
which i attribute to | 5 |
motion with reference to | 5 |
would it not be | 5 |
if it does not | 5 |
the product of the | 5 |
we conclude that the | 5 |
is one of those | 5 |
i have spoken above | 5 |
it will always be | 5 |
closed current on a | 5 |
the same name to | 5 |
the sensation of red | 5 |
the same in the | 5 |
two series sigma and | 5 |
equal to one another | 5 |
in place of the | 5 |
the same time a | 5 |
which we do not | 5 |
occupied by a at | 5 |
that if it is | 5 |
a relation between two | 5 |
to get out of | 5 |
obey the laws of | 5 |
it is interesting to | 5 |
it is convenient to | 5 |
by the same sensation | 5 |
can not be regarded | 5 |
it may be supposed | 5 |
a member of the | 5 |
the action of b | 5 |
proportional to the square | 5 |
slight differences in the | 5 |
we have no means | 5 |
in the midst of | 5 |
so far as it | 5 |
the theory of errors | 5 |
it would be easy | 5 |
the law of inertia | 5 |
in one of the | 5 |
is not at all | 5 |
the velocities with which | 5 |
the mutual distances of | 5 |
to the totality b | 5 |
we have been led | 5 |
the points of space | 5 |
of which i spoke | 5 |
be true of the | 5 |
it could not be | 5 |
that it may be | 5 |
that the laws of | 5 |
finite number of words | 5 |
we should have no | 5 |
the progress of science | 5 |
of the angles of | 5 |
it will suffice to | 5 |
and this is what | 5 |
square of the distance | 5 |
with that of the | 5 |
are infinite in number | 5 |
is the theory of | 5 |
the surface of the | 5 |
i have said that | 5 |
carried along in a | 5 |
on the point of | 5 |
as that of the | 5 |
the relations of the | 5 |
in regard to the | 5 |
this does not mean | 5 |
right to say that | 5 |
than two right angles | 5 |
where the finger does | 5 |
by a sort of | 5 |
occupied at the instant | 5 |
of the british association | 5 |
the probability of a | 5 |
period of conscious work | 5 |
as a function of | 5 |
the genesis of the | 5 |
would be easy to | 5 |
the logic of science | 5 |
can no longer be | 5 |
as we have just | 5 |
conservation of energy and | 5 |
theorem is true of | 5 |
a way that the | 5 |
is clear that if | 5 |
more convenient to suppose | 5 |
the two parts of | 5 |
our being able to | 5 |
to that of the | 5 |
it is only the | 5 |
the theorem is true | 5 |
have said above that | 5 |
the one or the | 5 |
does not suffice to | 5 |
have no right to | 5 |
if we try to | 5 |
it is to be | 5 |
the same sense as | 5 |
state of the system | 5 |
not a question of | 5 |
the theory of hertz | 5 |
we can not know | 5 |
that two of these | 5 |
the difference between the | 5 |
is more convenient to | 5 |
to make a choice | 5 |
that we could not | 5 |
in order to be | 5 |
by saying that the | 5 |
the law of gravitation | 5 |
the present state of | 5 |
we shall see that | 5 |
the other properties of | 5 |
which we have just | 5 |
field due to the | 5 |
it is only a | 5 |
experience teaches us that | 5 |
by a series of | 5 |
nature of mathematical reasoning | 5 |
i would have to | 5 |
this is because it | 5 |
that they do not | 5 |
in the study of | 5 |
this is only a | 5 |
synthetic judgment a priori | 5 |
we know that this | 5 |
not operate at a | 5 |
say that it is | 5 |
of the earth in | 5 |
the same sensation of | 5 |
it would no longer | 5 |
continuum of n dimensions | 5 |
and at the same | 5 |
a to the totality | 5 |
we say that the | 5 |
the value of science | 5 |
the finger does not | 5 |
is necessary to make | 5 |
and yet it is | 5 |
when we seek to | 5 |
the same for the | 5 |
the details of the | 5 |
rules of formal logic | 5 |
be supposed that the | 5 |
of the same nature | 5 |
the rules of formal | 5 |
the quantity of motion | 5 |
the result of a | 5 |
all the parts of | 5 |
we should have been | 5 |
if we wished to | 5 |
less than two right | 5 |
element of current is | 5 |
it is useless to | 5 |
that it is the | 5 |
axis of the instrument | 5 |
it is necessary therefore | 5 |
to regard it as | 5 |
laws of motion of | 5 |
one from the other | 5 |
the wave of acceleration | 5 |
are transmitted to me | 5 |
among all the possible | 5 |
to the motion of | 5 |
true of the number | 5 |
is the same in | 5 |
feel the impression a | 5 |
it often happens that | 5 |
finger does not budge | 5 |
the series of muscular | 5 |
i am about to | 5 |
can not give us | 5 |
i have spoken of | 5 |
this is a question | 5 |
but this is only | 5 |
would have no meaning | 5 |
to know how to | 5 |
is no absolute space | 5 |
between the instants alpha | 5 |
sum of the angles | 5 |
whatever may be the | 5 |
the probability of this | 5 |
along by the motion | 5 |
of more than three | 5 |
it is thus that | 5 |
as rule of action | 5 |
go back to the | 5 |
in the direction of | 5 |
seem to us to | 5 |
will be said that | 5 |
the order of the | 5 |
the mutual action of | 5 |
the parameters q and | 5 |
functions t and u | 5 |
but this is because | 5 |
initial position of the | 5 |
does not operate at | 5 |
i have just explained | 5 |
on the nature of | 5 |
will not be the | 5 |
this is not so | 5 |
we have the right | 5 |
do not yet know | 5 |
the relations between the | 5 |
different points of view | 5 |
of mathematical physics the | 5 |
of the probability of | 5 |
without our being able | 5 |
is always the same | 5 |
the distances of the | 5 |
not the same for | 5 |
all the properties of | 5 |
in the presence of | 5 |
i do not believe | 5 |
does this mean that | 5 |
when i say that | 5 |
is true of the | 5 |
the order in which | 5 |
we are free to | 5 |
enables us to foresee | 5 |
in virtue of the | 5 |
the distance of the | 5 |
due to the action | 5 |
in the latter case | 4 |
alone can teach us | 4 |
parameters q and their | 4 |
that it has been | 4 |
the corpuscles of lesage | 4 |
clerk maxwell from the | 4 |
one after the other | 4 |
with regard to our | 4 |
the true nature of | 4 |
laws according to which | 4 |
the class of which | 4 |
i shall be able | 4 |
when we wish to | 4 |
as functions of the | 4 |
compatible with the principle | 4 |
the border of the | 4 |
it would be seen | 4 |
the algebraic sum of | 4 |
the principles of geometry | 4 |
genesis of the notion | 4 |
it is not necessary | 4 |
to the milky way | 4 |
so long as we | 4 |
easy to see that | 4 |
i have sought to | 4 |
is the same with | 4 |
the science of to | 4 |
of the velocity of | 4 |
that it is not | 4 |
the coordinates of the | 4 |
identical with those of | 4 |
of the square root | 4 |
intuition of pure number | 4 |
in the same relative | 4 |
is the nature of | 4 |
on an open current | 4 |
it is in this | 4 |
but as i have | 4 |
i shall call the | 4 |
affecting the same point | 4 |
which makes the unity | 4 |
but at the same | 4 |
it is one of | 4 |
do not know what | 4 |
axes invariably bound to | 4 |
to me by the | 4 |
of this or that | 4 |
generalized principle of inertia | 4 |
eclipse happened at nine | 4 |
it has often been | 4 |
would be necessary that | 4 |
as we shall see | 4 |
space of four dimensions | 4 |
the class of the | 4 |
not be able to | 4 |
are accompanied by the | 4 |
it implies no contradiction | 4 |
of our ordinary geometry | 4 |
for the study of | 4 |
of blue at the | 4 |
complicated system of inequalities | 4 |
equality of two durations | 4 |
and this is not | 4 |
it is certain that | 4 |
in the narrower sense | 4 |
pass from one to | 4 |
move according to the | 4 |
not represent to ourselves | 4 |
the aggregate of all | 4 |
give the name of | 4 |
according to which the | 4 |
it is due to | 4 |
that this is not | 4 |
the language of the | 4 |
not the right to | 4 |
is something which remains | 4 |
touch does not operate | 4 |
the same with the | 4 |
of the fixed wire | 4 |
which we have spoken | 4 |
we can make the | 4 |
what do i mean | 4 |
the presence of a | 4 |
in the rough and | 4 |
let us see what | 4 |
equal to the action | 4 |
it is said that | 4 |
yet it is not | 4 |
it is often said | 4 |
must be able to | 4 |
velocity in relation to | 4 |
it is more convenient | 4 |
at the outset of | 4 |
motions of the ether | 4 |
each of them is | 4 |
that it is convenient | 4 |
the right to say | 4 |
at a glance the | 4 |
be the point of | 4 |
the definition by postulates | 4 |
it is just the | 4 |
it is only by | 4 |
a synthetic judgment a | 4 |
enunciation of the law | 4 |
only one side of | 4 |
is due to chance | 4 |
a direct intuition of | 4 |
in the first class | 4 |
indistinguishable from the preceding | 4 |
the shortest path from | 4 |
to a series of | 4 |
of these two objects | 4 |
the locus of points | 4 |
through a given point | 4 |
one upon the other | 4 |
that of the earth | 4 |
virtue of the principle | 4 |
enable us to reach | 4 |
it is not alone | 4 |
the number of possible | 4 |
the mass coefficient of | 4 |
at a given instant | 4 |
to represent to oneself | 4 |
i do not hesitate | 4 |
all in one piece | 4 |
of red at the | 4 |
the two sorts of | 4 |
the relation of the | 4 |
the principle of reaction | 4 |
to the needs of | 4 |
a little more closely | 4 |
those of the second | 4 |
the initial values of | 4 |
true for c gamma | 4 |
to the physical sciences | 4 |
we have seen the | 4 |
is it possible to | 4 |
the action of an | 4 |
that the motion of | 4 |
all the points of | 4 |
milky way is not | 4 |
of the semicircular canals | 4 |
true for b beta | 4 |
are very numerous and | 4 |
according to the theory | 4 |
duration of the transmission | 4 |
with the velocity of | 4 |
all we can say | 4 |
we can not say | 4 |
translated into another language | 4 |
of a rigid figure | 4 |
is to say a | 4 |
to the properties of | 4 |
we no longer have | 4 |
that of the conservation | 4 |
function of the velocity | 4 |
if we can not | 4 |
with the laws of | 4 |
the angles of a | 4 |
absolute position and orientation | 4 |
the lines of the | 4 |
and the theory of | 4 |
various parts of the | 4 |
since this is the | 4 |
the relations of bodies | 4 |
it is therefore necessary | 4 |
to pass from the | 4 |
we see that the | 4 |
is to say to | 4 |
distances of the planets | 4 |
will be equal to | 4 |
we are tempted to | 4 |
it would be to | 4 |
this is what i | 4 |
to account for this | 4 |
bodies a and b | 4 |
of which it is | 4 |
existence of the object | 4 |
on the magnetic needle | 4 |
something which remains constant | 4 |
we shall be able | 4 |
this is because the | 4 |
it may be asked | 4 |
that at the instant | 4 |
more and more complicated | 4 |
are not altered by | 4 |
perhaps it will be | 4 |
if we wish to | 4 |
it is in the | 4 |
that it is true | 4 |
the same way as | 4 |
the rough and the | 4 |
the aggregate of these | 4 |
to give the name | 4 |
the axioms of geometry | 4 |
of blue and yellow | 4 |
of which we can | 4 |
and it would be | 4 |
it will be necessary | 4 |
this it is that | 4 |
what is a point | 4 |
the laws according to | 4 |
the first principles of | 4 |
is that the first | 4 |
corrected by a correlative | 4 |
makes the unity of | 4 |
and which i shall | 4 |
two parts of the | 4 |
in the kinetic theory | 4 |
a tenth of a | 4 |
us that space has | 4 |
we have just spoken | 4 |
always be necessary to | 4 |
and that it is | 4 |
position with regard to | 4 |
the generalized principle of | 4 |
it might be supposed | 4 |
so much the more | 4 |
of a rigid solid | 4 |
comes to the same | 4 |
to act as if | 4 |
the mutual relations of | 4 |
the same if we | 4 |
distribution of the minor | 4 |
the position of this | 4 |
and b at the | 4 |
it will be impossible | 4 |
it is on the | 4 |
point occupied by a | 4 |
for the cathode rays | 4 |
end of a certain | 4 |
the results of this | 4 |
to show that the | 4 |
the theory of energy | 4 |
this is a very | 4 |
the mean value of | 4 |
as well as to | 4 |
the instant t a | 4 |
regard to our body | 4 |
am i led to | 4 |
greater than all the | 4 |
is the same for | 4 |
we should never have | 4 |
elements a and b | 4 |
that the object a | 4 |
the point of the | 4 |
the general principles of | 4 |
what i wish to | 4 |
the aggregate of the | 4 |
have just seen that | 4 |
of the number of | 4 |
our table of distribution | 4 |
that of the body | 4 |
in the motion of | 4 |
the same time to | 4 |
like that of the | 4 |
it is not only | 4 |
relation to those of | 4 |
the properties of the | 4 |
a series of muscular | 4 |
only a question of | 4 |
from all external action | 4 |
a rule of action | 4 |
is not the case | 4 |
to see in it | 4 |
the scientific fact is | 4 |
the future of mathematics | 4 |
we should not be | 4 |
let us pass to | 4 |
this is not enough | 4 |
there is only one | 4 |
that i have not | 4 |
a small number of | 4 |
one or several continua | 4 |
that we have not | 4 |
have spoken above of | 4 |
as many dimensions as | 4 |
way of looking at | 4 |
sensation of red at | 4 |
of the cathode rays | 4 |
that the science of | 4 |
be replaced by another | 4 |
two elements a and | 4 |
the beginning of this | 4 |
be said that this | 4 |
they are the most | 4 |
to the other by | 4 |
what do we mean | 4 |
tempted to say that | 4 |
admit the hypothesis of | 4 |
surfaces of constant curvature | 4 |
so far as concerns | 4 |
the molecules of a | 4 |
each of these elements | 4 |
of the same order | 4 |
as i have just | 4 |
the objective value of | 4 |
with an area of | 4 |
if we had not | 4 |
that each of them | 4 |
if we did not | 4 |
we are about to | 4 |
of the continuum c | 4 |
and of which we | 4 |
the distribution of the | 4 |
it is because the | 4 |
square with an area | 4 |
bodies and their mutual | 4 |
who do not understand | 4 |
the theory of the | 4 |
i shall confine myself | 4 |
not be the same | 4 |
can do is to | 4 |
objective value of science | 4 |
shortest path from one | 4 |
from one of the | 4 |
the presence of the | 4 |
that we represent to | 4 |
a system of postulates | 4 |
of reasoning by recurrence | 4 |
relative position with regard | 4 |
it would be only | 4 |
the straight line is | 4 |
and it will be | 4 |
we shall say c | 4 |
do not at all | 4 |
as well as the | 4 |
at the point a | 4 |
conclude that it is | 4 |
an idea of the | 4 |
it is that we | 4 |
but if it is | 4 |
on a closed current | 4 |
what we have said | 4 |
yet i can not | 4 |
when its clock marks | 4 |
the milky way and | 4 |
the free activity of | 4 |
theorem is true for | 4 |
the field due to | 4 |
of the possibility of | 4 |
the light coming from | 4 |
the mutual actions of | 4 |
characteristics of the physical | 4 |
angles of a triangle | 4 |
the unity of nature | 4 |
to the product of | 4 |
odd numbers divided by | 4 |
is no need of | 4 |
would be better to | 4 |
with the aid of | 4 |
two bodies a and | 4 |
be due to chance | 4 |
calculus of probabilities is | 4 |
not the same in | 4 |
that of the sun | 4 |
a property of the | 4 |
i shall try to | 4 |
from a to b | 4 |
is the cause of | 4 |
choice must be made | 4 |
is indistinguishable from the | 4 |
is clear that this | 4 |
to affirm that the | 4 |
of a triangle is | 4 |
the instant alpha and | 4 |
of a certain time | 4 |
a complicated system of | 4 |
the theory of numbers | 4 |
tell us that the | 4 |
is nothing but the | 4 |
of light is not | 4 |
the general theory of | 4 |
be a member of | 4 |
center of the retina | 4 |
a difference of a | 4 |
this is a problem | 4 |
we find that the | 4 |
by b at the | 4 |
is the origin of | 4 |
on the state of | 4 |
this is the only | 4 |
one of those which | 4 |
if this were so | 4 |
each other in the | 4 |
the existence of an | 4 |
in the development of | 4 |
of the science of | 4 |
their mutual distances at | 4 |
will appear to us | 4 |
of the object defined | 4 |
the stars of the | 4 |
it is because they | 4 |
we think we know | 4 |
that it is impossible | 4 |
but that would be | 4 |
of the body a | 4 |
parallel to the motion | 4 |
is identical with the | 4 |
my finger at the | 4 |
greater than that of | 4 |
relative motion with reference | 4 |
action at a distance | 4 |
of no use to | 4 |
in the light of | 4 |
i do not say | 4 |
may happen that the | 4 |
by one of the | 4 |
is because we have | 4 |
have we the right | 4 |
the same external change | 4 |
it is needless to | 4 |
the use of the | 4 |
to take account of | 4 |
james clerk maxwell from | 4 |
if they are not | 4 |
there is something which | 4 |
there can not be | 4 |
us that it is | 4 |
the moment of the | 4 |
position of the star | 4 |
of the constitution of | 4 |
the ray of light | 4 |
relation to the ether | 4 |
it would be better | 4 |
q and their derivatives | 4 |
without the aid of | 4 |
in the history of | 4 |
have not the right | 4 |
that a and b | 4 |
there would no longer | 4 |
to a sort of | 4 |
to those of the | 4 |
it would have been | 4 |
i should like to | 4 |
because it would be | 4 |
far as it is | 4 |
path from one point | 4 |
current on a portion | 4 |
we have said above | 4 |
to a given straight | 4 |
in the hands of | 4 |
the circuit c is | 4 |
can not represent to | 4 |
of the series sigma | 4 |
a system of n | 4 |
being able to perceive | 4 |
i do not wish | 4 |
is necessary therefore to | 4 |
it be said that | 4 |
must be regarded as | 4 |
one and the same | 4 |
less than all the | 4 |
what may be called | 4 |
if there is no | 4 |
side of the question | 4 |
be represented by a | 4 |
this is the principle | 4 |
the probable value of | 4 |
under the action of | 4 |
it is above all | 4 |
the absence of contradiction | 4 |
to the n th | 4 |
to their initial positions | 4 |
from b to a | 4 |
i have explained in | 4 |
and it is easy | 4 |
there would be nothing | 4 |
it is not at | 4 |
of muscular sensations s | 4 |
from the action of | 4 |
it would suffice to | 4 |
it is time to | 4 |
get an idea of | 3 |
is this the case | 3 |
by a continuous function | 3 |
of which we speak | 3 |
the same order of | 3 |
a law of nature | 3 |
this would no longer | 3 |
that we must be | 3 |
do not need to | 3 |
relative position of the | 3 |
a correlative voluntary movement | 3 |
impossible to represent to | 3 |
go from a to | 3 |
should have no means | 3 |
a small part of | 3 |
they would be led | 3 |
equality of two forces | 3 |
thence to conclude that | 3 |
us to the same | 3 |
idea came to me | 3 |
the fictitious electromagnetic mass | 3 |
may be supposed that | 3 |
be the same for | 3 |
remains in contact with | 3 |
to a given number | 3 |
the same direction as | 3 |
if this be so | 3 |
of the side of | 3 |
of two open currents | 3 |
this way of looking | 3 |
is above all because | 3 |
such a way as | 3 |
chalk on a blackboard | 3 |
be of no use | 3 |
and it is from | 3 |
of energy and the | 3 |
it would not have | 3 |
it would therefore be | 3 |
the method of the | 3 |
by the body it | 3 |
shall say that the | 3 |
of gravity of the | 3 |
the top number is | 3 |
at the present time | 3 |
finite number of objects | 3 |
that the properties of | 3 |
impression which i attribute | 3 |
us that a certain | 3 |
could just as well | 3 |
to the probability of | 3 |
to the radius of | 3 |
i am certain that | 3 |
yields an area of | 3 |
identity of two points | 3 |
would be no science | 3 |
from a certain initial | 3 |
is the belief in | 3 |
in the eyes of | 3 |
can not do without | 3 |
the totality a to | 3 |
more probable than a | 3 |
be so defined that | 3 |
data of our senses | 3 |
history of mathematical physics | 3 |
when we try to | 3 |
state of the world | 3 |
due to the motion | 3 |
as in the preceding | 3 |
a straight and uniform | 3 |
the point b is | 3 |
soul of the fact | 3 |
are equal to one | 3 |
objects with regard to | 3 |
identical with the point | 3 |
to the kinetic theory | 3 |
and it is because | 3 |
beyond the reach of | 3 |
represent to myself the | 3 |
of the third order | 3 |
then be regarded as | 3 |
to do is to | 3 |
elements of this continuum | 3 |
the errors of observation | 3 |
have the intuition of | 3 |
my muscular sense tells | 3 |
a rigid figure is | 3 |
mass will no longer | 3 |
to the consideration of | 3 |
in the same manner | 3 |
the investigation of the | 3 |
of the rotation of | 3 |
admit the principle of | 3 |
through these two points | 3 |
since it would have | 3 |
but it would not | 3 |
is true for c | 3 |
the sense of sight | 3 |
that this probability is | 3 |
we find that this | 3 |
the limit toward which | 3 |
that does not mean | 3 |
in the second place | 3 |
relations of bodies to | 3 |
the problem of the | 3 |
inertia of the ether | 3 |
of the solar system | 3 |
the side of the | 3 |
is necessary that the | 3 |
according to the laws | 3 |
given to this word | 3 |
this something else is | 3 |
i can not here | 3 |
so that we may | 3 |
with relation to the | 3 |
that all the world | 3 |
the same as that | 3 |
creation of the mathematical | 3 |
i know not whether | 3 |
only on the position | 3 |
the development of the | 3 |
in place of saying | 3 |
than in the other | 3 |
the midst of a | 3 |
of the body p | 3 |
the velocities of the | 3 |
the coordinates of these | 3 |
they could be made | 3 |
the measurement of time | 3 |
the importance of this | 3 |
in that of the | 3 |
remain true if the | 3 |
on the relations of | 3 |
shall say c has | 3 |
of our body in | 3 |
to apply it to | 3 |
equal to two right | 3 |
no right to say | 3 |
not to suppose that | 3 |
aggregate of all the | 3 |
of the history of | 3 |
can only be done | 3 |
same for all the | 3 |
a mechanical explanation of | 3 |
no one doubts that | 3 |
the weight of the | 3 |
the interior of the | 3 |
the properties of phosphorus | 3 |
as a consequence of | 3 |
because it is the | 3 |
as far as possible | 3 |
impossible for us to | 3 |
from one position to | 3 |
which is the object | 3 |
which we are accustomed | 3 |
probability in the physical | 3 |
no longer have any | 3 |
for the first time | 3 |
the question is to | 3 |
changes of state from | 3 |
is the effect of | 3 |
represent it to ourselves | 3 |
even numbers divided by | 3 |
of the electromagnetic field | 3 |
not only that it | 3 |
above all because it | 3 |
ratio of these two | 3 |
in a perfect fluid | 3 |
may happen that we | 3 |
which can be divided | 3 |
to the first of | 3 |
and i shall not | 3 |
of a very great | 3 |
but it suffices that | 3 |
value of sin nu | 3 |
of the earth with | 3 |
function of the parameters | 3 |
by the movements of | 3 |
question is to know | 3 |
the same as for | 3 |
represented by a continuous | 3 |
of energy and of | 3 |
it might always be | 3 |
the series s sigma | 3 |
movements corresponding to the | 3 |
which will divide c | 3 |
it be necessary to | 3 |
whether it is the | 3 |
history of the development | 3 |
represent to ourselves external | 3 |
so far as i | 3 |
may be corrected by | 3 |
with a finite number | 3 |
are those in which | 3 |
movements where the finger | 3 |
of the acceleration of | 3 |
in a certain order | 3 |
if we admit the | 3 |
we know that it | 3 |
the theory of gases | 3 |
the statement of a | 3 |
distinguishes it from the | 3 |
this is all that | 3 |
perceive at a glance | 3 |
between the instants beta | 3 |
is in the same | 3 |
a theorem is true | 3 |
action of two elements | 3 |
the test of experiment | 3 |
of which the only | 3 |
the meaning of the | 3 |
direct intuition of the | 3 |
and it is in | 3 |
of the earth would | 3 |
would be necessary for | 3 |
we pass from the | 3 |
they are those which | 3 |
locus of points where | 3 |
have no way of | 3 |
definition implies no contradiction | 3 |
of the same sense | 3 |
general principles of dynamics | 3 |
up to the present | 3 |
element of the continuum | 3 |
the measurement of the | 3 |
would be to forget | 3 |
the general to the | 3 |
is at once seen | 3 |
act on one another | 3 |
to see that the | 3 |
the totality of our | 3 |
subjected to the action | 3 |
such or such a | 3 |
to the class of | 3 |
we are obliged to | 3 |
by a correlative voluntary | 3 |
have a point in | 3 |
might be supposed that | 3 |
that the scientist creates | 3 |
all parts of the | 3 |
be true of all | 3 |
jupiter at the instant | 3 |
no longer be true | 3 |
be an even number | 3 |
i have not been | 3 |
is the part of | 3 |
we can say is | 3 |
the other hand the | 3 |
it is not in | 3 |
subjected to no force | 3 |
but we can not | 3 |
this is the first | 3 |
the sides of the | 3 |
from the totality a | 3 |
most recent conquests of | 3 |
but this is a | 3 |
b of the retina | 3 |
number is four times | 3 |
position of this body | 3 |
is easy to understand | 3 |
the same number of | 3 |
the aid of a | 3 |
at rest or in | 3 |
in the same class | 3 |
it is from this | 3 |
but they are not | 3 |
theories of modern physics | 3 |
curve has a tangent | 3 |
occupied by b at | 3 |
ratio of the charge | 3 |
to us to be | 3 |
by the principle of | 3 |
may be useful to | 3 |
that these two objects | 3 |
force is equal to | 3 |
this is one of | 3 |
by an even number | 3 |
the one hand the | 3 |
and consequently that the | 3 |
then we should have | 3 |
and to show that | 3 |
in two different ways | 3 |
a more or less | 3 |
of i know not | 3 |
you know what i | 3 |
nothing prevents our supposing | 3 |
of the relativity of | 3 |
respect to the time | 3 |
belongs to the class | 3 |
true if the figures | 3 |
which the only member | 3 |
of the n th | 3 |
will be by definition | 3 |
if the number of | 3 |
of the relations of | 3 |
try to represent to | 3 |
the science of mathematics | 3 |
and not of the | 3 |
may not say that | 3 |
to reveal to him | 3 |
part of the energy | 3 |
have said that the | 3 |
that these two sensations | 3 |
these two sorts of | 3 |
in the enunciation of | 3 |
if we look at | 3 |
not hesitate to say | 3 |
see in it only | 3 |
complexity of the causes | 3 |
the second degree of | 3 |
revealed to us by | 3 |
it is possible that | 3 |
which i wish to | 3 |
this is a fact | 3 |
let us now consider | 3 |
which is only a | 3 |
a square with an | 3 |
we refuse to admit | 3 |
only one of these | 3 |
conformity with the laws | 3 |
straight and uniform motion | 3 |
capable of correcting the | 3 |
a current of convection | 3 |
felt by the finger | 3 |
analogous to those we | 3 |
if it were so | 3 |
convergence of the eyes | 3 |
the density of the | 3 |
be true for a | 3 |
the laws of astronomy | 3 |
border of the retina | 3 |
we are no longer | 3 |
principles of mechanics and | 3 |
according to which these | 3 |
that we have a | 3 |
transmitted to me by | 3 |
that the rotation of | 3 |
instants beta and beta | 3 |
falls under our senses | 3 |
the values of these | 3 |
because they are the | 3 |
know how to recognize | 3 |
i have been able | 3 |
of the fact that | 3 |
can have only one | 3 |
a multitude of different | 3 |
themselves to the mind | 3 |
is the number of | 3 |
suffice to determine the | 3 |
which can neither be | 3 |
on a magnetic pole | 3 |
be as simple as | 3 |
is so great that | 3 |
be better to say | 3 |
rules of the game | 3 |
is necessary for the | 3 |
is only a particular | 3 |
one side of the | 3 |
totality a to the | 3 |
is that of the | 3 |
the same as in | 3 |
we say that it | 3 |
because these spaces are | 3 |
analytically that if it | 3 |
there could be no | 3 |
seen that it is | 3 |
us nothing about the | 3 |
of the eighteenth century | 3 |
apply it to the | 3 |
the means we have | 3 |
more or less imperfect | 3 |
of the human mind | 3 |
the principles of dynamics | 3 |
the object b has | 3 |
or that of the | 3 |
the influence of the | 3 |
a distance one upon | 3 |
as the square of | 3 |
work of the electrodynamic | 3 |
the problems of probability | 3 |
and for that it | 3 |
the scientist create science | 3 |
terms of the first | 3 |
rotation of the head | 3 |
in the ordinary theory | 3 |
in particular those of | 3 |
to compare the two | 3 |
acceleration of a body | 3 |
this is why these | 3 |
that at the end | 3 |
the result of this | 3 |
after what we have | 3 |
because they are not | 3 |
of state from changes | 3 |
for all these reasons | 3 |
the case of closed | 3 |
these spaces are both | 3 |
are accompanied by muscular | 3 |
or at least the | 3 |
present state of the | 3 |
is only a question | 3 |
does not depend upon | 3 |
between the fact in | 3 |
because i do not | 3 |
to show that a | 3 |
root of two is | 3 |
a way as to | 3 |
colours of the spectrum | 3 |
repugnant to the mind | 3 |
be necessary to have | 3 |
will be associated with | 3 |
the changes of position | 3 |
contradiction up to the | 3 |
will always be necessary | 3 |
properties of the straight | 3 |
teach us the true | 3 |
shall see that the | 3 |
what is the nature | 3 |
we have not been | 3 |
great differences in the | 3 |
we have not the | 3 |
which falls under our | 3 |
the image of a | 3 |
function of t u | 3 |
but it will be | 3 |
in place of being | 3 |
be said that the | 3 |
the theorems of analysis | 3 |
were identical with those | 3 |
of b upon a | 3 |
gravity of this system | 3 |
is it necessary to | 3 |
i only wish to | 3 |
what is the probable | 3 |
is seen in the | 3 |
the sum of two | 3 |
reconcile it with the | 3 |
that it was right | 3 |
but we know that | 3 |
the science of the | 3 |
to two right angles | 3 |
electromagnetic theory of light | 3 |
applied to the body | 3 |
the application of the | 3 |
that the algebraic sum | 3 |
we have no reason | 3 |
the distance from the | 3 |
certain point of view | 3 |
the first degree of | 3 |
do not know whether | 3 |
there is no way | 3 |
a complete mechanical explanation | 3 |
this is why we | 3 |
the muscular sensations which | 3 |
does the scientist create | 3 |
to be regarded as | 3 |
point occupied by b | 3 |
but it can not | 3 |
the age of the | 3 |
the same structure as | 3 |
form imposed upon our | 3 |
i have ascertained that | 3 |
the velocity according to | 3 |
we try to imagine | 3 |
their positions at the | 3 |
might be tempted to | 3 |
measure the velocity of | 3 |
the definition will be | 3 |
maxwell from the report | 3 |
which we can not | 3 |
if there were no | 3 |
cuts that are called | 3 |
acts at a distance | 3 |
of the sun and | 3 |
will depend on the | 3 |
teaches us that the | 3 |
it is always the | 3 |
the aid of astronomic | 3 |
in order to understand | 3 |
a portion of current | 3 |
depend on the absolute | 3 |
the effects of the | 3 |
we are thus led | 3 |
from a weight of | 3 |
precisely in the same | 3 |
may be as simple | 3 |
so far as to | 3 |
we have given above | 3 |
the name of straights | 3 |
the object a occupied | 3 |
it does not stand | 3 |
to the example of | 3 |
is a function of | 3 |
the difficulties raised by | 3 |
distances at any instant | 3 |
sum of two terms | 3 |
is a continuum of | 3 |
a given number x | 3 |
totality of impressions a | 3 |
a form imposed upon | 3 |
is the aggregate of | 3 |
the notion of point | 3 |
we can do is | 3 |
at the first glance | 3 |
it is which is | 3 |
sensations affecting the same | 3 |
by means of a | 3 |
c is a continuum | 3 |
contraction in the sense | 3 |
foreign to one another | 3 |
according to certain laws | 3 |
all the world will | 3 |
of straights to the | 3 |
to some of the | 3 |
strangers to one another | 3 |
the right to give | 3 |
that would be to | 3 |
of a closed solenoid | 3 |
be reduced to a | 3 |
the possibility of this | 3 |
of axes invariably bound | 3 |
regard to one another | 3 |
in a few words | 3 |
us the notion of | 3 |
they are accompanied by | 3 |
a property common to | 3 |
what do we see | 3 |
is necessary to see | 3 |
will be true of | 3 |
be regarded as identical | 3 |
is not enough that | 3 |
do we know that | 3 |
the origin of this | 3 |
the only member is | 3 |
the result of an | 3 |
much greater than that | 3 |
when multiplied by itself | 3 |
to justify this definition | 3 |
of the measurement of | 3 |
say that c is | 3 |
not be said that | 3 |
a point of the | 3 |
sense of the motion | 3 |
to distinguish among them | 3 |
parts of our body | 3 |
that we have the | 3 |
in the work of | 3 |
the attraction exercised by | 3 |
the demonstrations of the | 3 |
the probability that a | 3 |
invariably bound to our | 3 |
axes to which we | 3 |
to the ground like | 3 |
and if it is | 3 |
the vis viva of | 3 |
are no longer in | 3 |
to the surface of | 3 |
it is just this | 3 |
mean to say that | 3 |
not mean to say | 3 |
make movements which produce | 3 |
synthetic a priori judgment | 3 |
i represent to myself | 3 |
with those of non | 3 |
report of the british | 3 |
of all the known | 3 |
in a certain way | 3 |
be proportional to the | 3 |
from the report of | 3 |
we assume that the | 3 |
the intervention of the | 3 |
is only a crude | 3 |
state from changes of | 3 |
that we can not | 3 |
if we adopt the | 3 |
to a gas in | 3 |
when we shall have | 3 |
of representing to oneself | 3 |
science would be impossible | 3 |
and that is why | 3 |
in the initial conditions | 3 |
by the finger d | 3 |
from a certain point | 3 |
be true in the | 3 |
cut which will divide | 3 |
composed of two parts | 3 |
will still be true | 3 |
those of the ether | 3 |
of each of them | 3 |
by the same muscular | 3 |
a mechanical explanation to | 3 |
of the molecules of | 3 |
top number is four | 3 |
of bodies and their | 3 |
act as if it | 3 |
of a finite number | 3 |
is represented by a | 3 |
can be reduced to | 3 |
there is no reason | 3 |
which we shall call | 3 |
enable us to foresee | 3 |
which consists in adding | 3 |
the structure of the | 3 |
the charge to the | 3 |
the same as if | 3 |
which is that of | 3 |
a continuum of three | 3 |
the positions of the | 3 |
to the eyes of | 3 |
velocities and of the | 3 |
nothing of the sort | 3 |
continuum of one dimension | 3 |
school of the thread | 3 |
to depend upon the | 3 |
the body it traverses | 3 |
of space is not | 3 |
to bring in the | 3 |
which may be regarded | 3 |
i have not budged | 3 |
to those we have | 3 |
but how shall we | 3 |
which the calculus of | 3 |
is only in the | 3 |
position of the system | 3 |
distinguishable from one another | 3 |
have the same meaning | 3 |
case of closed currents | 3 |
the probability of the | 3 |
know that it is | 3 |
it is because of | 3 |
resistance of the medium | 3 |
two sorts of energy | 3 |
i have the right | 3 |
for the negative electrons | 3 |
with regard to one | 3 |
as an experimental law | 3 |
no longer in the | 3 |
to suppose the earth | 3 |
of mathematics and physics | 3 |
the forces to which | 3 |
would not be the | 3 |
the absolute position of | 3 |
of the universe and | 3 |
i mean by that | 3 |
great number of elementary | 3 |
but i do not | 3 |
calculus of probabilities to | 3 |
attribute it to chance | 3 |
a hundred years ago | 3 |
of which i shall | 3 |
that it must be | 3 |
probability of this or | 3 |
do we know whether | 3 |
point occupied by the | 3 |
i think i have | 3 |
to have the right | 3 |
this is just what | 3 |
acceleration of the motion | 3 |
of the left arm | 3 |
him to make a | 3 |
the same relations as | 3 |
to the body c | 3 |
of the fixed part | 3 |
an infinity of others | 3 |
indistinguishable from one of | 3 |
about the nature of | 3 |
is true that it | 3 |
the red sensations affecting | 3 |
are called changes of | 3 |
we are able to | 3 |
of a and b | 3 |
say that this continuum | 3 |
study of the laws | 3 |
have undergone the same | 3 |
those of the first | 3 |
and accompanied by muscular | 3 |
to adopt the first | 3 |
the constitution of bodies | 3 |
a thousand times greater | 3 |
the resistance of the | 3 |
be replaced by the | 3 |
the most important of | 3 |
have any means of | 3 |
give the same name | 3 |
two right angles in | 3 |
to the position b | 3 |
the foundations of science | 3 |
with those of the | 3 |
that it is proper | 3 |
in the same direction | 3 |
we are accustomed to | 3 |
the sensations of the | 3 |
to the movements of | 3 |
of the object a | 3 |
of an infinity of | 3 |
mutual distances of the | 3 |
it is not always | 3 |
we the right to | 3 |
no longer be constant | 3 |
i will explain myself | 3 |
only a part of | 3 |
we can no longer | 3 |
the nature of these | 3 |
equal to each other | 3 |
that it implies no | 3 |
is to know whether | 3 |
apparent position of the | 3 |
of the hypothetical molecules | 3 |
can teach us nothing | 3 |
of the nervous system | 3 |
see at a glance | 3 |
for a mechanical explanation | 3 |
with the object a | 3 |
shall we say that | 3 |
have no reason to | 3 |
the light of the | 3 |
have been subjected to | 3 |
what do we do | 3 |
is why i have | 3 |
not necessary that the | 3 |
had to make a | 3 |
see in it the | 3 |
finger at the instant | 3 |
is less than the | 3 |
a thousand times more | 3 |
know geometry can not | 3 |
light of the sun | 3 |
at a distance one | 3 |
something else is the | 3 |
is of no use | 3 |
and this is the | 3 |
this is what he | 3 |
we shall then have | 3 |
this is why the | 3 |
will correspond a point | 3 |
the reaction of the | 3 |
but the history of | 3 |
two series s and | 3 |
the laws of this | 3 |
are of the same | 3 |
the soul of the | 3 |
the displacement of the | 3 |
which would enable us | 3 |
the beginning of his | 3 |
physics of central forces | 3 |
i wish to speak | 3 |
for the most part | 3 |
the velocity of a | 3 |
the physical nature of | 3 |
the conditions under which | 3 |
geometry can not reason | 3 |
seems to me that | 3 |
the idea came to | 3 |
true nature of things | 3 |
touches my finger at | 3 |
a corner of the | 3 |
in the preceding pages | 3 |
would enable us to | 3 |
is difficult not to | 3 |
could not be done | 3 |
body depends only upon | 3 |
the instants beta and | 3 |
do not see that | 3 |
would have to give | 3 |
will be necessary to | 3 |
to the same danger | 3 |
point of view is | 3 |
the values of the | 3 |
the point corresponding to | 3 |
we may say that | 3 |
with the notion of | 3 |
position of the body | 3 |
muscular sensations which accompany | 3 |
would remain true if | 3 |
then it will be | 3 |
in a world where | 3 |
make the movements corresponding | 3 |
isolated from all external | 3 |
of a physical continuum | 3 |
we can pass from | 3 |
hypotheses in the narrower | 3 |
would not have the | 3 |
that it is so | 3 |
we do not yet | 3 |
the theory of algebraic | 3 |
less than that of | 3 |
one point of the | 3 |
rough and the scientific | 3 |
it there would be | 3 |
of the first class | 3 |
to have recourse to | 3 |
dimensions of the milky | 3 |
as the boundaries of | 3 |
saturn at the instant | 3 |
right to speak of | 3 |
does not enable us | 3 |
the aid of this | 3 |
to the point of | 3 |
the moment when the | 3 |
the study of these | 3 |
shall say that c | 3 |
space which is the | 3 |
is the probable value | 3 |
difference between the two | 3 |
confirmed nor refuted by | 3 |
eclipse happened at the | 3 |
for the same reason | 3 |
the new methods of | 3 |
theorems of analysis situs | 3 |
been led to distinguish | 3 |
logical point of view | 3 |
i do not mean | 3 |
the discovery of the | 3 |
the notion of this | 3 |
no longer be a | 3 |
what will be the | 3 |
the harmony of the | 3 |
the two energies t | 3 |
to us as a | 3 |
in relation to those | 3 |
is necessary to apply | 3 |
from the general to | 3 |
the importance of the | 3 |
by the action of | 3 |
of atoms and void | 3 |
can in no way | 3 |
of the wave of | 3 |
we must not forget | 3 |
be at the same | 3 |
lead us to the | 3 |
we shall have the | 3 |
as little as you | 3 |
at the time t | 3 |
as a synthetic judgment | 3 |
this condition is fulfilled | 3 |
the movements corresponding to | 3 |
and the origin of | 3 |
it be supposed that | 3 |
in contact with this | 3 |
a course of experimental | 3 |
and can not be | 3 |
if we can pass | 3 |
the conditions of the | 3 |
thus it is that | 3 |
all distinguishable from one | 3 |
other properties of the | 3 |
if we had known | 3 |
that the length of | 3 |
the earth in its | 3 |
nothing in common with | 3 |
the english and americans | 3 |
is that of a | 3 |
made known to us | 3 |
no longer anything but | 3 |
to which it is | 3 |
will be the same | 3 |
the characteristics of the | 3 |
is therefore impossible to | 3 |
cease to be true | 3 |
it does not suffice | 3 |
and it has been | 3 |
let us now see | 3 |
the variation of the | 3 |
be led to conclude | 3 |
an infinity of them | 3 |
a large number of | 3 |
their derivatives with respect | 3 |
to distinguish between the | 3 |
a reason for distrust | 3 |
place in the world | 3 |
to us by our | 3 |
that light is a | 3 |
i confine myself to | 3 |
led to distinguish the | 3 |
an example of a | 3 |
is a point of | 3 |
a cut which will | 3 |
the point a and | 3 |
can say is that | 3 |
made at the outset | 3 |
and it is for | 3 |
the definition of a | 3 |
inversely as the square | 3 |
four times some whole | 3 |
continuum of the second | 3 |
force which acts on | 3 |
of the nearest stars | 3 |
is in contact with | 3 |
the example of the | 3 |
we suppose the velocity | 3 |
is independent of the | 3 |
axes rigidly bound to | 3 |
the object a has | 3 |
as if it had | 3 |
say that they are | 3 |
the concept of the | 3 |
introduce the notion of | 3 |
sensations of the same | 3 |
be found in the | 3 |
every branch of physics | 3 |
come to us from | 3 |
he is about to | 3 |
in the existence of | 3 |
from that of the | 3 |
it has three dimensions | 3 |
corresponding to the series | 3 |
we do not wish | 3 |
the position of jupiter | 3 |
the same relative situation | 3 |
not enable us to | 3 |
general to the particular | 3 |
energies t and u | 3 |
the most recent conquests | 3 |
the intuition of pure | 3 |
to distinguish changes of | 3 |
since we can not | 3 |
of what use is | 3 |
same order of magnitude | 3 |
is not necessary that | 3 |
point of the body | 3 |
for us not to | 3 |
of two whole numbers | 3 |
as a branch of | 3 |
as simple as possible | 3 |
to the sides of | 3 |
to be content with | 3 |
which has taught us | 3 |
a system of axes | 3 |
mechanical explanation to be | 3 |
the finger is found | 3 |
it is because it | 3 |
the eyes of the | 3 |
the real mass is | 3 |
of the neighboring bodies | 3 |
any two elements a | 3 |
it is because i | 3 |
that not every one | 3 |
property common to all | 3 |
convenient to suppose the | 3 |
that the principles of | 3 |
the possibility of a | 3 |
do not believe that | 3 |
of a multitude of | 3 |
in no way be | 3 |
has often been said | 3 |
it would then be | 3 |
the number of these | 3 |
class of which the | 3 |
the two series of | 3 |
a and b of | 3 |
numerous and very different | 3 |
is no longer any | 3 |
principles of geometry are | 3 |
there is a law | 3 |
straights to the sides | 3 |
that the ether is | 3 |
we must be sure | 3 |
it would be proper | 3 |
the problems of the | 3 |
that it is to | 3 |
same time to produce | 3 |
we have no right | 3 |
will depend only on | 3 |
of all the forces | 3 |
in the inverse ratio | 3 |
of the equations of | 3 |
i well know that | 3 |
conservation of energy is | 3 |
aid of the senses | 3 |
that in such a | 3 |
positions at the instant | 3 |
that this mean value | 3 |
physical nature of the | 3 |
times some whole number | 3 |
in the hypothesis of | 3 |
most important of all | 3 |
of looking at it | 3 |
to tell us that | 3 |
will be proportional to | 3 |
of the rest of | 3 |
should be able to | 3 |
to decide between the | 3 |
physical continuum of three | 3 |
the point where the | 3 |
to the object b | 3 |
indistinguishable from a third | 3 |
the laws of their | 3 |
the simplicity of the | 3 |
the movements of our | 3 |
contact with the object | 3 |
as those of the | 3 |
a point in common | 3 |
such as that of | 3 |
was one of the | 3 |
that the theory of | 3 |
bodies to one another | 3 |
is four times some | 3 |
a magnetic pole is | 3 |
imposed upon our sensibility | 3 |
was none the less | 3 |
equal to that of | 3 |
notion of the physical | 3 |
have seen above that | 3 |
the relation of a | 3 |
it would only be | 3 |
the report of the | 3 |
elements of the cut | 3 |
corner of the universe | 3 |
is the result of | 3 |
that the velocities of | 3 |
generalized law of inertia | 3 |
at the point m | 3 |
far from one another | 3 |
there is not in | 3 |
is or is not | 3 |
a perturbation in the | 3 |
those which have been | 3 |
and it is this | 3 |
the two systems of | 3 |
know whether the point | 3 |
we thought we knew | 3 |
as you choose from | 3 |
at the cost of | 3 |
which gave birth to | 3 |
will cease to be | 3 |
will be impossible to | 3 |
the ultimate constitution of | 3 |
the situation of this | 3 |
such a point of | 3 |
these two objects occupy | 3 |
muscular sense tells me | 3 |
in the interior of | 3 |
state of the bodies | 3 |
to which we shall | 3 |
it is able to | 3 |
or at least that | 3 |
name of straights to | 3 |
probability of the cause | 3 |
is a constant relation | 3 |
what we do not | 3 |
be the same as | 3 |
to return to the | 3 |
that does not suffice | 3 |
and then we have | 3 |
it is therefore impossible | 3 |
the surfaces of constant | 3 |
object with regard to | 3 |
the whole visual space | 3 |
from changes of position | 3 |
i do not see | 3 |
the characteristics of a | 3 |
the propagation of heat | 3 |
no means of distinguishing | 3 |
the question of the | 3 |
i have not the | 3 |
even if it existed | 3 |
has one the right | 3 |
mixture of blue and | 3 |
visual space would have | 3 |
in which it is | 3 |
not yet know geometry | 3 |
be useful to us | 3 |
the events of the | 3 |
at the point of | 3 |
regarded as an experimental | 3 |
there is a second | 3 |
and that there is | 3 |
it is none the | 3 |
mind of the mathematician | 3 |
for that it is | 3 |
that they have only | 3 |
this is not a | 3 |
it is to the | 3 |
only a crude image | 3 |
we can not be | 3 |
if i wish to | 3 |
theory of the constitution | 3 |
a series of sensations | 3 |
have sought to explain | 3 |
the effect of a | 3 |
motions of the heavenly | 3 |
on the same point | 3 |
the inverse ratio of | 3 |
and yet this is | 3 |
is necessary to be | 3 |
the choice of facts | 3 |
perturbation in the ether | 3 |
the terms of the | 3 |
then am i led | 3 |
which seems to me | 3 |
it is difficult not | 3 |
to say there is | 3 |
not have been able | 3 |
to a system of | 3 |
as i have explained | 3 |
the reality of the | 3 |
the total number of | 3 |
of the work of | 3 |
it might be said | 3 |
will it be said | 3 |
of the world and | 3 |
the second case that | 3 |
enable us to decide | 3 |
the action of c | 3 |
synthetic a priori judgments | 3 |
can not reason thus | 3 |
field produced by the | 3 |
be by definition the | 3 |
and the sensation of | 3 |
of gravity of this | 3 |
a body depends only | 3 |
they are not sufficiently | 3 |
the belief in the | 3 |
no one has ever | 3 |
which can not be | 3 |
satisfy the principle of | 3 |
every curve has a | 3 |
the total apparent mass | 3 |
we simply mean that | 3 |
square of the aberration | 3 |
of no great interest | 3 |
the mutual impacts of | 3 |
and it is just | 3 |
facts in the rough | 3 |
a world where there | 3 |
on the position of | 3 |
of a body depends | 3 |
shall we conclude that | 3 |
is not enough to | 3 |
continua of one dimension | 3 |
the various bodies of | 3 |
that this something else | 3 |
what is the cause | 3 |
if the velocity of | 3 |
the masses of these | 3 |
of the charge to | 3 |
what i shall call | 3 |
do not believe they | 3 |
the liberty of contradiction | 3 |
little as you choose | 3 |
that the coordinates of | 3 |
and in particular those | 3 |
it is experience which | 3 |
the foundations of geometry | 3 |
are in no wise | 3 |
which is common to | 3 |
the group of displacements | 3 |
to each point of | 3 |
is not always the | 3 |
have nothing to do | 3 |
to divide a continuum | 3 |
to ourselves a point | 3 |
led to conclude that | 3 |
necessary to take account | 3 |
us to decide between | 3 |
to the complexity of | 3 |
in the neighborhood of | 3 |
it matters little that | 3 |
a is equal to | 3 |
we shall have an | 3 |
seems to us to | 3 |
of muscular sensations which | 3 |
by definition that which | 3 |
is straight and uniform | 3 |
the expression of the | 3 |
that in place of | 3 |
of the progress of | 3 |
me by the same | 3 |
the actual state of | 3 |
not every one can | 3 |
the rules of logic | 3 |
voluntary and accompanied by | 3 |
is therefore necessary to | 3 |
same laws as the | 3 |
be modified by the | 3 |
have been made to | 3 |
the elements of this | 3 |
it was seen that | 3 |
and first of all | 3 |
and we can represent | 3 |
the law according to | 3 |
act at a distance | 3 |
may be asked whether | 3 |
the object of geometry | 3 |
is true for a | 3 |
when it shall have | 3 |
in consequence of our | 3 |
with the velocity according | 3 |
the order of their | 3 |
velocity of the light | 3 |
number on the bottom | 3 |
the quotient of the | 3 |
but it does not | 3 |
every one knows that | 3 |
when we know the | 3 |
this mode of reasoning | 3 |
the law of homogeneity | 3 |
it is with the | 3 |
to that of light | 3 |
will be called a | 3 |
but if it were | 3 |
natural to suppose that | 3 |
to the witness of | 3 |
the inverse of the | 3 |
this is enough to | 3 |
will be capable of | 3 |
not the only one | 3 |
velocity according to the | 3 |
because we can not | 3 |
the aggregate of series | 3 |
but we are not | 3 |
we are reduced to | 3 |
the relative motion of | 3 |
i have just given | 3 |
of the results of | 3 |
but there is another | 3 |
one another according to | 3 |
derivatives with respect to | 3 |
suppose the earth turns | 3 |
which corresponds to the | 3 |
of the earth is | 3 |
as soon as we | 3 |
the manifold of points | 3 |
of a solid body | 3 |
mathematical continuum of several | 3 |
one is tempted to | 3 |
of the second space | 3 |
one position to another | 3 |
to the magnetic force | 3 |
is that there is | 3 |
that the ratio of | 3 |
gave birth to it | 3 |
velocity with respect to | 3 |
two energies t and | 3 |
the history of mathematical | 3 |
be true or false | 3 |
now we have just | 2 |
of the first tactile | 2 |
become smaller and smaller | 2 |
when we say space | 2 |
the republic of ecuador | 2 |
the whole of mathematics | 2 |
we should have of | 2 |
take a simple example | 2 |
the case for the | 2 |
all kinds of scientific | 2 |
of the hypothesis that | 2 |
of the postulates of | 2 |
the body in its | 2 |
or several continua of | 2 |
that all these phenomena | 2 |
the absolute value of | 2 |
little that it is | 2 |
the proposition to be | 2 |
shall not dwell on | 2 |
series will constitute a | 2 |
that part of the | 2 |
the foundations of the | 2 |
which has been observed | 2 |
and which would be | 2 |
actual state of the | 2 |
belong to a line | 2 |
mass coefficient of attraction | 2 |
and of the neighboring | 2 |
spheres have undergone the | 2 |
and he has put | 2 |
experiment shows us that | 2 |
numbers divided by even | 2 |
still be the same | 2 |
without interest to examine | 2 |
as we can not | 2 |
the ultimate elements of | 2 |
of less than a | 2 |
aid us the better | 2 |
this is the third | 2 |
space occupied at the | 2 |
the state of things | 2 |
without putting in motion | 2 |
is true in a | 2 |
he who invented the | 2 |
suffice to show that | 2 |
at only one side | 2 |
world tends toward uniformity | 2 |
that it furnishes us | 2 |
there are people who | 2 |
cease to be so | 2 |
tempted to believe they | 2 |
to the border b | 2 |
able to perceive its | 2 |
second degree of ignorance | 2 |
and that i should | 2 |
we shall see them | 2 |
number of combinations and | 2 |
the principle of newton | 2 |
the principle of continuity | 2 |
the simple under the | 2 |
law is only a | 2 |
the two series s | 2 |
the same direction and | 2 |
the differences of their | 2 |
confounded under the name | 2 |
and if we could | 2 |
than the straight and | 2 |
not accompanied by deformation | 2 |
the second degree with | 2 |
unity of the individual | 2 |
two series of movements | 2 |
attribute to the object | 2 |
will not be our | 2 |
the student of science | 2 |
object in the same | 2 |
a space of three | 2 |
that will be the | 2 |
it is on this | 2 |
ideas on the brownian | 2 |
existence of a class | 2 |
but it is experience | 2 |
there is something more | 2 |
study of the movements | 2 |
be what we are | 2 |
has already been said | 2 |
to feel the impression | 2 |
b are transmitted to | 2 |
whether a definition is | 2 |
think i have elsewhere | 2 |
from the center a | 2 |
giving to the word | 2 |