Free Essay

In: Science

Submitted By k0319060

Words 9329

Pages 38

Words 9329

Pages 38

By A. EINSTEIN June 30, 1905

It is known that Maxwell’s electrodynamics—as usually understood at the present time—when applied to moving bodies, leads to asymmetries which do not appear to be inherent in the phenomena. Take, for example, the reciprocal electrodynamic action of a magnet and a conductor. The observable phenomenon here depends only on the relative motion of the conductor and the magnet, whereas the customary view draws a sharp distinction between the two cases in which either the one or the other of these bodies is in motion. For if the magnet is in motion and the conductor at rest, there arises in the neighbourhood of the magnet an electric ﬁeld with a certain deﬁnite energy, producing a current at the places where parts of the conductor are situated. But if the magnet is stationary and the conductor in motion, no electric ﬁeld arises in the neighbourhood of the magnet. In the conductor, however, we ﬁnd an electromotive force, to which in itself there is no corresponding energy, but which gives rise—assuming equality of relative motion in the two cases discussed—to electric currents of the same path and intensity as those produced by the electric forces in the former case. Examples of this sort, together with the unsuccessful attempts to discover any motion of the earth relatively to the “light medium,” suggest that the phenomena of electrodynamics as well as of mechanics possess no properties corresponding to the idea of absolute rest. They suggest rather that, as has already been shown to the ﬁrst order of small quantities, the same laws of electrodynamics and optics will be valid for all frames of reference for which the equations of mechanics hold good.1 We will raise this conjecture (the purport of which will hereafter be called the “Principle of Relativity”) to the status of a postulate, and also introduce another postulate, which is only apparently irreconcilable with the former, namely, that light is always propagated in empty space with a deﬁnite velocity c which is independent of the state of motion of the emitting body. These two postulates suﬃce for the attainment of a simple and consistent theory of the electrodynamics of moving bodies based on Maxwell’s theory for stationary bodies. The introduction of a “luminiferous ether” will prove to be superﬂuous inasmuch as the view here to be developed will not require an “absolutely stationary space” provided with special properties, nor

1 The

preceding memoir by Lorentz was not at this time known to the author.

1

assign a velocity-vector to a point of the empty space in which electromagnetic processes take place. The theory to be developed is based—like all electrodynamics—on the kinematics of the rigid body, since the assertions of any such theory have to do with the relationships between rigid bodies (systems of co-ordinates), clocks, and electromagnetic processes. Insuﬃcient consideration of this circumstance lies at the root of the diﬃculties which the electrodynamics of moving bodies at present encounters.

I. KINEMATICAL PART

§ 1. Deﬁnition of Simultaneity

Let us take a system of co-ordinates in which the equations of Newtonian mechanics hold good.2 In order to render our presentation more precise and to distinguish this system of co-ordinates verbally from others which will be introduced hereafter, we call it the “stationary system.” If a material point is at rest relatively to this system of co-ordinates, its position can be deﬁned relatively thereto by the employment of rigid standards of measurement and the methods of Euclidean geometry, and can be expressed in Cartesian co-ordinates. If we wish to describe the motion of a material point, we give the values of its co-ordinates as functions of the time. Now we must bear carefully in mind that a mathematical description of this kind has no physical meaning unless we are quite clear as to what we understand by “time.” We have to take into account that all our judgments in which time plays a part are always judgments of simultaneous events. If, for instance, I say, “That train arrives here at 7 o’clock,” I mean something like this: “The pointing of the small hand of my watch to 7 and the arrival of the train are simultaneous events.”3 It might appear possible to overcome all the diﬃculties attending the deﬁnition of “time” by substituting “the position of the small hand of my watch” for “time.” And in fact such a deﬁnition is satisfactory when we are concerned with deﬁning a time exclusively for the place where the watch is located; but it is no longer satisfactory when we have to connect in time series of events occurring at diﬀerent places, or—what comes to the same thing—to evaluate the times of events occurring at places remote from the watch. We might, of course, content ourselves with time values determined by an observer stationed together with the watch at the origin of the co-ordinates, and co-ordinating the corresponding positions of the hands with light signals, given out by every event to be timed, and reaching him through empty space. But this co-ordination has the disadvantage that it is not independent of the standpoint of the observer with the watch or clock, as we know from experience. to the ﬁrst approximation. shall not here discuss the inexactitude which lurks in the concept of simultaneity of two events at approximately the same place, which can only be removed by an abstraction.

3 We 2 i.e.

2

We arrive at a much more practical determination along the following line of thought. If at the point A of space there is a clock, an observer at A can determine the time values of events in the immediate proximity of A by ﬁnding the positions of the hands which are simultaneous with these events. If there is at the point B of space another clock in all respects resembling the one at A, it is possible for an observer at B to determine the time values of events in the immediate neighbourhood of B. But it is not possible without further assumption to compare, in respect of time, an event at A with an event at B. We have so far deﬁned only an “A time” and a “B time.” We have not deﬁned a common “time” for A and B, for the latter cannot be deﬁned at all unless we establish by deﬁnition that the “time” required by light to travel from A to B equals the “time” it requires to travel from B to A. Let a ray of light start at the “A time” tA from A towards B, let it at the “B time” tB be reﬂected at B in the direction of A, and arrive again at A at the “A time” tA . In accordance with deﬁnition the two clocks synchronize if tB − tA = tA − tB . We assume that this deﬁnition of synchronism is free from contradictions, and possible for any number of points; and that the following relations are universally valid:— 1. If the clock at B synchronizes with the clock at A, the clock at A synchronizes with the clock at B. 2. If the clock at A synchronizes with the clock at B and also with the clock at C, the clocks at B and C also synchronize with each other. Thus with the help of certain imaginary physical experiments we have settled what is to be understood by synchronous stationary clocks located at different places, and have evidently obtained a deﬁnition of “simultaneous,” or “synchronous,” and of “time.” The “time” of an event is that which is given simultaneously with the event by a stationary clock located at the place of the event, this clock being synchronous, and indeed synchronous for all time determinations, with a speciﬁed stationary clock. In agreement with experience we further assume the quantity 2AB = c, tA − tA to be a universal constant—the velocity of light in empty space. It is essential to have time deﬁned by means of stationary clocks in the stationary system, and the time now deﬁned being appropriate to the stationary system we call it “the time of the stationary system.”

§ 2. On the Relativity of Lengths and Times

The following reﬂexions are based on the principle of relativity and on the principle of the constancy of the velocity of light. These two principles we deﬁne as follows:— 3

1. The laws by which the states of physical systems undergo change are not aﬀected, whether these changes of state be referred to the one or the other of two systems of co-ordinates in uniform translatory motion. 2. Any ray of light moves in the “stationary” system of co-ordinates with the determined velocity c, whether the ray be emitted by a stationary or by a moving body. Hence velocity = light path time interval

where time interval is to be taken in the sense of the deﬁnition in § 1. Let there be given a stationary rigid rod; and let its length be l as measured by a measuring-rod which is also stationary. We now imagine the axis of the rod lying along the axis of x of the stationary system of co-ordinates, and that a uniform motion of parallel translation with velocity v along the axis of x in the direction of increasing x is then imparted to the rod. We now inquire as to the length of the moving rod, and imagine its length to be ascertained by the following two operations:— (a) The observer moves together with the given measuring-rod and the rod to be measured, and measures the length of the rod directly by superposing the measuring-rod, in just the same way as if all three were at rest. (b) By means of stationary clocks set up in the stationary system and synchronizing in accordance with § 1, the observer ascertains at what points of the stationary system the two ends of the rod to be measured are located at a deﬁnite time. The distance between these two points, measured by the measuring-rod already employed, which in this case is at rest, is also a length which may be designated “the length of the rod.” In accordance with the principle of relativity the length to be discovered by the operation (a)—we will call it “the length of the rod in the moving system”— must be equal to the length l of the stationary rod. The length to be discovered by the operation (b) we will call “the length of the (moving) rod in the stationary system.” This we shall determine on the basis of our two principles, and we shall ﬁnd that it diﬀers from l. Current kinematics tacitly assumes that the lengths determined by these two operations are precisely equal, or in other words, that a moving rigid body at the epoch t may in geometrical respects be perfectly represented by the same body at rest in a deﬁnite position. We imagine further that at the two ends A and B of the rod, clocks are placed which synchronize with the clocks of the stationary system, that is to say that their indications correspond at any instant to the “time of the stationary system” at the places where they happen to be. These clocks are therefore “synchronous in the stationary system.” We imagine further that with each clock there is a moving observer, and that these observers apply to both clocks the criterion established in § 1 for the synchronization of two clocks. Let a ray of light depart from A at the time4 tA ,

4 “Time” here denotes “time of the stationary system” and also “position of hands of the moving clock situated at the place under discussion.”

4

let it be reﬂected at B at the time tB , and reach A again at the time tA . Taking into consideration the principle of the constancy of the velocity of light we ﬁnd that tB − tA = rAB rAB and tA − tB = c−v c+v

where rAB denotes the length of the moving rod—measured in the stationary system. Observers moving with the moving rod would thus ﬁnd that the two clocks were not synchronous, while observers in the stationary system would declare the clocks to be synchronous. So we see that we cannot attach any absolute signiﬁcation to the concept of simultaneity, but that two events which, viewed from a system of co-ordinates, are simultaneous, can no longer be looked upon as simultaneous events when envisaged from a system which is in motion relatively to that system.

§ 3. Theory of the Transformation of Co-ordinates and Times from a Stationary System to another System in Uniform Motion of Translation Relatively to the Former

Let us in “stationary” space take two systems of co-ordinates, i.e. two systems, each of three rigid material lines, perpendicular to one another, and issuing from a point. Let the axes of X of the two systems coincide, and their axes of Y and Z respectively be parallel. Let each system be provided with a rigid measuring-rod and a number of clocks, and let the two measuring-rods, and likewise all the clocks of the two systems, be in all respects alike. Now to the origin of one of the two systems (k) let a constant velocity v be imparted in the direction of the increasing x of the other stationary system (K), and let this velocity be communicated to the axes of the co-ordinates, the relevant measuring-rod, and the clocks. To any time of the stationary system K there then will correspond a deﬁnite position of the axes of the moving system, and from reasons of symmetry we are entitled to assume that the motion of k may be such that the axes of the moving system are at the time t (this “t” always denotes a time of the stationary system) parallel to the axes of the stationary system. We now imagine space to be measured from the stationary system K by means of the stationary measuring-rod, and also from the moving system k by means of the measuring-rod moving with it; and that we thus obtain the co-ordinates x, y, z, and ξ, η, ζ respectively. Further, let the time t of the stationary system be determined for all points thereof at which there are clocks by means of light signals in the manner indicated in § 1; similarly let the time τ of the moving system be determined for all points of the moving system at which there are clocks at rest relatively to that system by applying the method, given in § 1, of light signals between the points at which the latter clocks are located. To any system of values x, y, z, t, which completely deﬁnes the place and time of an event in the stationary system, there belongs a system of values ξ, 5

η, ζ, τ , determining that event relatively to the system k, and our task is now to ﬁnd the system of equations connecting these quantities. In the ﬁrst place it is clear that the equations must be linear on account of the properties of homogeneity which we attribute to space and time. If we place x = x − vt, it is clear that a point at rest in the system k must have a system of values x , y, z, independent of time. We ﬁrst deﬁne τ as a function of x , y, z, and t. To do this we have to express in equations that τ is nothing else than the summary of the data of clocks at rest in system k, which have been synchronized according to the rule given in § 1. From the origin of system k let a ray be emitted at the time τ0 along the X-axis to x , and at the time τ1 be reﬂected thence to the origin of the co1 ordinates, arriving there at the time τ2 ; we then must have 2 (τ0 + τ2 ) = τ1 , or, by inserting the arguments of the function τ and applying the principle of the constancy of the velocity of light in the stationary system:— 1 τ (0, 0, 0, t) + τ 2 0, 0, 0, t + x x + c−v c+v =τ x , 0, 0, t + x c−v .

Hence, if x be chosen inﬁnitesimally small, 1 2 or ∂τ v ∂τ + 2 = 0. 2 ∂t ∂x c −v It is to be noted that instead of the origin of the co-ordinates we might have chosen any other point for the point of origin of the ray, and the equation just obtained is therefore valid for all values of x , y, z. An analogous consideration—applied to the axes of Y and Z—it being borne in mind that light is always propagated along these axes, when viewed from the √ stationary system, with the velocity c2 − v 2 gives us ∂τ ∂τ = 0, = 0. ∂y ∂z Since τ is a linear function, it follows from these equations that τ =a t− v x c2 − v 2 1 1 + c−v c+v ∂τ ∂τ 1 ∂τ = + , ∂t ∂x c − v ∂t

where a is a function φ(v) at present unknown, and where for brevity it is assumed that at the origin of k, τ = 0, when t = 0. With the help of this result we easily determine the quantities ξ, η, ζ by expressing in equations that light (as required by the principle of the constancy of the velocity of light, in combination with the principle of relativity) is also

6

propagated with velocity c when measured in the moving system. For a ray of light emitted at the time τ = 0 in the direction of the increasing ξ ξ = cτ or ξ = ac t − c2 v x − v2 .

But the ray moves relatively to the initial point of k, when measured in the stationary system, with the velocity c − v, so that x = t. c−v If we insert this value of t in the equation for ξ, we obtain ξ=a c2 x. c2 − v 2

In an analogous manner we ﬁnd, by considering rays moving along the two other axes, that η = cτ = ac t − when √ Thus η = a√ c2 c c y and ζ = a √ z. 2 2 − v2 −v c c2 y = t, x = 0. − v2 v x c2 − v 2

Substituting for x its value, we obtain τ ξ η ζ = φ(v)β(t − vx/c2 ), = φ(v)β(x − vt), = φ(v)y, = φ(v)z,

where β= 1 1 − v 2 /c2 ,

and φ is an as yet unknown function of v. If no assumption whatever be made as to the initial position of the moving system and as to the zero point of τ , an additive constant is to be placed on the right side of each of these equations. 7

We now have to prove that any ray of light, measured in the moving system, is propagated with the velocity c, if, as we have assumed, this is the case in the stationary system; for we have not as yet furnished the proof that the principle of the constancy of the velocity of light is compatible with the principle of relativity. At the time t = τ = 0, when the origin of the co-ordinates is common to the two systems, let a spherical wave be emitted therefrom, and be propagated with the velocity c in system K. If (x, y, z) be a point just attained by this wave, then x2 + y 2 + z 2 = c2 t2 . Transforming this equation with the aid of our equations of transformation we obtain after a simple calculation ξ 2 + η 2 + ζ 2 = c2 τ 2 . The wave under consideration is therefore no less a spherical wave with velocity of propagation c when viewed in the moving system. This shows that our two fundamental principles are compatible.5 In the equations of transformation which have been developed there enters an unknown function φ of v, which we will now determine. For this purpose we introduce a third system of co-ordinates K , which relatively to the system k is in a state of parallel translatory motion parallel to the axis of Ξ,† such that the origin of co-ordinates of system K moves with velocity −v on the axis of Ξ. At the time t = 0 let all three origins coincide, and when t = x = y = z = 0 let the time t of the system K be zero. We call the co-ordinates, measured in the system K , x , y , z , and by a twofold application of our equations of transformation we obtain t x y z = = = = φ(−v)β(−v)(τ + vξ/c2 ) = φ(−v)β(−v)(ξ + vτ ) = φ(−v)η = φ(−v)ζ = φ(v)φ(−v)t, φ(v)φ(−v)x, φ(v)φ(−v)y, φ(v)φ(−v)z.

Since the relations between x , y , z and x, y, z do not contain the time t, the systems K and K are at rest with respect to one another, and it is clear that the transformation from K to K must be the identical transformation. Thus φ(v)φ(−v) = 1.

5 The equations of the Lorentz transformation may be more simply deduced directly from the condition that in virtue of those equations the relation x2 + y 2 + z 2 = c2 t2 shall have as its consequence the second relation ξ 2 + η 2 + ζ 2 = c2 τ 2 . † Editor’s note: In Einstein’s original paper, the symbols (Ξ, H, Z) for the co-ordinates of the moving system k were introduced without explicitly deﬁning them. In the 1923 English translation, (X, Y, Z) were used, creating an ambiguity between X co-ordinates in the ﬁxed system K and the parallel axis in moving system k. Here and in subsequent references we use Ξ when referring to the axis of system k along which the system is translating with respect to K. In addition, the reference to system K later in this sentence was incorrectly given as “k” in the 1923 English translation.

8

We now inquire into the signiﬁcation of φ(v). We give our attention to that part of the axis of Y of system k which lies between ξ = 0, η = 0, ζ = 0 and ξ = 0, η = l, ζ = 0. This part of the axis of Y is a rod moving perpendicularly to its axis with velocity v relatively to system K. Its ends possess in K the co-ordinates x1 = vt, y1 = and x2 = vt, y2 = 0, z2 = 0. The length of the rod measured in K is therefore l/φ(v); and this gives us the meaning of the function φ(v). From reasons of symmetry it is now evident that the length of a given rod moving perpendicularly to its axis, measured in the stationary system, must depend only on the velocity and not on the direction and the sense of the motion. The length of the moving rod measured in the stationary system does not change, therefore, if v and −v are interchanged. Hence follows that l/φ(v) = l/φ(−v), or φ(v) = φ(−v). It follows from this relation and the one previously found that φ(v) = 1, so that the transformation equations which have been found become = β(t − vx/c2 ), = β(x − vt), = y, = z, l , z1 = 0 φ(v)

τ ξ η ζ

where β = 1/ 1 − v 2 /c2 .

§ 4. Physical Meaning of the Equations Obtained in Respect to Moving Rigid Bodies and Moving Clocks

We envisage a rigid sphere6 of radius R, at rest relatively to the moving system k, and with its centre at the origin of co-ordinates of k. The equation of the surface of this sphere moving relatively to the system K with velocity v is ξ 2 + η 2 + ζ 2 = R2 .

6 That

is, a body possessing spherical form when examined at rest.

9

The equation of this surface expressed in x, y, z at the time t = 0 is x2 ( 1 − v 2 /c2 )2 + y 2 + z 2 = R2 .

A rigid body which, measured in a state of rest, has the form of a sphere, therefore has in a state of motion—viewed from the stationary system—the form of an ellipsoid of revolution with the axes R 1 − v 2 /c2 , R, R.

Thus, whereas the Y and Z dimensions of the sphere (and therefore of every rigid body of no matter what form) do not appear modiﬁed by the motion, the X dimension appears shortened in the ratio 1 : 1 − v 2 /c2 , i.e. the greater the value of v, the greater the shortening. For v = c all moving objects—viewed from the “stationary” system—shrivel up into plane ﬁgures.† For velocities greater than that of light our deliberations become meaningless; we shall, however, ﬁnd in what follows, that the velocity of light in our theory plays the part, physically, of an inﬁnitely great velocity. It is clear that the same results hold good of bodies at rest in the “stationary” system, viewed from a system in uniform motion. Further, we imagine one of the clocks which are qualiﬁed to mark the time t when at rest relatively to the stationary system, and the time τ when at rest relatively to the moving system, to be located at the origin of the co-ordinates of k, and so adjusted that it marks the time τ . What is the rate of this clock, when viewed from the stationary system? Between the quantities x, t, and τ , which refer to the position of the clock, we have, evidently, x = vt and τ= Therefore, τ =t 1 − v 2 /c2 = t − (1 − 1 − v 2 /c2 )t 1 1 − v 2 /c2 (t − vx/c2 ).

whence it follows that the time marked by the clock (viewed in the stationary system) is slow by 1 − 1 − v 2 /c2 seconds per second, or—neglecting magnitudes of fourth and higher order—by 1 v 2 /c2 . 2 From this there ensues the following peculiar consequence. If at the points A and B of K there are stationary clocks which, viewed in the stationary system, are synchronous; and if the clock at A is moved with the velocity v along the line AB to B, then on its arrival at B the two clocks no longer synchronize, but the clock moved from A to B lags behind the other which has remained at

† Editor’s note: In the 1923 English translation, this phrase was erroneously translated as “plain ﬁgures”. I have used the correct “plane ﬁgures” in this edition.

10

1 B by 2 tv 2 /c2 (up to magnitudes of fourth and higher order), t being the time occupied in the journey from A to B. It is at once apparent that this result still holds good if the clock moves from A to B in any polygonal line, and also when the points A and B coincide. If we assume that the result proved for a polygonal line is also valid for a continuously curved line, we arrive at this result: If one of two synchronous clocks at A is moved in a closed curve with constant velocity until it returns to A, the journey lasting t seconds, then by the clock which has remained at rest the travelled clock on its arrival at A will be 1 tv 2 /c2 second slow. Thence we 2 conclude that a balance-clock7 at the equator must go more slowly, by a very small amount, than a precisely similar clock situated at one of the poles under otherwise identical conditions.

§ 5. The Composition of Velocities

In the system k moving along the axis of X of the system K with velocity v, let a point move in accordance with the equations ξ = wξ τ, η = wη τ, ζ = 0, where wξ and wη denote constants. Required: the motion of the point relatively to the system K. If with the help of the equations of transformation developed in § 3 we introduce the quantities x, y, z, t into the equations of motion of the point, we obtain wξ + v t, 1 + vwξ /c2 1 − v 2 /c2 wη t, 1 + vwξ /c2

x y z

= = = 0.

Thus the law of the parallelogram of velocities is valid according to our theory only to a ﬁrst approximation. We set dx dt

2

V2 w2

=

+

dy dt

2

,

2 2 = wξ + wη ,

a =

tan−1 wη /wξ , †

7 Not a pendulum-clock, which is physically a system to which the Earth belongs. This case had to be excluded. † Editor’s note: This equation was incorrectly given in Einstein’s original paper and the 1923 English translation as a = tan−1 wy /wx .

11

a is then to be looked upon as the angle between the velocities v and w. After a simple calculation we obtain V = (v 2 + w2 + 2vw cos a) − (vw sin a/c)2 . 1 + vw cos a/c2

It is worthy of remark that v and w enter into the expression for the resultant velocity in a symmetrical manner. If w also has the direction of the axis of X, we get v+w V = . 1 + vw/c2 It follows from this equation that from a composition of two velocities which are less than c, there always results a velocity less than c. For if we set v = c − κ, w = c − λ, κ and λ being positive and less than c, then V =c 2c − κ − λ < c. 2c − κ − λ + κλ/c

It follows, further, that the velocity of light c cannot be altered by composition with a velocity less than that of light. For this case we obtain c+w = c. V = 1 + w/c We might also have obtained the formula for V, for the case when v and w have the same direction, by compounding two transformations in accordance with § 3. If in addition to the systems K and k ﬁguring in § 3 we introduce still another system of co-ordinates k moving parallel to k, its initial point moving on the axis of Ξ† with the velocity w, we obtain equations between the quantities x, y, z, t and the corresponding quantities of k , which diﬀer from the equations found in § 3 only in that the place of “v” is taken by the quantity v+w ; 1 + vw/c2 from which we see that such parallel transformations—necessarily—form a group. We have now deduced the requisite laws of the theory of kinematics corresponding to our two principles, and we proceed to show their application to electrodynamics.

II. ELECTRODYNAMICAL PART

§ 6. Transformation of the Maxwell-Hertz Equations for Empty Space. On the Nature of the Electromotive Forces Occurring in a Magnetic Field During Motion

Let the Maxwell-Hertz equations for empty space hold good for the stationary system K, so that we have

† Editor’s

note: “X” in the 1923 English translation.

12

1 ∂X c ∂t 1 ∂Y c ∂t 1 ∂Z c ∂t

= = =

∂N ∂y ∂L ∂z ∂M ∂x

− − −

∂M ∂z , ∂N ∂x , ∂L ∂y ,

1 ∂L c ∂t 1 ∂M c ∂t 1 ∂N c ∂t

= = =

∂Y ∂z ∂Z ∂x ∂X ∂y

− − −

∂Z ∂y , ∂X ∂z , ∂Y ∂x ,

where (X, Y, Z) denotes the vector of the electric force, and (L, M, N) that of the magnetic force. If we apply to these equations the transformation developed in § 3, by referring the electromagnetic processes to the system of co-ordinates there introduced, moving with the velocity v, we obtain the equations †

1 ∂X c ∂τ 1 ∂ c ∂τ 1 ∂ c ∂τ

= = = = = =

∂ ∂η ∂L ∂ζ ∂ ∂ξ ∂ ∂ζ ∂ ∂ξ ∂X ∂η

β N − vY c β M + vZ c β Y − vN c β Z + vM c

∂ − ∂ζ β M + v Z c ∂ − ∂ξ β N − v Y c

, ,

β Y − vN c β Z + vM c

1 ∂L c ∂τ

− ∂L , ∂η

∂ − ∂η β Z + v M c

,

1 ∂ c ∂τ 1 ∂ c ∂τ

β M + vZ c β N − vY c

− ∂X , ∂ζ

∂ − ∂ξ β Y − v N c

,

where β = 1/ 1 − v 2 /c2 .

Now the principle of relativity requires that if the Maxwell-Hertz equations for empty space hold good in system K, they also hold good in system k; that is to say that the vectors of the electric and the magnetic force—(X , Y , Z ) and (L , M , N )—of the moving system k, which are deﬁned by their ponderomotive eﬀects on electric or magnetic masses respectively, satisfy the following equations:— 1 ∂X c ∂τ 1 ∂Y c ∂τ 1 ∂Z c ∂τ

= = =

∂N ∂η ∂L ∂ζ ∂M ∂ξ

− − −

∂M ∂ζ ∂N ∂ξ ∂L ∂η

, , ,

1 ∂L c ∂τ 1 ∂M c ∂τ 1 ∂N c ∂τ

= = =

∂Y ∂ζ ∂Z ∂ξ ∂X ∂η

− − −

∂Z ∂η ∂X ∂ζ ∂Y ∂ξ

, , .

† Editor’s note: In the 1923 English translation, the quantities “ζ” and “ξ” were interchanged in the second equation. They were given correctly in the the original 1905 paper.

13

Evidently the two systems of equations found for system k must express exactly the same thing, since both systems of equations are equivalent to the Maxwell-Hertz equations for system K. Since, further, the equations of the two systems agree, with the exception of the symbols for the vectors, it follows that the functions occurring in the systems of equations at corresponding places must agree, with the exception of a factor ψ(v), which is common for all functions of the one system of equations, and is independent of ξ, η, ζ and τ but depends upon v. Thus we have the relations X Y Z = ψ(v)X, L = ψ(v)β Y − v N , M c = ψ(v)β Z + v M , N c = ψ(v)L, = ψ(v)β M + v Z , c = ψ(v)β N − v Y . c

If we now form the reciprocal of this system of equations, ﬁrstly by solving the equations just obtained, and secondly by applying the equations to the inverse transformation (from k to K), which is characterized by the velocity −v, it follows, when we consider that the two systems of equations thus obtained must be identical, that ψ(v)ψ(−v) = 1. Further, from reasons of symmetry8 and therefore ψ(v) = 1, and our equations assume the form X Y Z = X, L = β Y − vN , M c = β Z + vM , N c = L, = β M + vZ , c = β N − vY . c

As to the interpretation of these equations we make the following remarks: Let a point charge of electricity have the magnitude “one” when measured in the stationary system K, i.e. let it when at rest in the stationary system exert a force of one dyne upon an equal quantity of electricity at a distance of one cm. By the principle of relativity this electric charge is also of the magnitude “one” when measured in the moving system. If this quantity of electricity is at rest relatively to the stationary system, then by deﬁnition the vector (X, Y, Z) is equal to the force acting upon it. If the quantity of electricity is at rest relatively to the moving system (at least at the relevant instant), then the force acting upon it, measured in the moving system, is equal to the vector (X , Y , Z ). Consequently the ﬁrst three equations above allow themselves to be clothed in words in the two following ways:— 1. If a unit electric point charge is in motion in an electromagnetic ﬁeld, there acts upon it, in addition to the electric force, an “electromotive force” which, if we neglect the terms multiplied by the second and higher powers of

8 If, for example, X=Y=Z=L=M=0, and N = 0, then from reasons of symmetry it is clear that when v changes sign without changing its numerical value, Y must also change sign without changing its numerical value.

14

v/c, is equal to the vector-product of the velocity of the charge and the magnetic force, divided by the velocity of light. (Old manner of expression.) 2. If a unit electric point charge is in motion in an electromagnetic ﬁeld, the force acting upon it is equal to the electric force which is present at the locality of the charge, and which we ascertain by transformation of the ﬁeld to a system of co-ordinates at rest relatively to the electrical charge. (New manner of expression.) The analogy holds with “magnetomotive forces.” We see that electromotive force plays in the developed theory merely the part of an auxiliary concept, which owes its introduction to the circumstance that electric and magnetic forces do not exist independently of the state of motion of the system of co-ordinates. Furthermore it is clear that the asymmetry mentioned in the introduction as arising when we consider the currents produced by the relative motion of a magnet and a conductor, now disappears. Moreover, questions as to the “seat” of electrodynamic electromotive forces (unipolar machines) now have no point.

§ 7. Theory of Doppler’s Principle and of Aberration

In the system K, very far from the origin of co-ordinates, let there be a source of electrodynamic waves, which in a part of space containing the origin of co-ordinates may be represented to a suﬃcient degree of approximation by the equations X = X0 sin Φ, L = L0 sin Φ, Y = Y0 sin Φ, M = M0 sin Φ, Z = Z0 sin Φ, N = N0 sin Φ, where 1 Φ = ω t − (lx + my + nz) . c Here (X0 , Y0 , Z0 ) and (L0 , M0 , N0 ) are the vectors deﬁning the amplitude of the wave-train, and l, m, n the direction-cosines of the wave-normals. We wish to know the constitution of these waves, when they are examined by an observer at rest in the moving system k. Applying the equations of transformation found in § 6 for electric and magnetic forces, and those found in § 3 for the co-ordinates and the time, we obtain directly X = X0 sin Φ , Y = β(Y0 − vN0 /c) sin Φ , Z = β(Z0 + vM0 /c) sin Φ , Φ = ω τ − 1 (l c where L = L0 sin Φ , M = β(M0 + vZ0 /c) sin Φ , N = β(N0 − vY0 /c) sin Φ , ξ + m η + n ζ)

15

ω l m n

= ωβ(1 − lv/c), l − v/c = , 1 − lv/c m , = β(1 − lv/c) n . = β(1 − lv/c)

From the equation for ω it follows that if an observer is moving with velocity v relatively to an inﬁnitely distant source of light of frequency ν, in such a way that the connecting line “source-observer” makes the angle φ with the velocity of the observer referred to a system of co-ordinates which is at rest relatively to the source of light, the frequency ν of the light perceived by the observer is given by the equation ν =ν 1 − cos φ · v/c 1 − v 2 /c2 .

This is Doppler’s principle for any velocities whatever. When φ = 0 the equation assumes the perspicuous form ν =ν 1 − v/c . 1 + v/c

We see that, in contrast with the customary view, when v = −c, ν = ∞. If we call the angle between the wave-normal (direction of the ray) in the moving system and the connecting line “source-observer” φ , the equation for φ † assumes the form cos φ = cos φ − v/c . 1 − cos φ · v/c

This equation expresses the law of aberration in its most general form. If φ = 1 2 π, the equation becomes simply cos φ = −v/c. We still have to ﬁnd the amplitude of the waves, as it appears in the moving system. If we call the amplitude of the electric or magnetic force A or A respectively, accordingly as it is measured in the stationary system or in the moving system, we obtain

† Editor’s note: Erroneously given as “l ” in the 1923 English translation, propagating an error, despite a change in symbols, from the original 1905 paper.

16

A

2

= A2

(1 − cos φ · v/c)2 1 − v 2 /c2

which equation, if φ = 0, simpliﬁes into A

2

= A2

1 − v/c . 1 + v/c

It follows from these results that to an observer approaching a source of light with the velocity c, this source of light must appear of inﬁnite intensity.

§ 8. Transformation of the Energy of Light Rays. Theory of the Pressure of Radiation Exerted on Perfect Reﬂectors

Since A2 /8π equals the energy of light per unit of volume, we have to regard A /8π, by the principle of relativity, as the energy of light in the moving system. 2 Thus A /A2 would be the ratio of the “measured in motion” to the “measured at rest” energy of a given light complex, if the volume of a light complex were the same, whether measured in K or in k. But this is not the case. If l, m, n are the direction-cosines of the wave-normals of the light in the stationary system, no energy passes through the surface elements of a spherical surface moving with the velocity of light:—

2

(x − lct)2 + (y − mct)2 + (z − nct)2 = R2 . We may therefore say that this surface permanently encloses the same light complex. We inquire as to the quantity of energy enclosed by this surface, viewed in system k, that is, as to the energy of the light complex relatively to the system k. The spherical surface—viewed in the moving system—is an ellipsoidal surface, the equation for which, at the time τ = 0, is (βξ − lβξv/c)2 + (η − mβξv/c)2 + (ζ − nβξv/c)2 = R2 . If S is the volume of the sphere, and S that of this ellipsoid, then by a simple calculation 1 − v 2 /c2 S . = 1 − cos φ · v/c S Thus, if we call the light energy enclosed by this surface E when it is measured in the stationary system, and E when measured in the moving system, we obtain E A S 1 − cos φ · v/c = 2 = , E A S 1 − v 2 /c2 and this formula, when φ = 0, simpliﬁes into 17

2

E = E

1 − v/c . 1 + v/c

It is remarkable that the energy and the frequency of a light complex vary with the state of motion of the observer in accordance with the same law. Now let the co-ordinate plane ξ = 0 be a perfectly reﬂecting surface, at which the plane waves considered in § 7 are reﬂected. We seek for the pressure of light exerted on the reﬂecting surface, and for the direction, frequency, and intensity of the light after reﬂexion. Let the incidental light be deﬁned by the quantities A, cos φ, ν (referred to system K). Viewed from k the corresponding quantities are 1 − cos φ · v/c

A cos φ ν

, 1 − v 2 /c2 cos φ − v/c = , 1 − cos φ · v/c 1 − cos φ · v/c = ν . 1 − v 2 /c2

=

A

For the reﬂected light, referring the process to system k, we obtain A cos φ ν = A

= − cos φ = ν

Finally, by transforming back to the stationary system K, we obtain for the reﬂected light 1 + cosφ · v/c 1− v 2 /c2 1 − 2 cos φ · v/c + v 2 /c2 , 1 − v 2 /c2

A cos φ ν

= =

A

=A

cos φ + v/c (1 + v 2 /c2 ) cos φ − 2v/c =− , 1 + cos φ · v/c 1 − 2 cos φ · v/c + v 2 /c2 1 − 2 cos φ · v/c + v 2 /c2 1 + cos φ · v/c = ν =ν . 1 − v 2 /c2 1 − v 2 /c2

The energy (measured in the stationary system) which is incident upon unit area of the mirror in unit time is evidently A2 (c cos φ−v)/8π. The energy leaving the unit of surface of the mirror in the unit of time is A 2 (−c cos φ + v)/8π. 18

The diﬀerence of these two expressions is, by the principle of energy, the work done by the pressure of light in the unit of time. If we set down this work as equal to the product Pv, where P is the pressure of light, we obtain P=2· A2 (cos φ − v/c)2 . 8π 1 − v 2 /c2

In agreement with experiment and with other theories, we obtain to a ﬁrst approximation P=2· A2 cos2 φ. 8π

All problems in the optics of moving bodies can be solved by the method here employed. What is essential is, that the electric and magnetic force of the light which is inﬂuenced by a moving body, be transformed into a system of co-ordinates at rest relatively to the body. By this means all problems in the optics of moving bodies will be reduced to a series of problems in the optics of stationary bodies.

§ 9. Transformation of the Maxwell-Hertz Equations when Convection-Currents are Taken into Account

We start from the equations 1 c 1 c 1 c where ρ= ∂X ∂Y ∂Z + + ∂x ∂y ∂z ∂X ∂t ∂Y ∂t ∂Z ∂t

+ ux ρ + uy ρ + uz ρ

= = =

∂N ∂y ∂L ∂z ∂M ∂x

− − −

∂M ∂z , ∂N ∂x , ∂L ∂y ,

1 ∂L c ∂t 1 ∂M c ∂t 1 ∂N c ∂t

= = =

∂Y ∂z ∂Z ∂x ∂X ∂y

− − −

∂Z ∂y , ∂X ∂z , ∂Y ∂x ,

denotes 4π times the density of electricity, and (ux , uy , uz ) the velocity-vector of the charge. If we imagine the electric charges to be invariably coupled to small rigid bodies (ions, electrons), these equations are the electromagnetic basis of the Lorentzian electrodynamics and optics of moving bodies. Let these equations be valid in the system K, and transform them, with the assistance of the equations of transformation given in §§ 3 and 6, to the system k. We then obtain the equations

19

1 c 1 c 1 c where

∂X ∂τ ∂Y ∂τ ∂Z ∂τ

+ uξ ρ + uη ρ + uζ ρ

= = =

∂N ∂η ∂L ∂ζ ∂M ∂ξ

− − −

∂M ∂ζ ∂N ∂ξ ∂L ∂η

, , ,

1 ∂L c ∂τ 1 ∂M c ∂τ 1 ∂N c ∂τ

= = =

∂Y ∂ζ ∂Z ∂ξ ∂X ∂η

− − −

∂Z ∂η ∂X ∂ζ ∂Y ∂ξ

, , ,

uξ uη uζ

= = =

ux − v 1 − ux v/c2 uy β(1 − ux v/c2 ) uz , β(1 − ux v/c2 )

and ∂X ∂Y ∂Z + + ∂ξ ∂η ∂ζ 2 = β(1 − ux v/c )ρ. =

ρ

Since—as follows from the theorem of addition of velocities (§ 5)—the vector (uξ , uη , uζ ) is nothing else than the velocity of the electric charge, measured in the system k, we have the proof that, on the basis of our kinematical principles, the electrodynamic foundation of Lorentz’s theory of the electrodynamics of moving bodies is in agreement with the principle of relativity. In addition I may brieﬂy remark that the following important law may easily be deduced from the developed equations: If an electrically charged body is in motion anywhere in space without altering its charge when regarded from a system of co-ordinates moving with the body, its charge also remains—when regarded from the “stationary” system K—constant.

§ 10. Dynamics of the Slowly Accelerated Electron

Let there be in motion in an electromagnetic ﬁeld an electrically charged particle (in the sequel called an “electron”), for the law of motion of which we assume as follows:— If the electron is at rest at a given epoch, the motion of the electron ensues in the next instant of time according to the equations

20

m

d2 x dt2 d2 y m 2 dt d2 z m 2 dt

= = =

X Y Z

where x, y, z denote the co-ordinates of the electron, and m the mass of the electron, as long as its motion is slow. Now, secondly, let the velocity of the electron at a given epoch be v. We seek the law of motion of the electron in the immediately ensuing instants of time. Without aﬀecting the general character of our considerations, we may and will assume that the electron, at the moment when we give it our attention, is at the origin of the co-ordinates, and moves with the velocity v along the axis of X of the system K. It is then clear that at the given moment (t = 0) the electron is at rest relatively to a system of co-ordinates which is in parallel motion with velocity v along the axis of X. From the above assumption, in combination with the principle of relativity, it is clear that in the immediately ensuing time (for small values of t) the electron, viewed from the system k, moves in accordance with the equations d2 ξ dτ 2 d2 η m 2 dτ d2 ζ m 2 dτ

m

= = =

X, Y, Z,

in which the symbols ξ, η, ζ, X , Y , Z refer to the system k. If, further, we decide that when t = x = y = z = 0 then τ = ξ = η = ζ = 0, the transformation equations of §§ 3 and 6 hold good, so that we have ξ = β(x − vt), η = y, ζ = z, τ = β(t − vx/c2 ), X = X, Y = β(Y − vN/c), Z = β(Z + vM/c). With the help of these equations we transform the above equations of motion from system k to system K, and obtain d2 x = mβ 3 X dt2 d2 y v · · · (A) = mβ Y − c N 2 dt d2 z v = mβ Z + c M dt2

21

Taking the ordinary point of view we now inquire as to the “longitudinal” and the “transverse” mass of the moving electron. We write the equations (A) in the form x mβ 3 d 2 dt 2 y mβ 2 d 2 dt d2 z mβ 2 dt2

2

= = =

X β Y − vN c β Z + vM c

= = =

X, Y, Z,

and remark ﬁrstly that X , Y , Z are the components of the ponderomotive force acting upon the electron, and are so indeed as viewed in a system moving at the moment with the electron, with the same velocity as the electron. (This force might be measured, for example, by a spring balance at rest in the lastmentioned system.) Now if we call this force simply “the force acting upon the electron,”9 and maintain the equation—mass × acceleration = force—and if we also decide that the accelerations are to be measured in the stationary system K, we derive from the above equations m ( 1 − v 2 /c2 )3 m . 1 − v 2 /c2

Longitudinal mass Transverse mass

= =

.

With a diﬀerent deﬁnition of force and acceleration we should naturally obtain other values for the masses. This shows us that in comparing diﬀerent theories of the motion of the electron we must proceed very cautiously. We remark that these results as to the mass are also valid for ponderable material points, because a ponderable material point can be made into an electron (in our sense of the word) by the addition of an electric charge, no matter how small. We will now determine the kinetic energy of the electron. If an electron moves from rest at the origin of co-ordinates of the system K along the axis of X under the action of an electrostatic force X, it is clear that the energy withdrawn from the electrostatic ﬁeld has the value X dx. As the electron is to be slowly accelerated, and consequently may not give oﬀ any energy in the form of radiation, the energy withdrawn from the electrostatic ﬁeld must be put down as equal to the energy of motion W of the electron. Bearing in mind that during the whole process of motion which we are considering, the ﬁrst of the equations (A) applies, we therefore obtain v W

=

X dx = m

0

β 3 v dv

9 The deﬁnition of force here given is not advantageous, as was ﬁrst shown by M. Planck. It is more to the point to deﬁne force in such a way that the laws of momentum and energy assume the simplest form.

22

= mc2

1 1 − v 2 /c2

−1 .

Thus, when v = c, W becomes inﬁnite. Velocities greater than that of light have—as in our previous results—no possibility of existence. This expression for the kinetic energy must also, by virtue of the argument stated above, apply to ponderable masses as well. We will now enumerate the properties of the motion of the electron which result from the system of equations (A), and are accessible to experiment. 1. From the second equation of the system (A) it follows that an electric force Y and a magnetic force N have an equally strong deﬂective action on an electron moving with the velocity v, when Y = Nv/c. Thus we see that it is possible by our theory to determine the velocity of the electron from the ratio of the magnetic power of deﬂexion Am to the electric power of deﬂexion Ae , for any velocity, by applying the law Am v = . Ae c This relationship may be tested experimentally, since the velocity of the electron can be directly measured, e.g. by means of rapidly oscillating electric and magnetic ﬁelds. 2. From the deduction for the kinetic energy of the electron it follows that between the potential diﬀerence, P, traversed and the acquired velocity v of the electron there must be the relationship P= Xdx = m c2 1 1 − v 2 /c2 −1 .

3. We calculate the radius of curvature of the path of the electron when a magnetic force N is present (as the only deﬂective force), acting perpendicularly to the velocity of the electron. From the second of the equations (A) we obtain − or R= mc2 · v/c 1 − v 2 /c2 · 1 . N v2 d2 y v = = N 2 dt R mc 1− v2 c2

These three relationships are a complete expression for the laws according to which, by the theory here advanced, the electron must move. In conclusion I wish to say that in working at the problem here dealt with I have had the loyal assistance of my friend and colleague M. Besso, and that I am indebted to him for several valuable suggestions.

23

About this Document This edition of Einstein’s On the Electrodynamics of Moving Bodies is based on the English translation of his original 1905 German-language paper (published as Zur Elektrodynamik bewegter K¨rper, in Annalen der Physik. o 17:891, 1905) which appeared in the book The Principle of Relativity, published in 1923 by Methuen and Company, Ltd. of London. Most of the papers in that collection are English translations from the German Das Relativatsprinzip, 4th ed., published by in 1922 by Tuebner. All of these sources are now in the public domain; this document, derived from them, remains in the public domain and may be reproduced in any manner or medium without permission, restriction, attribution, or compensation. Numbered footnotes are as they appeared in the 1923 edition; editor’s notes are marked by a dagger (†) and appear in sans serif type. The 1923 English translation modiﬁed the notation used in Einstein’s 1905 paper to conform to that in use by the 1920’s; for example, c denotes the speed of light, as opposed the V used by Einstein in 1905. This edition was prepared by John Walker. The current version of this document is available in a variety of formats from the editor’s Web site: http://www.fourmilab.ch/

24

Free Essay

...Albert Einstein: A Timeline of his Life Albert Einstein: A Timeline of his Life Albert Einstein has been a common name among us all, but what actually is he famous for? In this I hope to provide you with a chronological summary of the important events in the life of Albert Einstein, from his birth in 1879 to his death in 1955. On March 14th 1879 Albert Einstein was born to Hermann and Pauline in Ulm, Germany. He was born to a middle-class German Jewish family. His parents were concerned that he scarcely talked until the age of three, but he was not so much a backward as he was a quiet child. Unlike more common children he would build tall houses of cards and he hated playing soldier. (www.aip.org/history/einstein) At the age of twelve he was fascinated by a geometry book. At the age of fifteen in 1895 Albert quit high school disgusted by rote learning and martinet teachers, and followed his family to Italy where they moved their failing electro technical business. After half a year of wandering and loafing, he attended a congenial Swiss school. The next year he entered the Federal Institute of Technology in Zurich. (www.aip.org/history/einstein) In 1900 after working hard in the laboratory but skipping lectures, Einstein graduated with an unexceptional record. For two grim years he could find only odd jobs, but he finally got a post as a patent examiner. He married his classmate Mileva Maric in 1903 they had a child Lieserl in 1902 whom......

Words: 967 - Pages: 4

Free Essay

...Informative Speech Outline Specific Purpose: To inform my audience about the life and discoveries of Albert Einstein. Central Idea: Einstein still remains as the most famous scientist of all time and his discoveries are still changing the way we look at the universe. Introduction: E=mc2(squared) is the most famous formula that is known by almost everyone. This famous formula, of course, belongs to the most famous scientist Albert Einstein. I am pretty sure many of you, if not all, has heard of this formula at one point of your lives. Because I have a passion for both science and physics, I have been studying Einstein’s theories and his life for the last couple of years. Today, I am going to talk about early years of Einstein’s life and some of his discoveries which changed the way we look at the world. Body: 1) Einstein was born in Germany and his passion for science started at a young age. A. Einstein was born in Ulm, in the Kingdom of Wurttemberg in the German Empire on March 14th 1879. B. In Einstein’s early ages, his father showed him a pocket compass; Einstein realized that there must be something causing the needle to move. This event sparked the passion inside Einstein for science and later on he began to build mechanical devices for fun. C. Unlike a general thought, he never struggled to pass the exams or talk. It was just his family who thought he had a learning disability. D. Even though being remarkably good at physics and mathematics, he was not as......

Words: 1198 - Pages: 5

Free Essay

...throughout 2012. Over 80,000 records of documents held in original and as copies in the Albert Einstein Archives at the Hebrew University (AEA) and at the Einstein Papers Project at Caltech (EPP) can now be accessed with a user-friendly interface via the internet. The system offers easy navigation, displaying the search results and additional information such as filters, related topics and similar items. Some of the digitized documents are accompanied by annotated transcriptions and translations, as edited by the EPP and published in the Collected Papers of Albert Einstein by Princeton University Press (PUP). These documents are searchable as full text. The Albert Einstein Archives include scientific writings and correspondence, non-scientific writings and correspondence, family letters and travel diaries. Einstein Archives Online presents images of Einstein's handwritten manuscripts; it includes correspondence, typewritten manuscripts, photos, audio material, etc. A word about the sponsors The newly launched digitization project is funded by The Polonsky Foundation UK. Through this foundation, Dr. Polonsky has initiated similar enterprises, such as the digitization of the writings of Sir Isaac Newton at the University of Cambridge. The www.alberteinstein.info website was launched in 2003 by the Albert Einstein Archives jointly with the Einstein Papers Project and Princeton University Press. The digitization of 900 papers displayed......

Words: 283 - Pages: 2

Free Essay

...It is very difficult to earn the title “genius”, but one person that earns this distinction in everybody’s perspective is Albert Einstein. This genius was born in Ulm, Germany on March 14, 1879 and died in Princeton, New Jersey on April 17, 1955. Einstein’s theories were groundbreaking and challenged many existing theories and assumptions at that time. His theories like relativity and photo-electricity made way to many inventions later. Einstein was one of the greatest innovators. He changed the world of physics with his easy-to-learn theories. Einstein once said “Imagination is more important than knowledge. Knowledge is limited. Imagination encircles the world.”. When he first published his Theory of relativity, Einstein was just a Patent Clerk in Switzerland and not a physicist or research scholar, like he wanted to be. This was how this genius made his entrance as an innovator. One of the most important events in Einstein’s life is his work on relativity. The relativity theory is about how speed of light affects time. Time is relative and can move slow or fast depending on the speed of light the matter moves. Another important event is Einstein’s contribution to the World War II. Einstein sent a letter to Franklin Roosevelt, recommending that the United States make the atomic bomb before Germany did. His theory of E=mc2 provided the basis for this invention that changed the outcome of World War II. He later regretted writing the recommendation......

Words: 485 - Pages: 2

Free Essay

...Einstien Albert Einstein Every era has its own heroes. People who stood out amongst the rest. The human race is such a young species compared to the others that we share this amazing planet with. Because we are so young, we still have a lot to learn. I was once told that a day without learning something new, is a day wasted. There is no reason that you should not learn one new thing every day. The world is an amazing place that has so much to offer and so much to learn. How one decides to accomplish the above statement is up to them. There are going to be people who take that a little more serious than others. Among the people of the 19th century that stand out, Albert Einstein is one that has become a house hold name because of the discoveries and theories he was able to come up with in his lifetime. As you read history books, it will be hard not to see Albert Einstein’s name. He alone has made some of the more significant discoveries in our history as a race. The way he was able to achieve this was not in the way one would think. When typically thinking of a person such as Einstein, what comes to mind is someone who spent their lives as a professor in a university, where they were able to spend their time expanding their knowledge and share theories with people of their same intelligence. This environment would allow for them to grow their knowledge by the influences of their surroundings. However this is not the case for Einstein. It wasn’t......

Words: 294 - Pages: 2

Free Essay

...Einstein, Albert (14 Mar. 1879-18 Apr. 1955), theoretical physicist, was born in Ulm, Germany, to Hermann Einstein and Pauline Koch, who had married in 1876. In 1880 the family moved to Munich. There Hermann ran various industrial concerns, eventually managing an electrical business in which his younger brother Jakob provided the technical direction. The two Einstein families lived together in a large house in a Munich suburb. Albert Einstein and his younger sister Maria (Maja) grew up surrounded by Jakob's electrical innovations. Jakob also provided young Albert with science textbooks, notably a seminal exposition of Euclidean geometry. Einstein went to a local primary school and then attended the Luitpold Gymnasium, a progressive secondary school. He succeeded admirably in all his subjects. Following elementary school practice, he received lessons in Judaism, the registered religion of his free-thinking parents. His mother had him study violin privately, and the instrument provided him solace throughout his life. The Einstein electrotechnical business foundered in the highly competitive environment of the middle 1890s. In 1894 Hermann and Jakob Einstein lost a bid to illuminate the streets of Munich. Hermann reestablished himself first in Milan and then in Pavia. Pauline and Maja accompanied him. Albert stayed behind to complete secondary school. After a number of months Albert abandoned school and joined his parents in Milan. He planned to study on his own in......

Words: 625 - Pages: 3

Free Essay

...Albert Einstein Albert Einstein had little resistance attending school. Some say that Einstein had dyslexia. Einstein showed language impairments at a very young age. His family believed he may be slow because of the abnormal period of time before he began to talk. Between the ages of two and three Einstein began to speak whole sentences. According to most researchers they believed that Einstein was withdrawn from the world as a boy. When Einstein started school he did surprisingly well. At the age of 16 Einstein failed the college exam the first time plainly because he did not study and later learned that it’s a bad choice to not prepare for a test. Einstein is a clear example of a person who is listed with learning disabilities in today's schools. If you have the right approach to education than labels can’t stop you from making great accomplishments, which is proven by Einstein and others like Thomas Edison, Leonardo de Vinci, George Washington, Thomas Jefferson, Winston Churchill, and Walt Disney. Einstein made many contributions to mathematics. The first is the Special Theory of Relativity, which essentially deals with the question of whether rest and motion are relative or absolute, and with the consequences of Einstein’s conjecture that they are relative. The second is the General Theory of Relativity, which primarily applies to particles as they accelerate, particularly due to gravitation, and acts as a radical revision of Newton’s theory, predicting important......

Words: 479 - Pages: 2

Free Essay

...them. Albert Einstein was a German-born physicist who developed the general theory of relativity, among other feats. He is considered the most influential physicist of the 20th century. Born in Ulm, Württemberg, Germany in 1879, Albert Einstein had a passion for inquiry that eventually led him to develop the special and general theories of relativity. In 1921, he won the Nobel Prize for physics for his explanation of the photoelectric effect and immigrated to the U.S. in the following decade after being targeted by the Nazis. Einstein is generally considered the most influential physicist of the 20th century, with his work also having a major impact on the development of atomic energy. With a focus on unified field theory during his later years, Einstein died on April 18, 1955, in Princeton, New Jersey. Einstein attended elementary school at the Luitpold Gymnasium in Munich. However, he felt alienated there and struggled with the institution's rigid pedagogical style. He also had what were considered to be speech challenges, though he developed a passion for classical music and playing the violin that would stay with him into his later years. Most significantly, Einstein's youth was marked by deep inquisitiveness and inquiry. Towards the end of the 1880s, Max Talmud, a Polish medical student who sometimes dined with the Einstein family, became an informal tutor to young Albert. Talmud had introduced his pupil to a children’s science text that inspired Einstein to dream......

Words: 286 - Pages: 2

Free Essay

...German-born American theoretical physicist, Albert Einstein, often regarded as the father of modern physics, had exceptional intellectual ability and unprecedented insight. Many believed him to be one of the most influential people in both science and mathematics, and quite possibly the most famous scientist of the 20th century (Severance, 1999). As cited by Fingon and Fingon, Einstein was well known for being a brilliant physicist and abstract thinker, applying his creativity and imagination in his scientific thought process (Parker, 2003). He received the 1921 Nobel Prize for his contribution to the study of physics, namely his special (1905) and general (1916) theories of relativity. The name “Einstein” is often thought of as being synonymous with the word genius. Einstein was not always thought of as a genius, however. His unique intellectual abilities as a young boy created challenges for him in his everyday home and school life, but his sense of wonder paired with persistence and determination led him to be the successful prodigy people know him as today. Abraham Maslow’s humanistic approach of self-actualization provides significant explanation for Einstein’s behaviors and achievements throughout his life. Heredity and environment played vital roles in Einstein’s psychological development. Einstein’s parents and teachers observed his early childhood developmental delays and had doubts regarding his intelligence. His parents worried about his intellectual......

Words: 1251 - Pages: 6

Premium Essay

...Albert Einstein Of all the scientists to emerge from the nineteenth and twentieth centuries there is one whose name is known by almost all living people. While most of these do not understand this man's work, everyone knows that its impact on the world of science is astonishing. Yes,many have heard of Albert Einstein's General Theory of relativity, but few know about the intriguing life that led this scientist to discover what some have called, "The greatest single achievement of human thought." Einstein was born in Ulm, Germany on March 14, 1874. Before his first birthday, his family had moved to Munich where young Albert's father, Hermann Einstein, and uncle set up a small electro-chemical business. He was fortunate to have an excellent family with which he held a strong relationship. Albert's mother, Pauline Einstein, had an intense passion for music and literature, and it was she that first introduced her son to the violin in which he found much joy and relaxation. Also, he was very close with his younger sister, Maja, and they could often be found in the lakes that were scattered about the countryside near Munich. As a child, Einstein's sense of curiosity had already begun to stir. A favorite toy of his was his father's compass, and he often marveled at his uncle's explanations of algebra. Although young Albert was intrigued by certain mysteries of science, he was considered a slow learner. His failure to become fluent in......

Words: 1696 - Pages: 7

Premium Essay

...Albert Einstein Of all the scientists to emerge from the nineteenth and twentieth centuries there is one whose name is known by almost all living people. While most of these do not understand this man's work, everyone knows that its impact on the world of science is astonishing. Yes,many have heard of Albert Einstein's General Theory of relativity, but few know about the intriguing life that led this scientist to discover what some have called, "The greatest single achievement of human thought." Einstein was born in Ulm, Germany on March 14, 1874. Before his first birthday, his family had moved to Munich where young Albert's father, Hermann Einstein, and uncle set up a small electro-chemical business. He was fortunate to have an excellent family with which he held a strong relationship. Albert's mother, Pauline Einstein, had an intense passion for music and literature, and it was she that first introduced her son to the violin in which he found much joy and relaxation. Also, he was very close with his younger sister, Maja, and they could often be found in the lakes that were scattered about the countryside near Munich. As a child, Einstein's sense of curiosity had already begun to stir. A favorite toy of his was his father's compass, and he often marveled at his uncle's explanations of algebra. Although young Albert was intrigued by certain mysteries of science, he was considered a slow learner. His failure to become fluent in......

Words: 1696 - Pages: 7

Free Essay

...Daniel Retta English 4 Essay: Albert Einstein Albert Pippy Einstein was born March 14, 1879 in Ulm, Kingdom of Württemberg, German Empire. He is well known for his scientific achievements in the field of theoretical physics. His achievements are so highly valued that he is commonly regarded as the father of modern physics. His father was Hermann Einstein and his mother was Pauline Koch. He had a sister two years younger named Maja Einstein. Although Einstein's family was Jewish, they were nonobservant and he attended a Catholic elementary school, Petersschule, from the ages of 5 till 10. He became highly religious around the age of 12 and actually began writing and singing During this time he had speech difficulties, though he was a top student. In 1889 a family friend Max Talmud introduced young Einstein, age 10, to some key texts in science, mathematics and philosophy, including Euclid's Elements and Kant's Critique of Pure Reason. Einstein's family went through a few moves in response to their economic status difficulties. Albert's father and uncle together held a business, Elektrotechnische Fabrik J. Einstein & Cie, which manufactured electrical equipment based on direct current. Because it was dependent upon the success of DC (direct current), during the War of the Currents, AC (alternating current) became the standard and their business went under. In search of better financial opportunity Herrman and his family moved to Italy, first to the city of......

Words: 1595 - Pages: 7

Premium Essay

...To explain the photoelectric effect, Einstein came up with the photon hypothesis. The energy of a photon is associated with its frequency with the relation (1.1) Where h is the Planck constant. And to solve the paradox that electrons goes around the nuclear without electromagnetic radiation, Bohr put forward the atom model. In this theory the electrons have stationary orbits (1.2) Where is called the reduced mass. When the electrons transit from the high energy levels to the lower ones, the energy of the photons emitted is just the energy difference between two levels. In terms of the wavenumber 1.2 The Pickering Series and the Hydrogen-like Ions In our textbook the Modern Atomic and Nuclear Physics by Fujia Yang it talked about the hydrogen-like ions. And the first well-researched hydrogen-like atom is the helium ions, and this ion...

Words: 3585 - Pages: 15

Premium Essay

...Psychological Development of Albert Einstein Erica Hopkins PSY 300 Psychological Development of Albert Einstein Albert Einstein was one of the most intelligent, driven and moral minds of the 20th century. His early preparation in education and wonder greatly contributed to his eventual success and scientific advancements for the world. Einstein had a great support system around him at all times it seems. He was born on March 14, 1879 as the first child to Hermann and Pauline Einstein in Ulm Germany. (Krakow, 2004). His father was a business owner and gave Einstein a head start in mechanics and technology. (Krakow, 2004). Einstein had a younger sister born 2 years after him which contributed to his family support system. (Krakow, 2004). He had several highly educated tutors most from a couple religious backgrounds. His family moved to Italy when he was fifteen. He stayed behind living with relatives in order to finish his education at Luitpold-Gynasium grammar school in Munich, Germany (Isaacson, 2007). He eventually followed his family to Italy just a few months later. He left his education to be with his family and had a hard time gaining a diploma after (Isaacson, 2007). Because Einstein had a strong support system he was probably comfortable making such life altering decisions. Having strong social support reduces stressful events and most likely stressful decisions (Kowalski & Westen, 2011). Throughout his life he maintained long-term friendships he gained......

Words: 1266 - Pages: 6

Premium Essay

...Globalization and Organization “I know not with what weapons World War III will be fought, but World War IV will be fought with sticks and stones.” Albert Einstein Devin Brown Economics 2015-2016 How I interpret this quote by Mr. Einstein is that humanity will one day annihilate themselves close to extinction, by the weapons they have and will create in the future. When it happens, the remaining inhabitants will have to repopulate and use the ancient methods of living again. In this assignment, the key debates are the socialist against the capitalist system respectively, how it affects the political, economical and cultural aspect of globalization, with reference to theories and examples to illustrate them. The dependency theory states that the poverty of low-income countries stems from their exploitation by wealthy countries and the multinational corporations that are based in wealthy countries. This is used due to the example of Coca-Cola (a multinational corporation from the west) abusing India’s water supply in villages to make their products because of the capitalist system of minimizing production costs without governmental interference (as India is quite high in terms of corruption) and the pollution it created. This situation got so problematic that India had to shut down the factories that produce the product, which may end up hurting their political ties with United States of America (U.S.A) and the economic as it losses jobs for the......

Words: 1278 - Pages: 6