4.5 Conventional Wisdom 

This, however, is thought to be a mere strain upon the text, for the words are these: ‘That all true believers break their eggs at the convenient end’, and which end is the convenient end, seems, in my humble opinion, to be left to every man’s conscience… 
Jonathan Swift, 1726 

It is a matter of empirical fact that the speed of light is invariant in terms of inertial coordinates, and yet the invariance of the speed of light is often said to be a matter of convention  as indeed it is. The empirical fact refers to the speed of light in terms of inertial coordinates, but the decision to define speeds in terms of inertial coordinates is conventional. It’s trivial to define systems of space and time coordinates in terms of which the speed of light is not invariant, but we ordinarily choose to describe events in terms of inertial coordinates, partly because of the invariance of light speed based on those coordinates. Of course, this invariance would be tautological if inertial coordinate systems were simply defined as the systems in terms of which the speed of light is invariant. However, as discussed in Section 1.3, the class of inertial coordinate systems is actually defined in purely mechanical terms, without reference to the propagation of light. They are the coordinate systems in terms of which mechanical inertia is homogeneous and isotropic (which are the necessary and sufficient conditions for Newton’s three laws of motion to be valid, at least quasistatically). The empirical invariance of light speed with respect to this class of coordinate systems is a nontrivial empirical fact, but nothing requires us to define “velocity” in terms of inertial coordinate systems. Such systems cannot claim to have any a priori status as the “true” class of coordinates. Despite the undeniable success of the principle of inertia as a basis for organizing our understanding of the processes of nature, it is nevertheless a convention. 

The conventionalist view can be traced back to Poincare, who wrote in "The Measure of Time" in 1898 

... we have no direct intuition about the equality of two time intervals. The simultaneity of two events or the order of their succession, as well as the equality of two time intervals, must be defined in such a way that the statements of the natural laws be as simple as possible. 

In the same paper, Poincare described the use of light rays, together with the convention that the speed of light is invariant and the same in all directions, to give an operational meaning to the concept of simultaneity. In his book "Science and Hypothesis" (1902) he summarized his view of time by saying 

There is no absolute time. When we say that two periods are equal, the statement has no meaning, and can only acquire a meaning by a convention. 

Poincare's views had a strong influence on the young Einstein, who avidly read "Science and Hypothesis" with his friends in the selfstyled "Olympia Academy". Solovine remembered that this book "profoundly impressed us, and left us breathless for weeks on end". Indeed we find in Einstein's 1905 paper on special relativity the statement 

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. 

In a later popular exposition, Einstein tried to make the meaning of this definition more clear by saying 

That light requires the same time to traverse the path A to M (the midpoint of AB) as for the path B to M is in reality neither a supposition nor a hypothesis about the physical nature of light, but a stipulation which I can make of my own freewill in order to arrive at a definition of simultaneity. 

Of course, this concept of simultaneity is also embodied in Einstein's second "principle", which asserts the invariance of light speed. Throughout the writings of Poincare, Einstein, and others, we see the invariance of the speed of light referred to as a convention, a definition, a stipulation, a free choice, an assumption, a postulate, and a principle... as well as an empirical fact. There is no conflict between these characterizations, because the convention (definition, stipulation, free choice, principle) that Poincare and Einstein were referring to is nothing other than the decision to use inertial coordinate systems, and once this decision has been made, the invariance of light speed is an empirical fact. As Poincare said in 1898, we naturally choose our coordinate systems "in such a way that the statements of the natural laws are as simple as possible", and this almost invariably means inertial coordinates. It was the great achievement of Galileo, Descartes, Huygens, and Newton to identify the principle of inertia as the basis for resolving and coordinating physical phenomena. Unfortunately this insight is often disguised by the manner in which it is traditionally presented. The beginning physics student is typically expected to accept uncritically an intuitive notion of "uniformly moving" time and space coordinate systems, and is then told that Newton's laws of motion happen to be true with respect to those "inertial" systems. It is more meaningful to say that we define inertial coordinate systems as those systems in terms of which Newton's laws of motion are valid. We naturally coordinate events and organize our perceptions in such a way as to maximize symmetry, and for the motion of material objects the most important symmetries are the isotropy of inertia, the conservation of momentum, the law of equal action and reaction, and so on. Newtonian physics is organized entirely upon the principle of inertia, and the basic underlying hypothesis is that for any object in any state of motion there exists a system of coordinates in terms of which the object is instantaneously at rest and inertia is homogeneous and isotropic (implying that Newton's laws of motion are at least quasistatically valid). 

The empirical validity of this remarkable hypothesis accounts for all the tremendous success of Newtonian physics. As discussed in Section 1.3, the specification of a particular state of motion, combined with the requirement for inertia to be homogeneous and isotropic, completely determines a system of coordinates (up to insignificant scale factors, rotations, etc), and such a system is called an inertial system of coordinates. Such coordinate systems can be established unambiguously by purely mechanical means (neglecting the equivalence principle and associated complications in the presence of gravity). The assumption of inertial isotropy with respect to a given state of motion suffices to establishes the loci of inertial simultaneity for that state of motion. Poincare and Einstein rightly noted the conventionality of this simultaneity definition because they were not presupposing the choice of inertial simultaneity. In other words, we are not required to use inertial coordinates. We simply choose, of our own free will, to use inertial coordinates  with the corresponding inertial definition of simultaneity  because this renders the statement of physical laws and the descriptions of physical phenomena as simple and perspicuous as possible, by taking advantage of the maximum possible symmetry. 

In this regard it's important to remember that inertial coordinates are not entirely characterized by the quality of being unaccelerated, i.e., by the requirement that isolated objects move uniformly in a straight line. It's also necessary to require the unique simultaneity convention that renders mechanical inertial isotropic (the same in all spatial directions), which amounts to the stipulation of equal oneway speeds for the propagation of physically identical actions. These comments are fully applicable to the Newtonian concept of space, time, and inertial reference frames. Given two objects in relative motion we can define two systems of inertial coordinates in which the respective objects are at rest, and we can orient these coordinates so the relative motion is purely in the x direction. Let t,x and T,X denote these two systems of inertial coordinates. That such coordinates exist is the main physical hypothesis underlying Galilean physics. An auxiliary hypothesis – one that was not always clearly recognized – concerns the relationship between two such systems of inertial coordinates, given that they exist. Galileo assumed that if the coordinates x,t of an event are known, and if the two inertial coordinate systems are the rest frames of objects moving with a relative speed of v, then the coordinates of that event in terms of the other system (with suitable choice of origins) are T = t, X = x  vt. Viewed in the abstract, this is a rather peculiar and asymmetrical assumption, although it is admittedly borne out by experience  at least to the precision of measurement available to Galileo. However, we now know, empirically, that the relation between relatively moving systems of inertial coordinates has the symmetrical form T = (t  vx)/g and X = (x  vt)/g where g = (1v^{2})^{1/2} when the time and space variables are expressed in the same units such that the constant (3)10^{8} meters/second equals unity. It follows that the oneway (not just the twoway) speed of light is invariant and isotropic with respect to any and every system of inertial coordinates. 

The empirical content of this statement is simply that the propagation of light is isotropic with respect to the same class of coordinate systems in terms of which mechanical inertia is isotropic. This is consistent with the fact that light itself is an inertial phenomena, e.g., it conveys momentum. In fact, the inertia of light can be seen as a common thread running through three of the famous papers published by Einstein in 1905. In the paper entitled "On a Heuristic Point of View Concerning the Production and Transformation of Light" Einstein advocated a conception of light as tiny quanta of energy and momentum, somewhat reminiscent of Newton's inertial corpuscles of light. It's clear that Einstein already understood that the conception of light as a classical wave is incomplete. In the paper entitled "Does the Inertia of a Body Depend on its Energy Content?" he explicitly advanced the idea of light as an inertial phenomenon, and of course this was suggested by the fundamental ideas of the special theory of relativity presented in the paper "On the Electrodynamics of Moving Bodies". 

The Galilean conception of inertial frames assumed that all such frames share a unique foliation of spacetime into "instants". Thus the relation "in the present of" constituted an equivalence relation across all frames of reference. If A is in the present of B, and B is in the present of C, then A is in the present of C. However, special relativity makes it clear that there are infinitely many distinct loci of inertial simultaneity through any given event, because inertial simultaneity depends on the velocity of the worldline through the event. The inertial coordinate systems do induce a temporal ordering on events, but only a partial one. (See the discussion of total and partial orderings in Section 1.2.) With respect to any given event we can still partition all the other events of spacetime into distinct causal regions, including "past", "present" and "future", but in addition we have the categories "future null" and "past null", and none of these constitute equivalence classes. For example, it is possible for A to be in the present of B, and B to be in the present of C, and yet A is not in the present of C. Being "in the present of" is not a transitive relation. 

It could be argued that a total unique temporal ordering of events is a more useful organizing principle than the isotropy of inertia, and so we should adopt a class of coordinate systems that provides a total ordering. We can certainly do this, as Einstein himself described in his 1905 paper 

To be sure, we could content ourselves with evaluating the time of events by stationing an observer with a clock at the origin of the coordinates who assigns to an event to be evaluated the corresponding position of the hands of the clock when a light signal from that event reaches him through empty space. However, we know from experience that such a coordination has the drawback of not being independent of the position of the observer with the clock. 

The point of this "drawback" is that there is no physically distinguished "origin" on which to base the time coordination of all systems of reference, so from the standpoint of assessing possible causal relations we must still consider the full range of possible "absolute" temporal orderings. This yields the same partial ordering of events as does the set of inertial coordinates, so the "total ordering" that we can achieve by imposing a single temporal foliation on all frames of reference is only formal, and not physically meaningful. Nevertheless, we could make this choice, especially if we regard the total temporal ordering of events as a requirement of intelligibility. This seems to have been the view of Lorentz, who wrote in 1913 about the comparative merits of the traditional Galilean and the new Einsteinian conceptions of time 

It depends to a large extent on the way one is accustomed to think whether one is attracted to one or another interpretation. As far as this lecturer is concerned, he finds a certain satisfaction in the older interpretations, according to which... space and time can be sharply separated, and simultaneity without further specification can be spoken of... one may perhaps appeal to our ability of imagining arbitrarily large velocities. In that way one comes very close to the concept of absolute simultaneity. 

Of course, the idea of "arbitrarily large velocities" already presupposes a concept of absolute simultaneity, so Lorentz's rationale is not especially persuasive, but it expresses the point of view of someone who places great importance on a total temporal ordering, even at the expense of inertial isotropy. Indeed one of Poincare's criticisms of Lorentz's early theory was that it sacrificed Newton's third law of equal action and reaction. (This can be formally salvaged by assigning the unbalanced forces and momentum to an undetectable ether, but the physical significance of a conservation law that references undetectable elements is questionable.) Oddly enough, even Poincare sometimes expressed the opinion that a total temporal ordering would always be useful enough to outweigh other considerations, and that it would always remain a safe convention. The approach taken by Lorentz and most others may be summarized by saying that they sacrificed the physical principles of inertial relativity, isotropy, and homogeneity in order to maintain the assumed Galilean composition law. This approach, although technically serviceable, suffers from a certain inherent lack of conviction, because while asserting the ontological reality of anisotropy in all but one (unknown) frame of reference, it unavoidably requires us to disregard that assertion and arbitrarily assume one particular frame as being "the" rest frame. 

Poincare and Einstein recognized that in our descriptions of events in spacetime in terms of separate space and time coordinates we're free to select our "basis" of decomposition. This is precisely what one does when converting the description of events from one frame to another using Galilean relativity, but, as noted above, the Galilean composition law yields anisotropic results when applied to actual observations. So it appeared (to most people) that we could no longer maintain isotropy and homogeneity in all inertial frames together with the ability to transform descriptions from one frame to another by simply applying the appropriate basis transformation. But Einstein realized this was too pessimistic, and that the new observations were fully consistent with both isotropy in all inertial frames and with simple basis transformations between frames, provided we adjust our assumption about the effective metrical structure of spacetime. In other words, he brilliantly discerned that Lorentz's anisotropic results totally vanish in the context of a different metrical structure. 

Even a metrical structure is conventional in a sense, because it relies on our ontological premises. For example, the magnitude of the interval between two events may seem to be one thing but actually be another, due (perhaps) to variations in our means of observation and measurement. However, once we have agreed on the physical significance of inertial coordinate systems, the invariance of the quantity (dt)^{2 } (dx)^{2 } (dy)^{2}  (dz)^{2} also becomes physically significant. This shows the crucial importance of the very first sentence in Section 1 of Einstein's 1905 paper: 

Let us take a system of coordinates in which the equations of Newtonian mechanics hold good. 

Suitably qualified (as noted in Section 1.3), this immediately establishes not only the convention of simultaneity, but also the means of operationally establishing it, and its physical significance. Any observer in any state of inertial motion can throw two identical particles in opposite directions with equal force (i.e., so there is no net disturbance of the observer's state of motion), and the convention that those two particles have the same speed suffices to fully specify an entire system of space and time coordinates, which we call inertial coordinates. It is then an empirical fact  not a definition, convention, assumption, stipulation, or postulate  that the speed of light is isotropic in terms of inertial coordinates. This obviously doesn't imply that inertial coordinates are "true" in any absolute sense, but the principle of inertia has proven to be immensely powerful for organizing our knowledge of physical events, and for discerning and expressing the apparent chains of causation. 

If a flash of light emanates from the geometrical midpoint between two spatially separate particles at rest in an inertial frame, the arrival times of the light wave at those two particles are simultaneous in terms of that rest frame’s inertial coordinates. Furthermore, we find empirically that all other physical processes are isotropic with respect to those inertial coordinates, e.g., if a sound wave emanates from the midpoint of a uniform steel beam at rest in an inertial frame, the sound reaches the two ends simultaneously in accord with this definition. If we adopt any other convention we introduce anisotropies in our descriptions of physical processes, such as sound in a uniform stationary steel beam propagating more rapidly in one direction than in the other. The isotropy of physical phenomena  including the propagation of light  is strictly a convention, but it was not introduced by special relativity, it is one of the fundamental principles which we use to organize our knowledge, and it leads us to choose inertial coordinates for the description of events. On the other hand, the isotropy of multiple distinct physical phenomena in terms of inertial coordinates is not purely conventional, because those coordinates can be defined in terms of just one of those phenomena. The value of this definition is due to the fact that a wide variety of phenomena are (empirically) isotropic with respect to the same class of coordinate systems. 

Of course, it could be argued that all these phenomena are, in some sense, “the same”. For example, the energy conveyed by electromagnetic waves has momentum, so it is an inertial phenomenon, and therefore it is not surprising that the propagation of such energy is isotropic in terms of inertial coordinates. From this point of view, the value of the definition of inertial coordinates is that it reveals the underlying unity of superficially dissimilar phenomena, e.g., the inertia of energy. This illustrates that our conventions and definitions are not empty, because they represent ways of organizing our knowledge, and the efficiency and clarity of this organization depends on choosing conventions that reflect the unity and symmetries of the phenomena. We could, if we wish, organize our knowledge based on the assumption of a total temporal ordering of events, but then it would be necessary to introduce a whole array of unobservable anisotropic "corrections" to the descriptions of physical phenomena. 

As we’ve seen, the principle of relativity constrains, but does not uniquely determine, the form of the mapping from one system of inertial coordinates to another. In order to fix the observable elements of a spacetime theory with respect to every member of the equivalence class of inertial frames we require one further postulate, such as the invariance of light speed (or the inversion symmetry discussed in Chapter 1.8). However, we should distinguish between the strong and weak forms of the lightspeed invariance postulate. The strong form asserts that the oneway speed of light is invariant with respect to the natural spacetime basis associated with any inertial state of motion, whereas the weak form asserts only that the roundtrip speed of light is invariant. To illustrate the different implications of these two different assumptions, consider an experiment of the type conducted by Michelson and Morley in their efforts to detect a directional variation in the speed of light, due to the motion of the Earth through the aether, with respect to which the absolute speed is light was presumed to be referred. To measure the speed of light along a particular axis they effectively measured the elapsed time at the point of origin for a beam of light to complete a round trip out to a mirror and back. At first we might think that it would be just as easy to measure the oneway speed of light, by simply comparing the time of transmission of a pulse of light from one location to the time of reception at another location, but of course this requires us to have clocks synchronized at two spatially separate locations, whereas it is precisely this synchronization that is at issue. Depending on how we choose to synchronize our separate clocks we can measure a wide range of light speeds. To avoid this ambiguity, we must evaluate the time interval for a transit of light at a single spatial location (in the coordinate system of interest), which requires us to measure a round trip, just as Michelson and Morley did. 

Incidentally, it might seem that Roemer's method of estimating the speed of light from the variations in the period between eclipses of Jupiter's moons (see Section 3.3) constituted a oneway measurement. Similarly people sometimes imagine that the oneway speed of light could be discerned by (for example) observing, from the center of a circle, pulses of light emitted uniformly by a light source moving at constant speed around the perimeter of the circle. Such methods are indeed capable of detecting certain kinds of anisotropy, but they cannot detect the anisotropy entailed by Lorentz’s ether theory, nor any of the other theories that are observationally indistinguishable from Lorentz’s theory (which itself is indistinguishable from special relativity). In any theory of this class, there is an ambiguity in the definition of a “circle” in motion, because circles contract to ellipses in the direction of motion. Likewise there is ambiguity in the definition of “uniformlytimed” pulses from a light source moving around the perimeter of a moving circle (ellipse). The combined effect of length contraction and time dilation in a Lorentzian theory is to render the anisotropies unobservable. 

The empirical indistinguishability between the theories in this class implies that there is no unambiguous definition of “the oneway speed of light”. We can measure without ambiguity only the lapses of time for closedloop paths, and such measurements cannot establish the “openloop” speed. The ambiguity in the oneway speed remains, because over any closed loop, by definition, the net change in each and every direction is zero. Hence it is possible to consistently interpret all observations based on the assumption of nonisotropic light speed. Admittedly the resulting laws take on a somewhat convoluted appearance, and contain unobservable parameters, but they can't be ruled out empirically. To illustrate, consider a measurement of the roundtrip speed of light, assuming light travels at a constant speed c relative to some absolute medium with respect to which our laboratory is moving with a speed v. Under these assumptions, we would expect a pulse of light to travel with a speed c+v (relative to the lab) in one direction, and cv in the opposite direction. So, if we send a beam of light over a distance L out to a mirror in the "c+v" direction, and it bounces back over the same distance in the "cv" direction, the total elapsed time to complete the round trip of length 2L is 

_{} 

Therefore, the average roundtrip speed relative to the laboratory would be 

_{} 

This shows why a roundtrip measurement of the speed of light would not be expected to reveal any dependency on the velocity of the laboratory unless the measurement was precise enough to resolve secondorder effects in v/c. The ability to detect such small effects was first achieved in the late 19th century with the development of precision interferometry (exploiting the wavelike properties of light.) The experiments of Michelson and Morley showed that, despite the movement of the Earth in its orbit around the Sun (to say nothing of the movement of the solar system, and even of the galaxy), there was no (v/c)^{2} term in the roundtrip speed of light. In other words, they found that 2L/Dt is always equal to c, at least to the accuracy they could measure, which was more than adequate to rule out a secondorder deviation. Thus we have a firm empirical basis for asserting that the roundtrip speed of light is independent of the motion of the source. This is the weak form of the invariant light speed postulate, but in his 1905 paper Einstein asserted something stronger, namely, that we should adopt the convention of regarding the oneway speed of light as invariant. This stronger postulate doesn't follow from the results of Michelson and Morley, nor from any other conceivable experiment or observation  but there is also no conceivable observation that could conflict with it. The invariant roundtrip speed of light fixes the observable elements of the theory, but it does not uniquely determine the presumed ontological structure, because multiple different interpretations can be made to fit the same set of appearances. The oneway speed of light is necessarily an interpretative element of our experience. 

To illustrate the ambiguity, notice that we can ensure a null result for the Michelson and Morley experiment while maintaining nonconstant light speed, merely by requiring that the speed of light v_{1} and v_{2} in the two opposite directions of travel (out and back) satisfy the relation 

_{} 

In other words, a linear roundtrip measurement of light speed will yield the constant c in every direction provided only that the harmonic mean of the oneway speeds in opposite directions always equals c. This is easily accomplished by defining the oneway velocity v_{1} as a function of direction arbitrarily for all directions in one hemisphere, and then setting the velocities in the opposite directions the velocities v_{2} in the opposite directions as v_{2} = cv_{1 }/ (2v_{1}  c). However, we also wish to cover more complicated roundtrips, rather than just back and forth on a single line. To ensure that a circuit of light around an equilateral triangle with edges of length L yields a roundtrip speed of c, the speeds v_{1}, v_{2}, v_{3} in the three equally spaced directions must satisfy 

_{} 

so again we see that the light speeds must have a harmonic mean of c. In general, to ensure that every closed loop of light, regardless of the path, yields the average speed c, it's necessary (and also sufficient) to have light speed v = C(q) as a function of angle q in a principal plane such that, for any positive integer n, 

_{} 

In units with c = 1, we need the n terms on the left side to sum to n, so the velocity function must be such that 1/C(q) = 1 + f(q) where the function f(q) satisfies 

_{} 

for all q. The canonical example of such a function is simply f(q) = k cos(q) for any constant k. Thus if we postulate that the speed of light varies as a function of the angle of travel q relative to some primary axis according to the equation 

_{} 

then we are assured that all closedloop measurements of the speed of light will yield the constant c, despite the fact that the oneway speed of light is distinctly nonisotropic (for nonzero k). This equation describes an ellipse, and no measurement can disprove the hypothesis that the oneway speed of light actually is (or is not) given by (1). It is, strictly speaking, a matter of convention. If we choose to believe that light has the same speed in all directions, then we assume k = 0, and in order to send a synchronizing signal to two points we would locate ourselves midway between them (i.e., at the location where round trips between ourselves and those two points take the same amount of time.) On the other hand, if we choose to believe light travels twice as fast in one direction as in the other, then we would assume k = 1/3, and we would locate ourselves 2/3 of the way between them (i.e., twice as far from one as the other, so round trip times are two to one). The latter case is illustrated in the figure below. 



Regardless of what value we assume for k (in the range from 1 to +1), we can synchronize all clocks according to our belief, and everything will be perfectly consistent and coherent. Of course, in any case it's necessary to account consistently for the lapse of time for information to get from one clock to another, but the lapse of time between any two clocks separated by a distance L can be anything we choose in the range from virtually 0 to 2L/c. The only real constraint is that that the speed be an elliptical function of the direction angle. 

The velocity profile given by (1) is simply the polar equation of an ellipse (or ellipsoid is revolved about the major axis), with the pole at one focus, the semilatus rectum equal to c, and eccentricity equal to k. This just projects the ellipse given by cutting the light cone with an oblique plane. Interestingly, there are really two light cones that intersect on this plane, and they are the light cones of the two events whose projections are the two foci of the ellipse  for timelike separated events. Recall that all rays emanating from one focus of an ordinary ellipse and reflecting off the ellipse will reconverge on the other focus, and that this kind of ray optics is timesymmetrical. In this context our projective ellipse is the intersection of two nullcones, i.e., it is the locus of all points in spacetime that are nullseparated from both of the "foci events". This was to be expected in view of the timesymmetry of Maxwell's equations (not to mention the relativistic Schrodinger equation), as discussed in Section 9. 

Our main reason for assuming k = 0 is our preference for symmetry, simplicity, and consistency with inertial isotropy. Within our empirical constraints, k can be interpreted as having any value between 1 and +1, but the principle of sufficient reason suggests that it should not be assigned a nonzero value in the absence of any rational justification. Nevertheless, it remains a convention (albeit a compelling one), but we should be clear about what precisely is – and what is not – conventional. The invariance of lightspeed is a convention, but the invariance of lightspeed in terms of inertial coordinates is an empirical fact, and this empirical fact is not a formal tautology, because inertial coordinates are determined by the mechanical inertia of material objects, independent of the propagation of light. 

Recall that Einstein’s 1905 paper states that if a pulse of light is emitted from an unaccelerated clock at time t_{1}, and is reflected off some distant object at time t_{2}, and is received back at the original clock at time t_{3}, then the inertial coordinate synchronization is given by stipulating that 

_{} 

Reichenbach noted that the formally viable simultaneity conventions correspond to the assumption 

_{} 

where e is any constant in the range from 0 to 1. This describes the same class of “elliptical speed” conventions as discussed above, with e = (k+1)/2 where k ranges from 1 to +1. The corresponding coordinate transformation is a simple time skew, i.e., x’ = x, y’ = y, z’ = z, t’ = t + kx/c. This describes the essence of the Lorentzian “absolutist” interpretation of special relativity. Beginning with the putative absolute rest frame inertial coordinates x,y, Lorentz associates with each state of motion v a system of coordinates x’,t’ related to x,y by a Galilean transformation with parameter v. In other words, x’ = x – vt and t’ = t. He then rescales the x’,t’ coordinates to account for what he regards as the physical contraction of the lengths of stable object and the slowing of the durations of stable physical processes, to arrive at the coordinates x” = x/ g and t” = t g where g = (1v^{2}/c^{2})^{1/2}. These he regards as the proper rest frame coordinates for objects moving with speed v in terms of the absolute frame. There is nothing logically unacceptable about these coordinate systems, but we must realize that they do not constitute inertial coordinate systems in the full sense. Mechanical inertia and the speed of light are not isotropic in terms of such coordinates, precisely because the time foliation (i.e., the simultaneity convention) is skewed relative to the e = 1/2 convention. 

If we begin with the inertial rest frame coordinates for the state of motion v (which Lorentz and Einstein agree are related to the putative absolute rest frame coordinate by a Lorentz transformation), and then apply the time skew transformation with parameter k = v/c, we arrive at these Lorentzian rest frame coordinates. Needless to say, our choice of coordinate systems does not affect the outcome of any physical measurement, except that the outcome will be expressed in different terms. For example, by the Einsteinian convention the speed of light is isotropic in terms of the rest frame coordinates of any material object, whereas by the Lorentzian convention it is not. This difference is simply due to different definitions of “rest frame coordinates”. If we specify inertial coordinate systems (i.,e., coordinates in terms of which inertia is isotropic and Newton’s laws are quasistatically valid) then there is no ambiguity, and both Lorentz and Einstein agree that the speed of light is isotropic in terms of all inertial coordinate systems. 

In subsequent sections we’ll see that the standard formalism of general relativity provides a convenient means of expressing the relations between spacetime events with respect to a larger class of coordinate systems, so it may appear that inertial references are less significant in the general theory. In fact, Einstein once hoped that the general theory would not rely on the principle of inertia as a primitive element. However, this hope was not fulfilled, and the underlying physical basis of the spacetime manifold in general relativity remains the set of primitive inertial paths (geodesics) through spacetime. Not only do these inertial paths determine the equivalence class of allowable coordinate systems (up to diffeomorphism), it even remains true that at each event we can construct a (local) system of inertial coordinates with respect to which the speed of light is c in all directions. Thus the empirical fact of lightspeed invariance and isotropy with respect to inertial coordinates remains as a primitive component of the theory. The difference is that in the general theory the convention of using inertial coordinates is less prevalent, because in general there is no single global inertial coordinate system, and noninertial coordinate systems are often more convenient on a curved manifold. 
