zotero/storage/IM4J4RYQ/.zotero-ft-cache

The c-equivalence principle and its implications for physics
Max Tran

arXiv:2208.14828v1 [physics.hist-ph] 27 Aug 2022

Abstract. The c-equivalence principle, commonly accepted as true by most physicists, is the unstated assumption that 1/√ oµo equals the kinematic speed of light. Should someone prove the principle false, it would render the composition of two Lorentz transformations meaningless. It would also invalidate the second hypothesis of the Special Theory of Relativity in its strong form. This paper examine some other consequences for physics, should this principle be proven false and outline some experiments to determine light speed, which could falsify the principle and provide evidence for the ether.

Keywords: c-equivalence principle, Maxwell’s constant, Lorentz transformation, light speed experiments, Special relativity theory, Sagnac Effect, Michelson-Morley, KennedyThorndike, Ives-Stilwell, Ether

1. Introduction

When James Clerk Maxwell formulated the equations of electromagnetism that now

bears his name, he based them upon an ether/medium model characterized by three

measurable quantities o, µo, and σo. Today we called these quantities respectively the electric permittivity, magnetic permeability, and electric conductivity of the vacuum.

Usually, the quantity σo is set to zero and so terms having it as a factor disappear. These σo-terms model the resistivity or dampening aspect of the medium to electromagnetic waves. Thus, in setting σo to zero, we are modeling electromagnetic waves that are isolated from matter and can propagate without losing energy. Without these damping

terms, the speed of electromagnetic in terms of the other two quantities

wbyavceos=in1M/√axowµeol.l’sTthheeqoruya,ndteitnyocteo disbryeaclol,yisthdeefiranteido

between the electrostatic and electromagnetic units and is called Maxwell’s constant.

As to why we usually take it to be the velocity of electromagnetic waves, we are just

continuing the practice of Maxwell. His words on the matter may provide some insight:

It is manifest that the velocity of light and the ratio of the units are quantities of the same order of magnitude. Neither of them can be said to be determined as yet with such degree of accuracy as to enable us to assert that the one is greater than the other. It is to be hoped that, by further experiment, the relation between the magnitudes of the two quantities may be more accurately

The c-equivalence principle and its implications for physics

2

determined. In the mean time our theory, which asserts that these two quantities are equal, and assigns a physical reason for this equality, are not contradicted by the comparison of these results such as they are. [19, p 436, Volume II]
Yet according to the widely accepted Einsteinian special theory of relativity (STR), the medium “does not exist” [3] and so can not have properties like o, µo, σo. Thus, STR can only define the speed of electromagnetic waves like light kinematically by c = path length/duration of travel. Prof. Einstein and most researchers tacitly assumed that c = co, but there is no obvious reason or evidence that the two definitions should agree.[6, 18] The assumption that c = co is called the c-equivalence principle by Jose Heras, in the same vein as inertial mass is equivalent to gravitational mass.[6] Before Heras named it, Roberto Monti analyzed this assumption in his insightful article.[23] Even Herbert Ives, of the Ives-Stillwell experiment, did not believe that the kinematic speed of light has the same value in all inertial frames. He assumed length contraction and time dilation to get an elaborate formula for light speed as measured by moving detectors in his paper “Light Signals on Moving Bodies as Measured by Transported Rods and clocks.” [9]
We will examine this principle and some consequences for physics should it be false, especially what it means to the Lorentz transformation. We will also outline some experiments that could invalidate the principle. In the first section, we look at the connection between the Lorentz transformation and the c-equivalence assumption. We then examine an ether model of light propagation and contrast it with STR and other theories in the third section. We briefly related three famous experiments used as evidence for the Lorentz transformation to the c-equivalent hypothesis in the fourth section. Lastly, we examine some experiments that could prove the c-equivalent proposition false.

2. The Lorentz transformation and the c-equivalence principle

Since the Lorentz transformation is the heart of the special theory of relativity, there are

many derivations of it since the days of Lorentz and Einstein. In particular, Jean-Marc

Levy-Leblond showed that the Lorentz transformation (LT) follows from five commonly

accepted hypotheses.[16] These being (1) the principle of relativity by which is meant the

covariancy of equations modeling physical phenomena, (2) the homogeneity of spacetime

and linearity of inertial transformations, (3) the isotropy of space, (4) the requirement

that the transformations form a mathematical group and (5) causality. Yet, in his

derivation, the value of the velocity constant is unclear. Requiring the covariancy of

Maxwell’s equations in the form derived by Heras will yield the value of this constant

for electromagnetism. In vacuum, Maxwell’s equations, with a partial time derivative

and not assuming the c-equivalence principle, have the forms:[6]

ρ ∇·E= ,
o

∇ · B = 0,

∇

×

E

=

−

c2o c2

∂B ,
∂t

1 ∂E ∇ × B = µ0J + c2o ∂t .

(1)

The c-equivalence principle and its implications for physics

3

Using the standard method to derive the wave equations from Maxwell’s equations on (1) yields the same undampened wave equation in free space:

∇2E

−

1 c2

∂2E ∂t2

=

0,

∇2B

−

1 c2

∂2B ∂t2

=

0,

(2)

showing that c is the speed of the EM wave. The Lorentz transformation with the

undetermined velocity parameter U in the standard situation of two inertial frames

moving with relative speed v along their common x-axis is given by:

x = γ(x − vt), y = y, z = z, t = γ(t − vx/U 2), γ = (1 − v2/U 2)−1/2. (3)

By using the inverse Lorentz transformation and standard relations among differentials

we get the following relations among the derivative operators:

v

∂x = γ ∂x + U 2 ∂t , ∂y = ∂y, ∂z = ∂z, ∂t = γ (∂t + v∂x) .

(4)

The most important equations to get the value of the LT velocity parameter are (1)

when the sources are zero. In fact, only one pair of equations from those equations

involving the partials derivative with respect to x and x are needed:

∂xEy

−

∂y Ex

=

−

c2o c2

∂tBz

1 ∂zBx − ∂xBz = c2o ∂tEy.

(5)

The corresponding equations for the moving frame are:

∂x Ey

− ∂y Ex

=

− c2o c2

∂t

Bz

1 ∂z Bx − ∂x Bz = c2o ∂t Ey .

(6)

Using (4) in (6) and rearranging the equations yield:

∂x(γEy

+

γ

vc2o c2

Bz

)

−

∂y Ex

=

−

c2o c2

∂t(γ

vc2 U 2c2o

Ey

+ γBz ),

(7)

and

∂z Bx

v − ∂x(γ c2o Ey

+ γBz ) =

1 c2o ∂t(γEy

+

γ

vc2o U2

Bz

).

(8)

The covariancy requirement of the equations forces (7) and (8) to have the same forms

as (5). This makes the quantity within the first parentheses on the left-hand side of (7)

equal to the one within the parentheses on the right-hand side of (8). Consequently, the

coefficients of the Bz terms must be equal:

γvc2o = γvc2o ,

(9)

c2

U2

so that U = c. This process, if carried out in full using all the equations, would yield the

transformations for the components of the E and B fields. Of course, if the c-equivalence

principle is accepted, everything agrees.

One reason not to accept the c-equivalence principle is revealed in the analysis of

time-of-flight experiments to determine light speed, which we examine next.

The c-equivalence principle and its implications for physics

4

Figure 1. A schematic drawing of a setup to measure the speed of light using timeof-flight methods. In actual devices, the light path may be more complicated.

3. Measuring Light Speed

To provide context for what follows, we summarize the various theories of light before

the wide acceptance of the special theory of relativity. In the 19th century, the leading

theory of light is that it is a wave requiring an all-pervading medium, the so-called

“luminiferous ether.” There were two main versions of the ether theory: (1A) the

Earth and all other bodies moved through the ether with little interaction and (1B) the

entrained ether, in which the Earth and other material bodies dragged the ether in their

motions. Movement through the ether as in (1A) would generate winds which would

affect the speed of light depending upon the direction of the wind/movement. Variant

(1B) encompasses a spectrum, from partial to total entrainment. The totally entrained

ether theories are often called local ether theories. In a local ether theory, there is

no relative motion of the Earth and the ether near the Earth’s surface where we live

and conduct most of our experiments, hence no ether wind to detect. A few scientists

supported an alternative to the wave theory of light, namely the particle/ballistic theory,

which requires no medium.

Assuming the existence of the ether, we now give a brief derivation of an equation

relating the two speed parameters for an ideal setup to measure the speed of light by the

time-of-flight method. Let S be a reference frame in which the electromagnetic speed

of light co equals ether. In essence,

the the

kinematic speed of light ether is defined to be the

c. This frame frame where c

is =

at co

rest relative to = 1/√ oµo. Let

the Sm

be a frame moving with a constant nonzero velocity v relative to S. At rest in Sm is a

transceiver and reflector separated by a distance L. In actual experiments, this frame

has historically been the lab frame near the Earth’s surface. We assumed the quantity

co to be invariant and unaffected by motion since it is a property of the ether. This assumption is akin to the constancy of light speed hypothesis in Einstein’s version of

The c-equivalence principle and its implications for physics

5

the special theory of relativity.

We need to find c in the moving frame as the quotient of distance traveled and the

duration of travel. Referring to figure 2, by solving the equation for the duration of

travel in the forward direction of L we get the forward travel duration to be

∆tf

=

L [(1
co(1 − βo2)

−

βo2 sin2 θ)1/2

+

βo cos θ],

βo = v/co,

(10)

and for the return trip, the duration is

∆tr

=

L co(1 −

[(1 βo2)

−

βo2

sin2

θ)1/2

−

βo

cos θ].

(11)

Note that ∆tf > ∆tr, implying that the one-way speed of light relative to the moving

detector and its rest frame is different in the forward and return paths even though the

speed of light has the same value with respect to the medium in either direction. We

can understand the difference in the two durations as follows. In the forward path, the

reflector is pulling away from the approaching light ray. Thus increasing the separation

distance the ray must travel in the medium’s frame. While on the return trip, the

detector is approaching the ray while the ray is approaching it. This action decreases

the separation distance between the ray and the detector in the medium’s frame. If we

superimpose the forward and return rays, fringe shifts due to any phase difference can

be detected. This phase difference between the two rays is often called the generalized

Sagnac effect and was confirmed in the experiments of Wang and collaborators.[46, 47]

But many researchers consider measuring one-way speed light to be impossible since

synchronization of clocks would be required.

The two-way speed of light is easier to do since it only requires one clock at the

transceiver and no synchronization. Toward the expression for the two-way speed, the

total duration of the back-and-forth travel along L is

∆tf r

=

∆tf

+

∆tr

=

2L [(1
co(1 − βo2)

−

βo2 sin2 θ)1/2].

(12)

Thus, the two-way kinematic speed of light along L according to the moving transceiver

is

c=

2L ∆tf r

=

(1

co(1 − βo2

− βo2) sin2 θ)1/2

.

(13)

For frames moving with respect to the ether frame, (13) implies that co > c, falsifying the c-equivalence principle. Consequently, (1) and (2) are the equations of the EM fields

and waves in these frames.

If we accept the c-equivalence principle as true and the above model approximates

reality, then (13) forces v = 0, contradicting our working assumption of nonzero v.

Many people today accept the c-equivalence principle and reject the above classical

Newtonian framework used in the analysis. Yet, even if length contraction and time

dilation are assumed, the contradiction does not disappear as a quick calculation will

reveal. The two remaining possibilities are the entrained ether model that the velocity

The c-equivalence principle and its implications for physics

6

Figure 2. Calculation of the optical paths for the forward and back directions of the light ray along the distance L using the standard vector addition law. For θ = 0, π, many would consider this situation as the addition of two velocities, but it is really just the calculation of the actually travel distance in the medium frame.
of the measuring device is zero relative to the local ether near the Earth’s surface, or that light travels like particles and is unaffected by the ether.
Unknown to most, there is a form of the entrained ether hidden within Einstein’s general relativity theory, as the following outline of his works will reveal. In 1905, Albert Einstein put forth the hypothesis that the speed of light is constant in his special theory of relativity to derive the Lorentz transformation. Once Professor Einstein developed the general theory of relativity, he made some interesting statements concerning the domain of validity of the constancy of light speed, a selection of which follows and can be found in his collected papers [4]:
1911: If co denotes the velocity of light at the coordinate origin, then the velocity of light c at a point with a gravitation potential φ will be given by the relation c = co(1 + φ/c2). The principle of the constancy of the velocity of light does not hold in this theory in the formulation in which it is normally used as the basis of the ordinary theory of relativity. [V3, D23, p 385] 1913: I have shown in previous papers that the equivalence hypotheses leads to the consequence that in a static gravitational field the velocity of light c depends on the gravitational potential. This led me to the view that the special theory of relativity provides only an approximation to reality; it should apply only in the limit case where differences in the gravitational potential in the space-time region under consideration are not too great. [V4, D13, p 153] 1916: In the second place our result shows that, according to the general theory of relativity, the law of the constancy of the velocity of light in vacuo, which constitutes one of the two fundamental assumptions in the special theory of relativity and to which we have already frequently referred, cannot claim any unlimited validity. [V6, D24, p 328]
More recently, Irwin Shapiro talked about the variable speed of light in his 1964 paper on what is now called the Shapiro delay.[35] All these statements imply that

The c-equivalence principle and its implications for physics

7

light speed is not constant. It is only approximately so for regions within a nearly

uniform gravitational potential. These statements also suggest that the medium for

light transmission is related to the dominant gravitational potential in the region of

space under observation. Thus, if we accept that gravity affects light speed, we are in

essence accepting a form of the entrained ether, because all material bodies carry their

gravitational potential along with them in their motion.

There is some evidence to support this in the experiment of Wolf and Petit

that measured directional dependence of light speed using the satellites of the Global

Positioning System (GPS).[49] For those who are unfamiliar with the GPS, this system

use satellites about 20,000 km above the Earth’s surface, equipped with synchronized

atomic clocks, and transmitters and receivers to broadcast signals carrying information

of both times and positions. It or systems like it used an Earth-Centered Inertial (ECI)

frame to calculate the positions and times of moving transmitters or receivers to high

accuracy.[7] The ECI frame is an approximate inertial frame so does not partake in the

Earth’s rotation. Earth’s gravity dominates this frame within the altitude of the GPS

satellites. It is where most experiments are conducted, including those of Wolf and Petit. Their experiment gave an upper limit to light speed anisotropy of δc/c < 5 × 10−9, and

thus showed that light speed is constant and independent of direction to a very high

degree for receivers at rest in this ECI frame.[49]

Those interested in modern entrained ether models may want to investigate the

works of C.C. Su and C. K. Thornhill. [36, 37, 38, 39, 40, 41, 42] They developed the

entrained model theory using a classical Newtonian framework in two different ways.

Su’s model even incorporated gravitational potential in its formulas/

Let us return to the c-equivalence principle. The same argument used to derive

(10), (11), and (13) can be applied to a transceiver moving relative to the ECI frame

with velocity u. Here c would play the role of co, and the two-way speed of light as

measured by the moving transceiver, cm, would be related to c by:

c(1 − β2)

u

cm

=

(1

−

β2

sin2

, φ)1/2

β= , c

(14)

with φ being the angle between u and the direction of the light path.

Some researchers have proposed experiments to test the formulas corresponding to

(10) and (11) where φ = 0 or φ = π, with modern technologies and the global positioning

system. [45, 48] Among them is Ronald Hatch, a GPS expert who held various patents on

GPS technologies as either inventor or co-inventor and who served numerous roles within

the Institute of Navigation (ION).[45] These experiments would disprove the second

hypothesis of STR–interpreted in its strong form that the speed of light is the same in

all inertial frames. It would also disprove the c-equivalence hypothesis, so that the two-

way kinematic speed of light, its wavefront, or group speed, would depend on the velocity

of the moving detector with respect to the ether frame. With the speed of light not

being the same in every inertial frame, the composition of two Lorentz transformations

would not yield a Lorentz transformation, as an elementary computation will reveal. It

would also invalidate some derivations of the Lorentz transformation.

The c-equivalence principle and its implications for physics

8

Since the Earth also rotates, in actual earth-based experiments conducted over several days, its velocity v relative to the ether frame is not constant from hour to hour, and so c would have minor daily variations. Such daily speed of light variations could appear in interferometry experiments like the ones of Michelson and Morley and the ones of Kennedy and Thorndike. We will briefly touch upon these experiments in the next section.

4. Michelson-Morley, Kennedy-Thorndike and Ives-Stilwell Type Experiments
Three famous experiments are often said to provide evidence for the Lorentz transformation, mainly because we can use them to derive the LT. Robertson was the first person to show that their results imply the Lorentz transformation.[30] These experiments are the Michelson-Morley (M-M), Kennedy-Thorndike (K-T), and IvesStilwell (I-S) experiments. We will examine the assumption and conclusions drawn from these three experiments to see if they have any bearing on the c-equivalence principle.
Albert Michelson was a firm believer in the ether theory and designed some experiments to detect the relative orbital motion of the Earth through the ether. To implement his plan, Michelson created a device now called an interferometer. This device splits the beam from a single light source with a half-silvered mirror and sends the two beams traveling at right angles to one another. After leaving the splitter, the beams traveled out to the ends of arms of nearly equal lengths, where small mirrors reflect them to the middle. These beams would recombine on the far side of the splitter to produce a pattern of constructive and destructive interference. Any slight change in the beams’ travel time due to a change in speed of light would then be observed as a shift in the positions of the interference fringes. The actual light path in real experimental setup-ups is more complicated than what we described above. In 1887, Michelson and Edward Morley conducted their first ether wind detection experiment together at the Physics Department of Case School of Applied Science (today Case Western Reserve University) and got a result that was much smaller than expected, “4 - 8 km/s” instead of “30 km/s” and was declared to be zero. [20]
Some researchers think that the shift is not zero when done at a high enough altitude, often quoting Dayton Miller’s interferometry experiments as evidence. In his 1933 paper, Miller comprehensively summarized his interferometry work and included the data that supported his conclusions. Miller’s experimental setup made over 200,000 individual readings, over 12,000 turns of the interferometer undertaken at different months of the year and different altitudes, starting in 1902 at the Case School and ending in 1926 with his Mt. Wilson experiments. After having plotted the data against sidereal time, Miller remarked “...a very striking consistency of their principal characteristics...azimuth and magnitude... as though they were related to a common cause... The observed effect is dependent upon sidereal time and is independent of diurnal and seasonal changes of temperature and other terrestrial causes, and...is a

The c-equivalence principle and its implications for physics

9

cosmical phenomenon.” [22, p 231] After Miller’s death, his former student Shankland and several other people, in
consultation with Einstein, reanalyzed some of Miller’s experimental data. They concluded that there must have been a thermal effect, but gave no evidence for it. The team admitted that it “...did not embark on a statistically sound recomputation of the cosmic solution, but... [searched for]...local disturbances such as may be caused by mechanical effects or by nonuniform temperature distributions in the observational hut.” [34, p 172] With this admission, their paper has little scientific value. Fortunately, Case school archived Miller’s data, so a more rigorous and systematic reanalysis is possible.
Thomas Roberts did this analysis and made it available for all to consider. He concluded:
...[Miller] was unknowingly looking at statistically insignificant patterns in his systematic drift that mimicked the appearance of a real signal. An upper limit on “absolute motion” of 6 km/sec is derived from his raw data, fully consistent with similar experimental results ... The key point of this paper is the need for a comprehensive and quantitative error analysis. The concepts and techniques used in this analysis were not available in Miller’s day, but are now standard. These problems also apply to the famous measurements of Michelson and Morley, and to most if not all similar experiments ...[29]
More recently, Consoli, Matheson and Pluchino reanalyzed the Michelson-Morley, Miller, Joos, and several other classical ether-drift experiments.[2] They assumed the existence of a preferred frame called the ether, which they identified as the Cosmic Microwave Background frame. They also include in their model the refractive index of the gases used in these experiments. Consoli et al. concluded
... by introducing the refractive index N of the gas, convective currents of the gas molecules would produce a small anisotropy, proportional to (N −1)(v/c)2, of the two-way velocity of light ... In the old times, experiments were performed with interferometers where light was propagating in gaseous media, air or helium at atmospheric pressure, where N − 1 is a very small number. In this regime, the theoretical fringe shifts expected ... are much smaller than the classical prediction (v/c)2... These arguments make more and more plausible that a genuine physical phenomenon, much smaller than expected and characterized by stochastic variations, might have been erroneously interpreted as an instrumental artifact thus leading to the standard ‘null interpretation’ of the experiments reported in all textbooks.[2, p 49-50]
In our estimate, these experimental results are inconclusive at best, but let us explore the logical ramification of a null result from the M-M type experiments. A null result only eliminates version (1A) of the ether theory, that the Earth moved through the ether without dragging it, and not that the ether is nonexistent, as many often claimed. To explain the null result, Lamor and Lorentz hypothesized that motion contracted the length of the arm parallel to the direction of the velocity by just the right amount.

The c-equivalence principle and its implications for physics

10

Thus, many claimed that the M-M null experimental results provide evidence for length contraction due to motion. This is an obvious example of circular reasoning, and the only way to break the circle is to have some independent evidence of length contraction. For emphasis, we repeat that experiments of the M-M type when done near the Earth’s surface, only revealed that its speed relative to the ether is close to zero near the surface, but does not eliminate other theories.
Even if we reject entrained ether models, we must explain why the ballistic theory of light is ruled out before we can claim that the null result of the M-M experiments is due to length contraction. Yet, if we accept light beams are streams of photons with wavelike behaviors emerging from large ensembles, we are adopting a form of the ballistic theory of light. In either of the above cases, there is no need for the length contraction hypothesis to explain the null results of M-M type experiments.
Let us now examine the Kennedy-Thorndike (K-T) type experiments. They are a variant of M-M experiments, with the distinguishing feature being an interferometer whose arms are of unequal lengths.[15] Because of the unequal arms’ lengths, their experimental apparatus acted like an optical gyroscope and could detect the rotation of the Earth, as mentioned in their paper. The most important point to consider is the havefollowing. Without length contraction, K-T type experiments are also inconclusive at best, since these experiments assumed length contraction to prove so-call time dilation. In the words of Kennedy and Thorndike:

The Michelson-Morley experiment indicates that a system moving with uniform velocity v with respect to such a system has dimensions in the direction of motion contracted in the ratio [1 − v2/c2]1/2 as compared to dimensions in the fixed system, while dimensions in the direction of and perpendicular to the motion are unchanged. This is in part assumption ... nevertheless it actually shows only that dimensions in the direction of and perpendicular to the motion are in the ratio mentioned; either of these dimensions might be any function of the velocity so long as that ratio is preserved. [15]

Both of these types of experiments give results smaller than expected near the Earth’s surface, so many researchers declared their results to be null. If we accept the entrained ether model, then Wolf and Petit experiment [49] implies that we must conduct these experiments in orbit above the altitude of the GPS satellites to get nonnull results. In truth, null result experiments can only eliminate theories and do not support any theory. In this sense, they can be used to support all sorts of theories, as was pointed out by many people, including Herbert Ives. Specifically, he showed that any theory that has length contraction in the direction of motion in the ratio

[1 − v2/c2](n+1)/2 : 1,

(15)

and in the perpendicular direction of the motion by

[1 − v2/c2]n/2 : 1,

(16)

The c-equivalence principle and its implications for physics

11

would give a null result for the M-M experiment. The null result of the K-T experiment is then explained if we alter the time scale at the origin in the ratio

[1 − v2/c2](1−n)/2 : 1.

(17)

Ives argued that the M-M and K-T experiments could not determine n, but his type of experiments could. [9]
To give some context to the Ives-Stilwell experiment, we need to describe his mindset. Herbert Ives was a firm believer in the Lorentz-Larmor relativity theory, an ether-based theory that uses different premises from those of Einstein to get the Lorentz transformation. He did not accept the constancy of light speed hypothesis and even thought that moving detectors would get different values depending upon their speed.[9] Let us turn to the last famous experiment. Unlike the previous two, the Ives-Stilwell type experiments give positive results. In our times, many people think experiments of the Ives-Stilwell type measure the traverse Doppler effect, often called time dilation. These experiments used moving light-emitting ion beams in various configurations and determined the shift in wavelength of the light. This shift seems to conform to a formula gotten by using the assumption of time dilation. In truth, experiments can only show that the data is consistent with a certain formula. If another theory can yield the same formula, experiments can not distinguish between them. Indeed, another way to get the same Doppler formula as the ones from STR exists. Schrodinger got the same equation in 1922 via a photon model and the laws of conservation of energy and linear momentum.[32, 5]
What conclusion can be obtained from the I-S experiments? We will quote someone who did a rigorous analysis, Wallace Kantor, to express our view. Not only did Kantor analyze the Ives-Stilwell experiments [10, 11], he also evaluates the Otting experiment [27] and the Mandelberg-Witten experiment.[17] He concluded they were inconclusive at best and expressed the opinion “ It is very doubtful if the formidable technical difficulties inherent in these ion beam experiments can be overcome.” [14] We agree with Kantor, and add that if the result of Ives-Stilwell is accepted, it would actually falsify the c-equivalence principle. As Monti pointed out, Ives and Stilwell claimed that their experiment showed the following equations to hold for the wavelength:[10, p 216]

λ = λo(1 − v2/c2)1/2,

(18)

and for the frequency, [10, p 226]

ν = νo(1 − v2/c2)1/2.

(19)

When multiplied together, we get the equation:

c = co(1 − v2/c2)1/2,

(20)

with c = λν, co = λoνo. Thus, if c = co and they are finite, we must have v = 0. This contradicts the motion of the ions in their experiment. If more recent Ives-Stilwell type experiments claimed to prove (18) and (19), then they are showing that the c-equivalent principle is false.

The c-equivalence principle and its implications for physics

12

5. Proposed Experiments

To falsify the c-equivalence principle, someone would need to conduct an experiment that shows c = co beyond all doubts. This requires measuring c0 and c independently, then comparing them. There are some experimental indications that c = co from the speed of radar signals that were bounced off of Venus,[24] Mars,[28] interplanetary spacecrafts,[1] and other interplanetary objects.[26] When Bryan Wallace analyzed the data from Venus, the data suggests that the classical velocity addition law holds for light, so that c is not constant.[44] An independent scientist from Russia, Tolchel’nikova confirmed Wallace’s observations and presented her finding at an international conference.[43] With more recent radar experiments on spacecrafts using an observation window of several months, the measured radar echo time of the spacecrafts and the theoretical formula agreed with each other to within 1µs or better.[28, 1] The theoretical formula came from a classical medium propagation model with a heliocentric inertial frame as the standard of rest for the radar signal. Models using other frames, such as the Earth-centered inertial or Earth-centered Earth-fixed frame, did not fit the data. The important implication for us is that the Earth’s nonzero rotational and orbital velocities with respect to this frame have to be added or subtracted away to get this agreement. So the first step to determine the truth of the c-equivalence principle should be a reanalysis of these interplanetary radar echo data. If these reanalyses are inconclusive, then more controlled experiments would be required. We considered these next.
Currently, there are several methods to determine light speed, such as using cavity resonance and interferometry. The most relevant to us is measuring the electromagnetic constants o and µo, and time-of-flight methods. The vacuum permittivity o is determined from measuring the capacitance and dimensions of a capacitor, while the value of the vacuum permeability is fixed at exactly µo = 4π × 10−7 H m−1 through the definition of the ampere. Rosa and Dorsey, the last recorded researchers to use EM measurements, used it in 1907 to get their result. [31] To determine if (13) hold, experimentalists would need to update the measure of o with modern technology and perform it again along with modernized time-of-flight measurements.
The last recorded time-of-flight measurement was the experiment designed by Albert Michelson, of the famous M-M experiment, and carried out by Pease and Pearson between September 1929 and March 1933 in California. In this experiment, a system of mirrors folded the path length of 12.8 to 16 km to fit within a 1.6 km long pipe, evacuated to pressures between 66 and 734 pascals. During its lifetime, it made 2885.5 determinations of light speed, giving the simple mean of c = 299,774 km/sec with an average deviation of 11 km/sec.[21] Since they did this experiment during different times of the day and year, variations due to the direction and speed of the Earth relative to the ether may exist within their experimental data. A reanalysis of their experimental data is worth doing to see if its variations can be accounted for. Methods that use interferometry to measure wavelength and independent ways to measure frequency yielding c as their product could replace the time-of-flight method, as long as they do not use standing

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waves. Modern kinematic measures of c can be done using the satellites of a global
navigation satellite system like GPS, or a modernized version of the Michelson, Pease, and Pearson experiment. If a modernized Michelson, Pease, and Pearson setup is used, we suggest having at least two identical devices far from urban centers and seismically active areas. We should also enclose them in climate control housing at a constant temperature. This would minimize error sources like temperature fluctuations and ground vibrations. One such experimental setup should be at sea level and one at a higher altitude, perhaps at the top of a mountain. The experimental apparatus should automatically send the raw daily data to independent labs for analysis. Experimenters would need to consider the CGPM (1983) definition of the meter in terms of the speed of light as pointed out by Mare and collaborators.[18]

6. Closing remarks
What are the consequences of falsifying the c-equivalence principle? As we mentioned previously, showing that c = co would invalidate the second postulate of the Special Theory of Relativity in its strong form interpretation that light speed has the same value in all inertial frames. If someone shows that (13) hold, then the ether exists! And we found a way to determine speed relative to the ether, although it may need to be done far enough away from the dominant gravity field. This would also imply that the forward time of travel is greater than the return time ∆tf > ∆tr, so that the kinematic speed of light is no longer isotropic with respect to moving detectors. Also, the transformations to preserve covariancy from one frame to another for the various electromagnetic fields will need to be changed. Since the Lorentz transformations of different frames depend on different c values, the composition of two Lorentz transformations is rendered meaningless. It would also invalidate any conclusion based upon the assumption that the two-way velocity of light is the same in all directions and all inertial systems, such as the Selleri transform. [33, p 326] What is this ether? Many think it is the frame of the fixed stars or the frame wherein the cosmic microwave background radiation is uniform in all directions.[25] Others think it is the quantum vacuum.

Acknowledgment We would like to express our appreciation to Steffen Kuhn for his comments and suggestions to improve the paper.

References
[1] Anderson J D, Esposito P B, Martin W, Thornton C L, Muhleman D O 1975, Astrophys J 200 221
[2] Consoli M, Matheson C and Pluchino A 2013, The classical ether-drift experiments: A modern reinterpretation Eur Phy Jour Plus 128 71
[3] Einstein A 1905, On the electrodynamics of moving bodies Annalen der Physik 17 891–921

The c-equivalence principle and its implications for physics

14

[4] The collected papers of Albert Einstein. Princeton University Press, open-access website. https://einsteinpapers.press.princeton.edu/
[5] Guiliani G 2015, Experiment and theory: the case of the Doppler effect for photons [6] Heras J A 2010, The c-equivalence principle and the correct form of writing Maxwell’s equations
Eur J Phys 31 1177-1185 DOI: 10.1088/0143-0807/31/5/018 [7] Hofmann-Wellenhof B, Lichtenegger H and Collins J, Global Positioning System: Theory and
Practice 5th Ed, (Springer-Verlag New York 2001) [8] Ives H E 1937, Graphical Exposition of the Michelson-Morley Experiment J Opt Soc Am 27, 177 [9] Ives H E 1937, Light Signals on Moving Bodies as Measured by Transported Rods and Clocks J
Opt Soc Am 27 389 (1937) [10] Ives H E and Stilwell G R 1938, An Experimental Study of the Rate of a Moving Atomic Clock J
Opt Soc Am 28 [11] Ives H E and Stilwell G R 1941, An Experimental Study of the Rate of a Moving Atomic Clock II
J Opt Soc Am 31 [12] Joos G 1930 Ann D Physik 7 385 [13] Joos G 1931 Naturwiss 38 784 [14] Kantor W 1971, Inconclusive Doppler Effect Experiments Spectroscopy Letters 4, 61–71 [15] Kennedy R J and Thorndike E M 1932, Experimental Establishment of the Relativity of Time
Physical Review 42 400–18 [16] Levy-Leblond J-M 1976, One more derivation of the Lorentz transformation Am J Phys 44 271–7
DOI: 10.1119/1.10490 [17] Mandelberg H I and Witten L 1962, J Opt Soc Am 52, 529 [18] Mares J J, Hubik P, Spicka V, Stavek J, Sestak J and Kristofik J 2012 Shadows over the speed of
light Physica Scripta, DOI: 10.1088/0031-8949/2012/T151/014080 [19] Maxwell J C, A Treatise on electricity and magnetism (Dover, 1954) [20] Michelson A A, Morley E W 1887, On the Relative Motion of the Earth and the Luminiferous
Ether, American Journal of Science, Third Series, XXXIV (203) [21] Michelson A A, Pease F and Pearson F 1935, Measurement of the velocity of light, Astrophysical
J 82, 26 [22] Miller D 1933, The Ether-Drift Experiment and the Determination of the Absolute Motion of the
Earth, Reviews of Modern Physics, 5 (2), 203–242 [23] Monti R A 1996, Theory of Relativity: A Critical Analysis, Physics Essays 9, 238 DOI:
10.4006/1.3029231 [24] Muhleman D O, Holdridge D B, Block N 1962, Astron J 67 191 [25] Muller R 1978, The Cosmic Background Radiation and the New Aether Drift Scientific American
18 64–74 [26] Ostro S J 1993 rev Mod Phys 65 1235 [27] Otting G 1939, Physik Z 40, 681 [28] Reasenberg R D, Shapiro I I, MacNeil P E, Goldstein R B, Breidenthal J C, Brenkle J P, Cain D
L, Kaufman T M, Komarek T A, Zygielbaum A I 1979, Astrophys J 234 L219 [29] Roberts T J 2006, An Explanation of Dayton Miller’s Anomalous “Ether Drift” Result,
https://arxiv.org/abs/physics/0608238 [30] Robertson H P 1994 Postulate versus Observation in the Special Theory of Relativity Review of
Modern Physics II 3 378–82 [31] Rosa E B and Dorsey N E 1907, A new determination of the ratio of the electromagnetic
to the electrostatic unit of electricity Bulletin of the Bureau of Standards 3 (6): 433 DOI: 10.6028/bulletin.070 [32] Schrodinger E 1922 Dopplerprinzip und Bohrsche Frequenzbedingung Phys Zeits 23 301 [33] Selleri F 2005, The Inertial Transformations and the Relativity Principle Foundations of Physics Letters 18 325–329 [34] Shankland R S, McCuskey S W, F.C. Leone and G. Kuerti 1955, New Analysis of the Interferometer

The c-equivalence principle and its implications for physics

15

Observations of Dayton C. Miller, Reviews of Modern Physics 27 (2) 167–78 [35] Shaprio I 1964, Fourth Test of General Relativity, Phys Rev Lett 13 789 DOI: 10.1103/Phys-
RevLett.13.789 [36] Su C-C 2001, A local-ether model of propagation of electromagnetic wave Eur Phys J C 21 701–715 [37] Thornhill C K 1985, The kinetic theory of electromagnetic radiation, Spec Sci and Tech 8 263–272 [38] Thornhill C K 1985, The triality of electromagentic-condensational waves in a gas-like ether, Spec
Sci and Tech 8 273–280 [39] Thornhill C K 1993, Real and apparent invariants in the transformation of the equations governing
wave motion in the general flow of a general fluid, Proc R Soc Lond A442 495–504 [40] Thornhill C K 1996, Real or imaginary space-time? Reality or Relativity? Hadronic J Supl 11
209–24 [41] Thornhill C K 2001, The refraction of light in stationary and moving refractive media, Hadronic
J 24 113–29 [42] Thornhill C K 2001, A non-singular ethereal cosmology, Hadronic J Supl 16 203–62 [43] Tolchel’nikova S A, Proceddings of the II International Congress “Space and Time” (St. Petersburg,
1991) [44] Wallace B G 1969, Radar Testing of the Relative Velocity of Light is Space, Spectrosc Lett, 2 (12),
361 [45] Wang R and Hatch R R 2002, Conducting a Crucial experiment of the Constancy of the Speed of
Light Using GPS, Proceedings of the 58th Annual Meeting of The Institute of Navigation and CIGTF 21st Guidance Test Symposium (2002), Albuquerque, NM, June , pp. 495-505 [46] Wang R, Zheng Y, Yao A and Langley D 2003, Modified Sagnac experiment for measuring traveltime difference between counter-propagating light beams in a uniformly moving fiber, Phys Letters A 312 7–10 DOI: 10.1016/S)375-9601(03)00575-9 [47] Wang R, Zheng Y and Yao A 2004, Generalized Sagnac Effect, Phys Rev Letters 93 14 DOI: 10.1103/PhysRevLett93.143901 [48] Wang R, Zheng Y and Yao A 2006, Test of the one-way speed of light and the first-order experiment of Special Relativity using phase-conjugate interferometers arXiv:physics/0609202 [49] Wolf P and Petit G 1997, Satellite Test of Special Relativity Using the Global Positioning System, Phys Rev A, 56 4405