Michelson-Morely Experiment

 

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Albert Abraham Michelson (1852-1931) 

American experimental physicist, professor at Case University and at the University of Chicago. He made precise measurements of the speed of light and interferometric methods to determine the wavelength of spectral lines in terms of the standard meter


The Ether

The ether is a hypothetical medium that served as the carrier of light waves in the later part of the 19th century and a few years of the 20th century. In earlier centuries the word ether was used to designate a ghostly substance that was believed to fill the upper regions of the universe beyond the orbit of the Moon. It is believed that Descartes (1596-1650) introduced into science the idea of a space-filling material (the ether), a transmitter of otherwise incomprehensible actions. The idea of an ether was employed by physicist studying electrodynamics as that medium in which light moves. It was believed that light moved relative to the ether and if you changed your frame of reference to a frame that is moving relative to the ether frame then the speed of light would take on a different value. The first to attempt to detect this motion was Albert Abraham Michelson in 1881. The experiment was repeated with increased accuracy in collaboration with Edward W. Morely in 1887. Michelson won the Nobel Prize in 1907 for this work.


The Michelson-Morely Experiment

Michelson and Morely used an interferometer in an attempt to measure the speed of light relative to the ether.  A schematic diagram appeared in the article Relative Motion of the Earth and The Luminiferous Ether, by Albert A. Michelson and Edward W. Morely, American Journal of Science, Nov. 1887. That diagram is shown below in Figure 1  

The sketches drawn of the actual interferometer are shown below in Figures 2 and 3

 

 

 

 

Figure 3 on the right shows a cross-section of the interferometer, which consists of a slab of concrete floating in a pool of mercury. This makes it easy to rotate the stone platform on which the interferometer is built. Rotating the interferometer in this experiment is crucial to the experiment itself. The beam paths of the interferometer shown in Figure 2 are shown schematically from above in Figure 4 below  

The length of the interferometer light path was extended but emplacing multiple mirrors which reflect the light multiple times so that the distance traveled by the light is a multiple of the distance between the mirrors, thus improving the accuracy of the interferometer.


Theory of Operation

The following schematic diagram is found in most discussions and derivations of the equation that is used to measure the phase difference of the two light beams. One such diagram is shown below and it will be this diagram that we will use to derive the phase relationship. In Figure 5 the velocity vectors for light traveling to the left, to the right and across the ether wind, respectively are shown.  

In these calculations it is assumed that the Galilean transformation is valid. That transformation is used to derive the transformation relations of velocity. The equation of interest here is

The following derivations are derived using velocities as measured in the frame moving to the right with respect to the ether with velocity V. The cross wind component of the velocity of light, cy, is given according to the above diagram, and thus has the velocity

 

 

Let the to-and-from time parallel to the ether wind be T1 and the to-and-fro time across the ether wind be T2. Then theses times are expected, within the ether model, to be

If the wavelength of the light is l, the phase difference between the emerging light beams is

Eq. (4) can be simplified using the approximation (1 + d)n = 1 + nd. This gives

The phase difference becomes

Thus, the ether wind should cause a phase difference between the beams, and they will interfere constructively and destructively. The appearance of the square of the velocity makes this a second order effect. The phase difference can be detected by rotating the entire interferometer by 90 degrees. During the rotation, the phase difference should gradually decreases from the value in Eq. (6) to its negative, and the interference of the beams alternates from constructive, to destructive, to constructive, etc. These changes in the interference thus serve as a sensitive test for the existence of an ether wind. The Michelson and Morely failed to detect any ether wind whatsoever with their interferometer.


Extinction

The null results in the Michelson-Morely experiment were interpreted as evidence that light does not require a medium, such as a luminiferous ether, to propagate in. The constancy of light and the Principle of Relativity when combined lead to the velocity transformation rules for special relativity. The above results were derived by assuming that the interferometer is in a vacuum or that the results will be independent of the presence of air. With this in mind I refer you to French [2] who writes

In the particular case that one of the combining velocities-say ux – is equal to c and b1 – is equal to c, giving b2 = 1, then Eq. (5-4) yields the result ux = c for any value of v. This then includes the result that light emitted from a source that is moving relative to the laboratory still has the speed c, no matter how fast the source is moving.
            As we mentioned in Chapter 3, this result, although an essential feature of Einstein’s formulation of relativity, did not receive a convincing demonstration until much later. One crucial reason is that propagation of light through a medium (even a transparent one) involves a continual process of absorption of the incident light and its reemission as secondary radiation by the medium – and it takes only a very small thickness of matter to bring about this replacement. Thus, for example, with visible light, a thickness of about 10-5 cm of glass or 0.1 mm of air at atmospheric pressure is enough to erase any possible memory, as it were, of the motion of the original source. This phenomenon, known as extinction (even tough it many not involve any appreciable loss of intensity in the light beam), has invalidated some of the observations (e.g. apparent motions of binary stars, already referred to in Chapter 3) that were at first believed to provide confirmation of Einstein’s second postulate – the invariance of c. We shall no describe two experiments which do not appear to be vitiated by the extinction phenomena. 1

The “1” superscript refers to an article by J.G. Fox which is listed in the references [3]. The phenomenon of extinction is almost always over looked in textbooks that discuss the Michelson-Morely experiment. French’s text seems to be the only one; or rather the only one I can find which mentions extinction.


References: 

[1] Relative Motion of the Earth and The Luminiferous Ether, by Albert A. Michelson and Edward W. Morely, American Journal of Science, Nov. 1887
[2] Special Relativity, by A.P. French, MIT Press (1968), page 127-128.
[3]
Evidence Against Emission Theories, J.G. Fox, Am. J. Phys. 33(1), January 1965


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