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The aberration of starlight that results from the relative motion between the star and the observer on Earth. The star emitted light in the past that will form the image observed in the present. The time delay is due to the finite speed of light. Stellar aberration arises from the finiteness of the speed of light and there would be no stellar aberration if the speed of light were infinite and the light from the star formed an image without delay. In navigational terms, the “past” position of a star (A) is analogous to its apparent position at the present time and the “present” position of a star (B) is analogous to its true position. While the apparent position of the star is relatively easy to consider as an instantaneous image, determining the true position of the star at the present instant of time, requires taking a number of significant physical phenomena into consideration, including the relative velocity of the Earth, the position of the observer, the exact time of day and the refraction of the atmosphere. The magnitude of the aberration, which is given by the aberration angle (α), depends on the ratio of the relative velocity of the star and the 

The aberration of starlight that results from the relative motion between the star and the observer on Earth. The star emitted light in the past that will form the image observed in the present. The time delay is due to the finite speed of light. Stellar aberration arises from the finiteness of the speed of light and there would be no stellar aberration if the speed of light were infinite and the light from the star formed an image without delay. In navigational terms, the “past” position of a star (A) is analogous to its apparent position at the present time and the “present” position of a star (B) is analogous to its true position. While the apparent position of the star is relatively easy to consider as an instantaneous image, determining the true position of the star at the present instant of time, requires taking a number of significant physical phenomena into consideration, including the relative velocity of the Earth, the position of the observer, the exact time of day and the refraction of the atmosphere. The magnitude of the aberration, which is given by the aberration angle (α), depends on the ratio of the relative velocity of the star and the 

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In a previous paper published in this journal, we described a new relativistic wave equation that accounts for the propagation of light from a source to an observer in two different inertial frames. This equation, which is based on the primacy of the Doppler effect, can account for the relativity of simultaneity and the observation that charged par...

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... tack involves a discussion of the complicated, contentious, and contradictory th mechanical properties of the 19 century aether, we want to emphasize at the onset that we have no intention of slipping such an aether back into modern physics. In the Results and Discussion section, we present a meta-analysis that shows that the new relativistic wave equation based on the Doppler effect is quantitatively more accurate than the standard theory in accounting for the results of the original and replicated versions of the Fizeau experiment concerning the optics of moving media. We also show that stellar aberration is mathematically related to the new relativistic Doppler effect through the angular derivative. The phenomenon of stellar aberration, which was so important for the development of the Special Theory of Relativity, was serendipitously discovered by James Bradley [3,4,5], who in his unsuccessful attempt to observe stellar parallax in his quest to provide evidence for the Copernican heliocentric universe, noticed that he had to tilt his telescope in the direction of the movement of the Earth (Figure 1) in order to see the bright star named γ Draconis in the constellation Draco, which is almost perpendicular to the elliptic path the Earth takes in its annual revolution around the sun. Bradley discovered that the position of the fixed star was not correlated with the change in the position of the Earth in its annual voyage around the sun, as would be expected from Robert Hooke’s [5,6] previous observations of stellar parallax, but with its annual change in velocity ...

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