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A light source at the bottom of a tower of height h emits light upwards. As the light reaches a stationary receiver at the top of a tower, its speed relative to that receiver is:
A) c' = c(1-gh/c^2) (Newton's emission theory) B) c' = c(1-2gh/c^2) (Einstein's general relativity) C) c' = c (Richard Epp, Stephen Hawking, Brian Cox) The following analysis clearly shows that A is correct while B and C are false predictions: http://physics.ucsd.edu/students/cou...ecture5-11.pdf "In 1960 Pound and Rebka and later, 1965, with an improved version Pound and Snider measured the gravitational redshift of light using the Harvard tower, h=22.6m. From the equivalence principle, at the instant the light is emitted from the transmitter, only a freely falling observer will measure the same value of f that was emitted by the transmitter. But the stationary receiver is not free falling. During the time it takes light to travel to the top of the tower, t=h/c, the receiver is traveling at a velocity, v=gt, away from a free falling receiver. Hence the measured frequency is: f'=f(1-v/c)=f(1-gh/c^2)." The frequency measured at the bottom of the tower is f=c/L, where L is the wavelength. The frequency measured by the stationary receiver at the top of the tower is: f' = f(1-gh/c^2) = (c/L)(1-gh/c^2) = c'/L where c'=c(1-gh/c^2) is the speed of the light relative to that receiver. From the equivalence principle, c'=c(1-gh/c^2)=c-v is also the speed of light relative to an observer/receiver moving, in gravitation-free space, away from the light source with speed v. Clearly both general and special relativity are false. Pentcho Valev |
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Thread | Thread Starter | Forum | Replies | Last Post |
VARIABLE SPEED OF LIGHT AFTER ALL | Pentcho Valev | Astronomy Misc | 4 | August 6th 12 02:41 PM |
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