Rothiemurchus
- 203
- 1
For the relativistic doppler shift:
change in wavelength = (c - Vs) To / (1 - Vs ^2 /c^2)^1/2
where Vs is emitter velocity, c is speed of light and To is time.
Suppose change in wavelength was equal to just 1 / (1 - Vs ^2 / c^2)^1/2
then (c - Vs) To = 1
c -Vs = 1 / To
c = Vs + 1 / To
c = Vs + frequency of emitted wave
I now suggest that for M = Mo / (1 - v^2 /c^2) ^ 1/2
that this relation is actually
M = Mo x (c - Vs) To / (1 - Vs ^2 /c^2)^1/2
when (c - Vs) To = 1
and c = Vs + frequency of emitted wave
In other words a mass emits a wave as it travels through space at constant velocity.The slower the mass travels, the greater the frequency of the
emitted wave.A mass at rest would emit the highest frequency.
change in wavelength = (c - Vs) To / (1 - Vs ^2 /c^2)^1/2
where Vs is emitter velocity, c is speed of light and To is time.
Suppose change in wavelength was equal to just 1 / (1 - Vs ^2 / c^2)^1/2
then (c - Vs) To = 1
c -Vs = 1 / To
c = Vs + 1 / To
c = Vs + frequency of emitted wave
I now suggest that for M = Mo / (1 - v^2 /c^2) ^ 1/2
that this relation is actually
M = Mo x (c - Vs) To / (1 - Vs ^2 /c^2)^1/2
when (c - Vs) To = 1
and c = Vs + frequency of emitted wave
In other words a mass emits a wave as it travels through space at constant velocity.The slower the mass travels, the greater the frequency of the
emitted wave.A mass at rest would emit the highest frequency.