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Is red shifted light travelling at a speed less than c?
Light emitted from a light source moving away from an observer at a speed v would intuitively be expected to be travelling at a speed (c – v) but is in fact still measured to be moving at a speed of c. The measurement of speed is based on the time interval between the light being emitted and the light being initially detected at the destination.
The difference between light detected from a stationary source and light detected from a receding source is that the latter is red shifted which means that it is less energetic. But what does that really mean?
Measured over a period of T seconds the light received is quantitatively and qualitatively different from the light that has been transmitted over a period of T seconds.
We can characterise light as a continuous waveform whereby there will be less peaks of the waveform detected per second by a measuring device at the destination than the number of peaks per second detected by a measuring device at the receding light source that is co-moving with the source.
Quantitatively there is less energy per second arriving at the destination from a receding light source than light from a relatively stationary light source.
Energy emitted per second = E
Energy received per second = (E – e)
Eventually the total quantity of energy emitted in T seconds will arrive at the destination but with a portion of that energy (e) delayed by t seconds.
Energy emitted in T seconds = ET
Energy received in T seconds = (E – e) x (T)
Energy received in T + t seconds = ET
Energy from the emitted light will start to arrive at the destination at a point in time T1 commensurate with a speed of c from the receding source. However a quantity of Energy E emitted cannot accurately be said to have arrived at the destination until the same quantity of energy E has been absorbed at the destination at time T2 resulting in (by this definition) an effective speed of light less than c.
As an analogy a locomotive leaves station A and collects one mile of carriages in front of it on its way to station B. The first carriage being pushed by the locomotive may arrive at a station B at 09:00 but the locomotive doesn’t arrive until 09:03.
In conclusion red shifted light from a receding light source can be characterised in terms of the respective rates of energy transmitted and received as travelling at a speed less than c.
Is red shifted light travelling at a speed less than c?
Light emitted from a light source moving away from an observer at a speed v would intuitively be expected to be travelling at a speed (c – v) but is in fact still measured to be moving at a speed of c. The measurement of speed is based on the time interval between the light being emitted and the light being initially detected at the destination.
The difference between light detected from a stationary source and light detected from a receding source is that the latter is red shifted which means that it is less energetic. But what does that really mean?
Measured over a period of T seconds the light received is quantitatively and qualitatively different from the light that has been transmitted over a period of T seconds.
We can characterise light as a continuous waveform whereby there will be less peaks of the waveform detected per second by a measuring device at the destination than the number of peaks per second detected by a measuring device at the receding light source that is co-moving with the source.
Quantitatively there is less energy per second arriving at the destination from a receding light source than light from a relatively stationary light source.
Energy emitted per second = E
Energy received per second = (E – e)
Eventually the total quantity of energy emitted in T seconds will arrive at the destination but with a portion of that energy (e) delayed by t seconds.
Energy emitted in T seconds = ET
Energy received in T seconds = (E – e) x (T)
Energy received in T + t seconds = ET
Energy from the emitted light will start to arrive at the destination at a point in time T1 commensurate with a speed of c from the receding source. However a quantity of Energy E emitted cannot accurately be said to have arrived at the destination until the same quantity of energy E has been absorbed at the destination at time T2 resulting in (by this definition) an effective speed of light less than c.
As an analogy a locomotive leaves station A and collects one mile of carriages in front of it on its way to station B. The first carriage being pushed by the locomotive may arrive at a station B at 09:00 but the locomotive doesn’t arrive until 09:03.
In conclusion red shifted light from a receding light source can be characterised in terms of the respective rates of energy transmitted and received as travelling at a speed less than c.
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