# Time dilation in relativistic Doppler effect

• I
In summary, the discussion is about the derivation of the Lorentz transformation and its reliance on two dimensions of space. It is noted that the standard derivation uses the Pythagorean theorem, which is only meaningful in two or more spatial dimensions. However, it is mentioned that the use of two dimensions is not essential and that the transformation can be derived starting with the assumption of linearly related coordinates. The importance of the principle of relativity is also emphasized in deriving the transformation.
Hello,
It kind of bothers me that the derivation for the Lorentz transformation relies on two dimensions of space. (Here I am referring to the standard derivation where one person is using a vertical light clock in a trolley traveling horizontally at speed v, and an observer outside is watching). My problem is that this derivation relies on the Pythagorean theorem which is an equation only meaningful in (at least) 2 spatial dimensions. So, how can the Lorentz transformation (and the resulting formula for time dilation) be used in one-dimensional derivations (e.g., the 1D relativistic Doppler effect)?

I think the idea applies to N dimensions, but 2 is as much as I can cope with.

What you are referring to is just a heuristic derivation. It is perfectly possible to derive it directly from the assumption that the light speed is invariant.

So, how can the Lorentz transformation (and the resulting formula for time dilation) be used in one-dimensional derivations (e.g., the 1D relativistic Doppler effect)?
Those aren't 1D derivations. They just look like they are because we've chosen the axes so that ##y'=y## and ##z'=z## so we don't have to do anything with them.

So, how can the Lorentz transformation (and the resulting formula for time dilation) be used in one-dimensional derivations (e.g., the 1D relativistic Doppler effect)?
Easy. You do the derivation of the transform in the full 1+3 D spacetime. By doing so you find that the formula for two of the space dimensions is trivial. So then you work problems in 1+1 D for simplicity.

The Doppler effect isn't inherently 1+1 D.

Hello,
It kind of bothers me that the derivation for the Lorentz transformation relies on two dimensions of space. (Here I am referring to the standard derivation where one person is using a vertical light clock in a trolley traveling horizontally at speed v, and an observer outside is watching). My problem is that this derivation relies on the Pythagorean theorem which is an equation only meaningful in (at least) 2 spatial dimensions. So, how can the Lorentz transformation (and the resulting formula for time dilation) be used in one-dimensional derivations (e.g., the 1D relativistic Doppler effect)?

If you start with the assumption that the coordinates are linearly related:

$x' = A x + B t$
$t' = D x + E t$

and you insist that:
1. Light has speed $c$ in both coordinate systems (so $x= \pm ct \Rightarrow x' = \pm c t'$)
2. The spatial origin of one coordinate system moves at speed $\pm v$ relative to the other coordinate system (so $x' = 0 \Rightarrow x = vt$ and $x=0 \Rightarrow x' = -vt'$)
Then this implies the transformation:

$x' = A (x - vt)$
$t' = A (t - \frac{vx}{c^2})$

with the inverse:
$x = \frac{\gamma^2}{A} (x' + vt')$
$t = \frac{\gamma^2}{A} (t' + \frac{vx'}{c^2})$

(where $\gamma = \frac{1}{\sqrt{1 - \frac{v^2}{c^2}}}$)

Any choice other than $A = \gamma$ would spoil the symmetry between forward and inverse transforms. A little more of an argument is needed to say what's wrong with that.

Thank you very much to all. I knew there had to be a way of deriving gamma in 1+1 D but I was not sure how.

stevendaryl said:
If you start with the assumption that the coordinates are linearly related:

$x' = A x + B t$
$t' = D x + E t$
Does not seem to be a very satisfying proof.

First it starts with a presupposition that coordinates are linearly related (treating this as a postulate?).
Second it never invokes the second of the SR postulates that the laws of physics are the same in all inertial frames of reference.

the_emi_guy said:
First it starts with a presupposition that coordinates are linearly related (treating this as a postulate?).
As was mentioned, this follows directly from the assumption of homogeneity, although the argumentation is more involved. The argument is presented in, eg, Rindler if I recall correctly.

Furthermore, it is exactly the same assumption that is made in deriving the Galilei transformation. The only difference lies in the second postulate. In the Galilean case that t=t' and in the Lorentz case that the speed of light is invariant.

the_emi_guy said:
Second it never invokes the second of the SR postulates that the laws of physics are the same in all inertial frames of reference.
The principle of relativity is used in finding the linear form ...

Orodruin said:
The principle of relativity is used in finding the linear form ...
Exactly.
I would think that a proper proof would start with the principal of relativity, and if the linear relationship follows from that then fine. Presupposing the linear relationship without demonstrating how you get there from the principal of relativity seems like skipping a step in the proof.

the_emi_guy said:
Exactly.
I would think that a proper proof would start with the principal of relativity, and if the linear relationship follows from that then fine. Presupposing the linear relationship without demonstrating how you get there from the principal of relativity seems like skipping a step in the proof.

You can look up dozens of proofs online. I was just sketching the derivation.

People have ridiculous (in my opinion) expectations for Physics Forums posts.

Dale
Agreed, all of this can be found online but the OPs original issue was specifically that Lorentz transformation derivations he was seeing depend on assumptions outside of the postulates of SR, such as the need for 2 dimensions for the benefit Pythagorean theorem. Seemed like we just provided another derivation with different non-SR postulates.

the_emi_guy said:
Agreed, all of this can be found online but the OPs original issue was specifically that Lorentz transformation derivations he was seeing depend on assumptions outside of the postulates of SR, such as the need for 2 dimensions for the benefit Pythagorean theorem. Seemed like we just provided another derivation with different non-SR postulates.

Well, I was just pointing out that the 2 spatial dimensions is not an essential assumption.

Hello,
It kind of bothers me that the derivation for the Lorentz transformation relies on two dimensions of space. (Here I am referring to the standard derivation where one person is using a vertical light clock in a trolley traveling horizontally at speed v, and an observer outside is watching).

You can use a light clock where the light beam moves parallel to the motion. In that case you are using only one dimension of space.

The derivations you usually see are the ones that are the easiest to follow. The analysis of the traditional light clock is easier to follow because it's more straight forward.

Mister T said:
You can use a light clock where the light beam moves parallel to the motion. In that case you are using only one dimension of space.

In this approach, the light clock parallel to the direction of motion is usually used to derive the length contraction. You can only get either length contraction or time dilation from this consideration, not both.

In Bondi's k-calculus (with the radar method),
the longitudinal Doppler Effect is used to derive the Lorentz Transformations
in (1+1)-Minkowski spacetime. (The standard effects can then be derived.)

https://en.wikipedia.org/wiki/Bondi_k-calculus
https://archive.org/details/RelativityCommonSense

m4r35n357
the_emi_guy said:
Agreed, all of this can be found online but the OPs original issue was specifically that Lorentz transformation derivations he was seeing depend on assumptions outside of the postulates of SR, such as the need for 2 dimensions for the benefit Pythagorean theorem. Seemed like we just provided another derivation with different non-SR postulates.

Just to clarify, my original issue was that 2 spatial dimensions are used in the derivation, not that well-established facts (such as the Pythagorean theorem) are used in the derivation.

Orodruin said:
In this approach, the light clock parallel to the direction of motion is usually used to derive the length contraction. You can only get either length contraction or time dilation from this consideration, not both.

I'm a little confused by this statement. Once you have time dilation, can you not use the fact that speed of light is constant to immediately derive length contraction?

I'm a little confused by this statement. Once you have time dilation, can you not use the fact that speed of light is constant to immediately derive length contraction?

Here's the issue: We pick one coordinate system, and call it the "stationary" frame. We pick another coordinate system that is moving relative to the "stationary" frame, and call that the "moving" frame. One way to derive the Lorentz transformations is by insisting that the observer in the "moving" frame uses "light-based measurements". The way you set up light-based measurements is this:
1. Use a light clock to measure time.
2. Measure distances between objects that are at rest in your frame by using radar: You bounce a light signal off the distant object, and time the round-trip. Divide the time by two to get the distance in light-seconds.
3. Synchronize distant clocks that are at rest in your frame by using light synchronization: Pick one clock to be the standard. Note the time on that clock, and send a signal to the distant clock. Set the distant clock to the time on the standard clock, plus the travel time (computed using the distance between clocks).
This procedure gives you a coordinate system for the moving frame, which you can relate to the coordinate system in the stationary frame. But it doesn't quite give you the Lorentz transformations. That's because there is one unknown parameter, namely the rate of the moving light clock as measured by the stationary observer. So that gives you an unknown time dilation factor. Since you use light clocks to measure distances, this unknown time dilation factor gives rise to an unknown length contraction factor.

I'm going to skip the tedious details, but it turns out to be the following:

The moving light clock runs slower by a factor $F$ as measured in the stationary frame.
A moving measuring rod (oriented in the direction of motion) that has length 1 meter in its own rest frame has length $\frac{1-\frac{v^2}{c^2}}{F}$ as measured in the "stationary" frame.

Light-based measurements alone don't allow you to compute $F$; it could be anything. However, if you use light-clocks that are oriented perpendicular to the direction of motion, and insist there is no length contraction in that direction, then you can uniquely compute $F$:

$F = \sqrt{1-\frac{v^2}{c^2}}$

Which also gives the length contraction $\frac{1-\frac{v^2}{c^2}}{F} = \sqrt{1-\frac{v^2}{c^2}}$

I'm a little confused by this statement. Once you have time dilation, can you not use the fact that speed of light is constant to immediately derive length contraction?

Well, you have to use constancy of light speed to derive time dilation. But if you then try to derive length contraction using the same apparatus (the unconventional light clock with the light moving parallel to the direction of the clock's motion) your reasoning will be circular. At least I think that's right.

Mister T said:
... reasoning will be circular...
I always thought π has something to do with it.

Once you have time dilation, can you not use the fact that speed of light is constant to immediately derive length contraction?
Once you have that the speed of light is invariant you can derive both time dilation snd length contraction, but you need to make sure that when you do so you do not use either result without showing it first.

## 1. What is time dilation in the relativistic Doppler effect?

Time dilation in the relativistic Doppler effect refers to the phenomenon where time appears to pass slower for an observer in motion relative to another observer. This effect is a consequence of Einstein's theory of special relativity and is caused by the stretching or compression of time intervals due to differences in velocity.

## 2. How does time dilation affect the perception of time?

Time dilation can cause time to appear slower or faster depending on the relative velocity between observers. For example, an observer in motion will perceive time to pass slower for a stationary observer, while the stationary observer will perceive time to pass faster for the moving observer. This effect becomes more significant as the relative velocity approaches the speed of light.

## 3. Does time dilation only occur in space or does it also occur on Earth?

Time dilation can occur both in space and on Earth. However, for time dilation to be noticeable, the relative velocities between observers must be close to the speed of light. This is not possible in everyday situations on Earth, so the effects of time dilation are extremely small and not noticeable.

## 4. How is the relativistic Doppler effect different from the classical Doppler effect?

The classical Doppler effect only takes into account relative motion between a source and observer, while the relativistic Doppler effect also takes into account the effects of time dilation due to differences in velocity. The relativistic Doppler effect is a more accurate and comprehensive theory that applies to high-speed motion, while the classical Doppler effect is limited to low speeds.

## 5. Can time dilation be reversed?

No, time dilation cannot be reversed. The effects of time dilation are a fundamental aspect of the laws of physics and cannot be reversed or undone. However, time dilation can be compensated for by using synchronized clocks or by adjusting for the effects of time dilation in calculations.

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