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I wonder why people use examples of light clocks to explain time dilation. But in reality it violates the speed of light.

My question is, if light speed in constant and absolute, why does a moving mirror velocity vector affect the velocity vector of light, making light to move diagonally? Light moving diagonally means that Speed of light just became speed of light + speed of mirror.

Wouldn't the light blip just miss to hit the opposite mirror after it's emitted?

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You are making a common mistake. The speed of light is constant, not its direction. The direction of any motion can be frame dependent. If I walk at right angles across the carriage of a moving train, in the frame of a person standing on the platform as the train passes, the path I take is at an acute angle to the platform, even though it is at a right angle on the train. It is the same with the path of light. If I shine a laser pointer vertically upwards at a spot directly over me on the ceiling of my office, in the frame of a passing motorist the light follows a path slightly off the vertical.

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  • $\begingroup$ It made sense with the statement, "The speed of the light is constant but not the direction". What would that angle be? Will that be changing based on the mirror speed? It's hard to grasp how speed is resulting into a direction. What's confusing is that how direction gets changed without affecting the velocity vector? (to an observer at rest) $\endgroup$ Dec 25, 2021 at 11:56
  • $\begingroup$ Wouldn't a change in direction once it starts moving is a result of change in magnitude of speed? like v1 + v2 = V3 (diagonal)? $\endgroup$ Dec 25, 2021 at 12:04
  • $\begingroup$ Perhaps you would find it helpful to imagine that the light clock remains ticking at rest, then consider how it would appear from different reference frames moving past it. $\endgroup$ Dec 25, 2021 at 12:17
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    $\begingroup$ No. If the light was fired off vertically when the light clock was stationary, and the light clock immediately started to move after the light had just been emitted, then the light would continue to move vertically. The direction of the light's motion is set when it is emitted. If the emitter accelerates subsequently then the direction of the light is not changed retrospectively. $\endgroup$ Dec 25, 2021 at 15:07
  • $\begingroup$ Really nice answer. The inertial motion of the (massive) observer just changes the direction of the velocity vector of massless light (but not its magnitude). $\endgroup$ Dec 29, 2021 at 21:58
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Look at relativistic aberration of light and relativistic photon momentum. This means, in special relativity, the light beam's velocity components $c_x,c_y,c_z$ as well as momentum components $p_x, p_y, p_z$ ("inertia") depend on the chosen inertial frame by the Lorentz transformation. Only the magnitude of light speed remains the same in all frames.

In terms of the light clock this means, that if the beam is propagating vertically in the clock's rest frame, it propagates at a certain angle in another frame.

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Light is an EM wave. Electric and magnetic vector fields change between inertial frames according to Lorentz transformations.

The E vector and B vector of the wave are orthogonal to its path for both frames. Supposing for example that they are respectively in direction $x$ and $y$ in frame A, for which the rays travels in $z$ direction.

In frame B, these vectors have different directions in general, according to the transformations. But being an EM travelling wave, they must remain orthogonal to the propagation.

So, it is expected a change in the direction of light rays for different inertial frames.

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This spatial diagram of the two transverse light clocks might help.

robphy-VisualizingProperTime-twoClocks-with-photons-spatial

Consider a light-flash, with light-signals in all spatial directions.
I've color-coded the light-signals that will meet

  • the distant mirror at rest in this frame
  • the distant mirror in motion in this frame.

Note that the speed of the signals is the same
---in a spacetime-diagram, the signals are on the light-cone of the [initial] light-flash.

Here is the spacetime diagram of the situation:

robphy-VisualizingProperTime-twoClocks-with-photons-spacetime

Here is an animation. https://www.youtube.com/watch?v=1-K3VDKjMdM

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