Implications of orthogonal clocks in rockets

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Discussion Overview

The discussion revolves around the implications of using orthogonal light clocks on a rocket that is accelerated to relativistic speeds. Participants explore how the orientation of the clocks—one parallel and one perpendicular to the direction of motion—affects their time measurements. The conversation includes considerations of different types of clocks, such as grandfather clocks and mechanical clocks, and the role of length contraction in these scenarios.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants propose that the clock oriented perpendicular to the direction of motion measures time differently than the parallel clock due to the geometry of light travel.
  • Others argue that after achieving terminal velocity, both clocks will tick at the same rate, but this is contested.
  • There is a discussion about how pendulum clocks would behave differently due to gravity, while balance clocks may tick the same regardless of orientation under constant velocity.
  • One participant suggests that the reason for the different rates of the clocks is related to length contraction, while another questions how the parallel clock could slow down.
  • Some participants calculate specific scenarios involving the time taken for light to travel in both types of clocks at relativistic speeds, emphasizing the importance of length contraction in these calculations.
  • There is a debate about the implications of moving the mirrors of the parallel clock closer together as speed increases to maintain the same tick rate as the perpendicular clock.
  • Participants express uncertainty about certain aspects of the discussion and seek clarification on complex points.

Areas of Agreement / Disagreement

Participants do not reach a consensus; multiple competing views remain regarding the behavior of the clocks and the effects of length contraction. Some calculations support the necessity of length contraction, while others question the interpretations of the results.

Contextual Notes

Limitations include assumptions about the behavior of different clock types under relativistic conditions, the dependence on definitions of time measurement, and unresolved mathematical steps in the calculations presented.

BOYLANATOR
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Hi.
If two light clocks are put on a rocket at rest and then accelerated to relativistic velocities with one of the light clocks parallel to the direction of motion and one perpendicular, will one clock continue to measure the rate of change of time in the rest plane while the other one measures a different time?
If instead grandfather clocks were used, would the result be the same?
What about mechanical clocks (i.e. with cogs of a certain orientation)
Any responses to my wondering are appreciated.
 
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BOYLANATOR said:
Hi.
If two light clocks are put on a rocket at rest and then accelerated to relativistic velocities with one of the light clocks parallel to the direction of motion and one perpendicular, will one clock continue to measure the rate of change of time in the rest plane while the other one measures a different time?
After the rocket achieves terminal velocity, both clocks will tick at the same rate.
BOYLANATOR said:
If instead grandfather clocks were used, would the result be the same?
A pendulum clock requires gravity and will tick at a different rate depending on the gravity.
BOYLANATOR said:
What about mechanical clocks (i.e. with cogs of a certain orientation)
Any responses to my wondering are appreciated.
Balance clocks will tick the same regardless of orientation under any constant velocity.
 
I thought the reason a light clock orientated perpendicular to the direction of movement measured time as slower than a rest frame was due to the idea that the light beam follows the hypotenuse of a triangle as viewed by the observer at rest. What causes the parallel light clock to relatively slow?
 
Length contraction.
 
BOYLANATOR said:
I thought the reason a light clock orientated perpendicular to the direction of movement measured time as slower than a rest frame was due to the idea that the light beam follows the hypotenuse of a triangle as viewed by the observer at rest. What causes the parallel light clock to relatively slow?
You're right about the perpendicularly oriented light clock but think about one that was moving very close to the speed of light. The triangle would be almost a flat line, wouldn't it? And if you approximated it to the parallel version, the two mirrors would have to be very close together in order to tick at the same rate, wouldn't they? But at slower speeds, you would have to move them farther apart to maintain the same rate until finally, with no motion at all, they would be the same distance apart as the perpendicular version, wouldn't they?
 
DaleSpam said:
Length contraction.


Well surely not. In a parallel light clock, moving at speed 0.9 c, light can travel across the clock in about half the normal time, because the clock is shortened to about half the length.

But the rate that the light - mirror distance changes is 30000 km/s (0.1 c).

So it takes about five times longer to travel across a light clock that is traveling at speed 0.9 c.


(Note: no incorrect velocity addition here)
 
ghwellsjr said:
But at slower speeds, you would have to move them farther apart to maintain the same rate until finally, with no motion at all, they would be the same distance apart as the perpendicular version, wouldn't they?

I don't really follow this part. Is it possible to describe it in another way?
 
DaleSpam said:
Length contraction.

I didn't even think about length contraction. This seems like the obvious solution.
 
jartsa said:
Well surely not.
Don't forget that in a parallel light clock the "forward" half of the tick takes significantly longer than the "backward" half. If you work it out, it gives the wrong time unless there is length contraction.
 
  • #10
Let us calculate one example case.

Rest length of a parallel light clock = 1 light second
Velocity of the clock = 0.866 c (relativistic factor is 2)

Light travels from rear to front a distance of half light seconds at speed 0.134 c.
That takes 3.73 seconds.
Then light travels from front to rear a distance of half light seconds at speed 1.866 c
That takes 0.268 seconds.

Back and forth travel takes 3.998 seconds.

We expected it to take twice the time of the time that it takes when the clock is standing still, which is 2 seconds.
 
  • #11
BOYLANATOR said:
ghwellsjr said:
But at slower speeds, you would have to move them farther apart to maintain the same rate until finally, with no motion at all, they would be the same distance apart as the perpendicular version, wouldn't they?
I don't really follow this part. Is it possible to describe it in another way?
Don't you agree that if there was no motion, there would be no difference between the perpendicular and the parallel versions? And so the mirrors would be the same distance apart. Then as the speed of the motion increases, the mirrors in the parallel case will have to move closer together in order to maintain the same tick rate as the perpendicular case? In the limit, where the speed is almost as fast as light, the mirrors will have to be very close together because the shape of the triangle will be almost a straight line and if the mirrors were as far apart in the parallel case as they were in the perpendicular case (and by that I mean the distance apart along the direction of motion, which is zero) then it would take a very long time for the light to make the round trip.
 
  • #12
Thanks jartsa. It's now clear to me that I have not found a flaw in the theory haha
 
  • #13
jartsa said:
Let us calculate one example case.

Rest length of a parallel light clock = 1 light second
Velocity of the clock = 0.866 c (relativistic factor is 2)

Light travels from rear to front a distance of half light seconds at speed 0.134 c.
That takes 3.73 seconds.
Then light travels from front to rear a distance of half light seconds at speed 1.866 c
That takes 0.268 seconds.
If there were no length contraction then we would expect the forward trip to take 7.46 s and the backwards trip to take .54 s, for a round trip duration of 8 s.

But with the length contraction factor of 2 the forward trip actually takes 3.73 s and the backward trip actually takes 0.27 s, for a round trip duration of 4 s, as expected.

Including length contraction is essential. That is the geometric piece which is different for the parallel and perpendicular clocks that BOYLANATOR was asking about.
 

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