How can a light clock tick once per meter even when in motion?

In summary: This conflicts with the concept of Special Relativity, as the distance traveled by light is not always the same in different frames of reference.
  • #1
DAC
99
2
Hello P.F.
I have previously raised the idea of a light clock that ticked each time the light traveled one metre. Dale has said if I could explain how it could be done, I could open a new thread. Here goes.
A normal light clock ticks each time the light goes mirror to mirror.
I propose a light clock that ticks each time the light goes one metre.With the mirrors one metre apart in the stationary frame, the two are the same.
What happens when the train is moving?
The mirrors will still be one metre apart in both frames.
The diagonal light path will still be the same diagonal light path.
The sensors locations however have to change. Remove the existing sensors and replace with sensors at one metre intervals along the light's path.
So if the perpendicular path is one metre, the clock ticks once. If the diagonal path is two metres the clock ticks twice. Both clocks tick at the same rate, once per metre, irrespective of the light paths length.
This conflicts with S.R. can you explain.
Thanks.
 
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  • #2
DAC said:
Hello P.F.
I have previously raised the idea of a light clock that ticked each time the light traveled one metre. Dale has said if I could explain how it could be done, I could open a new thread. Here goes.
A normal light clock ticks each time the light goes mirror to mirror.
I propose a light clock that ticks each time the light goes one metre.With the mirrors one metre apart in the stationary frame, the two are the same.
What happens when the train is moving?
The mirrors will still be one metre apart in both frames.
The diagonal light path will still be the same diagonal light path.
The sensors locations however have to change. Remove the existing sensors and replace with sensors at one metre intervals along the light's path.
So if the perpendicular path is one metre, the clock ticks once. If the diagonal path is two metres the clock ticks twice. Both clocks tick at the same rate, once per metre, irrespective of the light paths length.
This conflicts with S.R. can you explain.
Thanks.

There is no common definition of traveling one metre. The light will have traveled one metre in the ground frame when it is still short of the mirror.

And, of course, this is true in classical physics too. If someone on the train throws a ball up 1m, then someone on the ground sees that ball travel more than 1m up and across. Your confusion is not acually with light clocks and Special Relativity. Your confusion is actually in grasping the concept of two reference frames and basic trigonometry.
 
  • Like
Likes Ibix
  • #3
If the sensors are at rest in the train frame then you only need two of them - one at each mirror. If the sensors are not at rest in the train frame you need infinitely many of them, at various points at different heights along the zigzag path of the light (because in a frame moving at v with respect to the train the path length of the light on one leg is ##\sqrt {1+v/\sqrt {c^2-v^2}}##, if my mental algebra is correct, which is not 1m in general).

Which setup were you meaning?

To me, it still looks as if you are failing to recognise that the distance traveled to get from one end of a moving object to the other is not the same as its length. Until you grasp this fact (true in Galilean relativity as well as Einsteinian relativity) you will continue to fail to understand relativity.
 
  • #4
PeroK's and Ibix's replies are sound. Your problem seems to be in grasping that the same physical situation must be described by all frames without changing the basic setup. You cannot have the sensors located at the mirrors in one frame and at different places in another.

I stand by the suggestion that you should probably spend a significant amount of time to study Galilean relativity before trying to deal with special relativity.

From your posts, it is clear that you do not have a grasp of the subject equivalent to that of a graduate student in physics. I have therefore relabeled the thread accordingly.
 
  • #5
PeroK said:
There is no common definition of traveling one metre. The light will have traveled one metre in the ground frame when it is still short of the mirror.

And, of course, this is true in classical physics too. If someone on the train throws a ball up 1m, then someone on the ground sees that ball travel more than 1m up and across. Your confusion is not acually with light clocks and Special Relativity. Your confusion is actually in grasping the concept of two reference frames and basic trigonometry.
One
Ibix said:
If the sensors are at rest in the train frame then you only need two of them - one at each mirror. If the sensors are not at rest in the train frame you need infinitely many of them, at various points at different heights along the zigzag path of the light (because in a frame moving at v with respect to the train the path length of the light on one leg is ##\sqrt {1+v/\sqrt {c^2-v^2}}##, if my mental algebra is correct, which is not 1m in general).

Which setup were you meaning?

To me, it still looks as if you are failing to recognise that the distance traveled to get from one end of a moving object to the other is not the same as its length. Until you grasp this fact (true in Galilean relativity as well as Einsteinian relativity) you will continue to fail to understand relativity.
When the sensors are not at rest applies to the standard light clock as well. The sensors move with the clock/train. Yes, one metre will fall at different points along the diagonal path
 
  • #6
DAC said:
When the sensors are not at rest applies to the standard light clock as well. The sensors move with the clock/train. Yes, one metre will fall at different points along the diagonal path
But the key point is that you are then not describing the same physical situation. If you place the sensors at the mirrors, they will be at the mirrors in all frames. This is not something you can change from frame to frame.
 
  • #7
Orodruin said:
PeroK's and Ibix's replies are sound. Your problem seems to be in grasping that the same physical situation must be described by all frames without changing the basic setup. You cannot have the sensors located at the mirrors in one frame and at different places in another.

I stand by the suggestion that you should probably spend a significant amount of time to study Galilean relativity before trying to deal with special relativity.

From your posts, it is clear that you do not have a grasp of the subject equivalent to that of a graduate student in physics. I have therefore relabeled the thread accordingly.
The sensors are placed at the same interval, one metre apart. Why is that less valid than sensors every mirror to mirror apart? I have not changed the basic set up of the stationary frame, I have adhered to it.
 
  • #8
Orodruin said:
But the key point is that you are then not describing the same physical situation. If you place the sensors at the mirrors, they will be at the mirrors in all frames. This is not something you can change from frame to frame.
The clock ticks each time light goes one metre. This is the same in both frames. I have changed nothing.
 
  • #9
DAC said:
The clock ticks each time light goes one metre. This is the same in both frames. I have changed nothing.
No it is not, you are describing different clocks. One where the sensors are at the mirrors and one where they are not. It just so happens that you have constructed them in such a way that they tick at the same rate when one of them is moving. This does not violate SR as much as it demonstrates a fundamental misunderstanding of relativity (Galilean and special). Before you address this misunderstanding, you are in no position to make claims about inconsistencies.

As suggested by other posters, you first need to remedy your misconceptions before trying to implement your thoughts, or you will end up in the wrong place.
 
  • #10
@DAC: It's a pet peeve of me, but I would suggest you use a little more numbers and a little less words to describe the situation. That will (hopefully) help clear up what you misunderstand about the situation.
 
  • #11
Orodruin said:
No it is not, you are describing different clocks. One where the sensors are at the mirrors and one where they are not. It just so happens that you have constructed them in such a way that they tick at the same rate when one of them is moving. This does not violate SR as much as it demonstrates a fundamental misunderstanding of relativity (Galilean and special). Before you address this misunderstanding, you are in no position to make claims about inconsistencies
As suggested by other posters, you first need to remedy your misconceptions before trying to implement your thoughts, or you will end up in the wrong place.
In the stationary frame with the mirrors one metre apart, the clock ticks every one metre travelled. And in the moving frame it also ticks every one metre travelled. There is no difference between frames.
 
  • #12
DAC said:
In the stationary frame with the mirrors one metre apart, the clock ticks every one metre travelled. And in the moving frame it also ticks every one metre travelled. There is no difference between frames.
Yes there is! It is not the same clock! You have simply constructed two different clocks based on an underlying principle in two different frames. Due to time dilation, applying this construction to the moving clock will result in a clock which is physically different from one which is constructed at rest - as evidenced by the fact that one clock has its sensors at the mirrors and the other does not.
 
  • #13
DAC said:
Dale has said if I could explain how it could be done, I could open a new thread
You have not explained how you would build such a clock, you have only again asserted your wishful assumption that such a clock were possible. I gave you an example of how you could specify the design of a clock which could be analyzed.

https://www.physicsforums.com/threads/light-clock-confusion.839036/page-2#post-5277568

This thread is closed, we are done with this topic.
 

What is a light clock with problems?

A light clock with problems is a theoretical device used to demonstrate the effects of time dilation in Einstein's theory of relativity. It consists of a light source bouncing between two mirrors, with a detector measuring the time it takes for the light to make a round trip.

How does a light clock with problems illustrate time dilation?

A light clock with problems shows how time moves slower for an observer in motion than for an observer at rest. As the light travels back and forth, its path appears longer to the moving observer, causing the time measured by the detector to be longer. This illustrates how time is relative to the observer's frame of reference.

What are some other examples of time dilation?

Time dilation can also be observed in other experiments, such as the famous "twin paradox" where one twin stays on Earth while the other travels at high speeds in space. When they are reunited, the traveling twin will have aged less than the Earth-bound twin due to time dilation effects.

Are there any real-life applications of time dilation?

Yes, time dilation is a crucial concept in modern physics and is used in various practical applications. For example, GPS satellites must account for time dilation effects in order to accurately measure and transmit location data to Earth.

Is time dilation the same as time travel?

No, time dilation does not allow for time travel. While it may seem like time is moving faster or slower for different observers, they are still experiencing time in a linear and continuous manner. Time travel, on the other hand, involves moving between different points in time, which is not possible according to our current understanding of physics.

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