Solving Light Clock Question: Calculations for a Relativistic Light Clock

In summary, the conversation discusses the calculations for a relativistic light clock, where a stationary observer sees a light clock moving at c/2 and a photon traveling along the rod and hitting the receiver. Calculations are made for the base, hypotenuse, and time as seen from the observer's point of view, leading to a discrepancy with the actual values. The observer realizes they need to use the time of the other frame, not their own, in the calculations.
  • #1
liometopum
127
24
I am trying to understand the calculations for a relativisitic light clock and am doing something wrong.

I am the stationary observer.
A light clock goes by at c/2, or 93000 miles per second.
The length of the light clock 'rod', which is perpendicular to the line of motion is 186,000 miles so it takes one second in the other (.5c) frame of reference.
Photon fires off and travels along the rod and hits the receiver.

From my point of view:
The base of the triangle is 93,000 miles, which is c/2.
The light clock rod is 186,000 miles
The hypotenuse is 207954 miles.

The light should travel the 207,954 miles (hypotenuse) distance.

The ratio of the hypotenuse to the vertical is 207954/186000= 1.118. So it takes 1.118 seconds for the light to travel that distance.

Is this right so far?

Next, the light should hit the receiver at the same moment whether the light travels straight up from the other frame of reference or from my frame of reference.

I should be viewing the time to be slower for the moving frame, by 1/1.118 or 89.445 percent of my clock.

However, using the standard formula for SR at .5c, the clockrate should be about 86.6 percent of my clockrate.

Something is amiss. What?
 
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  • #2
liometopum said:
I am trying to understand the calculations for a relativisitic light clock and am doing something wrong.

I am the stationary observer.
A light clock goes by at c/2, or 93000 miles per second.
The length of the light clock 'rod', which is perpendicular to the line of motion is 186,000 miles so it takes one second in the other (.5c) frame of reference.
Photon fires off and travels along the rod and hits the receiver.

From my point of view:
The base of the triangle is 93,000 miles, which is c/2.
The light clock rod is 186,000 miles
The hypotenuse is 207954 miles.
If you want to figure out the length of the base and hypotenuse, start from the assumption that the light takes a time of T to get from bottom to top, that implies the light clock moves sideways a distance of v*T = 0.5c*T in that time so that's the length of the base. And the light must move at c, so the distance traveled by the light in time T must be c*T, so that's the length of the hypotenuse. With the height as 1 light-second (easier to use units of light-seconds and seconds, so c=1, rather than miles and seconds), we have:

(0.5c*T)^2 + (1 light-second)^2 = (cT)^2
0.25c^2 * T^2 + (1 light-second)^2 = c^2 * T^2

0.75c^2 * T^2 = (1 light-second)^2
T^2 = (1/0.75) second^2
T = 1/sqrt(0.75) seconds

So, this implies the length of the hypotenuse is 1/sqrt(0.75) light-seconds = 215,100 miles, and the length of the base is 0.5/sqrt(0.75) light-seconds = 107,550 miles.

The problem with your numbers is that it's impossible to find a time T such that c*T = 207954 miles (required by the fact that the light must travel along the hypotenuse at c) and that 0.5c*T = 93,000 miles (required by the fact that the light clock is moving at 0.5c)
 
  • #3
Thanks very much! I see that I need to use the time of the other frame, not my time. So instead of multiplying .5 by 1 second, I multiply by the relativistic time, in this case 1/.866.
 

What is a relativistic light clock?

A relativistic light clock is a theoretical device used in the study of special relativity. It consists of two mirrors facing each other, with a beam of light bouncing back and forth between them. By measuring the time it takes for the light to travel between the mirrors, one can make calculations about the effects of time dilation and length contraction at high speeds.

How does a light clock work?

The light clock works by bouncing a beam of light between two mirrors. The time it takes for the light to travel between the mirrors is measured, and this time can be used to make calculations about the effects of relativity. As an object approaches the speed of light, the time measured by the light clock will appear to slow down, demonstrating time dilation.

What are the equations used in solving the light clock question?

The equations used in solving the light clock question are the time dilation equation (t' = t / √(1-v^2/c^2)), the length contraction equation (L' = L √(1-v^2/c^2)), and the speed of light equation (c = 299,792,458 m/s). These equations can be used to calculate the time and length measurements for an observer moving at high speeds relative to the light clock.

What is the significance of the light clock question?

The light clock question is significant because it helps illustrate the concepts of time dilation and length contraction, which are fundamental principles of special relativity. It also demonstrates the effects of relative motion and the constant speed of light, which play a crucial role in our understanding of the universe.

How does the light clock question relate to other theories and experiments in physics?

The light clock question is related to other theories and experiments in physics, such as the Michelson-Morley experiment and the theory of special relativity. It also has implications for other areas of physics, such as quantum mechanics and general relativity. By providing a simple and tangible example of the effects of relativity, the light clock question helps us better understand and apply these complex theories in our understanding of the physical world.

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