Time Dilation/Length Contraction

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A rocket traveling away from Earth at (3/5)c sends a signal back after one hour as measured on the rocket. According to Earth clocks, the signal is sent after 4500 seconds, and it takes a total of 7200 seconds for the signal to arrive, accounting for the rocket's movement. The observer on the rocket calculates the arrival time as 5760 seconds, which aligns with the Twin Paradox. A key point of confusion arises regarding the distance the signal travels due to the Earth's motion, which must be factored into the calculations. Ultimately, the final time for the signal's arrival is confirmed to be 9000 seconds or 2.5 hours when considering the correct perspective and calculations.
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Homework Statement



A Rocket Moves away from the Earth at a speed of (3/5)c. When a clock on the rocket says that one hour has elapsed, the rocket sends a signal back to the earth.

(A). According to clocks on the earth, when was the signal sent?
(B). According tot eh Clocks on the earth, how long after the rocket left did the signal arrive at the earth?
(C). According to an observer on the rocket, how long after the rocket left did the signal arrive at the earth?

Homework Equations


\Delta t = 3600s

\beta = \frac{v}{c} = 0.6

\gamma = \frac{1}{(1-\beta^2)^.5}

\Delta t' = \Delta t \gamma

The Attempt at a Solution


For part A:
\gamma = \frac{1}{(1-\beta^2)^.5} = 1.25

\Delta t' = \Delta t \gamma = 4500s

This much I think is correct.

For part B:
\Delta t_t = \Delta t_1 + \Delta t_2

\Delta t_1 = \gamma \Delta t

\Delta t_2 = \frac{d_{rocket}}{c}

d_{rocket}=\gamma \beta c \Delta t = 2700c seconds

\Delta t_t = \gamma \Delta t + \frac{d_{rocket}}{c}

\Delta t_t = 4500s + 2700s = 7200s = 2hr

I don't feel comfortable with this answer. I found an analogous question in my textbook regarding time dilation and length contraction, and it followed the same procedure I did, but I feel my answer should just be double the time the rocket observed.

I've yet to do part C, to be frank I'm so burnt out on the last two parts that I've yet to get to it. When I get to it, I will edit this.

EDIT: Part C

\Delta t_t = \Delta t_1 + \Delta t_2

\Delta t_1 = \Delta t = 3600s

\Delta t_2 = \frac{\Delta x}{c}

\Delta x=\beta c \Delta t = 2160c seconds

\Delta t_t = \Delta t + \frac{\Delta x}{c}

\Delta t_t = 3600s + 2160s = 5760s = 1hr 36 min

Followed the same procedure, but from the reference point of the rocket. Comparing to part b, it seems to coincide with the results of the Twin Paradox, so I feel good about this one.
 
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Your answer looks fine to me.
 
Really? Thanks so much! I've been feeling really unsure about the class, mainly because we've yet to do any sort of problems until now, so I was getting worried. If you don't mind, can you look at my part C?
 
Ionian32492 said:
EDIT: Part C

\Delta t_t = \Delta t_1 + \Delta t_2

\Delta t_1 = \Delta t = 3600s

\Delta t_2 = \frac{\Delta x}{c}

\Delta x=\beta c \Delta t = 2160c seconds

\Delta t_t = \Delta t + \frac{\Delta x}{c}

\Delta t_t = 3600s + 2160s = 5760s = 1hr 36 min

Followed the same procedure, but from the reference point of the rocket. Comparing to part b, it seems to coincide with the results of the Twin Paradox, so I feel good about this one.
The problem here is that you fail to take account of the fact that the Earth is moving away from the rocket (from the rocket's frame). What you call Δx is the distance to the Earth at the moment that the signal is sent--not the total distance the light travels.
 
Doc Al said:
The problem here is that you fail to take account of the fact that the Earth is moving away from the rocket (from the rocket's frame). What you call Δx is the distance to the Earth at the moment that the signal is sent--not the total distance the light travels.

So would it be 2Δx then, to account for the distance from the Earth to the rocket and back?
 
Ionian32492 said:
So would it be 2Δx then, to account for the distance from the Earth to the rocket and back?
No. And the signal doesn't come back: It goes from rocket to Earth and that's it.

To find the time that the light takes to go from rocket to earth, you'll need to set up a kinematic equation that includes the fact that the Earth is moving. Give it a shot.

(There's an even easier way to solve this problem using time dilation.)
 
x_0 = d_{rocket} = \gamma \beta c \Delta t = 2700c s

\Delta x = x_0 + 0.6 c \Delta t_2

\Delta t_2 = \frac{\Delta x + x_0}{0.6c}

This is my best idea, but I don't know what \Delta x is

EDIT: I know \Delta x, its \beta c t
 
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Ionian32492 said:
x_0 = d_{rocket} = \gamma \beta c \Delta t = 2700c s
You want to view things from the rocket's viewpoint, so there's no factor of gamma needed.

\Delta x = x_0 + 0.6 c \Delta t_2
Good. Note that Δx here is the distance the light travels in time Δt2. Use that fact to solve for Δt2.
 
Thanks so much! I got \Delta t_t = 9000s = 2.5hr, which seems correct.
 
  • #10
Ionian32492 said:
Thanks so much! I got \Delta t_t = 9000s = 2.5hr, which seems correct.
Good!

Now use the answer from part B to solve this in a different way (using time dilation).
 
  • #11
\Delta t_{t2} = 2.5hr = \gamma \Delta t_t

Well that's painfully obvious now hahahaha. Thanks!
 
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