Special Relativity, accelerating frames, proper time

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SUMMARY

The discussion focuses on calculating the proper time experienced by a particle undergoing constant acceleration from 0 to 0.5c over a duration of 2 seconds in a laboratory frame. The participant successfully derives the relationship between the differential time intervals using the equation dt' = dt / sqrt(1 - v^2/c^2) and integrates it to find the proper time t' = (c/a) * arcsin(t^2/(c/a)^2), ultimately concluding that the proper time is approximately 0.501 seconds. The concept of proper time is clarified as the time elapsed in the frame of the accelerating particle, independent of external observations.

PREREQUISITES
  • Understanding of special relativity concepts, particularly proper time.
  • Familiarity with calculus, specifically integration techniques.
  • Knowledge of the Lorentz factor and its application in relativistic physics.
  • Basic understanding of kinematics, particularly constant acceleration equations.
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  • Study the derivation of the Lorentz transformation equations in special relativity.
  • Learn about the implications of proper time in different inertial frames.
  • Explore advanced integration techniques relevant to physics problems.
  • Investigate the relationship between acceleration and relativistic effects in particle physics.
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Students of physics, particularly those studying special relativity, as well as educators and anyone interested in the mathematical foundations of relativistic motion and proper time calculations.

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Homework Statement


A particle has a constant acceleration in a laboratory from 0 to 0.5c in 2 seconds. What time elapses for the particle (i.e. what is the proper time for the particle)?
Hint You will have to integrate the proper time of the particle over the two seconds as measured in the laboratory frame. You may need to look up an integral such as \int\sqrt{a^2 - x^2} dx


Homework Equations


You tell me



The Attempt at a Solution



I'm pretty sure this isn't a difficult problem, I think I may be going about it the wrong way.
I figure I need to integrate dt' over the interval of acceleration, but I'm confused about how I go about this. Any help would be greatly appreciated.
 
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It's constant acceleration in the lab frame. That means v=a*t. dt'=dt*sqrt(1-v^2/c^2). You are right, this shouldn't be at least that hard to start. Please start and tell us where you are confused.
 
Hi Dick, sorry for the late reply, busy weekend. Thanks for your help, I think I got it but I'd appreciate if you (or someone) could check to see if I did things right.

dt&#039; = \frac{dt}{\sqrt{1 - \frac{v^2}{c^2}}} = \frac{dt}{\sqrt{1-\frac{(at)^2}{c^2}}}<br />
= \frac{dt}{\sqrt{1 - t^2(\frac{a}{c})^2}}
= \frac{(\frac{c}{a})^2}{\sqrt{(\frac{c}{a})^2 - t^2}} dt
Therefore
t&#039; = \frac{c}{a} \int \frac{dt}{\sqrt{(\frac{c}{a})^2 - t^2}}
= \frac{c}{a} \arcsin{\frac{t^2}{(\frac{c}{a})^2}
= 4 \arcsin{\frac{2}{16}}
= 0.501 seconds

I'm not sure how to put limits of integration into Latex but it's implied throughout to be t=0 and t=2s

The answer seems reasonable but I'd appreciate if someone could quickly go over my maths to see if I bungled it. Thanks! :D
 
Last edited:
Also just so I'm clear, does "proper time" mean the amount of time that has passed in the frame of some object, regardless of whether it is accelerating or not? The words don't even appear in my textbook unfortunately.
 

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