Length Contraction & Time Dilation

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SUMMARY

The discussion centers on the calculation of the time it takes for a light signal to travel from the front to the back of a spaceship moving at speed v, with proper length L. The correct formula derived is L/[γ(c+v)], where γ is the Lorentz factor. Participants clarify that the term v+c represents the closing velocity between the light signal and the back of the spaceship as observed from the ground frame. Misunderstandings regarding the application of the equations L'=L/γ and t'=tγ are addressed, emphasizing the importance of reference frames in special relativity.

PREREQUISITES
  • Understanding of special relativity concepts, including Lorentz transformations
  • Familiarity with the Lorentz factor (γ)
  • Knowledge of light propagation in different reference frames
  • Basic grasp of relative and closing velocities
NEXT STEPS
  • Study the derivation of the Lorentz transformations in special relativity
  • Learn about the implications of the speed of light being constant across all reference frames
  • Explore examples of closing velocity versus relative velocity in physics
  • Investigate the concept of simultaneity in different inertial frames
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Students of physics, particularly those studying special relativity, educators teaching these concepts, and anyone interested in the implications of relativistic motion on time and distance measurements.

messier992
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Homework Statement


A spaceship of proper length L is moving with respect to the ground with speed v. As measured on the ground, how much time does a light signal need to get from the front to the end of the spaceship.

Homework Equations


L'=L/γ
t'=tγ

The Attempt at a Solution


The right answer is L/[γ(c+v)]
I don't understand how to get the answer from either possibilites. Where, conceptually, I'm misunderstanding the equations.

Distance of Spaceship Viewed From the Ground
L'=L/γ = L/γ

t=L'/(velocity)= [L/γ]/(v+c)]

v+c? But isn't light supposed to travel at the same speed in all reference frames?

Additionally, how would I approach the question using the equation t'=tγ?
 
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messier992 said:
Distance of Spaceship Viewed From the Ground
L'=L/γ = L/γ

t=L'/(velocity)= [L/γ]/(v+c)]

v+c? But isn't light supposed to travel at the same speed in all reference frames?
Yes. Observers on the ground would measure the light signal as traveling with speed c relative to the ground. Observers in the ship would measure the same signal as traveling with speed c relative to the ship.

v+c in this context represents the speed at which the light signal is traveling relative to the spaceship as measured by observers on the ground. For observers on the ground, the light signal is traveling in one direction with speed c while the back of the ship is moving in the opposite direction with speed v. So, observers on the ground would say that the distance between the light signal and the back of the ship is decreasing at a rate of v+c.

Additionally, how would I approach the question using the equation t'=tγ?
You have to be careful with this equation. The unprimed time t in this equation represents the time between two events as measured in a reference frame for which the two events occur at the same place. In this problem, one event is the light signal leaving the front of the ship and the other event is the signal arriving at the back of the ship. These two events do not occur at the same place for either the ground frame or the ship frame.
 
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Many thanks!
 
TSny said:
v+c in this context represents the speed at which the light signal is traveling relative to the spaceship as measured by observers on the ground.
I would emphasize this a bit differently. The "v+c" is not a relative velocity of anyone thing in the rest frame of any other thing. Instead it is a closing velocity -- the rate at which the distance between two moving objects is decreasing [as assessed from a single frame of reference where neither object is at rest].

In this case that would be the rate at which the distance between the rearward moving light and the forward-moving space-ship tail is decreasing as assessed from the Earth frame.

A relative velocity is the rate of change of position per unit time.
A closing velocity is the rate of change of distance per unit time. Similar notions, but not always identical.

In an inertial frame, relative velocities (of objects) cap out at c. Closing velocities (for pairs of objects)
cap out at 2c.
 
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messier992 said:

Homework Statement


A spaceship of proper length L is moving with respect to the ground with speed v. As measured on the ground, how much time does a light signal need to get from the front to the end of the spaceship.

Homework Equations


L'=L/γ
t'=tγ

The Attempt at a Solution


The right answer is L/[γ(c+v)]
I don't understand how to get the answer from either possibilites. Where, conceptually, I'm misunderstanding the equations.

Distance of Spaceship Viewed From the Ground
L'=L/γ = L/γ

t=L'/(velocity)= [L/γ]/(v+c)]

v+c? But isn't light supposed to travel at the same speed in all reference frames?

Additionally, how would I approach the question using the equation t'=tγ?
The length of the spaceship seen by the ground observer is L/ϒ .
Time taken by light L/ϒc
Or proper time of the light crossing the spaceship is L/c.
Time taken as seen from ground L/γc as dt=γdΓ ,dΓ is the proper time.
 
Apashanka said:
The length of the spaceship seen by the ground observer is L/ϒ .
Time taken by light L/ϒc
Or proper time of the light crossing the spaceship is L/c.
Time taken as seen from ground L/γc as dt=γdΓ ,dΓ is the proper time.

This is all wrong.

Note that this is someone else's homework. Someone trying to learn SR. You do not have the fundamental grasp of SR to be trying to help someone else.
 
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