Special Relativity, simultaneity and spatial separation

In summary: You could solve for v using the given information, but it would be more difficult. Alternatively, you could use the equation for x'2-x'1 to find v.
  • #1
zhillyz
67
0

Homework Statement


To an observer in frame [itex]S[/itex], two events are simultaneous and occur 600km apart. What is the time measured by an observer in frame [itex]S'[/itex] who measures their spatial separation to be 1200km? Explain the sign of your answer.


Homework Equations



Lorentz Transformation

[itex] t' = \gamma(t-vx/c^2)[/itex]

or

[itex] x' = \gamma(x - vt) [/itex]

The Attempt at a Solution



The question doesn't give a value for v, and as such is making it a little difficult to wrap my head round. My attempt was to insert in the first equation t=0, x=600 and rearrange a little which gave me;

[itex] t' = \dfrac{-600v^2}{c^2}[/itex]

Not sure if this is what the question wants me to stop at or not.
 
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  • #2
The given spatial separation in the second frame allows to calculate v.
The units of your final formula look wrong.
 
  • #3
zhillyz said:

Homework Statement


To an observer in frame [itex]S[/itex], two events are simultaneous and occur 600km apart. What is the time measured by an observer in frame [itex]S'[/itex] who measures their spatial separation to be 1200km? Explain the sign of your answer.


Homework Equations



Lorentz Transformation

[itex] t' = \gamma(t-vx/c^2)[/itex]

or

[itex] x' = \gamma(x - vt) [/itex]

The Attempt at a Solution



The question doesn't give a value for v, and as such is making it a little difficult to wrap my head round. My attempt was to insert in the first equation t=0, x=600 and rearrange a little which gave me;

[itex] t' = \dfrac{-600v^2}{c^2}[/itex]

Not sure if this is what the question wants me to stop at or not.
If you just apply the Lorentz transformation for length: x'1-x'2 you would get:

[itex]L' = x'_1 - x'_2 = \gamma(x_1-vt_1) - \gamma(x_2-vt_2) = \gamma(x_1-x_2 + v(t_2-t_1))[/itex]

Knowing the relationship between t1 and t2 (ie. the times of the two events in the S frame) this simplifies nicely. You know x1-x2 and x'1-x'2 so you can solve for γ and from γ you can find v. Then you can then apply the Lorentz transformation for time to find t1' - t2'.

AM
 
  • #4
Have you learned yet that if you square the equation for x' and subtract the square of the equation for ct', you get:
[tex](x')^2-(ct')^2=(x)^2-(ct)^2[/tex]
This equation is independent of the relative velocity v, and is a fundamental characteristic of the geometry of flat space-time. This should help you solve your problem.
 
  • #5
Thank you everyone for your responses. They helped greatly.
So, with the separation in frame S'(x'2-x'1) equalling 1200km and applying the Lorentz transformation to each event's position in that frame one would get;

[itex] x'_2 - x'_1 = \gamma (x_2 - x_1 - v(t_2 - t_1))[/itex]

[itex] 1200 = \gamma (600 - v(0))[/itex]

[itex] \gamma = 200 [/itex]

Now solve for v. Afterwards

[itex] \Delta t' = \gamma (\Delta t + \dfrac{v \Delta x'}{c^2}) [/itex]
[itex] \Delta t' = \gamma \dfrac{v \Delta x'}{c^2} [/itex]

Now solve for Δt' using calculated v?
 
  • #6
zhillyz said:
Thank you everyone for your responses. They helped greatly.
So, with the separation in frame S'(x'2-x'1) equalling 1200km and applying the Lorentz transformation to each event's position in that frame one would get;

[itex] x'_2 - x'_1 = \gamma (x_2 - x_1 - v(t_2 - t_1))[/itex]

[itex] 1200 = \gamma (600 - v(0))[/itex]

[itex] \gamma = 200 [/itex]

Now solve for v. Afterwards

[itex] \Delta t' = \gamma (\Delta t + \dfrac{v \Delta x'}{c^2}) [/itex]
[itex] \Delta t' = \gamma \dfrac{v \Delta x'}{c^2} [/itex]

Now solve for Δt' using calculated v?
γ=200?? Check that again! The rest is fine except you are using x' in the Lorentz transformation for t'! It should be x.

AM
 
  • #7
2 sorry haha. Thank you.
 
  • #8
[tex](x')^2-(ct')^2=(x)^2-(ct)^2[/tex]
[tex]1200^2-(ct')^2=600^2[/tex]
[tex](ct')^2=1200^2-600^2[/tex]
[tex]ct'=600\sqrt{3}[/tex]
 
  • #9
Chestermiller said:
[tex](x')^2-(ct')^2=(x)^2-(ct)^2[/tex]
[tex]1200^2-(ct')^2=600^2[/tex]
[tex](ct')^2=1200^2-600^2[/tex]
[tex]ct'=600\sqrt{3}[/tex]
Ok. But it is not so easy to determine v from that. Using the Lorentz transformations you can determine both v and t'.

AM
 
  • #10
Andrew Mason said:
Ok. But it is not so easy to determine v from that. Using the Lorentz transformations you can determine both v and t'.

AM

The original question didn't ask for v.
 

1. What is special relativity?

Special relativity is a theory developed by Albert Einstein that explains the relationship between space and time. It states that the laws of physics are the same for all observers in inertial frames of reference and that the speed of light is constant in all inertial frames.

2. How does special relativity affect simultaneity?

Special relativity states that simultaneity is relative and depends on the observer's frame of reference. This means that two events that seem simultaneous to one observer may not appear simultaneous to another observer in a different frame of reference.

3. What is the concept of time dilation in special relativity?

Time dilation is the idea that time passes differently for observers in different frames of reference. According to special relativity, time appears to pass slower for objects moving at high speeds compared to objects that are stationary.

4. How does special relativity explain spatial separation?

Special relativity states that space and time are interconnected and that the distance between two objects can appear differently depending on the observer's frame of reference. This means that the concept of spatial separation is relative and can vary between different observers.

5. Can special relativity be applied to everyday experiences?

Yes, special relativity has been tested and proven through various experiments and is used in many modern technologies, such as GPS systems. However, its effects are only noticeable at very high speeds or in extreme gravitational fields, so it may not be noticeable in everyday experiences.

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