Stationary observer meaning in relativity problem

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Homework Help Overview

The discussion revolves around the interpretation of a "stationary" observer in the context of relativity, particularly focusing on the implications of such a term within the framework of inertial reference frames. Participants are exploring the nuances of this concept and its relation to the problem at hand.

Discussion Character

  • Conceptual clarification, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants are questioning the meaning of "stationary" in relation to the observer's rest frame and whether it implies absolute rest. There is also discussion about the algebraic steps taken in solving a related problem, particularly regarding the manipulation of equations and the implications of imaginary velocities.

Discussion Status

The conversation is ongoing, with participants providing feedback on each other's reasoning and algebraic manipulations. Some guidance has been offered regarding the interpretation of equations, but there is still confusion about specific algebraic steps and their validity.

Contextual Notes

There are indications of confusion regarding the algebraic process and the assumptions made in the problem setup. Participants are encouraged to clarify their steps without jumping through them, highlighting the challenges of working through special relativity concepts under time constraints.

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Homework Statement
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Relevant Equations
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For this problem,
1715754592701.png

I don't understand what it means by the notation of a "stationary" observer. I thought there was no such thing as absolute rest. Does someone please know whether it means stationary with respect to the object?

Thanks!
 
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Supposedly that’s why they put it in quotation marks. The intended meaning is most likely stationary in their rest frame, ie, the rest frame is inertial.

Note that there is no requirement that another physical object should be at rest in that frame.
 
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Orodruin said:
Supposedly that’s why they put it in quotation marks. The intended meaning is most likely stationary in their rest frame, ie, the rest frame is inertial.

Note that there is no requirement that another physical object should be at rest in that frame.
THank you for your reply @Orodruin!

Sorry I'm still confused by this problem. For (a) I get an imaginary velocity.

##L = \frac{L_0}{γ}##
##\frac{L_0}{2} = \frac{L_0}{γ}##
##2 = \sqrt{1 - \frac{v^2}{c^2}}##
##4 = 1 - \frac{v^2}{c^2}##
##3 = -\frac{v^2}{c^2}##
##\sqrt{-3c^2} = v##

Thanks!
 
ChiralSuperfields said:
THank you for your reply @Orodruin!

Sorry I'm still confused by this problem. For (a) I get an imaginary velocity.

##L = \frac{L_0}{γ}##
##\frac{L_0}{2} = \frac{L_0}{γ}##
##2 = \sqrt{1 - \frac{v^2}{c^2}}##
##4 = 1 - \frac{v^2}{c^2}##
##3 = -\frac{v^2}{c^2}##
##\sqrt{-3c^2} = v##

Thanks!
Check the line 3.
 
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Hill said:
Check the line 3.
Thank you for your reply @Hill!

I have checked it, and it looks correct to me. I just flipped both of the fractions up and bottom which is allowed please?

Thanks!
 
ChiralSuperfields said:
Thank you for your reply @Hill!

I have checked it, and it looks correct to me. I just flipped both of the fractions up and bottom which is allowed please?

Thanks!
No, it is not correct. Show your steps.
 
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Hill said:
No, it is not correct. Show your steps.
Thank you for your reply @Hill!

That is my steps. That is the steps wrote down when solving the problem. Basically be law of algebra, if I flip one side I can flip the other right?

Thanks!
 
ChiralSuperfields said:
Thank you for your reply @Hill!

That is my steps. That is the steps wrote down when solving the problem. Basically be law of algebra, if I flip one side I can flip the other right?

Thanks!
Yes, you can flip. But this flipping does not produce your line 3 shown above.
 
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Hill said:
Yes, you can flip. But this flipping does not produce your line 3 shown above.
Thank you for you reply @Hill! Sorry I'm so confused.The ##L_0##s both cancel, do you please know what I am missing?

Thanks!
 
  • #10
ChiralSuperfields said:
Thank you for you reply @Hill! Sorry I'm so confused.The ##L_0##s both cancel, do you please know what I am missing?

Thanks!
Can you show how you get ##2 = \sqrt{1 - \frac{v^2}{c^2}}##? Not with words, only with algebra.
 
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  • #11
Hill said:
Can you show how you get ##2 = \sqrt{1 - \frac{v^2}{c^2}}##? Not with words, only with algebra.
Thank you for your reply @Hill!

No I can't sorry, it is something I learnt many years ago, I just know from the law of algebra if you do one thing to one side then you need to do the same thing to the other side. Do you please know the steps?

Thanks!
 
  • #12
ChiralSuperfields said:
Thank you for your reply @Hill!

No I can't sorry, it is something I learnt many years ago, I just know from the law of algebra if you do one thing to one side then you need to do the same thing to the other side. Do you please know the steps?

Thanks!
When you flip ##\frac{L_0}{2} = \frac{L_0}{γ}##, you get ##2 = γ##. It is not the same as ##2 = \sqrt{1 - \frac{v^2}{c^2}}##.
 
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  • #13
Hill said:
When you flip ##\frac{L_0}{2} = \frac{L_0}{γ}##, you get ##2 = γ##. It is not the same as ##2 = \sqrt{1 - \frac{v^2}{c^2}}##.
Oh thank you @Hill! Sorry I did't see that. That should fix the sign error then.

Thanks!
 
  • #14
ChiralSuperfields said:
Oh thank you @Hill! Sorry I did't see that. That should fix the sign error then.

Thanks!
Do NOT jump steps in algebra!
 
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  • #15
Hill said:
Do NOT jump steps in algebra!
Thank you for your reply @Hill! Sorry I did't consider that jump steps in agelbra. This is what trying to do SR on 2 hours of sleep does to my brain
 

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