Stationary observer meaning in relativity problem

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SUMMARY

The discussion centers on the concept of a "stationary observer" in the context of special relativity. Participants clarify that "stationary" refers to an observer's rest frame, which is inertial, and does not require another object to be at rest. The conversation also delves into a specific problem involving length contraction, where one participant struggles with deriving the correct relationship between length and velocity, ultimately realizing a sign error in their algebraic manipulation. The importance of showing all algebraic steps to avoid confusion is emphasized.

PREREQUISITES
  • Understanding of special relativity concepts, particularly length contraction
  • Familiarity with the Lorentz factor (γ)
  • Basic algebra skills for manipulating equations
  • Knowledge of inertial reference frames
NEXT STEPS
  • Study the derivation of the Lorentz transformation equations
  • Learn about the implications of length contraction in different inertial frames
  • Explore examples of algebraic manipulation in physics problems
  • Review the concept of inertial versus non-inertial reference frames
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Students and educators in physics, particularly those studying special relativity, as well as anyone interested in understanding the nuances of observer frames and algebraic problem-solving in physics.

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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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