Stationary observer meaning in relativity problem

In summary, the "stationary observer" in relativity refers to an observer who is not in motion relative to a particular frame of reference. This observer experiences time and space differently compared to moving observers due to the effects of time dilation and length contraction described by Einstein's theory of relativity. The implications of this concept play a critical role in understanding how different observers perceive events in the universe, particularly when they are moving at significant fractions of the speed of light.
  • #1
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Homework Statement
Please see below
Relevant Equations
Please see below
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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  • #2
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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  • #3
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!
 
  • #4
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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  • #5
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!
 
  • #6
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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  • #7
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!
 
  • #8
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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  • #9
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
 

FAQ: Stationary observer meaning in relativity problem

What does "stationary observer" mean in the context of relativity?

A stationary observer in relativity refers to an observer who is not moving relative to a particular frame of reference. This means that the observer is at rest with respect to the events or objects being studied, allowing them to measure time and space without the effects of relative motion influencing their observations.

How does the concept of a stationary observer relate to time dilation?

Time dilation is a phenomenon predicted by the theory of relativity, where time is measured to pass at different rates for observers in different frames of reference. A stationary observer can measure the proper time, which is the time experienced by an observer at rest relative to the event. For observers in motion, time appears to pass more slowly compared to the stationary observer's measurements.

Can a stationary observer exist in a non-inertial frame of reference?

Yes, a stationary observer can exist in a non-inertial frame of reference; however, their measurements may be affected by fictitious forces due to acceleration. In such cases, the observer may experience effects that do not correspond to the inertial frames of reference, complicating the analysis of relativistic effects like time dilation and length contraction.

How do stationary observers perceive light from moving objects?

Stationary observers perceive light from moving objects differently due to the Doppler effect. If an object is moving towards the observer, the light waves are compressed, resulting in a blue shift, while if the object is moving away, the light waves are stretched, resulting in a red shift. These shifts provide information about the relative motion between the observer and the source of light.

What role do stationary observers play in understanding the principles of relativity?

Stationary observers serve as a reference point for understanding the principles of relativity. They provide a baseline from which the effects of motion, time dilation, and length contraction can be measured and analyzed. By comparing observations from stationary and moving observers, scientists can better understand the implications of relativistic effects on time, space, and light.

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