Apparent Velocity Calculation for a Moving Rod in Special Relativity

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Homework Help Overview

The discussion revolves around calculating the apparent velocity of a rod moving towards an observer in the context of special relativity. The original poster presents a scenario where the rod's front and back points are defined, and they attempt to derive the apparent velocity based on the time it takes for light to travel from the rod to the observer.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants explore the relationship between the rod's velocity and the observer's frame of reference, questioning how the apparent velocity is affected by relativistic effects. There is discussion about whether a Lorentz factor (\gamma) should be included in the calculations and the implications of different inertial reference frames (IRFs) on the observed velocity.

Discussion Status

The conversation is ongoing, with participants raising questions about the definitions of velocity in different frames of reference and the implications for the apparent velocity calculation. Some participants suggest that the distance observed by the rod and the observer may differ due to relativistic effects, while others clarify the context of the problem.

Contextual Notes

There is a mention of the proper length of the rod and the specific conditions under which the observer measures the apparent velocity. The exact wording of the problem and the reference frames involved are under scrutiny, indicating potential ambiguities in the setup.

Warr
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The question is: Say a rod is traveling towards an observer O at a velocity v. The front of the rod is point A and the back is point B. First it wants me to calculate the apparent velocity of the rod to the observer.

So let's say at [tex]t_0=0[/tex], A is at O (ie x=0)

then when A is a distance d from O (x=-d), the time is [tex]t_2=\frac{-d}{v}[/tex]

The time at which the observer sees A at a distance d is [tex]t_1=t_2+\frac{d}{c}=d\left(\frac{1}{c}-\frac{1}{v}\right)[/tex]. (ie the time at which A is actually at d plus the time it takes the light to travel from x=-d to x=0)

therefore

When A gets to 0, the observer sees the object at the same time as it is actually there, [tex]t_0=0[/tex]

therefore the difference in the time between when he sees it at x=d and x=0 is[tex]{\Delta}t=t_0-t_1=0-d\left(\frac{1}{c}-\frac{1}{v}\right)=d\left(\frac{1}{v}-\frac{1}{c}\right)[/tex]

so the apparent velocity [tex]v_{app}[/tex] is then

[tex]v_{app}=\frac{{\Delta}d}{{\Delta}t}=\frac{0-(-d)}{d\left(\frac{1}{v}-\frac{1}{c}\right)}=v\left(\frac{c}{c-v}\right)[/tex]

What I'm confused about is whether I should this have a [tex]\gamma[/tex] term in it to account for special relativity?

The reason I think this is, is that if the rods system is O', then [tex]t_2[/tex] and consequenly [tex]t_1[/tex] should be instead [tex]t_2'[/tex] and [tex]t_1'[/tex] respectively, which would then make [tex]{\Delta}t[/tex] instead be [tex]{\Delta}t'[/tex]

so that [tex]{\Delta}t'=\frac{{\Delta}t}{\gamma}[/tex] which would then multiply my final solution by a factor of [tex]\gamma[/tex]. (ie. [tex]v_{app}=v\gamma\left(\frac{c}{c-v}\right)[/tex])

which method is correct...if either
 
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I am also confused. Special relativity is about the differences in observing the same event (a moving rod) in different IRFs that are experiencing relative motion. So the velocity of the rod, v, with respect to what reference frame is it? How is this IRF moving with respect to the observer? Only in this context do this question make sense to me.
 
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My question also. "a rod is traveling towards an observer O at a velocity v." Velocity v relative to whom? The only person mentioned is O and you are asked to find "the apparent velocity of the rod to the observer." The observer O? You were just told that it was v! If the velocity v is relative to something other than O, then we need to know the velocity of that frame of reference relative to O.
 
I suppose v is with respect to the rod's frame, and the apparent velocity is the velocity that observer O measures. The exact wording of the question is:

Consider a stick with the two ends A and B and a proper length of L moving towards an observer O with velocity v. Choose the reference frame with the origin at the position of O and t=0 for the moment when the front of the stick (A) arrives at O. What is the apparent velocity [tex]v_{app}[/tex] of the stick?

Then there is just a picture that looks like this
v--->
B-----------------A .... O

where (...) is just empty space
 
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That distance d ain't the same for for both the observers. If d is what O sees then the rod will see [itex]d' = d/\gamma[/itex]. Isn't that what you are missing?
 
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Well, I think I'm missing something. I don't think that's it, because A is on the rod, hence they are both in the same frame of reference.
 
Sorry, I meant O, because I was referring to 2 different IRF's, one on the rod (where the rod is in rest) and one where the rod is moving.
 

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