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 t_0=0, A is at O (ie x=0)
then when A is a distance d from O (x=-d), the time is t_2=\frac{-d}{v}
The time at which the observer sees A at a distance d is t_1=t_2+\frac{d}{c}=d\left(\frac{1}{c}-\frac{1}{v}\right). (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, t_0=0
therefore the difference in the time between when he sees it at x=d and x=0 is{\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)
so the apparent velocity v_{app} is then
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)
What I'm confused about is whether I should this have a \gamma term in it to account for special relativity?
The reason I think this is, is that if the rods system is O', then t_2 and consequenly t_1 should be instead t_2' and t_1' respectively, which would then make {\Delta}t instead be {\Delta}t'
so that {\Delta}t'=\frac{{\Delta}t}{\gamma} which would then multiply my final solution by a factor of \gamma. (ie. v_{app}=v\gamma\left(\frac{c}{c-v}\right))
which method is correct...if either
So let's say at t_0=0, A is at O (ie x=0)
then when A is a distance d from O (x=-d), the time is t_2=\frac{-d}{v}
The time at which the observer sees A at a distance d is t_1=t_2+\frac{d}{c}=d\left(\frac{1}{c}-\frac{1}{v}\right). (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, t_0=0
therefore the difference in the time between when he sees it at x=d and x=0 is{\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)
so the apparent velocity v_{app} is then
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)
What I'm confused about is whether I should this have a \gamma term in it to account for special relativity?
The reason I think this is, is that if the rods system is O', then t_2 and consequenly t_1 should be instead t_2' and t_1' respectively, which would then make {\Delta}t instead be {\Delta}t'
so that {\Delta}t'=\frac{{\Delta}t}{\gamma} which would then multiply my final solution by a factor of \gamma. (ie. v_{app}=v\gamma\left(\frac{c}{c-v}\right))
which method is correct...if either
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