Find out velocity of an observer (relativity)

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Homework Help Overview

The discussion revolves around a problem in the context of relativity, specifically focusing on the velocity of an observer and the implications of the Lorentz transformation. Participants explore the relationships between different reference frames and the timing of light signals emitted from two sources.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants discuss the setup of the problem, questioning the implications of an observer being at rest and the distances involved. There are inquiries about how the timing of light signals is perceived by different observers and the significance of their positions. Some participants express uncertainty about the relationship between distance, velocity, and the timing of events.

Discussion Status

The conversation is ongoing, with various interpretations being explored. Some participants have offered insights into the nature of simultaneity in different frames of reference, while others are still grappling with the mathematical aspects of the Lorentz transformation. There is no explicit consensus, but productive questions and clarifications are being raised.

Contextual Notes

Participants note the complexity of the problem due to multiple unknowns, including the distances between observers and light sources, as well as the velocities involved. The discussion reflects the challenges of applying the Lorentz transformation without complete information.

Istiak
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Homework Statement
An observer O at rest midway between two sources of light at x=0 and x=10m observes the
two sources to flash simultaneously. According to a second observer O’, moving at a constant
speed parallel to the x-axis, one source of light flash 13ns before the other. Which of the
following gives the speed of O’ relative to O?
Relevant Equations
##x\prime = \gamma (x-vt)##
Initial observer is at rest. So ##x\prime=0##, and according to question they are 10 meter apart. So lorentz transformation becomes
##vt=x##
##v=\frac{x}{t}##
##=\frac{10 \\ \mathrm m}{13\times10^{-9} \mathrm s}##

But I don't get the expected answer. I believe if I had took ##\beta c## instead of ##v## then I would get the same result. There was a problem into plugging numbers, wasn't it?
 
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What if ##O'## is at rest, but closer to one source of light than the other?
 
PeroK said:
What if ##O'## is at rest, but closer to one source of light than the other?
Then he would see that the closer one's light comes first then another ones
 
Istiakshovon said:
Then he would see that the closer one's light comes first then another ones
What do you think ##O## and ##O'## are measuring? When the flashes of light reach them or when the events that represent the emission of the light take place according to their frame of reference?
 
PeroK said:
What do you think ##O## and ##O'## are measuring? When the flashes of light reach them or when the events that represent the emission of the light take place according to their frame of reference?
I can't think much cause ##O## is at rest and ##O\prime## is moving. So ##O\prime##'s position is changing. So I don't know the distance between O' and sources of light. Velocity is unknown also. With two unknown variables I can't find out velocity. According to O' others are moving and he is at rest. But according to O he is at rest including sources of light.
 
Istiakshovon said:
So I don't know the distance between O' and sources of light.
Do you think that's important? Does the time of an event depend on the position of the observer?
 
PeroK said:
Do you think that's important? Does the time of an event depend on the position of the observer?
As far as I can say that is, NO.

Suppose, I sent a signal to you yesterday at 2'O clock. Then I can't say when you will receive it without knowing your position. But if I know that you received the signal at 3'O clock then I can't find out your position without knowing the velocity and vice versa, can I?
If possible then wouldn't you like to show the math?
 
Istiakshovon said:
As far as I can say that is, NO.
That's correct. SR and the Lorentz Transformation relate to reference frames, not to observers. Really ##O## and ##O'## should refer to reference frames and not to isolated observers.

The question emphasises than an observer in ##O## is half-way between the sources and "sees" the light from both sources at the same time. This means that the emission of light from the two sources is simultaneous in a frame of reference where this observer is at rest. That is the important thing. Any other observer at rest in ##O## must measure these events to be simultaneous, whether or not the light from the events reaches the observer at the same time. Or, even if the events emit no light, they still have well-defined time and position coordinates in every reference frame.

You can, therefore, give these two events coordinates of ##(0, 0)## and ##(0, 10m)## in frame ##O##.

Now, what happens if you transform these events to a frame ##O'## moving at speed ##v## relative to ##O##? Using the Lorentz Transformation.
 
PeroK said:
You can, therefore, give these two events coordinates of ##(0, 0)## and ##(0, 10m)## in frame ##O##.
Let ##O\prime(0,0)## So, ##x\prime=0=t\prime## ##t=0## ##x=10 m## (Didn't you write (t,x)?)

PeroK said:
Now, what happens if you transform these events to a frame O′ moving at speed v relative to O? Using the Lorentz Transformation.
I answered it already. ##O\prime## will see that ##O## is moving backward (from ##O\prime##'s frame of reference) while ##O## will see that ##O\prime## is moving forward (from O's frame of reference)
 
  • #10
Istiakshovon said:
I answered it already. ##O\prime## will see that ##O## is moving backward (from ##O\prime##'s frame of reference) while ##O## will see that ##O\prime## is moving forward (from O's frame of reference)
That's not a coordinate transformation!
 
  • #11
PeroK said:
That's not a coordinate transformation!
They are observer. Or frame of reference
 
  • #12
Istiakshovon said:
They are observer. Or frame of reference
Coordinates are things like ##(t', x')##. Coordinates are not statements like "O is moving backwards"!
 
  • #13
But i haven’t got my answer.
 
  • #14
Istiakshovon said:
But i haven’t got my answer.
You need to do the Lorentz Transformation of the event ##(t = 0, x = 10m)##.
 
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