Special relativity equation question

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Discussion Overview

The discussion revolves around the implications of special relativity, particularly focusing on time dilation, simultaneity, and the behavior of light in different reference frames. Participants explore various scenarios involving moving observers and the effects of relative motion on measurements of time and distance.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant presents a scenario involving Alice and Bob, questioning the time recorded on their clocks when a laser bolt is fired, highlighting the complexities of simultaneity.
  • Another participant emphasizes the importance of considering the reference frame when discussing the timing of events, noting that Alice's perception of the shot's timing differs from Bob's.
  • A participant introduces a new scenario with a train moving relative to Bob, asking how the timing of a shot fired from Bob's position would be perceived by Alice in the train.
  • There is a discussion about the necessity of spacetime diagrams to fully understand the implications of special relativity, with some participants suggesting that diagrams should represent both time and space.
  • Participants engage in mathematical reasoning to calculate the positions and times of events according to different observers, with one participant providing coordinates and applying Lorentz transformations.
  • Another participant questions the concept of perpendicularity in different reference frames, leading to a debate about how angles and measurements change between observers in relative motion.
  • There is a discussion about the perception of simultaneity when a light signal is emitted from a moving observer, with some participants affirming that the observer sees the light hitting both ends of a moving train simultaneously from their perspective.

Areas of Agreement / Disagreement

Participants express varying views on the implications of simultaneity and the effects of relative motion on measurements. There is no consensus on the interpretations of certain scenarios, particularly regarding the concept of perpendicularity and the timing of events across different reference frames.

Contextual Notes

Some discussions involve assumptions about the definitions of simultaneity and perpendicularity that may not be universally agreed upon. The calculations presented depend on specific reference frames and may not account for all variables involved in relativistic scenarios.

Alex Pavel
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Good evening. I think I've got it as far as time dilation is concerned. Could someone please let me know if this calculation is correct?

- From frame C( stationary camera) Bob is moving at 50,000KM/second parallel to Alice's path
- Bob is also 50,000KM behind Alice on the parallel path
- Bob's path is 299,972 kilometers (1 light second) north of Alice's
- Knowing this, Alice knows that if she fires a laser bolt straight north, Bob will run into it.
- Alice fires the shot. Her camera (C) remains on the spot, facing North. She does not alter her vector
- When the bolt hits Bob, the camera records the time as one second after the shot is taken
- When the bolt hits Bob, Alice's clock shows 0.972 seconds since the shot
- Bob's clock also shows 0.972 seconds since the shot
- I put H (hypotenuse) in for reference but i do not think we need it, even though this is the path Alice 'sees'.
- Key issue is the camera sees path Y and it takes one second to reach the target in that frame.
- What does Alice's clock show if she triggered the shot at 0? Is it the same as Bob's?

Thanks!

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Alex Pavel said:
Knowing this, Alice knows that if she fires a laser bolt straight north, Bob will run into it.
North in the reference frame of C, but not in the reference frame of A. Alice shoots slightly backwards.
Alex Pavel said:
Bob's clock also shows 0.972 seconds since the shot
Only if you define "the shot" in the reference frame of C. Otherwise B will start his clock at a different time than C.
Alex Pavel said:
When the bolt hits Bob, Alice's clock shows 0.972 seconds since the shot
Same problem here.

Relativity of simultaneity is often overlooked.
 
Thanks! I am working to understand simultaneity.

- Let's say a train is passing by Bob, heading east at a relative speed of 50,000 KM/Second.
- Bob has a laser rifle pointing geometrically perpendicular to the path of the train.
- He is not aiming at a specific target, rather, he is simply shooting due North relative to the train's eastern route.
- The shot whizzes right over Alice's head, who is at the southern window
- The northern wall of the train is 29,972 KM from the window (train is 1 light second wide)
- On Bob's clock, the shot hits the north wall at one second
- Relative to the entry point of the bolt, the bolt strikes the north wall 50,000 KM west
- Relative to Bob, the bolt strikes the northern wall at 0 (west or east)
- What time is it on Alice's clock when the bolt hits the north wall, taking the entry as 0 on her clock?

When I have this answer I think I will have this down, finally.
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Alex Pavel said:
I am working to understand simultaneity.

Trying to do this without using spacetime diagrams is, IMO, a bad idea. You are drawing diagrams, but they are diagrams in space only. But the whole issue in relativity is that "space" is not an entity by itself; only spacetime is. So to really see what's going on, you need to draw diagrams that explicitly represent time as well as space--i.e., spacetime diagrams.
 
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Spacetime diagrams with two spatial dimensions can be a bit tricky to draw (but it is possible).
Find the point in the train where it hits as seen by Alice, the time is then easy to find.
 
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Alex Pavel said:
geometrically perpendicular
Is there any other kind of perpendicular?
Alex Pavel said:
When I have this answer I think I will have this down, finally.
Write down the coordinates of events in Bob's frame. Apply the Lorentz transforms. When the results stop surprising you, you understand it.

According to Bob, the laser fires at x=0, y=0, t=0. It hits at x=0, y=1, t=1 (distances in light seconds). The train is moving at v=c/6. You just need to feed that velocity and those two sets of coordinates into the Lorentz transforms and you'll get the positions and times of the events according to Alice.
 
I think I have it.

The bolt hits the far wall for Bob at 1 second, X=0, Y=299972, and Z = 0.

Alice in the train going 50,000 / sec when the bolt hits:
X = -50709
Y = 29972
Z = 0
T = 1.01418

So, is it true when Alice is 50,000KM away from Bob from Bobs perspective.

However, when the bolt hits, Alice is 50,709 away from her perspective, and it happened 1.014 seconds ago?

And this is clearly not due to the 'catch up' time needed for the light information to reach Alice.

So, if Alice wants to bring the train to a stop so she can go get Bob arrested, what decrease in velocity is needed from her perspective?

I suppose she would need to apply enough braking power to reduce speed by 50,709 from her reckoning?

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Alex Pavel said:
However, when the bolt hits, Alice is 50,709 away from her perspective
Alice is 1.014 light seconds away. That's what you just calculated because there was a light beam going from Alice to the other wall (a bit behind her).
Alex Pavel said:
So, if Alice wants to bring the train to a stop so she can go get Bob arrested, what decrease in velocity is needed from her perspective?
She has to stop the train - both agree that it travels at 50,000 km/s.
 
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Thanks! These concepts are slowly sinking into my mind.
 
  • #10
Ibix said:
Is there any other kind of perpendicular?

Is there some sort of different measure for perpendicular in different reference frames where spacetime becomes curved?
 
  • #11
This is special relativity, no curved spacetime.

Even in General Relativity, locally you always see the spacetime of SR - you can always define "perpendicular" in your reference frame in a clear way. Different observers will measure different angles, however.
 
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  • #12
mfb said:
Different observers will measure different angles, however.
Depends what they're measuring, surely. The laser will be perpendicular to the track in all frames. Its beam won't.
 
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  • #13
So even with the phenomenon of length contraction, curved space time, etc, perpendicular remains perpendicular. Even in the case of, say, the aberration of light when you view through a telescope, you will see the object in a different place than it really is, the moment its light reaches the lens. Because the speed of light is finite, we are always somewhat 'seeing the past'. Therefore, even something that appears optically perpendicular is not necessarily considered geometrically perpendicular, depending on velocity.
 
  • #14
Ibix said:
Depends what they're measuring, surely. The laser will be perpendicular to the track in all frames.
Not in all frames. The angle changes in frames moving relative to laser and track but with the direction of motion not aligned with either of them.
Alex Pavel said:
So even with the phenomenon of length contraction, curved space time, etc, perpendicular remains perpendicular.
No, not in general.
 
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  • #15
So, my math shows that if I am in the middle of a train moving at .6C, and I shine a flashlight in both directions, the light hits both the front and back simultaneously by my perspective? Even if one end is coming toward me and the other end is moving away? Is this correct or have I missed something?
 
  • #16
Alex Pavel said:
So, my math shows that if I am in the middle of a train moving at .6C, and I shine a flashlight in both directions, the light hits both the front and back simultaneously by my perspective?
From your perspective, you aren't moving and neither is either end of the train, so your maths is correct. However this:
Alex Pavel said:
Even if one end is coming toward me and the other end is moving away?
...doesn't make sense because the ends of the carriage aren't moving from your perspective.
 
  • #17
Alex Pavel said:
So, my math shows that if I am in the middle of a train moving at .6C, and I shine a flashlight in both directions, the light hits both the front and back simultaneously by my perspective? Even if one end is coming toward me and the other end is moving away? Is this correct or have I missed something?

Imagine you are on an aeroplane with two friends, traveling at ##1000 km/h##. You are in the middle of the plane, one friend at the front another at the back.

Can you tell which direction the plane is moving?

If you toss a coin normally, does it go straight up and down relative to you?

If you throw something to your friend at the front, does it never reach them because you can't throw it at ##1000km/h+##?

If you throw something to your friend at the back, does it kill or seriously injure them because they are moving towards it at ##1000km/h##?
 
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  • #18
Ibix said:
From your perspective, you aren't moving and neither is either end of the train, so your maths is correct. However this:

...doesn't make sense because the ends of the carriage aren't moving from your perspective.

Therefore, no matter my velocity, if i shine a light on something, regardless of direction, it reaches the target at (c/distance). Hard to process in our primitive brains!
 
  • #19
Alex Pavel said:
Therefore, no matter my velocity, if i shine a light on something, regardless of direction, it reaches the target at (c/distance).
distance/c, I think. But this is true in any frame. The special thing about the rest frame is that the distance light travels is half the rest length of the carriage in both directions. In any other frame it's shorter in one direction than the other because the carriage ends are moving.
 
  • #20
Alex Pavel said:
Therefore, no matter my velocity, if i shine a light on something, regardless of direction, it reaches the target at (c/distance).
If "distance" is the distance to you at the time it hits the target: yes.
 

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