Deriving Equations for Light Sphere in Collinear Motion - O and O' Observers

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    Light Sphere
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Discussion Overview

The discussion revolves around deriving equations related to a spherical light pulse emitted by a moving observer O' in collinear motion relative to a stationary observer O. Participants explore the implications of the Lorentz transformation on the coordinates and proper time of both observers, focusing on the relationship between the light sphere's equations in their respective frames.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants assert that the equations for the light sphere in O' can be expressed as ct' = ± x', while seeking to derive corresponding equations in the frame of O.
  • Others challenge the validity of the equations, suggesting that ct = ± x violates the principles of relativity.
  • One participant presents transformation equations, t' = (t - vx/c^2)λ and x' = (x - vt)λ, arguing that these must hold for the light sphere of O'.
  • There is a contention regarding the simultaneity of events in both frames, with some arguing that events simultaneous in O cannot be simultaneous in O' due to relative motion.
  • Participants discuss the implications of simultaneity and how it affects the interpretation of events described in both frames, noting that two events viewed as simultaneous in one frame may not be so in another.
  • Some participants express frustration over the mathematical derivations, indicating that they have struggled to reconcile the equations with the principles of relativity.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the validity of the equations derived for the light sphere or the implications of simultaneity in different frames. Multiple competing views remain regarding the interpretation of the equations and the conditions under which they hold.

Contextual Notes

There are unresolved mathematical steps and assumptions regarding the definitions of simultaneity and the conditions of relative motion that participants have not fully clarified. The discussion reflects ongoing uncertainty about the correct application of the Lorentz transformation to this scenario.

  • #481
Al68 said:
I, and others better than I, have tried repeatedly, but still haven't given up yet.

But I would just read Einstein's 1905 paper for this. It's not the only source out there, and maybe not the best, but it's certainly more than good enough for this topic.

Yes, may I see the math please?
 
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  • #482
cfrogue said:
Well, actually if O' were a rigid body sphere, all points are struck at the same time, the same as O.

So, yes, all the points of O' are struck at the same time.

Say, do you have the math to refute the light postulate in O'?
There's a big difference in saying that all points in O' are struck at the same time and saying only that all points on a sphere in O' are struck at the same time.

The light postulate says all points on the sphere in O', not all points in O', would be hit at the same time in O'.

I have to assume that's what you really meant.
 
  • #483
Al68 said:
There's a big difference in saying that all points in O' are struck at the same time and saying only that all points on a sphere in O' are struck at the same time.

The light postulate says all points on the sphere in O', not all points in O', would be hit at the same time in O'.

I have to assume that's what you really meant.

Yes, that is what I meant. Just the surface of the sphere would O' see see simultaneity.

Thanks
 
  • #484
cfrogue said:
Yes, may I see the math please?
Sure. What specifically do you want to see the math for?
 
  • #485
Al68 said:
Sure. What specifically do you want to see the math for?

Well, you said there exists two points in O that are simultaneous in O'

Can I see this?
 
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  • #486
cfrogue said:
I used the light postulate to conclude in O' x +- ct' are simultaneous.
inxs - elegantly wasted

Thanks for the music! Yes, x'= +-ct' means for one t' there are two x's. You omitted the +- in your derivation below. In the final sentence there you refer to "points of O' are struck at the same time". However, by omitting the +- in your derivation, you are excluding one point. Since there are only two points on the x' axis for fixed t', only one point remains. So the plural "points" is not justified.

cfrogue said:
I proceed by reductio ad absurdum there exists only time t in O for this t'.

Assume there exists a tx < t such that the points in O' are struck at the same time.
Then tx < r/(λ(c-v))
tx = (t' + vx'/c^2)λ < r/(λ(c-v))
We have by the SR spherical light sphere,
ct' = x', t' = x'/c
Also, by selection x' = r.
( x'/c + vx'/c^2)λ < r/(λ(c-v))
(r/c + rv/c^2)λ < r/(λ(c-v))
(1/c + 1v/c^2)λ < 1/(λ(c-v))
((c + v)/c^2)λ < 1/(λ(c-v))
(c + v) < c^2/(λ^2(c-v))
(c + v) < (c^2/(c-v))((c^2 - v^2)/c^2)
c + v < (c^2 - v^2)/(c - v)
c + v < c + v
0 < 0

This is a contradiction. The same argument hold for tx > t.
Thus, the calculated t is the unique time in O when the points of O' are struck at the same time.
 
  • #487
cfrogue said:
Well, you said there exists two point in O that are simultaneous in O'

Can I see this?
I never said that. "Points" can't be simultaneous, events can be. I said that two events simultaneous in O' (light reaching either rod end) occur at two different times in O.

For that single t' in O', t = gamma(t' - vx'/c^2). Since there are two different values for x', there will be two different values for t.
 
  • #488
atyy said:
Thanks for the music! Yes, x'= +-ct' means for one t' there are two x's. You omitted the +- in your derivation below. In the final sentence there you refer to "points of O' are struck at the same time". However, by omitting the +- in your derivation, you are excluding one point. Since there are only two points on the x' axis for fixed t', only one point remains. So the plural "points" is not justified.

I do not need to include "You omitted the +- in your derivation below" +-, because the light postulate says the points are simultaneous.

This is axiomatic and I do not need to prove it.

So, given the simultaneity by the light postulate, I need only consider one point.
 
  • #489
Al68 said:
I never said that. "Points" can't be simultaneous, events can be. I said that two events simultaneous in O' (light reaching either rod end) occur at two different times in O.

For that single t' in O', t = gamma(t' - vx'/c^2). Since there are two different values for x', there will be two different values for t.

It is OK to have two different values for t.



It is not OK to have two different values for the simultaneity of O' ie, two different t'.

You said it was.

Do you have the proof?
 
  • #490
cfrogue said:
I do not need to include "You omitted the +- in your derivation below" +-, because the light postulate says the points are simultaneous.

This is axiomatic and I do not need to prove it.

So, given simultaneity by the light postulate, I need only consider one point.
That's not true. The light postulate only says the events are simultaneous in O'. They are still two separate events that correspond to two different locations in O' and therefore two different times in O.
 
  • #491
cfrogue said:
It is not OK to have two different values for the simultaneity of O' ie, two different t'.

You said it was.

Do you have the proof?
When did I say that?
 
  • #492
cfrogue said:
I do not need to include "You omitted the +- in your derivation below" +-, because the light postulate says the points are simultaneous.

This is axiomatic and I do not need to prove it.

So, given the simultaneity by the light postulate, I need only consider one point.

If what you say is true, then you should be able to obtain the same result with x'=-r.
 
  • #493
Looks like I missed a lot last night. I don't know if this was already resolved, but cfrogue's proof is incorrect. Specifically:
cfrogue said:
We have by the SR spherical light sphere,
ct' = x', t' = x'/c
Also, by selection x' = r.
These two lines are wrong. It should be:
"We have by the SR spherical light sphere,
ct' = ±x', t' = ±x'/c
Also, by selection ±x' = r."

The fact that there are two times in the unprimed frame follows from that.
 
  • #494
atyy said:
If what you say is true, then you should be able to obtain the same result with x'=-r.

This is curious.

When x'=-r in O', that is at the time r/(λ(c+v)) in O.
When x'=+r in O', that is at the time r/(λ(c-v)) in O.

Thus, two different times in O are producing simultaneity in O'.

I'm thinking about all this.

What is your view at this point?
 
  • #495
DaleSpam said:
Looks like I missed a lot last night. I don't know if this was already resolved, but cfrogue's proof is incorrect. Specifically:These two lines are wrong. It should be:
"We have by the SR spherical light sphere,
ct' = ±x', t' = ±x'/c
Also, by selection ±x' = r."

The fact that there are two times in the unprimed frame follows from that.

Yes, I agree and just caught that also at the same time you posted.
 
  • #496
DaleSpam said:
Looks like I missed a lot last night. I don't know if this was already resolved, but cfrogue's proof is incorrect. Specifically:These two lines are wrong. It should be:
"We have by the SR spherical light sphere,
ct' = ±x', t' = ±x'/c
Also, by selection ±x' = r."

The fact that there are two times in the unprimed frame follows from that.


This seems strange.

As t starts at zero in O and advances to t1 = r/(λ(c+v)), ct' < |x'|.
At that point in the time of O, ct' = -x'.

Then the negative x' continues to go more negative as time increases in O.

Then when the time in O reaches, t2 = r/(λ(c-v)), ct' = +x'.

Is this correct?
 
  • #497
cfrogue said:
Yes, I agree and just caught that also at the same time you posted.
No problem. I have updated my spacetime diagram to highlight the events where the light cone strikes the ends of the rods. The green dots are the events where the light cone strikes the ends of the unprimed rod. The red dots are the events where the light cone strikes the ends of the primed rod.
 

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  • #498
DaleSpam said:
No problem. I have updated my spacetime diagram to highlight the events where the light cone strikes the ends of the rods. The green dots are the events where the light cone strikes the ends of the unprimed rod. The red dots are the events where the light cone strikes the ends of the primed rod.

You do produce some excellent graphics.
 
  • #499
DaleSpam said:
No problem. I have updated my spacetime diagram to highlight the events where the light cone strikes the ends of the rods. The green dots are the events where the light cone strikes the ends of the unprimed rod. The red dots are the events where the light cone strikes the ends of the primed rod.

This implies there are two times in O t1, t2, such that the light stikes of the endpoints of the rod of O' are simultaneous in O' and t1 < t2.

Is this correct?
 
  • #500
cfrogue said:
This is curious.

When x'=-r in O', that is at the time r/(λ(c+v)) in O.
When x'=+r in O', that is at the time r/(λ(c-v)) in O.

Thus, two different times in O are producing simultaneity in O'.

I'm thinking about all this.

What is your view at this point?

My view is that you are calculating the same thing as you did here, which was correct, and you had no problem interpreting:

cfrogue said:
Let's see if I understand R of S.

O sees the strikes of O' at
t_L = d/(2cλ(c+v))
t_R = d/(2cλ(c-v))

t_L < t_R
Is this R of S?

[Edited for correction]

[t_L = d/(2λ(c+v))
t_R = d/(2λ(c-v))]
 
  • #501
atyy said:
My view is that you are calculating the same thing as you did here, which was correct, and you had no problem interpreting:

Perhaps.

Using the expanding light sphere in O, and allowing time to increase in O based on the expanding light sphere, I have found ct' = |r| at two different times in O', ie t1', t2'. I am not sure what this means though.
 
  • #502
cfrogue said:
Perhaps.

Using the expanding light sphere in O, and allowing time to increase in O based on the expanding light sphere, I have found ct' = |r| at two different times in O', ie t1', t2'. I am not sure what this means though.

I would suggest you study DaleSpam's diagram in #497 and JesseM's diagram in #182 very carefully. In DaleSpam's diagram, there are two light spheres, marked by a pair of green points and a pair of red points respectively. There is only one light cone, which are the yellow lines, showing the left going photon and the right going photon.
 
  • #503
atyy said:
I would suggest you study DaleSpam's diagram in #497 and JesseM's diagram in #182 very carefully. In DaleSpam's diagram, there are two light spheres, marked by a pair of green points and a pair of red points respectively. There is only one light cone, which are the yellow lines, showing the left going photon and the right going photon.

I did look at them.

There is a light sphere in O and one in O'.

LT says, for two times in O, the condition ct' = ±r is true.

Also, LT says there are two different times in O' in which ct' = ±r is true based on the emerging light sphere in O.

That seems to mean there are two in O'.

I am not sure though.

Do the diagrams show this?
 
  • #504
cfrogue said:
This implies there are two times in O t1, t2, such that the light stikes of the endpoints of the rod of O' are simultaneous in O' and t1 < t2.

Is this correct?
Yes, where t1 is the t coordinate of the event indicated by the red dot on the left and t2 is the t coordinate of the event indicated by the red dot on the right. In this drawing (c=1, v=0.6, d=2) we have t1=0.5 and t2=2.0 so t1<t2 is correct.
 
  • #505
cfrogue said:
I have found ct' = |r| at two different times in O', ie t1', t2'. I am not sure what this means though.
It means simultaneity is relative.
 
  • #506
cfrogue said:
There is a light sphere in O and one in O'.
Yes, the light sphere at t=1 in O is indicated by the green dots and the light sphere at t'=1 in O' is indicated by the red dots.
cfrogue said:
LT says, for two times in O, the condition ct' = ±r is true.
Yes. Note that the left and right red dots are at t=0.5 and t=2.0 respectively.
cfrogue said:
Also, LT says there are two different times in O' in which ct' = ±r is true
No. Note that the left and right red dots are both at t'=1.
 
  • #507
DaleSpam said:
Yes, the light sphere at t=1 in O is indicated by the green dots and the light sphere at t'=1 in O' is indicated by the red dots.Yes. Note that the left and right red dots are at t=0.5 and t=2.0 respectively.No. Note that the left and right red dots are both at t'=1.

Are you using a particular relative v?
 
  • #508
Yes, as I mentioned in post 504 I used v=0.6, c=1, and d=2 (or r=1) for this drawing. The exact times will be different for different v, c, or d, but it is always given by the Lorentz transform.
 
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  • #509
DaleSpam said:
Yes, as I mentioned in post 504 I used v=0.6, c=1, and d=2 (or r=1) for this drawing. The exact times will be different for different v, c, or d, but it is always given by the Lorentz transform.

OK, thanks .6c is a good one to use.

Please evaluate the below and tell me what you think. Perhaps, I made a math error or
something.


Assume v = 3/5(c). Let r be one half to rest distance of the rod in O'
λ = 5/4, (c-v) = 2/5, (c + v) = 8/5

When t reaches r/(2c), the radius of the light sphere is ct = r/2 in O.
For the left light beam, its x location is -r/2 or x = -ct = -r/2.
t' = ( t - xv/c^2)λ
t' = ( t + tv/c )λ = t ( 1 + v/c )λ = t ( 1 + 3/5 )5/4 = 2t = r/c.

Thus, (ct')^2 = r^2 and therefore, the light sphere in O' strikes both points at +r and -r.


Then when t reaches 2r/c, x = 2r, so
t' = ( 2r/c - 2rv/c^2)λ = 2r/c(1 - v/c)λ = 2r/c(2/5)5/4 = r/c
Thus, (ct')^2 = r^2 and therefore, the light sphere in O' strikes both points at +r and -r.

Hence, there are two different times in O when O' sees the simultaneous strikes.
This is different from R of S.

Thus, time proceeds from 0 to t = r/(2c) then the light sphere in O' strikes the endpoints at the same time. Then time proceeds forward as the light sphere expands in O and then again, another simultaneous strikes occurs at t = 2r/c.
 
  • #510
cfrogue said:
For the left light beam, its x location is -r/2 or x = -ct = -r/2.
t' = ( t - xv/c^2)?
t' = ( t + tv/c )? = t ( 1 + v/c )? = t ( 1 + 3/5 )5/4 = 2t = r/c
Don't forget to do the same for the right:

For the right light beam, its x location is r/2 or x = ct = r/2.
t' = ( t - xv/c^2)?
t' = ( t - tv/c )? = t ( 1 - v/c )? = t ( 1 - 3/5 )5/4 = t/2 = r/(4c)
 

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