From Lorentz transformatios to Bondi's approach

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Discussion Overview

The discussion centers on the relationship between Lorentz transformations and Bondi's approach to deriving them, particularly through the lens of radar detection of space-time coordinates and the Doppler factor. Participants explore the implications of these transformations in both theoretical and pedagogical contexts.

Discussion Character

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

Main Points Raised

  • Some participants propose that Bondi's derivation of Lorentz transformations can be expressed in terms of the Doppler factor, suggesting that this approach could be beneficial for beginners learning about Lorentz transformations.
  • Others question the clarity of the symbols and definitions used, particularly regarding the meaning of event E and the implications of using the same symbol x for different contexts.
  • A participant emphasizes that the Lorentz transformations account for all scenarios compatible with physics, while another suggests that the transformations can be derived from Bondi's method without using the Lorentz-Einstein transformations.
  • There is a discussion about the synchronization of clocks in Bondi's derivation and its equivalence to Einstein's synchronization, with references to specific equations and the Doppler shift formula.
  • Some participants express uncertainty about the specific equations being referenced and seek clarification on how they relate to the broader discussion of Lorentz transformations and Doppler effects.
  • A later reply points out a small error in a previous post regarding the dimensional correctness of an equation, highlighting the interconnectedness of various results in relativity.

Areas of Agreement / Disagreement

Participants express differing views on the clarity of the discussion and the specific equations involved. While some agree on the potential pedagogical value of the approach, others remain uncertain about the definitions and implications being presented. No consensus is reached on the overall validity of the arguments or the clarity of the exposition.

Contextual Notes

Limitations include potential ambiguities in the definitions of symbols and the assumptions underlying the derivations discussed. There is also a noted dependence on the synchronization method used in the transformations.

bernhard.rothenstein
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As we know, Bondi derives the Lorentz transformations (LT) via the radar detection of the space-time coordinates of a distant event.
Once derived from other starting points the LT should account for the results obtained by Bondi expressing them as a function of the Doppler factor
D=sqrt[(1+b)/(1-b)] which can be derived without using the LT (b=V/c). The outgoing radar signal generates the event E(x,y=0,t=x/c) when detected from I and E'(x'=ct',y'=0,t'=x'/c). In accordance with the LT we have
x=(x'+cbt')/sqrt(1-b^2). (1)
But
b=(D^2-1)/1+D^2
sqrt(1-b^2)=2D/(1+D^2)
with which (1) becomes
x=[x'(1+D^2)+ct'(D^2-1)]/2D=Dx'=Dct' (2)
In a simillar way we obtain
t=[(1+D^2)x'+(D^2-1)x'/c]/2D=Dt'=Dx'/c. (3)
If the event is generated by a tardyon moving with speed u(u') the generated events are
E(x=ut,y=0,t=x/u) and E'(x'=u't',y'=0,t'=x'/u') and the corresponding LT could be espressed again as a function of D.
Do you find flows above? Do you consider that it could be a good exercise for the beginner teaching him to handle the LT?
Thanks in advance for your answers.
 
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bernhard.rothenstein said:
As we know, Bondi derives the Lorentz transformations (LT) via the radar detection of the space-time coordinates of a distant event.

Once derived from other starting points the LT should account for the results obtained by Bondi expressing them as a function of the Doppler factor D=sqrt[(1+b)/(1-b)] which can be derived without using the LT (b=V/c). The outgoing radar signal generates the event E(x,y=0,t=x/c) when detected from I and E'(x'=ct',y'=0,t'=x'/c). In accordance with the LT we have

x=(x'+cbt')/sqrt(1-b^2). (1)

But

b=(D^2-1)/1+D^2

sqrt(1-b^2)=2D/(1+D^2)

with which (1) becomes

x=[x'(1+D^2)+ct'(D^2-1)]/2D=Dx'=Dct' (2)

In a simillar way we obtain

t=[(1+D^2)x'+(D^2-1)x'/c]/2D=Dt'=Dx'/c. (3)

If the event is generated by a tardyon moving with speed u(u') the generated events are
E(x=ut,y=0,t=x/u) and E'(x'=u't',y'=0,t'=x'/u') and the corresponding LT could be espressed again as a function of D.

Do you find flows above? Do you consider that it could be a good exercise for the beginner teaching him to handle the LT?

Thanks in advance for your answers.
I think you need to explain more carefully the situation and the symbols you use. What exactly is E? And what are you trying to prove?

You seem to be using the same symbol x with two different meanings when you say x=0 and t=x/c, because otherwise that would imply t=0.

By the way, it would make your posts easier to read if you left a blank line between paragraphs (as I have done to your quoted message above).
 
lorentz and bondi

DrGreg said:
I think you need to explain more carefully the situation and the symbols you use. What exactly is E? And what are you trying to prove?

You seem to be using the same symbol x with two different meanings when you say x=0 and t=x/c, because otherwise that would imply t=0.

By the way, it would make your posts easier to read if you left a blank line between paragraphs (as I have done to your quoted message above).
Thanks for your answer. E(x,y,t) stands "event E characterized in I by its space-time coordinates x,y,t. The approach I propose is in a single space dimension. When I say x=0 I mean an event that takes place at the origin O. E(x,0,t=x/c) characterizes an event generated by a light signal emitted from O at a point M(x,0).
My purpose is to show that the Lorentz transformations for the space-time coordinates of the same event are derived without using Bondi's approach we can recover them.
In short I think that the Lorentz transformations account for all scenarios compatible with physics.
Regards
 
Lorentz and Bondi

I rephrase my initial thread as follows:
1. Are the times, in the transformation equations obtained by Bondy displayed by clock synchronized a la Einstein?
2. If so in order to obtain them we could start with the Lorentz transformation replacing there the relative velocity V with the Doppler factor from the Doppler shift formula D=sqrt[(1+V/c)/(1-V/c)] which can be derived without using the Lorentz-Einstein transformations?
Thanks for your answer.
 
bernhard.rothenstein said:
I rephrase my initial thread as follows:

1. Are the times, in the transformation equations obtained by Bondy displayed by clock synchronized a la Einstein?

2. If so in order to obtain them we could start with the Lorentz transformation replacing there the relative velocity V with the Doppler factor from the Doppler shift formula D=sqrt[(1+V/c)/(1-V/c)] which can be derived without using the Lorentz-Einstein transformations?

Thanks for your answer.
I am not 100% sure exactly which equations you mean by "the transformation equations obtained by Bondi".

Take a look at this post, where I derive the Lorentz Transform using Bondi's k-calculus method, directly from Einstein's postulates and using Einstein synchronization to define a time coordinate t.

If you can rephrase your questions in terms of the equations and concepts in that post, then I may understand what you are asking. The k in my post is the same as the D in your post.

There was a small error in my original post. The equation v = (k-k-1)/(k+k-1) is dimensionally incorrect; it is missing a c. It should really be

v = c(k-k-1)/(k+k-1)

In general terms, there are lots of different results in relativity which depend on each other. So, for example, if you assume results A and B you can prove result C, but equally if you assume results A and C you can prove result B. And so on.
 
lorentz bondi

DrGreg said:
I am not 100% sure exactly which equations you mean by "the transformation equations obtained by Bondi".

Take a look at this post, where I derive the Lorentz Transform using Bondi's k-calculus method, directly from Einstein's postulates and using Einstein synchronization to define a time coordinate t.

If you can rephrase your questions in terms of the equations and concepts in that post, then I may understand what you are asking. The k in my post is the same as the D in your post.

There was a small error in my original post. The equation v = (k-k-1)/(k+k-1) is dimensionally incorrect; it is missing a c. It should really be

v = c(k-k-1)/(k+k-1)

In general terms, there are lots of different results in relativity which depend on each other. So, for example, if you assume results A and B you can prove result C, but equally if you assume results A and C you can prove result B. And so on.

Thanks. I have seen your derivation and I will use it.
I rephrase my question:
The Bondi derivation is based on clock synchronization a la Einstein. So it should be equivalent with
x=g(x'-Vt') (1)
t=g(t'-Vx'/cc)
where g stands for gamma.
The Doppler factor D=k enable us to express V/c via the Doppler shift formula that can be derived without using the Lorentz transformations.
 
bernhard.rothenstein said:
Thanks. I have seen your derivation and I will use it.
I rephrase my question:
The Bondi derivation is based on clock synchronization a la Einstein. So it should be equivalent with
x=g(x'-Vt') (1)
t=g(t'-Vx'/cc)
where g stands for gamma.
The Doppler factor D=k enable us to express V/c via the Doppler shift formula that can be derived without using the Lorentz transformations.
Sorry, I'm still not sure what you are asking.

You can use the Bondi method to prove the Lorentz transformation, as you quoted, for Einstein-synced coords, and to find Einstein-velocity v as a function of Doppler factor k. (As I did in my previous post.)

Or you can start with the Lorentz transformation and find the Doppler factor k as a function of Einstein-velocity v, a standard result in most textbooks, e.g. Relativistic Doppler effect. Actually, you don't need the full Lorentz transformation, you need only time-dilation, but how do you prove that?
 
Lorentz Bondi

DrGreg said:
Sorry, I'm still not sure what you are asking.

You can use the Bondi method to prove the Lorentz transformation, as you quoted, for Einstein-synced coords, and to find Einstein-velocity v as a function of Doppler factor k. (As I did in my previous post.)

Or you can start with the Lorentz transformation and find the Doppler factor k as a function of Einstein-velocity v, a standard result in most textbooks, e.g. Relativistic Doppler effect. Actually, you don't need the full Lorentz transformation, you need only time-dilation, but how do you prove that?
Thanks again. I think our discussion could be more easier in front of a blackboard.
The classical Doppler shift formula performed in I and involving say a stationary laser which emits successive short light signals and a moving target relates the proper emission period t(e) and the coordinate (nonproper) reception period t(r). An observer attached to the target, measures using his wrist watch a proper reception time interval t'(r) related to t(r) by the time dilation formula which can be derived without using the LT with which the classical Doppler shift formula becomes the relativistic one.
I learned much from Peres' "Relativistic telemetry"*in what concerns how formulas that account for relativistic effects could be derived without using the LT.
Such discussions are of big help for me. Thanks again.
*Asher Peres, "Relativistic telemetry," Am.J.Phys.55, 516-519 1987
 

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