Help with special relativity mathematics

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Discussion Overview

The discussion revolves around understanding the mathematical transformations related to Lorentz transformations in the context of special relativity. Participants are exploring specific equations and their derivations, seeking clarification on the steps involved and the assumptions made during the process.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • One participant expresses difficulty in understanding a transformation related to Lorentz equations and questions the transition between specific equations.
  • Another participant challenges the validity of the transformation presented, suggesting it may not be a proper Lorentz transformation without additional context.
  • Some participants provide references to the source material, including a translation of Einstein's original paper, and discuss the implications of the translation quality.
  • Several participants offer insights into the mathematical steps required to transition between equations, including the application of the total derivative and chain rule.
  • There is a discussion about the treatment of partial derivatives, with some participants questioning assumptions made about their values in specific contexts.
  • One participant requests clarification on how to derive a specific equation using LaTeX, indicating a desire for more detailed guidance.
  • Another participant emphasizes the importance of doing the work independently while offering to provide assistance.

Areas of Agreement / Disagreement

There is no clear consensus among participants. While some agree on the steps to derive certain equations, others express confusion and challenge the assumptions made. The discussion remains unresolved regarding the specific transformations and the treatment of partial derivatives.

Contextual Notes

Participants highlight the need for additional context regarding the source material and the specific equations being discussed. There are unresolved questions about the assumptions made in the mathematical derivations, particularly concerning the treatment of partial derivatives.

Santilopez10
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I am having a hard time trying to understand this transformation from lorentz:https://imgur.com/a/WYWMO

(You should ignore the spanish part and just focus on the math). I can’t understand well why they turn into what you can see in the second picture, when taking really small values of x.
Also, I tried to approximate to the fourth equation, but I get minus partial derivative of tau respect of x prime, instead of plus.
I would appreciate your help, thanks. I hope this is understandable, it is my first post, and I have no knoweldge of latex.
 
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Santilopez10 said:
I am having a hard time trying to understand this transformation from lorentz

What you're showing isn't a Lorentz transformation; at best, it's a small piece of one particular attempt to teach the Lorentz transformation. Without more context, I don't think anyone is going to be able to help. What book is this from? What chapter?
 
PeterDonis said:
What you're showing isn't a Lorentz transformation; at best, it's a small piece of one particular attempt to teach the Lorentz transformation. Without more context, I don't think anyone is going to be able to help. What book is this from? What chapter?
“Great illusion”, greatest works of alber einstein” Stephen hawking edition, chapter 3

If you want I can write the things stated before the equations, it is all things about references systems, with more than 1 system.

Also, I would really appreciate how to get from the second equation to the third, thanks.
 
The text is a translation of Einstein's original paper "On the electrodynamics of moving bodies", part I section 3.

The third equation to the fourth seems to me to follow correctly. Post your working if you can't get it (you can use LaTeX for maths - there is a guide linked below the reply box).

The second equation to the third is simply applying the total derivative d/dx' to both sides, applying the chain rule and cancelling some terms, I believe.
 
Incidentally, the Spanish title of Hawking's book is indeed "The great illusion" ("La gran ilusion" - amazon.es link) which seems like a terrible translation of an allusion to Einstein's "distinction between past, present and future is only a stubbornly persistent illusion" quotation. I realize that book titles are often changed by publishers who know nothing about the subject, but I'd worry slightly about the quality of this translation from its title.
 
Last edited:
Ibix said:
The text is a translation of Einstein's original paper "On the electrodynamics of moving bodies", part I section 3.

The third equation to the fourth seems to me to follow correctly. Post your working if you can't get it (you can use LaTeX for maths - there is a guide linked below the reply box).

The second equation to the third is simply applying the total derivative d/dx' to both sides, applying the chain rule and cancelling some terms, I believe.
Could you show me by latex how to get from the second to the third please?
 
Ibix said:
The text is a translation of Einstein's original paper "On the electrodynamics of moving bodies", part I section 3.

The third equation to the fourth seems to me to follow correctly. Post your working if you can't get it (you can use LaTeX for maths - there is a guide linked below the reply box).

The second equation to the third is simply applying the total derivative d/dx' to both sides, applying the chain rule and cancelling some terms, I believe.

\begin{equation}
\frac {1}{2} \left( \frac 1{c-v} + \frac 1{c+v} \right) \frac {\partial \tau} {\partial t} = \frac {\partial \tau} {\partial x´} + \frac 1 {c-v} \frac {\partial \tau} {\partial t}

\end{equation}
then by summing and assuming partial tau over partial t is 0 I get:
\begin{equation}

\frac {v} {c^2 - v^2} \frac {\partial \tau}{\partial t} = \frac {\partial \tau}{\partial x´}

\end{equation}

which obviously comes into:

\begin{equation}
\frac {v} {c^2 - v^2} \frac {\partial \tau}{\partial t} - \frac {\partial \tau}{\partial x´} = 0
\end{equation}

And thus, I cannot realize how to get it as a plus instead of a minus. (the ##\frac {\partial \tau}{\partial x´}## term)
 
  • #10
Santilopez10 said:
assuming partial tau over partial t is 0
Try again without assuming that.
 
  • #11
DrGreg said:
Try again without assuming that.
Would you mind showing me? I thought a partial derivative of a constant was just 0.
 
  • #12
Santilopez10 said:
Would you mind showing me? I thought a partial derivative of a constant was just 0.
In equation (1) ##\partial \tau / \partial t## appears on both sides. Why would you set it zero on one side but not on the other, which is what you seem to have done?
 
  • #13
DrGreg said:
In equation (1) ##\partial \tau / \partial t## appears on both sides. Why would you set it zero on one side but not on the other, which is what you seem to have done?
I don’t really know, please teach me! Jajaja
 
  • #14
Santilopez10 said:
I thought a partial derivative of a constant was just 0.

Why do you think ##\partial \tau / \partial t## is a partial derivative of a constant?

Santilopez10 said:
I don’t really know, please teach me!

You need to do the work yourself. We can give you some help, but we're not going to just hand you the solution. If you want to learn, you need to do your part.
 
  • #15
Santilopez10 said:
I don’t really know, please teach me! Jajaja
My advice: don't try to be clever. This is just algebra.

Edit: and re-read Dr Greg's post #10.
 
Last edited:
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