Lorentz contraction and Spacetime diagram

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Homework Help Overview

The discussion revolves around understanding the relationship between the variables in the context of Lorentz contraction and spacetime diagrams, particularly focusing on the derivation of expressions related to the Lorentz Transformation and time dilation. Participants are exploring geometric interpretations and the implications of these concepts within special relativity.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants are attempting to derive expressions geometrically and are questioning the logic behind certain results. There is a focus on understanding the graphical representation of the Lorentz Transformation and the implications of invariant hyperbolas. Some participants express confusion over the derivation process and seek insights without relying on interval invariance.

Discussion Status

The discussion is ongoing, with participants sharing insights and questioning the clarity of the material. Some guidance has been offered regarding the geometric interpretation of the concepts, but there is no explicit consensus on the derivation methods or the clarity of the source material.

Contextual Notes

Participants mention the book "A First Course in GR" by Bernard Schutz, noting that it may not provide a comprehensive foundation for special relativity. There is a concern about the completeness of the derivations presented in the text, which may affect understanding.

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Homework Statement
...
Relevant Equations
...
1613471450045.png

Hello, i can't understand how does the author found this expression relating ##x_{c}## and v. I already tried by a lot of geometrical ways, knowing that the tangent of the angle between the dotted line and the x-axis should be v, but the results are illogical. Could you help me? I am start to thinking it is a postulate ...
 
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It's from the Lorentz Transformation, which I assume is the "identical calculation from before".
 
PeroK said:
It's from the Lorentz Transformation, which I assume is the "identical calculation from before".
But he derive the Lorentz transformation after this, before it there is just the time dilatation:
1613477091707.png

The figure he cites is another figure, but at least this expression for the time i could found using the interval invariance ds². For the length contraction, i can't see how he deduced it. And i don't want to use the interval invariance again, i am trying to gain some insights using just the graphic.
 
Herculi said:
But he derive the Lorentz transformation after this, before it there is just the time dilatation:
View attachment 278102
The figure he cites is another figure, but at least this expression for the time i could found using the interval invariance ds². For the length contraction, i can't see how he deduced it. And i don't want to use the interval invariance again, i am trying to gain some insights using just the graphic.
This is difficult without seeing the full derivation of everything in your book.

What book is this? Just out of interest.
 
PeroK said:
This is difficult without seeing the full derivation of everything in your book.

What book is this? Just out of interest.
Bernard Schutz, a first course.
1613503896690.png
That's the image for the time dilatation, the curves in the graph are hyperbolae.
 
A first course in GR?
 
If so, a GR book is usually not the best place to learn SR. You generally get a concise review of SR aimed at refreshing what you already know and to familiarize yourself with the authors notation.
 
I think what you are supposed to do is note that ##\mathcal{C}## lies on an invariant hyperbola (see the curve ##\mathcal{EF}## in Figure 1.11) that satisfies ##-t^2+x^2=l^2## (section 1.7). You also note that the ##\bar{x}## axis is the line ##t=vx## and solve simultaneously for ##x## and ##t##.

I find Schutz helpful, but he does sometimes seem to skim over things which (IMO) need a bit more detail.
 
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Say angle between t axis and ##\bar{t}## axis ##\theta##, law of sines on triangle ABC says
\frac{AC}{sin(\frac{\pi}{2}+\theta)}=\frac{AB}{sin(\frac{\pi}{2}-2\theta)}
AB=\frac{\cos 2\theta}{\cos\theta}AC=\frac{\cos^2\theta-sin^2\theta}{\cos\theta}AC

Magic : sin and cos are replaced by sinh and cosh,
where ##\tanh \theta=v## where c=1

AB=\sqrt{1-v^2}AC

We can do the similar to take ##\theta## pure imaginary angle.
I hope this magic is meaningful.
 
Last edited:
  • #10
Do you still need help? This seems like a trivial case of length contraction with ##c## replaced by 1. The formula is saying the proper length ##l## is contracted down to ##\gamma l##.

Herculi said:
Homework Statement:: ...
Relevant Equations:: ...

View attachment 278099
Hello, i can't understand how does the author found this expression relating ##x_{c}## and v. I already tried by a lot of geometrical ways, knowing that the tangent of the angle between the dotted line and the x-axis should be v, but the results are illogical. Could you help me? I am start to thinking it is a postulate ...
 

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