Re: The problem of relativistic synchronisation

Liste des GroupesRevenir à p relativity 
Sujet : Re: The problem of relativistic synchronisation
De : relativity (at) *nospam* paulba.no (Paul.B.Andersen)
Groupes : sci.physics.relativity
Date : 01. Sep 2024, 10:58:17
Autres entêtes
Organisation : A noiseless patient Spider
Message-ID : <vb1dpe$1evqr$1@dont-email.me>
References : 1 2 3 4 5 6 7 8 9 10 11
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Den 31.08.2024 23:14, skrev Richard Hachel:
Le 31/08/2024 à 22:10, "Paul.B.Andersen" a écrit :
Den 31.08.2024 09:05, skrev Richard Hachel:
 
https://paulba.no/pdf/Mutual_time_dilation.pdf
 ? ? ?
Thanks to Python, I see that you fail to understand
the very first equation in the paper.
https://ibb.co/7C0S4nJ
It probably won't help, but I will point out what is clearly
defined in the paper.
https://paulba.no/pdf/Mutual_time_dilation.pdf
Quote:
| Event E₂: clock A and clock B' are adjacent
| In frame K', A will be at the position -d when B' shows  t₂'= d/v
I considered this to be obvious for a reasonable knowledgeable reader.
Explanation for the less knowledgeable reader:
-----------------------------------------------
In frame K' the clock A has moved from the position X' = 0
to the position x' = -d with the speed v.
Since t' = 0 when A was at  x' = 0, t' = d/v when A is at x' = -d.
So the coordinates of event E₂ in K' are  x₂'= -d, t₂' = d/v
In frame K the temporal coordinate will be:
t₂ = γ⋅(t₂' + (v/c²)⋅x₂') = equation (1) in the paper
The spatial coordinate was irrelevant, but it would be:
x₂ =  γ⋅(x₂' + v⋅t₂') = γ⋅(-d + v⋅d/v) = 0
which is a trivial result since clock A is stationary at x = 0.
--------------
Your d' is probably the distance between the clocks in K measured
in frame K', and vice versa.
But this 'contacted' distance is never used, and is irrelevant.
In the Lorentz transform you never use contacted distances and
dilated times. You _only_ use proper distances and proper times.
Didn't you know that?
--
Paul
https://paulba.no/

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23 Aug 24 * The problem of relativistic synchronisation104Richard Hachel
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