Can All Clocks in an Inertial Frame Simultaneously Read Zero?

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    Clock Synchronization
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Discussion Overview

The discussion revolves around the possibility of having all clocks in a given inertial reference frame read zero time simultaneously. Participants explore synchronization methods, particularly in the context of special relativity, and the implications of different approaches to achieving this synchronization.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants propose that it is possible to synchronize clocks using a spherical light pulse emitted from a fixed point.
  • Others question the timing of the emission of the synchronizing light signal, suggesting that it may require waiting a significant amount of time to achieve all clocks reading zero.
  • One participant describes a method involving pairwise signaling to establish the round trip light signal time to each clock, allowing for synchronization at zero time.
  • Another participant emphasizes that the assumption of synchronizing at half the round trip time is crucial to Einstein's synchronization method, which introduces relativity into special relativity.
  • There is a discussion about the implications of different synchronization methods, with one participant noting that different clocks could be synchronized by different light signals, contrasting with the single light signal approach.
  • Some participants engage in clarifying the mechanics of synchronization, including the necessity of knowing the positions of the clocks beforehand and the role of to-and-fro light signals in establishing this knowledge.
  • A later reply raises a question about the geometric locus of simultaneous events as perceived from different inertial frames, indicating a deeper inquiry into the implications of synchronization across frames.

Areas of Agreement / Disagreement

Participants express differing views on the methods and assumptions involved in synchronizing clocks to read zero time. While some agree on the feasibility of synchronization, others contest the methods proposed and the underlying assumptions, indicating that the discussion remains unresolved.

Contextual Notes

The discussion highlights limitations related to the assumptions made about clock positions and the timing of light signals, as well as the dependence on definitions of synchronization in the context of special relativity.

bernhard.rothenstein
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Is it possible to realize a situation in which all the synchronized and ticking clocks of a given inertial reference frame read a zero time?
Thanks
 
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bernhard.rothenstein said:
Is it possible to realize a situation in which all the synchronized and ticking clocks of a given inertial reference frame read a zero time?
Thanks
Why not? There shouldn't be any problem at all, if you synchronize them with a spherical light pulse starting from a fixed point.
 
synchronization

lightarrow said:
Why not? There shouldn't be any problem at all, if you synchronize them with a spherical light pulse starting from a fixed point.
Thanks. At which time should I emit the synchronizing light signal?
 
bernhard.rothenstein said:
Thanks. At which time should I emit the synchronizing light signal?
-00. (So you have to wait a lot of time to record all "0" times!)
 
bernhard.rothenstein said:
Is it possible to realize a situation in which all the synchronized and ticking clocks of a given inertial reference frame read a zero time?
Thanks
Yes it is, for a finite number of clocks. Having established from a given clock by pairwise signalling, the round trip light signal time to every other clock, a series of synchronising signals is sent to each specific clock at zero minus [half the round trip time for that clock], upon receipt of which each clock is zeroed. Thus all the clocks in the inertial system are [Einstein] synchronised at zero.
Of course the assumption that the clock be synchronised at half the to-and-fro time is the crucial assumption of Einstein synchronisation that puts the "relativity" into special relativity. The clocks will be "synchronised" only for observers actually in the inertial system concerned.
 
clock synchronization

Boustrophedon said:
Yes it is, for a finite number of clocks. Having established from a given clock by pairwise signalling, the round trip light signal time to every other clock, a series of synchronising signals is sent to each specific clock at zero minus [half the round trip time for that clock], upon receipt of which each clock is zeroed. Thus all the clocks in the inertial system are [Einstein] synchronised at zero.
Of course the assumption that the clock be synchronised at half the to-and-fro time is the crucial assumption of Einstein synchronisation that puts the "relativity" into special relativity. The clocks will be "synchronised" only for observers actually in the inertial system concerned.
Thank you for your help. Please let me know what do you mean by "pairwise signaling" (outgoing and reflected light signals?) .
Considering the clocks C(x) located at the different points of the OX axis to be synchronized with clock C(0) located at the origin O, clock C(x) is stopped and fixed to read -x/c. A light signal emitted from O at t=0 arriving at C(x) starts it and so all the C(x) clocks read the same running time.
In order to obtain the situation when all the clocks C(x) read a zero time,each of them is stoped, read t=0 being synchronized by different light signals emitted at -x/c respectivelly. Of course your proposal is more in the spirit of Einstein's special relativity. I think that this simple fact is worth to be mentioned in a relativity lecture: In the first case a single light signal synchronizes all the clocks, whereas in the second case different clocks are synchronized by different light signals.
Regards
Bernhard
 
bernhard.rothenstein said:
Thank you for your help. Please let me know what do you mean by "pairwise signaling" (outgoing and reflected light signals?) .
Yes.
bernhard.rothenstein said:
clock C(x) is stopped and fixed to read -x/c. A light signal emitted from O at t=0 arriving at C(x) starts it and so all the C(x) clocks read the same running time.
In order to obtain the situation when all the clocks C(x) read a zero time,each of them is stoped, read t=0 being synchronized by different light signals emitted at -x/c respectivelly.
Er, no. I think you mean to say C(x) is stopped at +x/c, otherwise the clocks would not synchronise.
In any case your method requires that x be already known for each clock, and the only practicable way of establishing this is with a to-and-fro light signal between already synchronised clocks !
So one comes back anyway to the method I described, which is not merely "in the spirit of" SR but is the very method on which SR is based.
Regards.
 
synchronization

Boustrophedon said:
Yes.

Er, no. I think you mean to say C(x) is stopped at +x/c, otherwise the clocks would not synchronise.
In any case your method requires that x be already known for each clock, and the only practicable way of establishing this is with a to-and-fro light signal between already synchronised clocks !
So one comes back anyway to the method I described, which is not merely "in the spirit of" SR but is the very method on which SR is based.
Regards.
Could you tell me which is the geometric locus of the simultaneous events which read t'=0 in I' when detected from I?
Regards
 

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