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what will be the events relative to the ground observer , a time-like or space like? |
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| Mar5-12, 09:21 AM | #52 |
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what will be the events relative to the ground observer , a time-like or space like?To your point of the "common ancestor", I think you're missing the significance of this with regard to FTL information "transmission". If I give you a box, And you travel away from me to the other side of the world, and you open the box and find half a banana and deduce I have the other half that is not FTL transfer of information... |
| Mar5-12, 10:01 AM | #53 |
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| Mar5-12, 10:26 AM | #54 |
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Secondly, this math could be considered as follow: The ground observer calculate what the train observer would see. So he must includes v But there is just one ground observer to observe all events from the point where midpoint of the train coincides with the source |
| Mar5-12, 10:38 AM | #55 |
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| Mar5-12, 11:02 AM | #56 |
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There's a simple relation between t`a and t`b which you can use to check your result. I'll label with "C" the place on the train from where the light flash starts. It's clear that the distances add up like this: [itex]CA`+ CB` = AB`[/itex] [itex]CA`[/itex] is [itex]t`_{a}c[/itex] and [itex]CB`[/itex] is [itex]t`_{b}c[/itex], so: [itex]t`_{a}c + t`_{b}c = AB`[/itex] and therefore: [itex]t`_{a} + t`_{b} = \frac{AB`}{c}[/itex] Since [itex]t`_{a}[/itex] and [itex]t`_{b}[/itex] are both positive (light isn't going backwards in time!), it's clear that their difference can never exceed [itex]\frac{AB`}{c}[/itex]. |
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