I Coordinate and time transformations

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The discussion centers on the limitations of Galilean and Lorentz transformations in describing events that occur away from an observer. It emphasizes that coordinates are merely labels assigned to events in spacetime, not direct representations of information transmission, which is constrained by the speed of light. The conversation highlights that measurements of distant events require physical travel to those locations, and simultaneity can only be assessed after data comparison. Theoretical frameworks allow for mathematical calculations of speeds and distances, but the actual observation of events remains crucial. Ultimately, the transformations serve as a systematic way to assign coordinates, rather than a complete depiction of event transmission.
Ahmed1029
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In describing the Galelian or Lorentz transformations, All books I've read keep talking about clocks and meter sticks, but I don't see how an event happening away from the observer could be instantaneously described by a set of coordinates and a point in time; information conveying the event travels at most at the speed of light and measurement is only going to be detecting its past. In the light of this, what do those transformations really say?
 
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Coordinates have nothing to do with information actually being transmitted. It is an assignment of number labels to events in spacetime.
 
When you talk about an observer in an inertial reference frame, you can imagine that there is an observer, stationary at every point of his reference frame, who records events. It is really a matter of how events would be recorded at those locations in his reference frame, not how that information would be transmitted to him at a central location.
 
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There is nowhere you can stand where you can see the whole surface of the Earth, yet somehow we manage to assign coordinates to all of it (excluding one point, for the pedantic).

Coordinates are just labels we assign to events. As long as we assign them systematically we can assign them to events we can't see yet. We don't know what happened (if anything) at those events until we see them, but that doesn't matter. It's just the same as drawing a grid and filling in the map as we explore.
 
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Ahmed1029 said:
In describing the Galelian or Lorentz transformations, All books I've read keep talking about clocks and meter sticks, but I don't see how an event happening away from the observer could be instantaneously described by a set of coordinates and a point in time; information conveying the event travels at most at the speed of light and measurement is only going to be detecting its past. In the light of this, what do those transformations really say?
When you measure the distance to something at some point you actually have to travel the distance to get there in order to measure it. (Or some other similar method.) You might think of it as the events that are talked about in these problems are times people recorded at certain positions and the data are compared later when the people get together. When the data are compared, only then we can start making statements about if the times for events are simultaneous or not.

Then once the theory is proven we can just use the Mathematics to figure out speeds and distances and such.

-Dan
 
Thank you guys I got the point!
 
In Birkhoff’s theorem, doesn’t assuming we can use r (defined as circumference divided by ## 2 \pi ## for any given sphere) as a coordinate across the spacetime implicitly assume that the spheres must always be getting bigger in some specific direction? Is there a version of the proof that doesn’t have this limitation? I’m thinking about if we made a similar move on 2-dimensional manifolds that ought to exhibit infinite order rotational symmetry. A cylinder would clearly fit, but if we...