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by appstateguy
2128 days ago
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This makes intuitive sense to me, but isn't the issue that relativity states that time is intrinsically coupled with space? Ones experience of time relative to another's is directly related to the topological features of the space they're in. If it's more curved, time also "curves" and slows down relative to another observer in flatter space. How does this notion of time become decoupled from space? One way I imagine it is that "time" as a concept encapsulates at least two properties: 1) The degree of freedom (i.e., dimension) through which things can change; and
2) The unidirectional flow of causal events Relativity seems more concerned with defining time in terms of casual events (e.g., event horizons) than its dimensionality. If we define "fundamental time" as a dimension that allows for change can it then be decoupled from space? |
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Thinking in terms of 3 dimensional euclidean space, this makes sense. If you fix your 3 dimensional coordinate system and pick 2 points in space, you can have:
Another observer could pick a different orientation for their coordinate system, and arrive at different values for dx, dy, and dz; but they would still have the same ds. This is just the pythagorean theorem. The distance between two points is the same regardless of how you define your axis. This also means that your 3 spatial dimensions are inherently coupled; because there was no particular reason to pick your axis the way you did.Simmilarly, in the 4 dimensional spacetime defined by the metric:
There is no particular reason to pick the particular time axis that you happened to pick. It is coupled with the other 3 dimensions in exactly the same way that the 3 dimensions are coupled in euclidean space.The only complication here is that rotating your axis under the Lorentzian metric require the Lorentz transform; whereas rotating them under the Euclidean metric requires the Galilean transform.
The coupling described here involves no notion of causality. Nothing in the metric prevents a path from traveling in both directions along the time axis.