jbriggs444
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This is the idea used for Fermi normal coordinates. You can set up coordinates in this manner to cover a "world-tube" which is centered on your world-line. For any particular reading ##t## on your wristwatch, you can consider your "now" to be all events in the cross-section of your world-tube that share that ##t## coordinate.Buckethead said:If I am at an event, on my timeline, and I create a plane through that event perpendicular to my timeline, and that plane slices other timelines, what is the significance of that? Does that plane intersect those events at meaningful locations on those timelines? Are those "now" moments from my location?
I like to think of this in two Euclidean dimensions like a winding country road. You want to set up (x,y) coordinates. Your odometer reads off the y coordinate directly. The car is always at (0,y). You look directly left or right through narrow blinders. The x coordinate for any point distant from the road is how far right or left it is when it comes momentarily into view.
As your road veers left and right or even when it goes straight, your plane of "simultaneity" sweeps forward more or less rapidly along nearby almost-parallel roads. Their mile markers do not keep pace with your coordinate system. That's time dilation. If your line of sight stops sweeping forward and actually sweeps backward along an almost parallel road, that region is outside the world-tube within which these coordinates work properly.
The notion of "now" that you get from Fermi normal coordinates has no particular significance. It is just one of many possible coordinate choices.
In the flat space-time of special relativity with unaccelerated observers, Fermi normal coordinates are often taken for granted. In such a context, they are the vanilla coordinates for which the Lorentz transforms apply.
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