*Re 2) Note that for a body at rest, coordinate and proper time are 
identical. Hence, d(tau)/dt = 1, where t is coordinate time and tau is 
proper time. But this is not true for a body not at rest. How does a 
physical clock "know" is it moving, making that derivative non-zero. AG *
On Friday, October 31, 2025 at 2:40:07 AM UTC-6 Alan Grayson wrote:

> 1) For a body at rest, we multiply clock time, aka proper time, and/or 
> coordinate time by some velocity, so its units become spatial. But why 
> multiply by c? Is this procedure really a *definition* to get a velocity 
> of c in spacetime?
>
> 2) Proper time and coordinate time are not equal along some arbitrary path 
> in spacetime. How does a clock "know" it isn't reading coordinate time, but 
> something else called proper time? Alternatively, what principle can we 
> apply to put proper time on a logically necessary footing?
>
> 3) When moving along some arbitrary path in spacetime, the Pythagorean 
> theorem holds; that is, (ds)^2 = (ct)^2 + (dx)^2. So how do we get a 
> negative sign preceding the spatial differentials? Here I'm referring to a 
> YouTube video whose link I will post later. 
>
> 4) If (ds)^2 is an *invariant *under SR, does this hold only for the LT, 
> but is it true for any linear transformation, as well as non-linear 
> transformations?
>
> AG

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