On Sat, Jan 25, 2025 at 8:07 PM Alan Grayson <[email protected]> wrote:

>
>
> On Monday, December 9, 2024 at 2:01:28 PM UTC-7 Brent Meeker wrote:
>
> >
> > Nothing odd about dilation and contraction when you know its cause.
> > But what is odd is the fact that each frame sees the result
> > differently -- that the car fits in one frame, but not in the other --
> > and you see nothing odd about that, that there's no objective reality
> > despite the symmetry. AG
>
> The facts are events in spacetime.  There's an event F at which the
> front of the car is even with the exit of the garage and there's an
> event R at which the rear of the car is even with the entrance to the
> garage.  If R is before F we say the car fitted in the garage. If R is
> after F we say the car did not fit.  But if F and  R are spacelike, then
> there is no fact of the matter about their time order.  The time order
> will depend on the state of motion.
>
> Brent
>
>
> Jesse; it's the last two of Brent's sentences that I find ambiguous. What
> does he mean?
>

What about them do you find ambiguous? He's just saying that if there's a
spacelike separation between the events F and R (as there was in his
numerical example), then you can find a frame where R happens after F (as
is true in the car frame where the car doesn't fit), and another frame
where F happens after R (as is true in the garage frame where the car does
fit).


> I also wonder what happens when we transform in the
> reverse direction from the pov of simultaneity, from the car frame to the
>  garage frame? TY, AG
>

Brent didn't mention a direction in which the transformation is being
taken, but regardless of whether you start with the coordinates of F and R
in the garage frame and transform to the car frame, or start with the
coordinates of F and R in the car frame and transform to the garage frame,
you get the same answers about what the coordinates of these F and R are in
each frame. For instance if you start with the coordinates x,t of F in the
garage frame and apply the LT to get the coordinates x',t' of F in the car
frame, then apply the LT to x',t' (this time using a velocity of -0.8c
rather than +0.8c since the garage frame is moving in the -x direction as
seen in the car frame) you will get back the original coordinates x,t for
the garage frame.

Jesse

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