Passionflower, back in post #111, I asked you:
ghwellsjr said:
Ever since your first post on this thread, you have not used the term "spacetime interval":
Passionflower said:
In Galilean spacetime time is surely a dimension, but is that the case in relativity?
I think in relativity time is the length of a path between two events in four dimensions. You think I am wrong?
Is that because you are talking about something entirely different?
And now for the first time you are using the word "interval" in the same sentence with "spacetime" but not the term "spacetime interval":
Passionflower said:
So are you saying that a clock does not measure the path length between two events in spacetime but instead measures an interval of a single dimension of spacetime?
So for two different observers traveling between these two events with different path lengths, would you claim that they each measure an interval of the same dimension of spacetime?
So I still can't tell if you are talking about the "spacetime interval" or something else.
But, just in case you are talking about "spacetime interval", let me explain what it is and then you can tell me if it helps.
First you have to understand what an event is. It is nothing more than a specified location (in three dimensions) at a specified time as defined by a specified coordinate system. It does not necessarily have anything to do with observers or paths or any actual event, although it may. You can then transform the event (location plus time) to any other coordinate system and the numbers you get to describe the four components of the event could be totally different.
In Galilean spacetime, if you have two events, the spatial distance between any two events can be calculated by taking the square root of the sum of the squares of the differences in the three dimensions and the time difference is merely the difference in the two times. Then if you transform the two events into a different coordinate system, even though all the numbers are different to describe the locations and times of the two events, if you perform the same computation, you will get the same answers for the spatial distance and time difference between the same two events defined by the second coordinate system, even if this second coordinate system is in motion with respect to the first one.
By Galilean spacetime, we mean that the relative speed between the two coordinate sytems, otherwise known as frames of reference, is much less than the speed of light.
But if the two coordinate systems (frames of reference) have a high speed between them, then the calculations that we did under the Galilean spacetime do not give the same spatial distance and time difference in the two frames of reference. However, we can define a new "distance" or "difference" between the two events which is called the "spacetime interval" that will be the same no matter what frame of reference we do the computation in, but instead of getting two numbers, a spatial distance and time difference, we get just one, the spacetime interval, based on a calculation of the two previous values.
The computation is very similar to the spatial distance, in fact we start with that prior to taking the square root but instead we subtract the square of the time difference multiplied by the square of the speed of light.
It should be no surprise that this computaton yields a frame invariant quantity, since we use the Lorentz Transform to produce the numbers for the second frame of reference, and the transform guarantees that the spacetime interval is frame invariant.
Does that help or are you talking about something completely different?