Mike_Fontenot
- 249
- 17
I haven't previously ever derived an expression for c_hat, the velocity of any given light-pulse, relative to an accelerating observer, according to that accelerating observer. I hadn't done that derivation before, because I never felt the need for that result, and I didn't regard the issue as particularly important.
But a few days ago, I finally decided to do the derivation.
I chose to do the derivation in a very "first-principles" sort of way, starting with a Minkowski diagram of the accelerating traveler's world-line, plotted in some (arbitrary) inertial frame, much as I did when I originally derived the CADO equation. I had expected it to be fairly quick and easy, but it wasn't.
I had expected to get an expression for c_hat that contained the observer's acceleration "a" (as measured on his accelerometer), as a parameter. That's because of the fact that, for the idealized case of an instantaneous velocity change (for which the acceleration is a Dirac delta function), the distance (according to the accelerating observer) to any object (including a light-pulse), instantaneously changes ... seemingly implying an infinite value of c_hat.
The result of the derivation, for the case where the acceleration "a" is finite, but arbitrarily large, was very surprising to me ... so much so that at first, I didn't believe the result I was getting. (In hindsight, though, I can now see that it SHOULDN'T have been a surprise).
The result is that
c_hat = c.
I.e., according to an observer accelerating at "a" (in ly/y/y, say), the velocity of any light-pulse, relative to that observer, is always equal to c, just as it is for an inertial observer.
Mike Fontenot
But a few days ago, I finally decided to do the derivation.
I chose to do the derivation in a very "first-principles" sort of way, starting with a Minkowski diagram of the accelerating traveler's world-line, plotted in some (arbitrary) inertial frame, much as I did when I originally derived the CADO equation. I had expected it to be fairly quick and easy, but it wasn't.
I had expected to get an expression for c_hat that contained the observer's acceleration "a" (as measured on his accelerometer), as a parameter. That's because of the fact that, for the idealized case of an instantaneous velocity change (for which the acceleration is a Dirac delta function), the distance (according to the accelerating observer) to any object (including a light-pulse), instantaneously changes ... seemingly implying an infinite value of c_hat.
The result of the derivation, for the case where the acceleration "a" is finite, but arbitrarily large, was very surprising to me ... so much so that at first, I didn't believe the result I was getting. (In hindsight, though, I can now see that it SHOULDN'T have been a surprise).
The result is that
c_hat = c.
I.e., according to an observer accelerating at "a" (in ly/y/y, say), the velocity of any light-pulse, relative to that observer, is always equal to c, just as it is for an inertial observer.
Mike Fontenot