- #1
jjustinn
- 164
- 3
It sounds like an easy-enough problem, but even writing down the ridiculously nonlinear equation that would need to be solved is making my face hurt.
I'm talking classical/Newtonian gravitation, action-at-a-distance, constant-force. It could really be any external non-EM conserved force; gravity just seemed like the easiest.
However, the charge is NOT a test charge: e.g. its own self-field reactions are important.
Let's say it's a spherical marble, 1cm diameter, weighing 5g and charged to 1C, released from rest in a vacuum 50m above the surface.
Now I seem to recall that there is no "radiative braking" on a charge with uniform acceleration -- which is what the trajectory would be if there was no radiative braking...so you see why my face hurts.
Has anyone tackled this (or something similar) in he past? It seems like it should be about the simplest possible situation -- ye olde one-body problem -- but I can't find any references to it.
Thanks,
Justin
I'm talking classical/Newtonian gravitation, action-at-a-distance, constant-force. It could really be any external non-EM conserved force; gravity just seemed like the easiest.
However, the charge is NOT a test charge: e.g. its own self-field reactions are important.
Let's say it's a spherical marble, 1cm diameter, weighing 5g and charged to 1C, released from rest in a vacuum 50m above the surface.
Now I seem to recall that there is no "radiative braking" on a charge with uniform acceleration -- which is what the trajectory would be if there was no radiative braking...so you see why my face hurts.
Has anyone tackled this (or something similar) in he past? It seems like it should be about the simplest possible situation -- ye olde one-body problem -- but I can't find any references to it.
Thanks,
Justin
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