Agerhell
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AndromedaRXJ said:I know, but a change in velocity doesn't have to be a change in speed.
That's why I brought up the particle going in a circle at a constant speed of 0.99c. Is it's inertia growing due to it's circular path?
So would γ increase to a change in direction?
For the case of electromagnetism and a small particle of charge q and mass "invariant mass" m accelerated in an electromagnetic field classically we have:
\frac{d}{dt}(m\bar{v})=q(\bar{E}+\bar{v}\times\bar{B})
Assuming "m" not to vary with time we get:
\frac{d\bar{v}}{dt}=\frac{q}{m}(\bar{E}+\bar{v}\times\bar{B})
Instead assuming that the classical momentum m\bar{v} in the first expression above should be replaced by its relativistic counterpart m\gamma\bar{v} where
\gamma=\frac{1}{\sqrt{1-\frac{v^2}{c^2}}}
and solving the differential equation we get:
\frac{{\rm d}\bar{v}}{{\rm d}t}=\frac{q(\bar{E}\cdot\hat{v})}{m\gamma}\left(1-\frac{v^2}{c^2}\right)\hat{v}-\frac{q}{m\gamma}((\bar{E}+\bar{v}\times\bar{B})\times\hat{v}) \times \hat{v}.
As you can se there is a factor of 1/\gamma also in the second term on the right side. This means that it is harder to accelerate a particle in an electromagnetic field also in the direction transverse to its velocity, such as for a circular orbit.