Rick16
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- TL;DR Summary
- developing the Lorentz force law from the Lagrangian for the magnetic field
Susskind (in The Theoretical Minimum, volume 1, pages 203-205) writes the Lagrangian for the magnetic field as ##L=\frac m 2(\dot x^2+\dot y^2 + \dot z^2)+ \frac e c (\dot x A_x +\dot y A_y +\dot z A_z)## and then calculates ##\dot p_x =ma_x + \frac e c \frac d {dt} A_x=ma_x + \frac e c(\frac {\partial A_x} {\partial x}\dot x + \frac {\partial A_x} {\partial y}\dot y + \frac {\partial A_x} {\partial z}\dot z)##.
I have problems with the last step. I might have written ##\frac {dA_x} {dt} =\frac {dA_x} {dx} \frac {dx} {dt}##, ignoring the other terms. How can I know that each component of the vector potential depends on all the coordinates? I would have to somehow picture the vector potential in order to come to this conclusion, but the vector potential seems to be a purely theoretical construct. How can I know how to treat it in situations like this one?
I have problems with the last step. I might have written ##\frac {dA_x} {dt} =\frac {dA_x} {dx} \frac {dx} {dt}##, ignoring the other terms. How can I know that each component of the vector potential depends on all the coordinates? I would have to somehow picture the vector potential in order to come to this conclusion, but the vector potential seems to be a purely theoretical construct. How can I know how to treat it in situations like this one?