Let's say that I have a charged mass that is moved by some non-electromagnetic means such as gravity or fluid flow.
I expect Maxwell's equations to hold in this case. However, I am confused as to how the relation $$J = \sigma E $$ will behave. I know that $\sigma$ is tensorial in general and that it can depend on a variety of factors (space, time, E, B...), however, I do not expect $J = \sigma E $ to hold linearly (in the context of Maxwell's equations) because the flow of current is not due to the electromagnetic field.
I tried looking at this scenario in terms of the macroscopic formulation of Maxwell's equations as well (https://en.wikipedia.org/wiki/Maxwell%27s_equations#Macroscopic_formulation) but all I could do was attempt to make mental analogies from this scenario to bound/free charges.
In some literature, I saw that $$J = \sigma E + J_s$$ (i.e. with some source term). This can make sense to me in the sense that the charged mass will contribute some specific $J_s$, making $J$ nonlinear. Otherwise, the other option is $J=0$.
Something is clearly amiss with my understanding, so I would appreciate it if someone could fix my perspective. My main concern is about how the J term in Maxwell’s equations (Ampere’s Law with Maxwell’s addition) and the equation for charge conservation (i.e. the continuity equation) will be affected (if at all) in this case.
Thanks!