Let's look at a very crude model of an electric motor: the railgun. (scheme attached)
there are two conducting rails and a cylindrical conductive bar can roll on them freely. There is also a magnetic field perpendicular to the plane of the rails. The load is drawn by the rolling bar.
There are two governing equations for the motor: the Kirchoff loop equation and Newton's Second Law.
Let's start with Newton's Second Law for the bar. There are two forces acting on the bar:
Ampere's force: [itex]F_{a} = B l I[/itex]
external force (opposite of what the force with which the bar pulls the load) - it is an external parameter [itex]F[/itex]
The bar has mass [itex]m[/itex]
The acceleration of the bar is [itex]a = dv/dt[/itex]
So, Second Newton's Law gives:
[tex]
m \, \frac{dv}{dt} = B L I - F[/tex]
Let's consider Kirchoff's Law now.
There are two voltage sources acting in the loop:
external voltage [itex]V[/itex] which is an external force
induced EMF: [itex]E_{i} = -B L v[/itex]
The resistance of the whole circuit is [itex]R[/itex].
The current through the circuit is [itex]I[/itex].
Second Kirchoff's Rule gives:
[tex]
V - B L v = R I[/tex]
The mechanical variable for the system is [itex]v[/itex] - the velocity of the bar (or, in rotary geometries the angular velocity of the rotor). The electric variable of the motor is the current passing through it [itex]I[/itex]. The external parameters are the generated force [itex]F[/itex] (or, generated torque in rotary geometries) and the applied voltage [itex]V[/itex]. The internal parameters are the mass of the bar [itex]m[/itex] (or, the moment of inertia of the rotor in rotary geometries), the length of the bar [itex]L[/itex], the magnetic field [itex]B[/itex] and the total Ohmic resistance of all the conducting elements (rails and bar) [itex]R[/itex].
If you wish, you can eliminate the mechanical variable [itex]v[/itex] completely and get an equation involving only the electric state variable [itex]I[/itex]. Namely, solve the second equation with respect to [itex]v(t)[/itex]:
[tex]
v(t) = \frac{V(t) - R I(t)}{B L}[/tex]
differentiate it with respect to time (keeping in mind that the external voltage as well as the current might vary in time)
[tex]
\frac{dv}{dt} = \frac{V'(t) - R I'(t)}{B L}[/tex]
and substitute this into the first equation:
[tex]
\frac{m}{B L} \left(V'(t) - R I'(t)\right) = B L I(t) - F(t)[/tex]
That is, we get a first order linear differential equation:
[tex]
\frac{d I(t)}{d t} + \frac{(B L)^{2}}{m R} \, I(t) = \frac{1}{R} \left(V'(t) + \frac{B L}{m} F(t)\right)[/tex]
How is this equation like Ohm's Law? If anything, it looks like there is a capacitative element:
[tex]
\begin{array}{l}<br />
v_{\mathrm{ef}} - \frac{Q}{C_{\mathrm{ef}}} = R_{\mathrm{ef}} \, I \\<br />
<br />
I = \frac{d Q}{d t}<br />
\end{array}[/tex]
[tex]
\frac{d I}{d t} + \frac{1}{R_{\mathrm{ef}} C_{\mathrm{ef}}} I = \frac{V'_{\mathrm{ef}}(t)}{R_{\mathrm{ef}}}[/tex]
and, taking the effective resistance to be the same as the Ohmic resistance of the true motor (which can be done, by taking [itex]F = 0[/itex] - free running motor), then we see that the effective voltage applied on this circuit is:
[tex]
V_{\mathrm{ef}} = V(t) + \frac{B L}{m} \int_{t_{0}}^{t}{F(t') \, dt'}[/tex]
i.e. it is time dependent even if the external parameters V(t) and F(t) are constant, and, the effective capacitance is:
[tex]
C_{\mathrm{ef}} = \frac{m}{(B L)^{2}}[/tex]