In a parallel plate capacitor, the conduction current \( I_c \) is the current flowing through the plates, and the displacement current \( I_d \) is the current that is related to the changing electric field between the plates. The total current is the sum of both:
\[
I = I_c + I_d
\]
For a capacitor, the conduction current \( I_c \) is given by:
\[
I_c = \frac{Q}{t}
\]
where \( Q \) is the charge on the capacitor. The displacement current is related to the rate of change of the electric field between the plates:
\[
I_d = \epsilon_0 A \frac{dE}{dt}
\]
where \( A \) is the area of the plates and \( E \) is the electric field between the plates. Since the displacement current is equivalent to the conduction current in terms of charge flow, we have:
\[
I_c = I_d
\]
Thus, the sum of the conduction and displacement currents is the same at all points in the circuit.