Trial ends in

# 30.14: Ampere-Maxwell's Law: Problem-Solving

TABLE OF
CONTENTS

### 30.14: Ampere-Maxwell's Law: Problem-Solving

A parallel-plate capacitor with capacitance C, whose plates have area A and separation distance d, is connected to a resistor R and a battery of voltage V. The current starts to flow at t = 0. What is the displacement current between the capacitor plates at time t? From the properties of the capacitor, what is the corresponding real current?

To solve the problem, we can use the equations from the analysis of an RC circuit and Maxwell's version of Ampère's law.

For the first part of the problem, the voltage between the plates at time t is given by

Suppose that the z-axis points from the positive plate to the negative plate. In this case, the z-component of the electric field between the plates as a function of time t is given by

Therefore, the z-component of the displacement current Id between the plates of the capacitor can be evaluated as

where the capacitance  is being used.

Further, to solve the second part of the above-stated problem, the current into the capacitor after the circuit is closed can be obtained by the charge on the capacitor, which in turn can be evaluated by using the expression for VC. As a result, the real current into the capacitor is found to be the same as the displacement current.