Current Flow in a Capacitor

Consider a series circuit containing a voltage source v, a switch, a resistor R,
and a capacitor C. This is called a series RC circuit.

The moment the switch is closed:

  1. There will be no charge on the plates of the capacitor and therefore, no voltage across the plates of the capacitor.

  2. At the mall the source voltage appears across the resistor. This means that there is a current flow equal to v/R. As the current flows, electrons build up on one plate and holes with positive charge on the other plate.

  3. An electric field (E) will build up between the plates as the charges accumulate on the plates.

In the circuit shown in Figure 12.2, the top plate of the capacitor would be positively charged and its bottom plate negatively charged since the plates are arbitrarily assigned as + and - according to their proximity to the nearest voltage source terminal.

The electric field E intimates a voltage across the plates of the capacitor. As the voltage across the capacitor increases, the voltage across the resistor decreases reducing the current flow. Eventually, the capacitor is completely charged up and no more current will flow. The capacitance of a two-conductor capacitor is defined as

(12.4)




Figure 12.2 Series RC Circuit.


The charge q is equal to the integral of the surface charge density s over surface S

(12.5)

The voltage v is related to E by the following equation
(12.6)

Substituting into the equation of the capacitance

(12.7)

Where l is the integration path from conductor 2 to conductor 1.

               

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