 # Capacitor Part – 9

Charging and discharging of a capacitor:

Charging: Let us consider a capacitor C is connected to a battery of emf E through a resistance R. During charging of the capacitor the potential difference across the plates becomes equal to the emf of the battery. Let at any time t, I is the current through the resistance R and q is the charge of capacitor. Using KVL, VC + VR = E

Or, + IR = E

Or, + R = E

Or, R = E – Or, CRdq = (EC – q)dt

Or, =  Or,  =  Or, – loge = Or, 1 – = e– t/RC

Or, q = EC(1 – e– t/RC)

Or, q = q0(1 – e– t/RC) at t = , q = q0 = EC.  = CR is called capacitive time constant, i.e. the time in which charge of the capacitor is 0.632 times of its maximum value during charging.

The charging current is I = = = I0e– t/RC where I0 = = .

At t = 0, I = I0 i.e. initially it acts as short circuit or as a simple conducting wire.

At t = , I = 0 it acts as an open circuit.

Discharging: If a capacitor C with charge q0 is discharged through a resistance R then at any time t, the PD of the resistance is V = IR.

Using KVL, VC + VR = 0

Or, R + = 0

Or,  = –   Or, q = q0e– t/RC [This is the charge of the capacitor during discharging.]

The capacitive time constant = CR is the time in which charge becomes i.e. 0.368 times the initial value of charge q0.

The discharging current is I = – = – = I0e– t/RC where I0 = = . Click the button to go to the next part of this chapter.

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