An RC (Resistor-Capacitor) circuit is a circuit that contains both resistors and capacitors.
These circuits are fundamental in understanding how electrical charge is stored and dissipated in various components.
Charging a Capacitor
When a capacitor is charged through a resistor, the voltage across the capacitor and the current through the circuit change over time according to the following relationships:
VC(t)=V0(1−e−RCt)
I(t)=RV0e−RCt
V0 is the initial voltage, R is the resistance, C is the capacitance, and t is time.
The time constant (τ) of an RC circuit is defined as τ=RC. It indicates how quickly the capacitor charges or discharges.
Example of Charging RC Circuit
Given:
Capacitance: C=0.30μF
Resistance: R=20kΩ
Battery emf: E=12V
Calculate:
Time constant (τ): τ=RC=(0.30×10−6F)(20×103Ω)=6ms
Maximum charge (Qmax): Qmax=CE=(0.30×10−6F)(12V)=3.6μC
Time to reach 99% of Qmax: Solve for t in Q(t)=Qmax(1−e−τt)
Discharging a Capacitor
When a fully charged capacitor discharges through a resistor, the charge and the current through the circuit decrease over time as given by:
Q(t)=Q0e−RCt
I(t)=−RCQ0e−RCt
Q0 is the initial charge on the capacitor.
Example of Discharging RC Circuit
Given:
Capacitance: C=1.02μF
Battery emf: E=20V
Current decreases to 0.50 of its initial value in 40μs
Calculate:
Initial charge on the capacitor (Q0): Q0=CE=(1.02×10−6F)(20V)=20.4μC
Value of R: Derived from given info that current reduces by half in 40μs[1]``[2]``[3].