During the transient response of an RC circuit, the voltage across the capacitor increases exponentially until it reaches the supply voltage.

After one time constant (τ), the voltage across the capacitor will be V0/e, where V0 is the initial voltage.

The charge stored in the capacitor is given by Q = C*V = 2μF * 10V = 20μC.

In a discharging RC circuit, the voltage across the capacitor at time t is given by V = V0*e^(-t/RC), where V0 is the initial voltage.

In a series RC circuit, the total impedance is given by Z = R + Xc, where Xc is the capacitive reactance.

The time constant τ in an RC circuit is defined as τ = R*C, where R is the resistance and C is the capacitance.

As time approaches infinity after the switch is closed, the current in an RC circuit decreases to zero.

Increasing the capacitance in an RC circuit increases the time constant τ = R*C, making the charging and discharging processes slower.

The electric potential across a capacitor is given by the formula V = Q/C, where Q is the charge and C is the capacitance.

The capacitive reactance is given by Xc = 1/(2πfC), where f is the frequency and C is the capacitance.

The final voltage across a capacitor after it has been fully charged in an RC circuit is V0, where V0 is the supply voltage.

The final voltage across a capacitor in a series RC circuit after a long time is V0, where V0 is the supply voltage.

The charge on a capacitor during charging in an RC circuit is given by Q = C*V(1 - e^(-t/RC)).

The relationship between the charge and the voltage across a capacitor is given by Q = C*V, where C is the capacitance.