Charge (Q) on a capacitor is given by Q = C * V. Thus, Q = 4μF * 12V = 48μC.

The voltage across the capacitor decreases exponentially over time when connected to a resistor due to discharge.

The time constant (τ) of an RC circuit is given by τ = RC.

When a capacitor is disconnected from the battery, the charge remains constant. Increasing the distance decreases capacitance but does not affect the charge.

When the distance is doubled, the capacitance decreases, leading to an increase in voltage since Q = CV is constant.

Once disconnected from the battery, the charge on the capacitor remains constant as there is no path for charge to flow.

When a capacitor is disconnected from the battery, the charge remains constant. Increasing the distance decreases capacitance but does not change the charge.

The charge on a capacitor is given by Q = C * V. If the voltage is doubled, the charge also doubles, assuming capacitance remains constant.

The energy stored in a capacitor is proportional to the square of the voltage (U = 1/2 CV²). If the voltage is halved, the energy becomes U/4.

When connected in parallel, the total charge is conserved. The final voltage across both capacitors is V/2.

The energy stored in a capacitor is given by U = 1/2 CV². If the voltage is halved, the new energy becomes U' = 1/2 C(V/2)² = U/4.

When the charged capacitor C is connected to an uncharged capacitor 2C, the final voltage is V_final = Q_total / C_eq = V/(1 + 1/2) = V/3.

The charge (Q) on a capacitor is given by Q = C * V. Here, Q = 10 µF * 5 V = 50 µC.

When a charged capacitor is short-circuited, the charge flows through the circuit, and the charge on the capacitor becomes zero.

When connected in parallel, charge redistributes, and the final voltage across both capacitors will be V/2.

The time constant τ of an RC circuit is given by τ = R * C.

Short-circuiting a capacitor allows charge to flow off, resulting in the charge becoming zero.

When a capacitor is short-circuited, the stored energy is dissipated as heat in the circuit.

In a DC circuit, the current through a capacitor decreases to zero as it becomes fully charged.

In an AC circuit, the current through a capacitor leads the voltage by 90 degrees.

When a capacitor is fully discharged and connected to a voltage source, the initial current is maximum as it starts charging.

Charge (Q) on a capacitor is given by Q = C * V. Here, Q = 4μF * 12V = 48μC.

The energy (U) stored in a capacitor is given by the formula U = 1/2 CV^2.

The charge (Q) on a capacitor is given by Q = CV when connected to a voltage source V.

The charge (Q) stored in a capacitor is given by the formula Q = C * V.

Capacitance is inversely proportional to the distance between the plates. If the distance d is doubled, the capacitance C becomes C/2.

Capacitance is inversely proportional to the distance between the plates. If the distance is halved, the capacitance doubles.

The equivalent capacitance C_eq of capacitors in series is given by 1 / C_eq = 1 / C1 + 1 / C2.

Capacitance is directly proportional to the plate area A. Increasing A increases capacitance.

The dielectric constant represents the ability of a material to increase the capacitance of a capacitor compared to a vacuum.