Charging and Discharging of a Capacitor

Charging and Discharging of a Capacitor: MDCAT Physics notes

Charging and Discharging of a Capacitor for MDCAT: capacitance C = Q/V, C = εA/d, stored energy, series and parallel combinations and RC time constant.

Unit: Electrostatics · Updated

Capacitor and capacitance

A capacitor is a device that stores charge, and with it electrical potential energy in the electric field between its plates. The charge on it is proportional to the potential difference:

$$Q = CV$$

$C$ is the capacitance. SI unit: farad, 1 F = 1 C V$^{-1}$.

Parallel plate capacitor

$$C = \frac{\varepsilon_0\varepsilon_rA}{d}$$

  • Increases with plate area $A$ and dielectric constant $\varepsilon_r$.
  • Increases when separation $d$ decreases.
  • Does not depend on the charge, the voltage or the thickness of the plates.

Examples: doubling the area and halving $d$ gives $4C$. Doubling the length, width and separation gives $(2\times2)/2 = 2C$.

Role of the dielectric

A dielectric increases $C$ by $\varepsilon_r$. For a capacitor that is isolated (charge fixed), inserting a dielectric reduces the field between the plates by $\varepsilon_r$; removing it makes the field rise again.

Energy stored

As the capacitor charges, the voltage rises from 0 to $V$, so the average voltage is $V/2$:

$$U = \tfrac12QV = \tfrac12CV^2 = \frac{Q^2}{2C}$$

The energy per unit volume is $u = \tfrac12\varepsilon_0\varepsilon_rE^2$.

  • Doubling $Q$ (same $C$) gives $4U$.
  • Doubling $E$ between the plates gives $4U$.
  • Charged capacitor with energy $U$, disconnected, joined in parallel to an identical uncharged one: charge shares equally, each has $Q/2$, so each stores $U/4$ (total $U/2$; the rest is lost as heat and radiation).

Combinations

ConnectionSame for allEquivalent capacitance
Series (end to end)Charge $Q$$\frac{1}{C_e} = \frac{1}{C_1} + \frac{1}{C_2} + \dots$
Parallel (side by side)Voltage $V$$C_e = C_1 + C_2 + \dots$

In parallel, the larger capacitor stores more energy ($\tfrac12CV^2$). In series, the same $Q$ means the smaller capacitor stores more energy ($Q^2/2C$).

Charging and discharging through a resistor

When a capacitor charges through a resistance $R$, charge builds up exponentially:

$$q = Q_0\left(1 - e^{-t/RC}\right) \qquad \text{(discharge: } q = Q_0e^{-t/RC})$$

  • $RC$ is the time constant; ohm × farad = second.
  • In one time constant the capacitor charges to about 63% of its final charge; on discharge it falls to about 37%.
  • Theoretically full charge is reached only after infinite time; in practice about 5 time constants.
  • Large $RC$ means slow charging and discharging.

Ultracapacitors

Ultracapacitors (supercapacitors) store charge using an electrical double layer at the electrode surface, giving very large capacitance.

Key formulas

  • $Q = CV$; $C = \varepsilon_0\varepsilon_rA/d$
  • $U = \tfrac12CV^2 = \tfrac12QV = Q^2/2C$
  • Series: $1/C_e = \sum 1/C_i$; parallel: $C_e = \sum C_i$
  • $\tau = RC$

Common MDCAT traps

  • Energy is $\tfrac12QV$, not $QV$.
  • Capacitance depends on geometry and medium, not on $Q$ or $V$.
  • Parallel capacitors add directly; series use reciprocals (opposite of resistors).
  • Energy goes as $Q^2$ or $E^2$: doubling gives four times.
  • Plate thickness has no effect on $C$.

Quick revision

  • 1 F = 1 C V$^{-1}$.
  • $RC$ has the unit of time.
  • Capacitor stores energy in its electric field.
  • Closer plates mean larger capacitance.
  • Ultracapacitors use the double-layer effect.

Test yourself

More in Electrostatics