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.
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
| Connection | Same for all | Equivalent 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.