Capacitance is the ability of a system to store electric charge per unit potential difference. For a capacitor the capacitance $C$ is defined as
$$C = \frac{Q}{V}$$where $Q$ is the magnitude of charge on each plate and $V$ is the potential difference between the plates.
For an ideal parallel‑plate capacitor filled with a dielectric of permittivity $\varepsilon$, the capacitance is
$$C = \frac{\varepsilon A}{d}$$where $A$ is the plate area and $d$ is the separation between the plates.
The total capacitance $C_{\text{eq}}$ for $n$ capacitors in series is given by
$$\frac{1}{C_{\text{eq}}} = \frac{1}{C_1} + \frac{1}{C_2} + \dots + \frac{1}{C_n}$$The total capacitance for $n$ capacitors in parallel is the sum of the individual capacitances:
$$C_{\text{eq}} = C_1 + C_2 + \dots + C_n$$The electric potential energy $U$ stored in a charged capacitor can be expressed in three equivalent forms:
$$U = \frac{1}{2} QV = \frac{1}{2} C V^{2} = \frac{Q^{2}}{2C}$$This energy is released when the capacitor discharges.
Solution:
Series combination:
$$\frac{1}{C_{\text{eq}}} = \frac{1}{4.0\;\mu\text{F}} + \frac{1}{6.0\;\mu\text{F}} = \frac{3}{12\;\mu\text{F}} + \frac{2}{12\;\mu\text{F}} = \frac{5}{12\;\mu\text{F}}$$ $$C_{\text{eq}} = \frac{12\;\mu\text{F}}{5} = 2.4\;\mu\text{F}$$Charge on each capacitor (same in series):
$$Q = C_{\text{eq}} V = 2.4\;\mu\text{F} \times 12\;\text{V} = 28.8\;\mu\text{C}$$Energy stored:
$$U = \frac{1}{2} C_{\text{eq}} V^{2} = \frac{1}{2} \times 2.4\;\mu\text{F} \times (12\;\text{V})^{2} = 0.5 \times 2.4 \times 144\;\mu\text{J} = 172.8\;\mu\text{J}$$| Type | Dielectric Material | Typical Applications | Capacitance Range |
|---|---|---|---|
| Ceramic | Metal oxide ceramic | High‑frequency circuits, decoupling | pF – $\mu$F |
| Electrolytic | Aluminium oxide (wet) or tantalum | Power supply filtering | $\mu$F – mF |
| Film | Polypropylene, polyester | Audio, precision timing | nF – $\mu$F |
| Mica | Natural mica | RF circuits, stable capacitance | pF – nF |