Q1. Two capacitors of 3 µF and 6 µF are connected in series. Find the equivalent capacitance.
1/C = 1/C₁ + 1/C₂ = 1/3 + 1/6 = 2/6 + 1/6 = 3/6
C = 6/3 = 2 µF (series capacitance is smaller than either)
Capacitors store energy in an electric field. Use the calculator to link charge, voltage, capacitance and stored energy, then practise the standard numericals.
Enter the charge and voltage to read the capacitance and the energy stored (values in micro-units).
Energy depends on the SQUARE of voltage (½CV²) — doubling the voltage stores four times the energy.
Capacitance, energy and combination problems with steps.
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Q1. Two capacitors of 3 µF and 6 µF are connected in series. Find the equivalent capacitance.
1/C = 1/C₁ + 1/C₂ = 1/3 + 1/6 = 2/6 + 1/6 = 3/6
C = 6/3 = 2 µF (series capacitance is smaller than either)
Q2. A 5 µF capacitor is charged to 200 V. Find the charge and the energy stored.
Q = CV = 5×10⁻⁶ × 200 = 1×10⁻³ C = 1000 µC
U = ½CV² = ½ × 5×10⁻⁶ × 200² = 0.1 J
| Quantity | Formula | SI unit |
|---|---|---|
| Electric potential (point charge) | V = kQ/r | volt (V) |
| Capacitance | C = Q / V | farad (F) |
| Parallel-plate capacitor | C = ε₀A / d | F |
| Energy stored | U = ½CV² = ½QV | joule (J) |
| Capacitors in series | 1/C = 1/C₁ + 1/C₂ | F |
| Capacitors in parallel | C = C₁ + C₂ | F |
The work done per unit positive charge in bringing it from infinity to a point in an electric field, measured in volts.
The ability of a conductor to store charge per unit potential difference, C = Q/V, measured in farads.
In the electric field between its plates; the stored energy is U = ½CV² = ½QV = Q²/2C.
It increases by a factor equal to the dielectric constant K of the material, because the dielectric reduces the effective field.
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