A capacitor stores electrical energy by accumulating separated charge on two conductors. Capacitors are everywhere in electronics — from smoothing power supplies to tuning radio receivers to storing energy in defibrillators. The key insight is that the energy is stored in the electric field between the plates, not in the charges themselves.
Key Concepts
Capacitance
The capacitance C of a capacitor is the ratio of the charge stored on each plate to the potential difference between the plates: C=Q/V. Unit: farad (F = C/V). A larger capacitance stores more charge per volt.
Parallel-Plate Capacitor
Two large parallel conducting plates of area A separated by gap d. Capacitance: C=ε0A/d. Larger area and smaller gap both increase capacitance.
Dielectric Materials
Inserting an insulating material (dielectric) between the plates increases capacitance by the dielectric constant κ>1: C=κε0A/d. The dielectric's polar molecules align with the field, reducing the effective electric field and allowing more charge to be stored at the same voltage.
Energy Stored in a Capacitor
The energy stored is U=21CV2=2CQ2=21QV. This energy resides in the electric field between the plates.
Capacitors in Series
Capacitors in series all carry the same charge Q; their voltages add. Equivalent capacitance: 1/Ceq=1/C1+1/C2+⋯. The equivalent is always less than the smallest individual capacitor.
Capacitors in Parallel
Capacitors in parallel all share the same voltage V; their charges add. Equivalent capacitance: Ceq=C1+C2+⋯. The equivalent is the sum.
Key Equations
Capacitance definition
C=VQ
Charge Q stored per unit voltage V. Unit: farad (F).
Parallel-plate capacitor
C=dκε0A
κ = dielectric constant (1 for air), ε₀ = 8.85×10⁻¹² F/m, A = plate area, d = plate separation.
Energy stored
U=21CV2=2CQ2
Energy (in joules) stored in the electric field of the capacitor.
Series combination
Ceq1=C11+C21+⋯
Equivalent capacitance for capacitors connected in series (same Q, voltages add).
Parallel combination
Ceq=C1+C2+⋯
Equivalent capacitance for capacitors connected in parallel (same V, charges add).
Worked Example
Parallel-Plate Capacitor with a Battery
Problem
A parallel-plate capacitor has plate area A=0.020 m² and separation d=2.0 mm (air gap, κ=1). It is connected to a 12 V battery. Find (a) the capacitance, (b) the charge stored, and (c) the energy stored.
Solution
(a) Capacitance:
C=dε0A=2.0×10−3(8.85×10−12)(0.020)=88.5 pF
(b) Charge stored at V=12 V:
Q=CV=(88.5×10−12)(12)=1.06 nC
(c) Energy stored:
U=21CV2=21(88.5×10−12)(12)2=6.37 nJ
AnswerC = 88.5 pF; Q = 1.06 nC; U = 6.37 nJ.
Practice
Exercises
7 problems
1of 7
A capacitor stores Q=60 nC of charge when connected to a V=12 V source. What is its capacitance (in nF)?
nF
2of 7
A parallel-plate capacitor has plate area A=0.050 m² and separation d=1.0 mm with air between the plates. What is its capacitance (in pF)?
pF
3of 7
How much energy (in mJ) is stored in a C=10μF capacitor charged to V=100 V?
mJ
4of 7
Two capacitors C1=4μF and C2=6μF are connected in **series**. What is the equivalent capacitance (in μF)?
μF
5of 7
The same two capacitors C1=4μF and C2=6μF are now connected in **parallel**. What is the equivalent capacitance (in μF)?
μF
6of 7
A capacitor has capacitance C0=200 pF with air between its plates. A dielectric with κ=3.5 is inserted to fill the gap. What is the new capacitance (in pF)?
pF
7of 7
A parallel-plate capacitor (air, κ=1) has plate area A=0.040 m² and must have capacitance C=100 pF. What plate separation d (in mm) is needed?
mm
Key Takeaways
Capacitance measures how much charge is stored per volt — larger C means more charge for the same voltage.
For a parallel plate: C∝A/d — bigger plates or smaller gap increases capacitance.
A dielectric multiplies C by κ because aligned molecules reduce the internal field, allowing more charge for the same V.
In series: equivalent C is less than the smallest (reciprocals add). In parallel: equivalent C is the sum (capacitances add).
Energy stored scales as V2 — doubling the voltage quadruples the stored energy.