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Capacitors store electric charge and electrical potential energy in an electric field. This reference helps students connect the physical structure of a capacitor to the equations used in circuit problems. It is useful for reviewing charge, voltage, capacitance, energy storage, and dielectric materials before tests or labs.

Key Facts

  • Capacitance is defined by C=QΔVC = \frac{Q}{\Delta V}, where QQ is charge and ΔV\Delta V is potential difference.
  • The SI unit of capacitance is the farad, with 1F=1CV1\,\mathrm{F} = 1\,\frac{\mathrm{C}}{\mathrm{V}}.
  • For a parallel-plate capacitor, C=κϵ0AdC = \kappa \epsilon_0 \frac{A}{d}, where AA is plate area, dd is plate separation, and κ\kappa is the dielectric constant.
  • The electric field between ideal parallel plates is approximately E=ΔVdE = \frac{\Delta V}{d}.
  • The energy stored in a capacitor can be written as U=12QΔV=12C(ΔV)2=Q22CU = \frac{1}{2}Q\Delta V = \frac{1}{2}C(\Delta V)^2 = \frac{Q^2}{2C}.
  • Capacitors in parallel have equivalent capacitance Ceq=C1+C2+C3+C_{\mathrm{eq}} = C_1 + C_2 + C_3 + \cdots and share the same voltage.
  • Capacitors in series satisfy 1Ceq=1C1+1C2+1C3+\frac{1}{C_{\mathrm{eq}}} = \frac{1}{C_1} + \frac{1}{C_2} + \frac{1}{C_3} + \cdots and carry the same charge.
  • Adding a dielectric increases capacitance by the factor κ\kappa, so C=κC0C = \kappa C_0 for the same geometry.

Vocabulary

Capacitor
A device that stores separated electric charge and electric potential energy in an electric field.
Capacitance
The ratio of stored charge to potential difference, given by C=QΔVC = \frac{Q}{\Delta V}.
Dielectric
An insulating material placed between capacitor plates that increases capacitance and reduces the effective electric field.
Equivalent capacitance
The single capacitance value that can replace a network of capacitors while producing the same overall circuit behavior.
Potential difference
The voltage between two points, equal to the electric potential energy change per unit charge.
Stored energy
The energy held in a capacitor's electric field, often calculated with U=12C(ΔV)2U = \frac{1}{2}C(\Delta V)^2.

Common Mistakes to Avoid

  • Using resistor rules for capacitor combinations is wrong because capacitors add directly in parallel and reciprocally in series.
  • Assuming charge is the same on parallel capacitors is wrong because parallel capacitors share the same voltage, while charge depends on Q=CΔVQ = C\Delta V.
  • Assuming voltage is the same on series capacitors is wrong because series capacitors carry the same charge and the voltage divides according to ΔV=QC\Delta V = \frac{Q}{C}.
  • Forgetting to square the voltage in U=12C(ΔV)2U = \frac{1}{2}C(\Delta V)^2 is wrong because capacitor energy depends quadratically on potential difference.
  • Ignoring unit conversions is wrong because values like μF\mu\mathrm{F} and nF\mathrm{nF} must be converted before using SI formulas.

Practice Questions

  1. 1 A 12μF12\,\mu\mathrm{F} capacitor is connected to a 9.0V9.0\,\mathrm{V} battery. What charge QQ is stored on the capacitor?
  2. 2 Two capacitors, C1=4.0μFC_1 = 4.0\,\mu\mathrm{F} and C2=6.0μFC_2 = 6.0\,\mu\mathrm{F}, are connected in parallel. What is CeqC_{\mathrm{eq}}?
  3. 3 A 5.0μF5.0\,\mu\mathrm{F} capacitor stores 2.5×104J2.5 \times 10^{-4}\,\mathrm{J} of energy. What voltage ΔV\Delta V is across it?
  4. 4 A dielectric is inserted between the plates of an isolated charged capacitor. Explain what happens to the capacitance, voltage, and stored energy.