AP Physics C E&M- 10.3 Capacitors - Study Notes- New Syllabus
AP Physics C E&M- 10.3 Capacitors – Study Notes
AP Physics C E&M- 10.3 Capacitors – Study Notes – per latest Syllabus.
Key Concepts:
- Physical Properties of a Parallel-Plate Capacitor
Parallel-Plate Capacitor
A parallel-plate capacitor consists of two conducting plates of area \(A\), separated by a distance \(d\), with a dielectric material (or vacuum) between them. It is used to store electric charge and energy.
Capacitance:
Capacitance relates the magnitude of charge stored on each plate to the potential difference across the plates:
\( \mathrm{C = \dfrac{Q}{V}} \)
For a parallel-plate capacitor with a dielectric:
\( \mathrm{C = \kappa \varepsilon_0 \dfrac{A}{d}} \)
- \(\mathrm{Q}\) = charge on one plate
- \(\mathrm{V}\) = potential difference between plates
- \(\mathrm{A}\) = plate area
- \(\mathrm{d}\) = plate separation
- \(\mathrm{\varepsilon_0 = 8.85 \times 10^{-12} \, C^2/(N \cdot m^2)}\)
- \(\mathrm{\kappa}\) = dielectric constant of material between plates
Electric Field Between Plates:
The electric field between the plates (ignoring edge effects) is uniform:
\( \mathrm{E = \dfrac{V}{d} = \dfrac{\sigma}{\varepsilon}} \)
- \(\mathrm{\sigma = Q/A}\) = surface charge density
- \(\mathrm{\varepsilon = \kappa \varepsilon_0}\) = permittivity of dielectric
Electric Potential Energy:
A charged capacitor stores energy equal to the work required to separate charges onto the plates:
\( \mathrm{U = \tfrac{1}{2} C V^2 = \tfrac{1}{2} Q V = \dfrac{Q^2}{2C}} \)
Summary of Properties:
- Capacitance: proportional to plate area, inversely proportional to separation.
- Dielectric increases capacitance by factor \(\kappa\).
- Capacitance defined by \( \mathrm{C = Q/V} \).
- Electric field between plates is uniform (except at edges).
- Capacitor stores electrical potential energy in the separated charges.
Example :
A parallel-plate capacitor with plate area \(0.02 \, m^2\), separation \(1.0 \times 10^{-3} \, m\), and dielectric constant \(\kappa = 4\) is connected to a \(12 \, V\) battery. Find the capacitance, charge stored, and energy.
▶️ Answer/Explanation
Step 1: Capacitance: \( \mathrm{C = \kappa \varepsilon_0 \dfrac{A}{d} = 4 (8.85 \times 10^{-12}) \dfrac{0.02}{1.0 \times 10^{-3}}} \) \( \mathrm{C \approx 7.1 \times 10^{-10} \, F} \)
Step 2: Charge stored: \( \mathrm{Q = C V = (7.1 \times 10^{-10})(12)} \approx 8.5 \times 10^{-9} \, C \)
Step 3: Energy stored: \( \mathrm{U = \tfrac{1}{2} C V^2 = 0.5 (7.1 \times 10^{-10})(144)} \approx 5.1 \times 10^{-8} \, J \)
Final Answer: \( C \approx 7.1 \times 10^{-10} \, F \), \( Q \approx 8.5 \times 10^{-9} \, C \), \( U \approx 5.1 \times 10^{-8} \, J \).
Example :
A parallel-plate capacitor with capacitance \(2.0 \, \mu F\) is charged to \(V = 50 \, V\). It is then disconnected from the battery. Find the charge on the plates, the stored energy, and the electric field if plate separation is \(2.5 \, mm\).
▶️ Answer/Explanation
Step 1: Charge: \( \mathrm{Q = C V = (2.0 \times 10^{-6})(50) = 1.0 \times 10^{-4} \, C} \)
Step 2: Energy: \( \mathrm{U = \tfrac{1}{2} C V^2 = 0.5 (2.0 \times 10^{-6})(2500)} = 2.5 \times 10^{-3} \, J \)
Step 3: Electric field: \( \mathrm{E = \dfrac{V}{d} = \dfrac{50}{2.5 \times 10^{-3}} = 2.0 \times 10^4 \, N/C} \)
Final Answer: \( Q = 1.0 \times 10^{-4} \, C \), \( U = 2.5 \times 10^{-3} \, J \), \( E = 2.0 \times 10^4 \, N/C \).