Parallel Plate Capacitor
Two parallel conducting plates with equal and opposite charge densities create a uniform electric field between them and zero field outside. This configuration is fundamental to capacitors and many electrostatic devices.
Setup
- Two large parallel conducting plates
- Plate separation $d$ (small compared to plate dimensions)
- Surface charge density $+\sigma$ on one plate, $-\sigma$ on the other
Electric Field Analysis
Each plate produces a field $E_{single} = \frac{\sigma}{2\varepsilon_0}$ (from Electric Field of Charged Plane).
Regions
Region A (outside, near positive plate):
- Field from $+\sigma$ plate: points right (away from positive)
- Field from $-\sigma$ plate: points left (toward negative)
- Result: $E_A = \frac{\sigma}{2\varepsilon_0} - \frac{\sigma}{2\varepsilon_0} = 0$
Region B (between plates):
- Field from $+\sigma$ plate: points right
- Field from $-\sigma$ plate: points right (toward negative plate)
- Result: $E_B = \frac{\sigma}{2\varepsilon_0} + \frac{\sigma}{2\varepsilon_0} = \frac{\sigma}{\varepsilon_0}$
Region C (outside, near negative plate):
- Field from $+\sigma$ plate: points right
- Field from $-\sigma$ plate: points left
- Result: $E_C = \frac{\sigma}{2\varepsilon_0} - \frac{\sigma}{2\varepsilon_0} = 0$
Final Result
| Region | Electric Field |
|---|---|
| Between plates | $E = \frac{\sigma}{\varepsilon_0}$ |
| Outside plates | $E = 0$ |
Key Properties
- Uniform field between plates (constant magnitude and direction)
- Zero field outside (fields cancel)
- Field points from positive plate to negative plate
- Field strength proportional to charge density
Alternative Forms
Using $Q = \sigma A$ (total charge on plate of area $A$):
$$E = \frac{Q}{\varepsilon_0 A}$$
Or in terms of voltage $V$ and plate separation $d$:
$$E = \frac{V}{d}$$
Example Calculation
Problem: Two parallel plates with area $A = 100$ cm² = $10^{-2}$ m² produce $E = 7.20 \times 10^3$ N/C between them. Find the charge on each plate.
Solution: $$E = \frac{\sigma}{\varepsilon_0} = \frac{Q}{\varepsilon_0 A}$$
$$Q = \varepsilon_0 A E = (8.85 \times 10^{-12})(10^{-2})(7.20 \times 10^3)$$
$$Q = 6.37 \times 10^{-10} \text{ C} = 0.637 \text{ nC}$$
Applications
- Capacitors — Store electrical energy
- Deflection plates — In oscilloscopes, particle accelerators
- Uniform field region — For experiments requiring constant $E$
- Electrostatic precipitators — Remove particles from air
Related
- Concept: Electric Field of Charged Plane
- Concept: Gauss's Law
- Concept: Capacitance
- FAD1022 L4 — Electric Flux and Gauss Law
- FAD1022 L5 — Electric Flux and Gauss Law (continued)