Electrostatic Potential and Capacitance — Physics Class 12 Notes (CBSE & HBSE)
Free NCERT Physics notes for Electrostatic Potential and Capacitance (Class 12) on Siksha Sarovar, aligned to CBSE and Haryana Board (HBSE). This chapter is broken into 3 topics with clear explanations, formulas, solved examples and board-pattern practice — free to read, no sign-up required.
Board exam focus — Electrostatic Potential and Capacitance (CBSE & HBSE)
CBSE emphasizes derivation of potential energy, capacitor combinations, effect of dielectrics, and energy density. HBSE focuses on definition of potential, capacitance formula, parallel plate capacitor, and basic numericals on charge and energy.
Electric Potential and Potential Difference
Electric Potential
The electric potential at a point in an electric field is defined as the work done per unit positive charge in bringing a test charge from infinity to that point:
V = W/q₀ = kQ/r
Unit: Volt (V) = J/C. Electric potential is a scalar quantity.
Potential Difference
The potential difference between two points A and B:
V_AB = V_A − V_B = W_AB/q₀
Work done in moving charge q from B to A = q(V_A − V_B)
Electric Potential due to a Point Charge
V = kQ/r = Q/(4πε₀r)
- V is positive for +Q, negative for −Q
- V = 0 at infinity
- V depends on r, not on test charge
Potential due to an Electric Dipole
V_axial = kp cosθ/r² (general formula)
- Axial point (θ=0): V = kp/r²
- Equatorial point (θ=90°): V = 0
Potential due to System of Charges (Superposition)
V = kΣ(qᵢ/rᵢ) — algebraic sum (scalar addition)
Relation between E and V
E = −dV/dr (in 1D)
E⃗ = −∇V (general 3D)
- E points in direction of decreasing potential
- For uniform field: E = −ΔV/Δr = V/d
Equipotential Surfaces
Surfaces on which electric potential is the same everywhere.
| Shape of Charge | Equipotential Surface Shape |
|---|---|
| Point charge | Concentric spheres |
| Uniform field | Parallel planes ⊥ to E |
| Electric dipole | Complex closed curves |
Properties of Equipotential Surfaces:
- No work done in moving charge along equipotential
- E⃗ is always ⊥ to equipotential surface
- Equipotential surfaces never intersect
- Closer surfaces → stronger field
Electric Potential Energy
PE of two-charge system: U = kq₁q₂/r PE of dipole in field: U = −pE cosθ = −p⃗·E⃗
Work-Energy Theorem for Charges
W_ext = q(V_B − V_A) = ΔPE
Diagram Indicator: [Graph of V vs r for point charge showing V=kQ/r hyperbola; also diagram of equipotential circles around a point charge with E-field lines perpendicular to them.]
Capacitors and Capacitance
Capacitor
A capacitor is a system of two conductors separated by an insulating medium (dielectric), capable of storing electric charge and energy.
Capacitance
Capacitance is defined as the ratio of charge stored to potential difference across the capacitor:
C = Q/V
Unit: Farad (F). 1 F = 1 C/V. Common units: μF, nF, pF.
Parallel Plate Capacitor
Two large parallel plates each of area A, separated by distance d:
C = ε₀A/d (in vacuum/air) C = Kε₀A/d = ε₀εᵣA/d (with dielectric K)
Electric field between plates: E = σ/ε₀ = Q/(ε₀A) = V/d
Spherical Capacitor
Inner sphere radius a, outer sphere radius b: C = 4πε₀ab/(b−a)
For isolated sphere (b → ∞): C = 4πε₀R
Cylindrical Capacitor
Inner cylinder radius a, outer radius b, length L: C = 2πε₀L/ln(b/a)
Capacitors in Combination
Series Combination:
- 1/C_eq = 1/C₁ + 1/C₂ + 1/C₃
- Same charge Q on each capacitor
- V = V₁ + V₂ + V₃
- C_eq < smallest individual C
Parallel Combination:
- C_eq = C₁ + C₂ + C₃
- Same voltage V across each capacitor
- Q = Q₁ + Q₂ + Q₃
- C_eq > largest individual C
Comparison: Series vs Parallel
| Property | Series | Parallel |
|---|---|---|
| Charge | Same on all | Different (Q = CV) |
| Voltage | Different (V = Q/C) | Same on all |
| Equivalent C | Less than smallest | More than largest |
| Formula | 1/C_eq = Σ(1/Cᵢ) | C_eq = ΣCᵢ |
Effect of Dielectric on Capacitance
When a dielectric (K > 1) is inserted between plates:
- C increases: C_new = KC₀
- If connected to battery: Q increases, V unchanged
- If isolated: V decreases, Q unchanged, E decreases
Dielectric Polarization
- External field aligns dipoles in dielectric
- Creates opposing field E_induced
- Net field E = E₀/K (reduced)
- Dielectric constant K = E₀/E ≥ 1
Diagram Indicator: [Parallel plate capacitor with plates labeled +Q and -Q, field lines E between plates, dielectric slab inserted, and arrows showing induced dipoles opposing the field.]
Energy Stored in Capacitors and Dielectrics
Energy Stored in a Capacitor
Work done in charging a capacitor = energy stored in the electric field:
U = Q²/(2C) = ½CV² = QV/2
All three forms are equivalent and useful depending on known quantities.
Derivation
When charge dq is added to a capacitor at potential V = q/C: dW = V·dq = (q/C)dq
Total work: W = ∫₀ᴼ (q/C)dq = Q²/(2C) = ½CV²
Energy Density
Energy stored per unit volume in the electric field:
u = ½ε₀E² (in vacuum) u = ½Kε₀E² = ½εE² (in dielectric)
Total energy: U = u × Volume = ½ε₀E² × (A·d) = ½(ε₀A/d)V² = ½CV² ✓
Effect of Inserting Dielectric
Case 1: Battery connected (V = constant)
| Quantity | Before | After |
|---|---|---|
| Voltage V | V₀ | V₀ (same) |
| Capacitance C | C₀ | KC₀ |
| Charge Q | Q₀ = C₀V₀ | KQ₀ |
| Energy U | ½C₀V₀² | K×½C₀V₀² = KU₀ |
| E field | E₀ | E₀ (same) |
Energy increases — extra energy supplied by battery.
Case 2: Battery disconnected (Q = constant)
| Quantity | Before | After |
|---|---|---|
| Charge Q | Q₀ | Q₀ (same) |
| Capacitance C | C₀ | KC₀ |
| Voltage V | V₀ | V₀/K |
| Energy U | Q₀²/(2C₀) | Q₀²/(2KC₀) = U₀/K |
| E field | E₀ | E₀/K |
Energy decreases — energy released into mechanical work (pulling dielectric in).
Common Dielectric Materials
| Material | Dielectric Constant K |
|---|---|
| Vacuum | 1 (exactly) |
| Air | ~1.0006 |
| Paper | 3.5 |
| Glass | 5–10 |
| Water | 80 |
| Mica | 5–8 |
| Barium Titanate | ~1200 |
Capacitor Applications
- Energy storage (flash cameras, defibrillators)
- Filtering and smoothing in power supplies
- Timing circuits (RC oscillators)
- Memory storage (DRAM)
- Coupling in amplifiers
Diagram Indicator: [Energy vs charge graph for capacitor showing parabola U = Q²/2C; also comparison table diagram showing energy before/after dielectric insertion for both cases (battery connected vs disconnected).]
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Concept explanations, key formulas and definitions, fully solved examples and board-pattern practice questions for Electrostatic Potential and Capacitance.