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JEE · NEET Physics

Class 12 · Chapter 2

Electrostatic Potential & Capacitance

Overview, notes, short notes, formula sheet, daily practice problems, previous year questions, and videos for this chapter — all in one place.

Electrostatic Potential & Capacitance Formula Sheet

8 formulas across 3 topics in Electrostatic Potential & Capacitance.

1 min read

Updated 2026-07-05 · v1.0.0

Electric Potential & Potential Energy

Potential is potential energy per unit charge, with zero at infinity. Unlike field, it is a scalar — add potentials with signs, no vectors.

V = (1/4πε₀) q/r

Potential due to a point charge

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Variables used in this formula, with units and dimensions
SymbolMeaningUnitDimension
Velectric potentialV (= J/C)[ML²T⁻³A⁻¹]
qsource charge (with sign)C[AT]
rdistance from the chargem[L]

Valid when

  • Scalar: total potential is the algebraic sum over all charges
  • Zero reference at infinity

Common mistakes

  • Potential can be zero where the FIELD is non-zero (midpoint of a dipole) and vice versa (inside a charged conductor)

E = −dV/dr; V(B) − V(A) = −∫ E·dl

Field–potential relationship

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Variables used in this formula, with units and dimensions
SymbolMeaningUnitDimension
Eelectric fieldV/m[MLT⁻³A⁻¹]
dV/drpotential gradientV/m[MLT⁻³A⁻¹]

Valid when

  • Field points from HIGH to LOW potential — down the gradient
  • Field is always perpendicular to equipotential surfaces

Common mistakes

  • Uniform field between plates: V = Ed, so E = V/d — a much-used shortcut

U = (1/4πε₀) q₁q₂/r (pair); sum over all pairs for a system

Potential energy of a system of charges

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Variables used in this formula, with units and dimensions
SymbolMeaningUnitDimension
Uelectrostatic potential energyJ[ML²T⁻²]
rseparation of a charge pairm[L]

Valid when

  • Add over every DISTINCT pair — three charges give three pairs
  • Sign matters: unlike charges give negative U

Common mistakes

  • Work done by an EXTERNAL agent to assemble the system equals U (with slow, kinetic-energy-free assembly)

Worth remembering

  • Every point of a conductor (surface and interior) is at the SAME potential — a conductor is an equipotential volume
  • A charge moving along an equipotential surface requires zero work

Capacitance & Capacitor Combinations

A capacitor stores charge at a cost of potential; C = Q/V depends only on geometry and the dielectric. Series and parallel are the reverse of resistors.

C = ε₀A/d; with dielectric C = Kε₀A/d

Parallel plate capacitance

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Variables used in this formula, with units and dimensions
SymbolMeaningUnitDimension
CcapacitanceF[M⁻¹L⁻²T⁴A²]
Aplate area[L²]
dplate separationm[L]
Kdielectric constant of the mediumdimensionless[M⁰L⁰T⁰]

Valid when

  • Depends only on geometry and dielectric, NOT on charge or voltage

Common mistakes

  • Isolated sphere is also a capacitor: C = 4πε₀R

Series: 1/C(eq) = Σ 1/Cᵢ; Parallel: C(eq) = Σ Cᵢ

Capacitors in series and parallel

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Variables used in this formula, with units and dimensions
SymbolMeaningUnitDimension
C(eq)equivalent capacitanceF[M⁻¹L⁻²T⁴A²]

Valid when

  • OPPOSITE of resistors: capacitors ADD in parallel, combine reciprocally in series
  • Series: every capacitor holds the SAME charge; Parallel: same VOLTAGE

Common mistakes

  • In series the smallest capacitor dominates C(eq) and takes the largest share of voltage

With battery connected: Q → KQ, V same; Disconnected: V → V/K, Q same

Effect of inserting a dielectric

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Variables used in this formula, with units and dimensions
SymbolMeaningUnitDimension
Kdielectric constantdimensionless[M⁰L⁰T⁰]

Valid when

  • Capacitance always increases by K
  • Battery CONNECTED (V fixed): charge and energy rise; DISCONNECTED (Q fixed): voltage, field and energy fall

Common mistakes

  • Track WHICH quantity is held constant — the whole answer flips depending on whether the battery stays connected

Worth remembering

  • A dielectric slab of thickness t in a gap d: C = ε₀A/(d − t + t/K) — reduces the effective gap

Energy Stored in a Capacitor

Charging a capacitor stores energy in the field between the plates — half of what the battery supplies; the other half is lost as heat.

U = ½ CV² = ½ QV = Q²/2C

Energy stored in a capacitor

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Integrating dW = (q/C)dq as charge builds from 0 to Q

Variables used in this formula, with units and dimensions
SymbolMeaningUnitDimension
Uenergy storedJ[ML²T⁻²]
QchargeC[AT]
Vvoltage across the capacitorV[ML²T⁻³A⁻¹]

Valid when

  • Energy density in the field: u = ½ε₀E²

Common mistakes

  • The battery supplies QV; only ½QV is stored, the other ½QV is dissipated as heat while charging — independent of the resistance

V = (C₁V₁ + C₂V₂)/(C₁ + C₂); heat lost = ½ C₁C₂(V₁ − V₂)²/(C₁ + C₂)

Sharing charge between two capacitors

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Charge conservation on connecting the plates

Variables used in this formula, with units and dimensions
SymbolMeaningUnitDimension
Vcommon potential after connectionV[ML²T⁻³A⁻¹]

Valid when

  • Energy is ALWAYS lost (as heat/radiation) when two capacitors at different potentials are joined

Common mistakes

  • The energy-loss formula mirrors the inelastic-collision energy loss — same reduced-quantity structure

Worth remembering

  • Force between capacitor plates F = Q²/2ε₀A = ½ε₀E²A — always attractive

NEET focuses on C combinations, dielectric shifts and energy; JEE Advanced adds partial dielectrics, force on plates, and multi-capacitor charge-sharing networks.

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