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Monday, April 6, 2026

Chapter: Electrostatics | CUET Level | PHYSICS

Electrostatics

1. Electric Charge

  • Electric charge is a fundamental property of matter that produces electric and magnetic effects.
  • There are two types: Positive (+) and Negative (−).
  • Like charges repel each other; unlike charges attract each other.
  • Quantization of Charge: q = ±ne, where n is an integer and e = 1.6 × 10⁻¹⁹ C (elementary charge).
  • Conservation of Charge: The total charge in an isolated system remains constant. Charge can neither be created nor destroyed.

2. Coulomb’s Law

The electrostatic force between two stationary point charges is given by:

F=14πϵ0q1q2r2=kq1q2r2F = \frac{1}{4\pi\epsilon_0} \frac{q_1 q_2}{r^2} = k \frac{q_1 q_2}{r^2}
  • k = 9 × 10⁹ N m² C⁻² (in vacuum).
  • The force is attractive if charges are opposite and repulsive if they are similar.
  • In a medium: F = F₀ / εᵣ, where εᵣ is the relative permittivity (dielectric constant).

3. Electric Field

  • Electric field intensity (E) at a point is the force experienced by a unit positive test charge placed at that point: E = F / q₀
  • Electric field due to a point charge q at distance r:
E=14πϵ0qr2r^E = \frac{1}{4\pi\epsilon_0} \frac{q}{r^2} \hat{r}
  • Principle of Superposition: The total electric field is the vector sum of the fields due to individual charges.
  • Electric Field Lines: Emerge from positive charges and terminate on negative charges. Parallel lines indicate uniform field.

4. Electric Flux and Gauss’s Law

  • Electric flux: Φ = E ⋅ A (for plane surface) or Φ = ∫ E ⋅ dA.
  • Gauss’s Law: The total electric flux through any closed surface is equal to (1/ε₀) times the total charge enclosed by the surface.
EdA=Qenclosedϵ0\oint \mathbf{E} \cdot d\mathbf{A} = \frac{Q_{\text{enclosed}}}{\epsilon_0}
  • Very useful for calculating electric field in cases of symmetric charge distributions (spherical, cylindrical, or plane symmetry).

5. Electric Potential

  • Electric potential (V) at a point is the work done in bringing a unit positive charge from infinity to that point.
  • Electric potential due to a point charge q at distance r:
V=14πϵ0qrV = \frac{1}{4\pi\epsilon_0} \frac{q}{r}
  • Potential is a scalar quantity. SI unit is Volt (V).
  • Electrostatic Potential Energy: U = qV For two charges: U = (1/(4πε₀)) (q₁q₂ / r)
  • Relation between field and potential: E = – dV/dr (Electric field is the negative gradient of potential).

6. Electric Dipole

  • An electric dipole consists of two equal and opposite charges separated by a small distance (2a).
  • Dipole moment p = q × 2a (direction from negative to positive charge).
  • Electric field due to dipole:
    • On axial line: E = (1/(4πε₀)) (2p / r³)
    • On equatorial line: E = (1/(4πε₀)) (p / r³)
  • Torque on a dipole in uniform electric field: τ = p × E

7. Properties of Conductors in Electrostatics

  • Inside a conductor (in electrostatic equilibrium), E = 0.
  • Electric field just outside the surface is perpendicular to the surface.
  • Excess charge resides only on the outer surface of the conductor.
  • The entire conductor is at the same potential (equipotential surface).

8. Important Formula Summary

  • Coulomb’s Law: F=kq1q2r2 F = k \frac{q_1 q_2}{r^2}
  • Electric Field (point charge): E=kqr2 E = k \frac{q}{r^2}
  • Electric Potential (point charge): V=kqr V = k \frac{q}{r}
  • Gauss’s Law: Φ=Qϵ0 \Phi = \frac{Q}{\epsilon_0}
  • Capacitance of parallel plate capacitor: C=ϵ0Ad C = \frac{\epsilon_0 A}{d} (With dielectric: C' = κC)

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