Electrostatics – Stage 1

Chapter 1: Electric Charges & Fields – Page 8


1. Strategy for Applying Gauss’s Law

  1. Identify symmetry of charge distribution
  2. Choose correct Gaussian surface
  3. Find electric flux Φ = ∮𝐄·d𝐀
  4. Use Φ = Qenclosed/ε₀

Golden Rule: Choose Gaussian surface where E is constant or zero.


2. Spherical Charge Distribution

(a) Point Charge at Center

Gaussian Surface: Sphere of radius r

E · 4πr² = q / ε₀

E = (1 / 4πε₀) · (q / r²)

✔ Same as Coulomb’s law ✔ Field radial and symmetric


(b) Uniformly Charged Solid Sphere (Radius R)

Case 1: Outside Sphere (r ≥ R)

E = (1 / 4πε₀) · (Q / r²)

Entire charge acts as if concentrated at center.

Case 2: Inside Sphere (r < R)

Enclosed charge:

Qenc = Q · (r³ / R³)

E = (1 / 4πε₀) · (Q r / R³)

Important: Inside a solid sphere, E ∝ r


3. Infinite Line Charge (Linear Charge Density λ)

Gaussian Surface: Cylindrical surface (radius r, length L)

Flux = E · (2πrL)

Qenc = λL

E = λ / (2πε₀r)

  • E ∝ 1/r
  • Independent of length

4. Infinite Plane Sheet of Charge

Surface charge density = σ

Gaussian Surface: Pillbox

2EA = σA / ε₀

E = σ / (2ε₀)

Key Result: Electric field is independent of distance.


5. Conducting Sphere (Electrostatic Equilibrium)

  • Electric field inside conductor = 0
  • All charge resides on surface
  • Field just outside: E = σ/ε₀

JEE Favorite: Inside any conductor → E = 0


6. Comparison Table (Must Remember)

System E Dependence
Point charge 1 / r²
Infinite line 1 / r
Infinite plane Constant
Solid sphere (inside) ∝ r

Stage 1 – Page 8 Takeaway

  • Gauss law simplifies symmetric systems
  • Correct surface choice is crucial
  • Most JEE field questions come from this page

Next → Stage 1, Page 9: Electric Field due to Ring, Disc & Non-Uniform Systems

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