Electrostatics – Stage 3
Electric Charges & Fields – Page 7
1. Electric Field due to a Uniformly Charged Ring
Consider a ring of radius R carrying total charge Q. Find electric field at a point on the axis at distance x from center.
- Radial components cancel by symmetry
- Only axial components add
Electric Field:
E = (1 / 4π ε₀) · (Q x) / (x² + R²)3/2
Special cases:
- x = 0 → E = 0 (center)
- x ≫ R → behaves like point charge
2. Electric Field due to a Uniformly Charged Disc
Disc of radius R, surface charge density σ.
Method: Divide disc into concentric rings and integrate.
Electric Field on Axis:
E = (σ / 2ε₀) · [1 − x / √(x² + R²)]
Limiting Cases:
- x = 0 → E = σ / (2ε₀)
- R → ∞ → behaves like infinite sheet
3. Electric Field due to Infinite Sheet (Revision)
E = σ / (2ε₀)
- Independent of distance
- Direction normal to sheet
4. Electric Field due to Thin Spherical Shell
Total charge Q, radius R.
(a) Outside the Shell (r ≥ R)
E = 1 / (4π ε₀) · Q / r²
(b) Inside the Shell (r < R)
E = 0
Key Result: Electric field inside hollow charged shell is zero.
5. Comparison: Ring vs Disc vs Shell
| Distribution | Field at Center |
|---|---|
| Ring | 0 |
| Disc | σ / (2ε₀) |
| Spherical Shell | 0 |
6. JEE Advanced Thinking Points
- Ring & disc → integration based problems
- Shell → Gauss law shortcut
- Disc → infinite sheet as limiting case
JEE Trap:
Do not apply Gauss law to ring or disc directly.
Stage 3 – Page 7 Completed ✅
Next → Stage 3 – Page 8 (Electric Dipole, Field & Torque)
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