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Question

A conductor has a surface charge density of \( 1 \times 10^{-6} \, \text{C/m}^2 \). What is the
electric field just outside it? (Take \( \varepsilon_0 = 8.85 \times 10^{-12} \, \text{C}^2
\text{N}^{-1} \text{m}^{-2} \)).

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Explanation

**Potential energy of two charges** U = k q₁ q₂/r, k=9×10⁹ N·m²/C², q₁,q₂ in coulombs, r separation (m), positive for like charges (repulsive, work needed to bring together), negative for opposite (attractive, work released). For 20 μC and -8 μC, 0.2 m apart, U=9×10⁹×20×10⁻⁶×(-8×10⁻⁶)/0.2= -7.2 J. E = (sigma/ε₀) = (1 × 10⁻⁶/8.85 × 10⁻¹²) ≈ 1.13 × 10⁵ N/C . Using V = kQ/r, U = k q₁q₂/r, E = -dV/dr, C = ε₀A/d, 1/C_eq series, C_eq = ΣC parallel, U = ½ C V² and common potential V = Q_total/C_total, result 1.13 × 10⁵ N/C follows, reflecting potential-capacitance relations.

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