Electrostatics: Common Mistakes and Fixes (9)

hard 3 min read

Question

A charge +Q+Q is placed at the centre of a hollow conducting sphere of inner radius aa and outer radius bb. Find the electric field at distances (i) r<ar < a, (ii) a<r<ba < r < b, (iii) r>br > b. State what charge sits on each surface.

Solution — Step by Step

Inside a conductor in electrostatic equilibrium, the field is zero. So inside the metal (a<r<ba < r < b), E=0E = 0. This is the strongest constraint.

Apply Gauss’s law to a sphere of radius rr with a<r<ba < r < b. Since E=0E = 0 inside the conductor, the enclosed charge must be zero. So the inner surface (at r=ar = a) carries induced charge Q-Q. By overall neutrality of the conductor, the outer surface (at r=br = b) carries +Q+Q.

Gauss’s law on a sphere of radius r<ar < a encloses only +Q+Q:

E=14πϵ0Qr2(radially outward)E = \frac{1}{4\pi\epsilon_0}\frac{Q}{r^2}\quad\text{(radially outward)}

Gauss’s law on a sphere of radius r>br > b encloses +Q+Q (centre) Q-Q (inner) +Q+Q (outer) =+Q= +Q:

E=14πϵ0Qr2(radially outward)E = \frac{1}{4\pi\epsilon_0}\frac{Q}{r^2}\quad\text{(radially outward)}

Final answer: E=kQr2E = \dfrac{kQ}{r^2} for r<ar<a and r>br>b; E=0E = 0 for a<r<ba<r<b. Inner surface: Q-Q, outer surface: +Q+Q.

Why This Works

A conductor cannot tolerate a non-zero field inside it — free charges would migrate until the field cancels. This redistribution creates exactly the right surface charges to cancel the field of the enclosed charge within the metal. The outer surface, however, “knows” only that the conductor as a whole is neutral and that some charge is sealed inside; it spreads +Q+Q uniformly over itself, and the field outside looks identical to a point charge QQ at the centre.

This is a JEE Advanced staple. The cleanest way to see it: Einside metal=0E_{\text{inside metal}} = 0 forces the induced charges by Gauss’s law alone.

Alternative Method

Use superposition. The field at a point is the sum of contributions from the central +Q+Q plus the induced surface charges. By symmetry, induced charges arrange uniformly. Solve for them by demanding E=0E = 0 inside the metal — same answer, more algebra.

A frequent error: students think the inner surface gets +Q+Q and the outer Q-Q. The induced charge on the facing surface is always opposite to the source charge. Picture field lines starting on +Q+Q and ending on the inner wall — those endpoints are negative.

Common Mistake

If we now ground the outer surface, the +Q+Q on the outside drains away to earth and the field outside becomes zero. Don’t forget grounding kills only what’s electrically connected to the ground; the inner Q-Q stays put.

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