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Q.Using Gauss theorem derive an expression for electric field intensity due to uniformly charged hollow sphere (shell) at a point outside the shell and at a point inside the shell. OR Derive an expression for capacitance of parallel plate capacitor with a dielectric slab between the plates.

Punjab PsebPSEB Punjab Class 12 Board 2025Subjective· 5mImportance★★★★★
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Applying Gauss's law with a spherical Gaussian surface: outside the shell the field behaves exactly as if all the charge were concentrated at the centre (E∝1/r2E \propto 1/r^2); inside the (empty) shell, the enclosed charge is zero, so E=0E = 0 everywhere inside.

Consider a thin hollow spherical shell of radius RR, carrying a total charge QQ uniformly distributed over its surface. By symmetry, the electric field at any point due to the shell must be radial and must have the same magnitude at all points equidistant from the centre. This symmetry lets us use a concentric spherical Gaussian surface of radius rr through the point where we want the field, and apply Gauss's law:

∮E⃗⋅dA⃗=qenclosedε0\oint \vec{E}\cdot d\vec{A} = \frac{q_{enclosed}}{\varepsilon_0}

Since E⃗\vec{E} is radial and constant in magnitude over the Gaussian sphere, and dA⃗d\vec{A} is also radial, E⃗⋅dA⃗=E dA\vec{E}\cdot d\vec{A} = E\,dA, so the left side becomes E×4πr2E \times 4\pi r^2 (the surface area of the Gaussian sphere).

(a) Point outside the shell (r>Rr > R): The Gaussian sphere of radius rr encloses the entire charge QQ of the shell, so qenclosed=Qq_{enclosed} = Q. Gauss's law gives

E(4πr2)=Qε0  ⟹  E=14πε0Qr2E(4\pi r^2) = \frac{Q}{\varepsilon_0} \implies E = \frac{1}{4\pi\varepsilon_0}\frac{Q}{r^2}

This is identical to the field of a point charge QQ placed at the centre — i.e., a uniformly charged shell behaves, from outside, exactly like a point charge at its centre. …

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