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1 - N u m e r i c a l   6

Problem

A hollow sphere is charged to 14 μC14 \, \mu \mathrm{C}. Find the potential:

(a) at its surface,
(b) inside the sphere, and
(c) at a distance of 0.2 m0.2 \, \mathrm{m} from the surface.

The radius of the sphere is 0.3 m0.3 \, \mathrm{m}.

Data

  • Charge: q=14 μC=14×10−6 Cq = 14 \, \mu \mathrm{C} = 14 \times 10^{-6} \, \mathrm{C}
  • Radius: r=0.3 mr = 0.3 \, \mathrm{m}
  • Distance from surface: d=0.2 md = 0.2 \, \mathrm{m}
  • Coulomb’s constant: k=9×109 Nm2C−2k = 9 \times 10^9 \, \mathrm{Nm^2C^{-2}}

Prerequisite Concepts

  • Potential at Surface:
Vsurface=kqr V_{\text{surface}} = k \frac{q}{r}
  • Potential Inside: Vinside=VsurfaceV_{\text{inside}} = V_{\text{surface}}
  • Potential at Distance:
V=kqr+d V = k \frac{q}{r + d}

Answer

Part (a): Potential at Surface

Vsurface=kqrV_{\text{surface}} = k \frac{q}{r}

Substitute values:

Vsurface=(9×109)(14×10−6)0.3V_{\text{surface}} = \frac{(9 \times 10^9)(14 \times 10^{-6})}{0.3} Vsurface=42×104 VV_{\text{surface}} = 42 \times 10^4 \, \mathrm{V} Vsurface=4.2×105 VV_{\text{surface}} = 4.2 \times 10^5 \, \mathrm{V}

Part (b): Potential Inside

The potential inside a hollow sphere is the same as that on the surface:

Vinside=Vsurface=4.2×105 VV_{\text{inside}} = V_{\text{surface}} = 4.2 \times 10^5 \, \mathrm{V}

Part (c): Potential at Distance 0.2 m0.2 \, \mathrm{m} from Surface

The total distance from the center is r+d=0.3+0.2=0.5 mr + d = 0.3 + 0.2 = 0.5 \, \mathrm{m}.

V=kqr+dV = k \frac{q}{r + d}

Substitute values:

V=(9×109)(14×10−6)0.5V = \frac{(9 \times 10^9)(14 \times 10^{-6})}{0.5} V=25.2×104 VV = 25.2 \times 10^4 \, \mathrm{V} V=2.52×105 VV = 2.52 \times 10^5 \, \mathrm{V}

Final Answer

  • (a) Potential at surface: 4.2×105 V4.2 \times 10^5 \, \mathrm{V}.
  • (b) Potential inside: 4.2×105 V4.2 \times 10^5 \, \mathrm{V}.
  • (c) Potential at 0.2 m0.2 \, \mathrm{m} from surface: 2.52×105 V2.52 \times 10^5 \, \mathrm{V}.