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Chapter 4

Chapter 4

Chapter 4

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Note again the discontinuity in electric field as we cross the plane:<br />

Example 4.3: Spherical Shell<br />

σ ⎛ σ ⎞ σ<br />

∆ Ez = Ez+ − Ez−<br />

= −⎜− ⎟=<br />

2ε0 ⎝ 2ε0<br />

⎠ ε0<br />

(4.2.21)<br />

A thin spherical shell of radius a has a charge + Q evenly distributed over its surface.<br />

Find<br />

the electric field both inside and outside the shell.<br />

Solutions:<br />

The charge distribution is spherically symmetric, with a surface charge density<br />

2<br />

2<br />

σ = Q/ As= Q/4πa , where As = 4π<br />

a is the surface area of the sphere. The electric field<br />

E must be radially symmetric and directed outward (Figure 4.2.12). We treat the regions<br />

and separately.<br />

<br />

r ≤ a r ≥ a<br />

Case 1:<br />

r ≤ a<br />

Figure 4.2.12 Electric field for uniform spherical shell of charge<br />

We choose our Gaussian surface to be a sphere of radius<br />

4.2.13(a).<br />

(a)<br />

r ≤ a,<br />

as shown in Figure<br />

Figure 4.2.13 Gaussian surface for uniformly charged<br />

spherical shell for (a) r< a,<br />

and<br />

(b ) r ≥ a<br />

(b)<br />

11

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