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