Chapter 4
Chapter 4
Chapter 4
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When we move the supports together the charges are pulled together by the tension<br />
transmitted<br />
parallel to the electric field. We artificially terminate the field lines at a fixed<br />
distance<br />
from the charges to avoid visual confusion.<br />
4.7 Problem-Solving Strategies<br />
In this chapter, we have shown how electric field can be computed using Gauss’s law:<br />
qenc<br />
Φ E = ∫∫ E⋅ dA<br />
=<br />
ε<br />
S<br />
The procedures are outlined in Section 4.2. Below we summarize how the above<br />
procedures can be employed to compute the electric field for a line of charge, an infinite<br />
plane of charge and a uniformly charged solid sphere.<br />
0<br />
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