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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 />

29

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