Introduction to Electrodynamics
Introduction to Electrodynamics
4th Edition
ISBN: 9781108420419
Author: David J. Griffiths
Publisher: Cambridge University Press
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Chapter 2.3, Problem 2.20P

One of these is an impossible electrostatic field. Which one?
(a) E = k [ x y x ^ +2 y z y ^ + 3 x z z ^ ] ;
(b) E = k [ y 2 x ^ + ( 2 x y + z 2 ) y ^ + 2 y z z ^ ] .
Here k is a constant with the appropriate units. For the possible one, find the potential, using the origin as your reference point. Check your answer by computing V . [Hint: You must select a specific path to integrate along. It doesn’t matter what pathyou choose, since the answer is path-independent, but you simply cannot integrateunless you have a definite path in mind.]

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A particle with an electrostatic poten- tial φ = x2y + xz moves in the direction A⃗ = 2ˆi − 2ˆj + kˆ. Then the rate of change of the particle at (−1,2,3) is Hint: the rate of change is same as the directional derivative.
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