In Griffiths Chapter 12, pg 527:
Suppose a point charge is moving along x, we obtain the following E-fields:
Questions
1. Is the vector R solely in the x-y plane?
2. What happened to the coordinate 'z' ?
3. Why are they only doing things in the 2-D plane? Can we use rotational symmetry somewhere?
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Suppose a point charge is moving along x, we obtain the following E-fields:
Questions
1. Is the vector R solely in the x-y plane?
2. What happened to the coordinate 'z' ?
3. Why are they only doing things in the 2-D plane? Can we use rotational symmetry somewhere?
