Electric field of a point charge in uniform motion

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unscientific
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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?

2ih5bn4.png
 
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When instead, I assume the particle to be moving along z-axis it fixes everything!

and i use x=Rsinθcosø, y = Rsinθsinø, z = R cos ø

The end result turns out beautifully to be the one as described, in 3 dimensions:

2n9icmg.png



I suspect that since Polar coordinates is usually defined with θ as angle between R and z-axis and ø as angle in x-y plane, everything matches.