The charge distribution described in Prob. 4.4.3 is now at infinity (a) Show that the potential…
The charge distribution described in Prob. 4.4.3 is now at infinity
(a) Show that the potential in the neighborhood of the origin takes the form 2
2
. (b) How would you position the line charges so that in the limit where they moved to infinity, the potential would take the form of (4.1.18)?
The only charge is restricted to a square patch centered at the origin and lying in the plane, as shown in Fig. P4.5.1.
(a) Assume that the patch is very thin in the z direction compared to other dimensions of interest. Over its surface there is a given surface charge density s
. Express the potential
along the
axis for
in terms of a two-dimensional integral.
(b) For the particular surface charge distribution s
o|
y|
2 where
o and a are constants, determine
along the positive z axis.
(c) What is at the origin?
(d) Show that has a
dependence for
that is the same as for a point charge at the origin. In this limit, what is the equivalent point charge for the patch?
(e) What is along the positive
axis?
Fig. P4.5.1