In this problem, you will find the capacitance per unit length of two
cylindrical conductors of radii \(R_{1}\) and \(R_{2}\) the distance between whose
centers is \(D\) by looking for two line charge densities \(+\lambda\) and
\(-\lambda\) such that the two cylinders are two of the equipotential surfaces.
From Problem \(10.10\), we have
$$R_{i}=\frac{a}{\sinh \left(u_{i} / 2 \lambda\right)}, \quad y_{i}=a
\operatorname{coth}\left(u_{i} / 2 \lambda\right), \quad i=1,2,$$
where \(y_{1}\) and \(y_{2}\) are the locations of the centers of the two
conductors on the \(y\) -axis (which we assume to connect the two centers).
(a) Show that \(D=\left|y_{1}-y_{2}\right|=\left|R_{1} \cosh \frac{u_{1}}{2
\lambda}-R_{2} \cosh \frac{u_{2}}{2 \lambda}\right|\).
(b) Square both sides and use \(\cosh (a-b)=\cosh a \cosh b-\sinh a \sinh b\)
and the expressions for the \(R\) 's and the \(y\) 's given above to obtain
$$\cosh \left(\frac{u_{1}-u_{2}}{2
\lambda}\right)=\left|\frac{R_{1}^{2}+R_{2}^{2}-D^{2}}{2 R_{1} R_{2}}\right|$$
(c) Now find the capacitance per unit length. Consider the special case of two
concentric cylinders.
(d) Find the capacitance per unit length of a cylinder and a plane, by letting
one of the radii, say \(R_{1}\), go to infinity while \(h \equiv R_{1}-D\) remains
fixed.