The heat flow between two concentric cylinders of radii $r_{1}$ and $r$ at temperatures $T_{1}$ and $T$, respectively, is, from Eq. (2.14),
$$
\dot{Q}=\frac{2 \pi k L\left(T_{1}-T\right)}{\ln \left(r / r_{1}\right)} \quad \text { or } \quad T=T_{1}-\frac{\dot{Q}}{2 \pi k L} \ln \frac{r}{r_{1}}
$$
which can be interpreted as the temperature due to a line source of strength $\dot{Q}$ at $r=0$, expressed in terms of the temperature $T_{1}$ at a reference radius $r_{1}$. Derive the shape factor $S$ given by item 8 of Table $3.2$ by superimposing the temperature fields of a line source $Q$ below the ground and a line $\sin \mathrm{k}-\underline{Q}$ above the ground, in a mirror image position as shown. Define an excess temperature $T-T_{2}$, where $T_{2}$ is the ground surface temperature, and show that the isotherms are concentric circles with origins at $x=0, y=a(1+c) /(1-c)$, and radii $2 c^{1 / 2} a /(1-c)$, where $c$ is a constant parameter. Also show that the ground surface is an isotherm.