a
Thermal resistance of spherical sheet of thicleness \(dr\) and radius \(r\) is

\({d} {R}=\frac{{dr}}{{K}\left(4 \pi {r}^{2}\right)}\)

\({R}=\int_{{r}_{1}}^{{r}_{2}} \frac{{dr}}{{K}\left(4 \pi {r}^{2}\right)}\)

\({R}=\frac{1}{4 \pi {K}}\left(\frac{1}{{r}_{1}}-\frac{1}{{r}_{2}}\right)=\frac{1}{4 \pi {K}}\left(\frac{{I}_{2}-{r}_{1}}{{r}_{1} {I}_{2}}\right)\)

Thermal current (i) \(=\frac{\theta_{2}-\theta_{1}}{R}\)

\({i} =\frac{4 \pi {Kr}_{1} {r}_{2}\left(\theta_{2}-\theta_{1}\right)}{{r}_{2}-{r}_{1}}\)