Radiation heat transfer from conductor surface to inner wall of the GIL enclosure.

Symbol
$W_{\mathrm{rad_{\mathrm{ce}}}}$
Unit
W/m
Formulae
$D_{\mathrm{c}} K_{\mathrm{r}} n_{\mathrm{c}} \pi \sigma \left(\left(\theta_{\mathrm{c}} + 273\right)^{4} - \left(\theta_{\mathrm{encl}} + 273\right)^{4}\right)$Stefan–Boltzmann law
$D_{\mathrm{c}} h_{\mathrm{rad_{\mathrm{ce}}}} \pi \left(\theta_{\mathrm{c}} - \theta_{\mathrm{encl}}\right)$using heat transfer coefficient
Related
$D_{\mathrm{c}}$
$h_{\mathrm{rad_{\mathrm{ce}}}}$
$K_{\mathrm{r}}$
$n_{\mathrm{c}}$
$\sigma$
$\theta_{\mathrm{c}}$
$\theta_{\mathrm{encl}}$
Used in
$T_{\mathrm{rad_{\mathrm{ce}}}}$