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

Symbol
$W_{rad_{ce}}$
Unit
W/m
Formulae
 $D_{c} K_{ce} n_{c} \pi \sigma \left(\left(\theta_{c} + 273\right)^{4} - \left(\theta_{encl} + 273\right)^{4}\right)$ Stefan–Boltzmann law $D_{c} h_{rad_{ce}} \pi \left(\theta_{c} - \theta_{encl}\right)$ using heat transfer coefficient
Related
$D_{c}$
$h_{rad_{ce}}$
$\sigma$
$\theta_{c}$
$\theta_{encl}$
Used in
$T_{1}$
$T_{rad_{ce}}$