With crossing heat sources, a temperature rise of $\Delta\theta_{0x}$ applies at the hottest point.
| $\theta_{c}-T_{1} \left(W_{c}+\frac{W_{d}}{2}\right)-n_{ph} T_{2} \left(W_{c} \left(1+\lambda_{1}\right)+W_{d}\right)-n_{ph} T_{3} \left(W_{I}+W_{d}\right)$ | cables |
| $\theta_{hsf}-W_{hs} T_{hs}$ | heat sources |
| $\theta_{a}+\Delta \theta_{s}$ | PAC/GIL in air |
| $\theta_{a}+v_{4} \Delta \theta_{p}+\left(1-v_{4}\right) \Delta \theta_{x}+W_{tot} v_{4} T_{4\mu}$ | PAC/GIL buried without duct |
| $\theta_{di}+T_{4i} n_{cc} W_{tot}$ | PAC/GIL with duct |
| $\theta_{at}+\Delta \theta_{s}$ | PAC/GIL in trough in air |
| $\theta_{t}+T_{4iii} W_{tot}$ | PAC/GIL in channel (Heinhold) |
| $\delta \theta_{c,t}-T_{1} W_{c}-n_{ph} T_{2} W_{c} \left(1+\lambda_{1}\right)-n_{ph} T_{3} W_{I}$ | transient (approximation) CIGRE WG B1.72 |