A heat source is defined as having a positive heat dissipation, whereas a heat sink is defined by a negative value.
*** These formulae are valid when the outer temperature defines the load.
| $\frac{\theta_{e}-\theta_{a}-v_{4} \Delta \theta_{p}+\left(v_{4}-1\right) \Delta \theta_{x}}{T_{4\mu} v_{4}}$ | heat sources buried |
| $\frac{\theta_{e} \left(T_{sa}+T_{st}\right)-\theta_{t} T_{sa}-\theta_{at} T_{st}}{T_{st} T_{sa}}$ | heat sources in ventilated tunnel |
| $\frac{\theta_{e}-\theta_{t}}{T_{4iii}}$ | heat sources in channel (Heinhold) |
| $\frac{\theta_{e}-\theta_{at}}{T_{4iii}}$ | heat sources in trough |
| $\frac{\theta_{e}-\theta_{a}-v_{4} \Delta \theta_{p}+\left(v_{4}-1\right) \Delta \theta_{x}}{\left(T_{4iii}+T_{tr}\right) v_{4}}$ | heat sources in filled troughs |