“…where α = 100 µV K −1 , ρ = 10.0 µΩ m, and κ = 10.5 W m −1 K −1 are the Seebeck coefficient, the electrical resistivity, and thermal conductivity, respectively, of undoped CrSi 2 at 298 K taken from [15,41], A is the cross-section area of the leg, d the length of the leg, T h = 736 K the hot-side temperature; T c = 309 K the cold-side temperature, and ZT avg = 0.085 the figure of merit ZT of CrSi 2 at the average temperature T avg = 522 K. It should be noted that relations (5) to (8) were based on the constant properties model, i.e., no variation of the TE properties with the temperature, which was not rigorously the case for CrSi 2 [42]. However, in the present case, the low ∆T = 50 K made the variation of the properties negligible between the hot and cold sides and these relations were, thus, considered as acceptable models to predict V oc , R, and Q out .…”