This work investigated, using a 3-D modelling, the influence of electrons losses on the performance of a polycrystalline silicon PV cell. The electrons transport equations have been solved by taking into account the rate of electrons lost at the junction (Sf0) to find the expression of the electrons’ density which allowed to derive the expressions of the electrical parameters (Jph, Vph, P) then those of the performance parameters (η, Rsh) of the PV cell grain. Then we analyzed, from a numerical simulation, the effects of the rate of electrons lost at the junction (Sf0) on the performance parameters (η, Rsh) found from the curves of output power (PT) -diffusion velocity (Sfj). Results of simulation showed that, in open circuit, there is a leakage current at the junction of the PV cell grain whose density increases from 0 mA.cm-2 à 58.80 mA.cm-2 resulting in a drastic drop in the shunt resistance from infinity to 4.273 Ω.cm 2 and a drop in the conversion efficiency of 34.376%. Considering the manufacturers’ standards, 20% drop in efficiency, so for Sf0 = 1,790×104 cm.s-1 the PV cell is degraded.

This work investigated, using a 3-D modelling, the influences of the magnitude and the inclination angle of an electromagnetic field (EMF) carried by AM radio waves on the current and the voltage of a polycrystalline silicon PV cell. The electrons transport equations were solved to find the density of electrons and then to derive the current density and the voltage. Through numerical simulation, the effects of both the magnitude and the inclination angle of the EMF on the density of electrons, the current density and the open circuit voltage were studied. Results of simulation showed that depending on the inclination angle (0 rad; π/2 rad and π rad), the EMF acts differently on the electrical parameters (Jsc and Voc). The analysis also showed that, regardless of the inclination angle of the EMF, there is an open circuit current (Joc) proportional to the magnitude of the EMF (inversely proportional to the distance). This current (Joc) is lost by Joule heating either at the junction (θ = 0 rad) or in the base (θ = π/2 rad and θ = π rad). Finally, the analysis showed that, for θ = π rad (reverse polarization of the PV cell), there is an operating domain (Sf ≤ Sfeq) in which the PV cell is blocked. And another operating domain (Sf > Sfeq) in which the PV cell is a current generator unlike a PN junction diode which remains blocked in reverse bias.