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Chapter 8 • Photovoltaics: The Basics  165






















                 FIGURE 8.12  The influence of series resistance R s  on PV cell efficiency in dependence on irradiance.

                   Figs. 8.12 and 8.13 demonstrate that operating temperature is a very important param-
                 eter for the efficiency of PV energy conversion. In a linear approximation, the temperature
                 dependence of cell efficiency can be described by
                                              η T() =  η STC  + K T η T( STC  −T ),         (8.22)                                         η(T)=ηsTC+KTη(TsTC−T),

                 where η sTC  is the PV cell efficiency at sTC, K Tη  is the thermal coefficient of efficiency, and
                 T sTC  = 25°C. The thermal coefficient K Tη  depends on the material bandgap, as shown in
                 Fig. 8.14.
                   The PV cell equivalent circuit and the I–V characteristics have been discussed for the
                 case of a constant or slowly varying irradiance. For fast changes (e.g., using a flash simu-
                 lator), it is also necessary to take into account the Pn junction capacitance that can be
                 (under conditions of a forward biased junction) relatively large and that can influence the
                 measured I–V characteristic shape.


                 8.3.3  In-Series and In-Parallel Connection of PV Cells
                 The open-circuit voltage V oC  of individual cells is usually lower than 1.5 V and the photo-
                 generated current density is in order of tens of milliampere per square centimeter. solar
                 cells can be connected in series to obtain a higher output voltage or in parallel to obtain
                 higher output currents. The case of a series connected cell is demonstrated in Fig. 8.15A.
                 In this case, the same current flows through all solar cells. If the current generated in in-
                 dividual cells differs, the short-circuit current I sC  of the series connected cells will be the
                 minimum I sC  of all in-series connected cells and the voltage for currents I ≤ I sC  will be the
                 sum of voltages at individual cells at the current I, as indicated in Fig. 8.15B. The maximum
                 power current I mp  of a series connected cell will be limited by a cell with the minimum I sC
                 and, consequently, the output power of the series connected cells will be lower than the
                 sum of output power of individual cells. only in the case when the current I mp  of a series
                 connected cells is the same, will the output power be the sum of output power of indi-
                 vidual cells, as indicated in Fig. 8.15C.
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