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38     CHAPTER 1 Solar Cells and Arrays: Principles, Analysis, and Design




                            This relationship is the required IeV of the module. It has the form of a
                         single solar cell, with the current multiplied by n s , the number of strings, and the
                         cell voltage is multiplied by n e , the number of cells in the string. Because the power
                         output ¼ IV, the power output of a single cell will be multiplied by (n e n s ).
                            Solar cells with the same type are not identical because of fabrication toler-
                         ances. Basically, the produced solar cells from a production line must be sorted
                         to select the matched cells. Matched cells have very high tolerances. On the other
                         hand, if the solar cells are not matched, the string short circuit current will be the
                         smallest short cell current, and the module output voltage under open circuit con-
                         dition will be equal to the smallest open circuit voltage of the strings connected in
                         parallel and the curve factor of the overall module becomes smaller because of the
                         larger internal losses in the module. Hence, cell mismatch leads to additional in-
                         ternal losses and reduces the efficiency of the array in comparison to that of the
                         single cells [29].


                         5.2 THE IeV CHARACTERISTICS OF MISMATCHED CELLS IN THE
                             MODULE

                         Now each cell i has its own parameters, I sci , V oci , FF i , n i , I si , I phi , and R si . For a string
                         current I st , the voltage developed on the ith cell can be expressed according to
                         Eq. (1.49) as

                                                       I ph   I st   I si
                                           V ci ¼ n i V T ln        þ I st R si        (1.54)
                                                            I si
                         The total string voltage is then

                                                           n e
                                                          X
                                                     V m ¼   V ci                      (1.55)
                                                           1
                         If n s unmatched strings are connected in parallel with the jth string, which is para-
                         metric, then

                                         V m1 ¼ V rn2 ¼ V m3. ¼ V mj. ¼ V mns ¼ V m    (1.56)
                         The string currents I st1 , I st2 , I st3 ., I stj , ., I sns are different. From Eqs. (1.54) and
                         (1.55), the jth string has the characteristics:
                                                        n e;j
                                                        X
                                                  V mj ¼   V ci ¼ V m                  (1.57)
                                                        i¼1
                            This equation can split into (n s  l) equations in I stj . One needs one additional
                         equation to determine I stj . This equation is the output node equation

                                                           n s
                                                          X
                                                     I m ¼   I stj                     (1.58)
                                                          i¼1
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