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V    I  R    K ĭ N              (12.2)
                                                        m   m  a
                                 The electromagnetic torque (IJ e ) developed by such a motor is proportional to
                                 the armature current (and hence I m ) and also the flux density ĭ (which is a
                                 constant). This gives us
                                                          IJ    K  ĭ c  I               (12.3)
                                                           e      m
                                 where K' is a constant related to the physical dimensions of the motor and the
                                 number of windings in the armature (Hambley, 2002).
                                 When the motor drives a load (such as a water pump), the speed of the motor
                                 will continue to alter until steady state is reached; that is, when

                                                            IJ    IJ l                   (12.4)
                                                             e
                                 where IJ l  is the torque required to drive the load at that particular speed.
                                 For any commercial pump, the torque versus speed (IJ l versus N)
                                 characteristics should be available from the supplier. For each value of N, IJ l  is
                                 thus obtainable and, using Eqns. (12.3) and (12.4), I m can be calculated.
                                 Subsequent use of I m and N in Eqn. (12.2) gives the corresponding value of
                                 V m . Therefore, for each N of the pump, the motor voltage and current required
                                 from the solar panels are determined. However, the actual voltage generated
                                 by the solar panels needs to be about 2% higher than that calculated, to allow
                                 for resistive losses in the wiring.
                              7. Appropriate sizing of the photovoltaic system will enable overall system
                                 specifications to be met, while simultaneously maximising overall system
                                 efficiency. For this, both the voltage and current at maximum power point
                                 need to be optimised. Unfortunately, little choice exists with regard to the
                                 voltages available with standard commercial modules. They are normally
                                 designed for 12 V systems (including considerable excess voltage capacity to
                                 allow for battery charging, regulation, blocking diode etc.), and can be
                                 connected in series to increase system voltage to multiples of 12 V. This
                                 restriction can be overcome by the use of a DC-to-DC converter. In
                                 comparison, a reasonable choice in short circuit currents exists, owing to the
                                 range of solar cell sizes and technologies used by different manufacturers. An
                                 approach for optimising the photovoltaic configuration by matching the
                                 requirements of the water pumping subsystem to the output of the
                                 photovoltaics is provided in Appendix H.



                                                     REFE RE NCES
                          Updated World Wide Web links can be found at www.pv.unsw.edu.au/apv_book_refs.

                          Arab, A. H., Chenlo, F. & Benghanem, M. (2004), ‘Loss-of-load probability of
                          photovoltaic water pumping systems’, Solar Energy, 76(6), pp. 713–723.








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