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Fig. 1.17 shows the effect of array tilting on the daily solar energy incidence for a
                     location at latitude 23.5°N with a clear sky. Meinel and Meinel (1976, p. 108)
                     tabulate the theoretical, clear sky daily energy interception for a range of fixed and
                     tracking orientations at two representative latitudes for summer and winter solstices
                     and the equinoxes.
































                            Figure 1.17. The effect of array tilting on the total insolation received each day for
                            a location at latitude 23.4°N (Used with permission of McGraw-Hill Companies,
                            Hu, C. & White, R.M. (1983), Solar Cells: From Basic to Advanced Systems,
                            McGraw-Hill, New York.).

                     Tilt towards equator

                     Lorenzo (2003) outlines the general method for converting monthly average daily
                     radiation on the horizontal to monthly average daily radiation on an arbitrarily tilted
                     surface. It requires estimation of hourly horizontal global, direct and diffuse
                     components, their transposition to the tilted surface, and integration over a day. This
                     procedure is computationally intensive and is done by some available PV system
                     sizing computer programs.
                     However, as noted by Duffie and Beckman (1991, Section 2.19), a method has been
                     devised by Liu and Jordan (1962) and extended by Klein (1977) for the special case
                     of a flat surface tilted towards the horizon, for which a simple approximation may be
                     used; that is

                                             §   R d  ·   1   cos  ȕ  1   cos  ȕ
                                             ¨
                                    R( ȕ)    R 1    ¸     R          R       ȡ    (1.23)
                                            b ¨     ¸   d
                                             ©    R  ¹       2           2




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