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4.2 STATE VALUES OF HUMID AIR; MOLLIER DIAGRAMS AND THEIR APPLICATIONS     85
                       has to be iterated because steam pressure p h and therefore humidity x are at
                       this stage unknown. When humidity is low, as in this example, an approxima-
                       tion is pCp^piCpi. The calculation can be repeated when needed using the
                       steam pressure from Eq. (4.117). In this example, we don't do that. For calcu-
                       lating the density and heat capacity, we will use an approximation p cp - p,, so
                       p = p, and cp = Cpi. From this approximation it follows that



                       whose value is




                          From Eq. (4.76) we get the partial pressure of dry air:








                       The Lewis number in cases a and b is as follows:




                       It is assumed that n = 0.5, so Le  = Le  = 1.073




                                   n
                          Thus Le    — 1.017. Substituting all values into Eq. (4.117), we obtain
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