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8 γ57 −0Θ7 β=7DQ 027 L = β − β′ 0Θ7 = 0Θ − (3.8) (3.9) (3.10) 07 = 027 + 0Θ7 Once Mr1 has been determined, the program will use the compressible flow relations to solve for Ptr1 and Ttr1. In addition, with knowledge of Mr1, the non- dimensionalized mass flow function MFFr1 can be resolved using Equation 3.12. (3.12) Note that the MFF is a function of Mach number M and the ratio of specific heats γ. MFFr2 is solved for using Equation 3.13 P79 γ γ+ γ − (3.11) MFF=39$ =05γ− + 0 797397$ P 797 =P 797 P 397$ 397$ P 797 397 $ (3.13) 797 797 relative flow, determined from Equation 3.14. $ &RVβ = MVDR (3.14) $ &RVβ 397 The relative total pressure ratio is found by solving Equations (3.15), (2.4), and =1 from continuity, and streamtube contraction ratio of the cross-sectional areas which are perpendicular to the where =1 by assuming constant rothalpy, P $ is the (3.16). 397 397 397 397/0, = (3.15) 397 397/0, 397 21 $ P PDF Image | Gas Turbine Design Axial Flow Compressors
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