Page 87 - Fluid Mechanics and Thermodynamics of Turbomachinery
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68 Fluid Mechanics, Thermodynamics of Turbomachinery






































                          FIG. 3.11. A sample plot of inlet and outlet stagnation pressures and fluid outlet angle
                                                  (adapted from Todd 1947).

                          in Re. Mach number effects are negligible when M 1 < 0.3. Thus, the performance
                          laws, eqn. (3.28), for this flow simplify to,
                               , a 2 D f.a 1 /.                                          (3.28a)

                            There is a fundamental difference between the flows in turbine cascades and those
                          in compressor cascades which needs emphasising. A fluid flowing through a channel
                          in which the mean pressure is falling (mean flow is accelerating) experiences a
                          relatively small total pressure loss in contrast with the mean flow through a channel
                          in which the pressure is rising (diffusing flow) when losses may be high. This
                          characteristic difference in flow is reflected in turbine cascades by a wide range of
                          low loss performance and in compressor cascades by a rather narrow range.


                          Compressor cascade performance

                            A typical set of low-speed compressor cascade results (Howell 1942) for a blade
                          cascade of specified geometry, is shown in Figure 3.12. These results are presented
                                                                        2
                                                                     1
                          in the form of a pressure loss coefficient p 0 /.  c / and fluid deflection 2D
                                                                        1
                                                                     2
                                                        0
                                                       a (refer to Figure. 3.2 for nomenclature). Note
                          a 1  a 2 against incidence i D a 1
                                                        1
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