Page 163 - Fluid Mechanics and Thermodynamics of Turbomachinery
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144 Fluid Mechanics, Thermodynamics of Turbomachinery



























                            FIG. 5.4. Asymmetry of velocity diagrams for reactions greater or less than 50%.


                            If R> 0.5 then ˇ 2 >˛ 1 and the velocity diagram is skewed to the right as shown
                          in Figure 5.4a. The static enthalpy rise in the rotor exceeds that in the stator (this
                          is also true for the static pressure rise).
                            If R< 0.5 then ˇ 2 <˛ 1 and the velocity diagram is skewed to the left as indi-
                          cated in Figure 5.4b. Clearly, the stator enthalpy (and pressure) rise exceeds that in
                          the rotor.
                            In axial turbines the limitation on stage work output is imposed by rotor blade
                          stresses but, in axial compressors, stage performance is limited by Mach number
                          considerations. If Mach number effects could be ignored, the permissible tempera-
                          ture rise, based on incompressible flow cascasde limits, increases with the amount of
                          reaction. With a limit of 0.7 on the allowable Mach number, the temperature rise and
                          efficiency are at a maximum with a reaction of 50%, according to Horlock (1958).


                          Stage loading

                            The stage loading factor   is another important design parameter of a compressor
                          stage and is one which strongly affects the off-design performance characteristics.
                          It is defined by

                                  h 03  h 01  c y2  c y1
                                D          D         .                                   (5.14a)
                                     U 2        U
                          With c y2 D U  w y2 this becomes,

                                D 1    .tan ˛ 1 C tan ˇ 2 /,                             (5.14b)

                          where   D c x /U is called the flow coefficient.
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