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262 Fluid Mechanics, Thermodynamics of Turbomachinery



                                                          0.6
                                                             (l - cos n i)




                                                          0.4
                                         n = 1.75
                                                                                n = 2.5
                                            (i < 0)
                                                                                  (i > 0)

                                                          0.2





                           -60       -40        -20          0         20         40        60
                                                     Incidence angle, i (deg)

                          FIG. 8.11. Variation of incidence loss function at rotor inlet as a function of the incidence
                                                          angle.


                            EXAMPLE 8.6(a): For the IFR turbine described in Example 8.3, and using the
                          data and results in Example 8.4 and 8.5, deduce a value for the rotor enthalpy loss
                          coefficient,   R , at the optimum efficiency flow condition.

                            (b) The rotor speed of rotation is now reduced so that the relative flow enters the
                          rotor radially (i.e. at the nominal flow condition). Assuming that the enthalpy loss
                          coefficients,   N and   R remain the same, determine the total-to-static efficiency of
                          the turbine for this off-design condition.

                            Solution. (a) From eqn. (8.10), solving for   R ,
                                                      2
                                                          2
                                R D [.1    ts /c 2  c 2    N c ]/w .
                                           0    3     2   3
                          We need to find values for c 0 , c 3 , w 3 and c 2 .
                            From the data,
                                c 3 D c m3 D 0.25 ð 538.1 D 134.5 m/s.
                              w 3av D 2w 2 D 2c m2 / cos ˇ 2 D 2 ð 135.4/ cos 33.560 D 324.97 m/s.
                               1 2                   3                  3
                                c D W/  ts D 230 ð 10 /0.81 D 283.95 ð 10
                               2 0
                                c 2 D 468.8 m/s.
                                                                               2
                                                   3
                              ∴   R D .2 ð 283.95 ð 10 ð 0.19  134.5 2  0.06 ð 468.8 //324.97 2
                                  D 76, 624/105, 605
                                  D 0.7256.
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