Page 172 - Fluid Mechanics and Thermodynamics of Turbomachinery
P. 172

Axial-flow Compressors and Fans  153
                                                Ł
                          The nominal deflection ε D 0.8  max and, from Figure 3.12, ε max D 37.5 ° . Thus,
                           Ł
                          ε D 30 ° and the nominal incidence is
                               Ł
                                   Ł
                              i D ˇ C ε Ł  ˇ 0 1
                                   2
                                                       °
                                D 10.2 C 30  44.5 D4.3 .
                                                           Ł
                                                               Ł
                            (ii) At the operating point i D 0.4ε C i D 7.7 ° . Thus, the actual inlet flow
                          angle is
                                    0
                                              °
                              ˇ 1 D ˇ C i D 52.2 .
                                    1
                          From Figure 3.12 at i D 7.7 ° , the deflection ε D 37.5 ° and the flow outlet angle is
                                              °
                              ˇ 2 D ˇ 1  ε D 14.7 .
                            (iii) From Figure 5.2, U D c x1 .tan ˛ 1 C tan ˇ 1 / D c x2 .tan ˛ 2 C tan ˇ 2 /. For c x D
                          constant across the stage and R D 0.5
                                           °
                              ˇ 1 D ˛ 2 D 52.2 and ˇ 2 D ˛ 1 D 14.7 °
                          and the flow coefficient is
                                  c x        1
                                D    D              D 0.644.
                                  U    tan ˛ 1 C tan ˇ 1
                                                           2
                          The stage loading factor,   D h 0 /U D   .tan ˛ 2  tan ˛ 1 / using eqn. (5.29).
                          Thus, with   D 0.86,
                                D 0.568.
                            (iv) The lift coefficient can be obtained using eqn. (3.18)
                                                      tan ˇ 2 /
                              C L D 2.s/l/ cos ˇ m .tan ˇ 1
                          ignoring the small effect of the drag coefficient. Now tan ˇ m D .tan ˇ 1 C tan ˇ 2 //2.
                          Hence ˇ m D 37.8 ° and so
                              C L D 2 ð 0.9 ð 0.7902 ð 1.027 D 1.46.

                            (v) Combining eqns. (3.7) and (3.17) the drag coefficient is
                                            !
                                                3
                                    s  p 0   cos ˇ m
                              C D D                 .
                                                 2
                                    l  1  w 2  cos ˇ 1
                                       2  1
                          Again using Figure 3.12 at i D 7.7 ° , the profile total pressure loss coefficient
                                1
                                   2
                          p 0 /.  w / D 0.032, hence the profile drag coefficient for the blades of either
                                2  1
                          row is
                                                      3
                                                             2
                                  D 0.9 ð 0.032 ð 0.7902 /0.6129 D 0.038.
                              C D p
                            Taking account of the annulus wall drag coefficient C Da and the secondary loss
                          drag coefficient C Ds
                              C Da D 0.02.s/l/.l/H/ D 0.02 ð 0.9 ð 0.5 D 0.009
                                          2
                                                         2
                              C Ds D 0.018C D 0.018 ð 1.46 D 0.038.
                                          L
   167   168   169   170   171   172   173   174   175   176   177