Page 166 - Fluid Mechanics and Thermodynamics of Turbomachinery
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Axial-flow Compressors and Fans  147
























                          FIG. 5.6. Effect of design stage loading (  d ) on simplified off-design performance
                                           characteristics (adapted from Horlock 1958).

                          Stage pressure rise

                            Consider first the ideal compressor stage which has no stagnation pressure losses.
                          Across the rotor row p 0rel is constant and so

                                                 2
                                        1
                                   p 1 D  .w 2  w /.                                     (5.23a)
                              p 2           1    2
                                        2
                          Across the stator row p 0 is constant and so
                                                2
                                        1
                                   p 2 D  .c 2  c /.                                     (5.23b)
                              p 3          2    3
                                        2
                          Adding together the pressure rise for each row and considering a normal stage
                          (c 3 D c 1 ), gives
                                                             2
                                                  2
                              .p 3  p 1 /2/  D .c 2  w / C .w 2  c /.                     (5.24)
                                              2   2      1   1
                                                                                       2
                                                                                            2
                          For either velocity triangle (Figure 5.2), the cosine rule gives c 2  U C w D
                          2Uw cos. /2  ˇ/ or
                                    2
                              c 2  w D U 2  2Uw y .                                       (5.25)
                          Substituting eqn. (5.25) into the stage pressure rise,
                              2.p 3  p 1 //  D .U 2  2Uw y2 /  .U 2  2Uw y1 /
                                          D 2U.w y1  w y2 /.
                                                                             c y1 and
                          Again, referring to the velocity diagram, w y1  w y2 D c y2
                              .p 3  p 1 //  D U.c y2  c y1 / D h 3  h 1 .                 (5.26)
                          It is noted that, for an isentropic process, Tds D 0 D dh  .1/ /dp and therefore,
                          h D .1/ /p.
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