Page 30 - Fluid Mechanics and Thermodynamics of Turbomachinery
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Introduction: Dimensional Analysis: Similitude  11
                          It is a simple matter to combine any pair of these expressions in such a way as to
                          eliminate the diameter. For a pump the customary way of eliminating D is to divide
                           1/2    3/4
                            1  by   1  . Thus
                                    1/2       1/2
                                     1     NQ
                              N s D  3/4  D   3/4  ,                                       (1.8)
                                          .gH/
                                     1
                          where N s is called the specific speed. The term specific speed is justified to the
                          extent that N s is directly proportional to N. In the case of a turbine the power
                          specific speed N sp , is more useful and is defined by,
                                    O
                                    P 1/2  N.P/ / 1/2
                                     1
                              N sp D  5/4  D                                               (1.9)
                                            .gH/ 5/4
                                     1
                          Both eqns. (1.8) and (1.9) are dimensionless. It is always safer and less confusing
                          to calculate specific speed in one or other of these forms rather than dropping the
                          factors g and   which would make the equations dimensional and any values of
                          specific speed obtained using them would then depend upon the choice of the units
                          employed. The dimensionless form of N s (and N sp ) is the only one used in this
                          book. Another point arises from the fact that the rotational speed, N, is expressed
                          in the units of revolutions per unit of time so that although N s is dimensionless,
                          numerical values of specific speed need to be thought of as revs. Alternative versions
                          of eqns. (1.8) and (1.9) in radians are also in common use and are written
                                     Q 1/2
                                s D       ,                                              .1.8a/
                                    .gH/ 3/4
                                      p
                                     P/
                               sp D       .                                              .1.9a/
                                    .gH/ 5/4

                          There is a simple connection between N s and N sp (and between  s and  sP ). By
                          dividing eqn. (1.9) by eqn. (1.8) we obtain

                                     N.P/ / 1/2  .gH/ 3/4     P    1/2
                              N sp
                                  D                  D            .
                               N s    .gH/ 5/4  NQ 1/2    gQH
                          From the definition of hydraulic efficiency, for a pump we obtain:

                              N sp    sp   1
                                  D      D p ,                                            (1.9b)
                               N s    s
                          and, for a turbine we obtain:
                              N sp    sp  p
                                  D      D   .                                            (1.9c)
                               N s    s
                            Remembering that specific speed, as defined above, is at the point of maximum
                          efficiency of a turbomachine, it becomes a parameter of great importance in selecting
                          the type of machine required for a given duty. The maximum efficiency condition
                          replaces the condition of geometric similarity, so that any alteration in specific
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