Page 204 - Fluid Mechanics and Thermodynamics of Turbomachinery
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Three-dimensional Flows in Axial Turbomachines 185





























                             FIG. 6.7. Design and off-design velocity triangles for a free-vortex turbine stage.

                          The radial equilibrium equation at rotor outlet gives

                              dh 03    dc x3  c  3 d          d
                                   D c x3   C      .rc  3 / D  .rc  3 /,                 (6.38)
                               dr       dr     r dr           dr
                          after combining with eqn. (6.33), nothing that dh 02 /dr D 0 and that .d/dr/.rc  2 / D 0
                          at all mass flows. From eqn. (6.37),

                                  c  3   c x3         2  c x3
                               C    D     ,rc  3 D r       1 ,
                                   r     c Ł            c Ł
                                          x3             x3
                          which when substituted into eqn. (6.38) gives,
                                                          2
                                dc x3   2        c x3     r dc x3
                                    D     2r        1 C          .
                                 dr   c Ł     c Ł        c Ł  dr
                                       x3      x3         x3
                          After rearranging,
                                               2 2
                                dc x3       d. r /
                                      D             .                                     (6.39)
                                    Ł
                                                2 2
                                   c     .c Ł2  C  r /
                              c x3
                                    x3    x3
                          Equation (6.39) is immediately integrated in the form
                                           Ł2
                                                2 2
                               c x3  c Ł x3  D  c x3  C  r m                             (6.40)
                                                2 2
                                    c Ł   c Ł2  C  r
                              c x3m
                                     x3    x3
                          where c x3 D c x3m at r D r m . Equation (6.40) is more conveniently expressed in a
                                                                                     Ł    Ł
                          non-dimensional form by introducing flow coefficients   D c x3 /U m ,   D c /U m
                                                                                          x3
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