Page 276 - Fluid Mechanics and Thermodynamics of Turbomachinery
P. 276

Radial Flow Gas Turbines  257
                          rotor tip radius ratio, r 3s /r 2 , and the exit hub to shroud radius ratio,   D r 3h /r 3s , all
                          have to be considered. It is assumed that the absolute flow at rotor exit is entirely
                          axial so that the relative velocity can be written:
                                          2
                               2
                              w D c 2  C U .
                               3    m3    3
                          If values of c m3 /U 2 and r 3av /r 2 can be chosen, then the exit flow angle variation
                          can be found for all radii. From the rotor exit velocity diagram in Figure 8.3,
                              c m3  r 3av        r 3
                                  D     cot ˇ 3av D  cot ˇ 3 .                            (8.45)
                              U 2    r 2         r 2
                          The meridional velocity c m3 should be kept small in order to minimise the exhaust
                          energy loss, unless an exhaust diffuser is fitted to the turbine.
                            Rodgers and Geiser (1987) correlated attainable efficiency levels of IFR turbines
                          against the blade tip speed/spouting velocity ratio, U 2 /c 0 , and the axial exit flow
                          coefficient, c m3 /U 2 , and their result is shown in Figure 8.8. From this figure it can
                          be seen that peak efficiency values are obtained with velocity ratios close to 0.7 and
                          with values of exit flow coefficient between 0.2 and 0.3.
                            Rohlik (1968) suggested that the ratio of mean rotor exit radius to rotor inlet
                          radius, r 3av /r 2 , should not exceed 0.7 to avoid excessive curvature of the shroud.
                          Also, the exit hub to shroud radius ratio, r 3h /r 3s , should not be less than 0.4 because
                          of the likelihood of flow blockage caused by closely spaced vanes. Based upon the
                          metal thickness alone it is easily shown that,
                              .2 r 3h /Z/ cos ˇ 3h >t 3h ,

                          where t 3h is the vane thickness at the hub. It is also necessary to allow more than
                          this thickness because of the boundary layers on each vane. Some of the rather
                          limited test data available on the design of the rotor exit, comes from Rodgers and
                          Geiser (1987), and concerns the effect of rotor radius ratio and blade solidity on
                          turbine efficiency (see Figure 8.9). It is the relative efficiency variation,  /  opt , that
                          is depicted as a function of the rotor inlet radius/exit root mean square radius ratio,


                                   0.8



                                   0.7                  88
                                  U 2 /c o                     86   84

                                                                        82    80
                                   0.6
                                                                             = 78
                                                                          h ts
                                   0.5
                                     0.1           0.2      0.3   0.4      0.6   0.8  1.0
                                                              c m3 /U 2
                          FIG. 8.8. Correlation of attainable efficiency levels of IFR turbines against velocity ratios
                                            (adapted from Rodgers and Geiser 1987).
   271   272   273   274   275   276   277   278   279   280   281