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respectively. The distributions are similar to those of case d. The two have exactly the same locations of point A and B, but case i has a smaller value of ( )m),,.a The value of (' ),, has been reduced to avoid reversed loading (i.e., an overshoot in the curve of 2 ) near the trailing edge. As a result the Wrap Factor here is larger than that of case d (see Table 6.1 above) and the blade shape tends to be more radial, as shown in Fig 6.29. The Wrap Factor is computed to be 0.08 and again, we see a strong correlation between the Wrap Factor and the difference in wrap angle at the trailing edge. The value of AfT.. is 17.10, which again is consistent with the trend shown in Table 6.1. The reversed flow regions, shown in Fig. 6.30 and 6.31, are reduced in comparison to those of case d (see Fig. 6.12a and 6.13a). This can be attributed to a smaller value of ( e),na., which has been made possible because the loading ( 're) is distributed more evenly from the leading edge to the trailing edge. With the condition , 0 at the leading edge and the trailing edge is specified, the loading at the blade near the leading and trailing edges is relatively small. Hence for the particular example examined here, the removal of the constraint that 2 = 0 at the leading and trailing edges has worked in favor of reducing the reversed flow region. 6.6 Blockage Effects So far the blades have been assumed to be infinitely thin in the design calculations. However, a blade thickness distribution can be specified and accounted for partially through the use of the blockage distribution (see Eq.(2.35)). The normal thickness distributions t, on the main and splitter blades are shown in Fig. 6.32 and 6.33. The tangential thickness distributions to that result from the design calculation are shown in Fig. 6.34 and 6.35. The rVe distribution that is used in this case, which is referred to as case j, isPDF Image | Radial Inflow Splitter Blades in Three-Dimensional
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