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6.3 Distribution of .L and the Wrap Factor The camber distribution of the main blade for case d is shown in Fig. 6.14 and the distribution of .L for the same case is shown in Fig. 6.15. It is seen that the contours of - - near the stacking axis are oriented in approximately the same direction as that r of the stacking axis. However, toward the trailing edge, the contour lines of wL become more radial (invariant with r-coordinates) while the contours of the blade camber have approximately the same orientation as that at the stacking axis. For blade with more radial blade filament along constant z section, it is desirable to have blade contour distribution similar to the -d distribution. In the iteration process, the blade shape is updated in each iteration through Eq.(5.1) which is rewritten here for convenience: Oh-f+w j =We Wr+ -=- + )bi*0Va, (6.1) where = C ]- w. The - distribution; the (PV) 1,j* Va term, however, is updated in each iteration. Nevertheless, term is fixed once we specify a certain rVo ifweassumethatthe(V)b,j*Vajtermismuchsmallerthanthe suggests that the key in obtaining more radial blade shape lies in the specification of It is more difficult to examine the WO distribution on the whole blade region than to examine its distribution along the hub and shroud only. Moreover, the distribution of rVo (and EA) along the hub and shroud is obtained through polynomials, and not any differential equation, so it is far easier to control. Comparing the results in Fig. 6.14 and Fig. 6.15, we observe that downstream of the stacking axis, the values of 1* along the hub and along the shroud both decrease approximately from a value of 0.0 to -3.6. The blade wrap angle along the hub and shroud can be obtained approximately from the value of -A along the hub and shroud. r term, then thisPDF Image | Radial Inflow Splitter Blades in Three-Dimensional
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