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implies that in the absence of the splitter blade rVo is zero for the splitter, and when the splitter is of the same length as the main blade (i.e., we have twice the number of blades) rVo for the splitter is identical to that for the main blade. There is another reason for choosing the above procedure for the specification of the value of rVo at the splitter leading edge. This is described in the following. Suppose the swirl to be removed varies linearly from leading edge to trailing edge; because of this, the main and the splitter blades will have exactly the same value of , along the hub and the shroud. A similar value in the first derivative of rVg is desirable, as it is related to the loading on the blades. However, in the present study, the specified swirl schedule is such that it is not removed linearly; accordingly the above procedure for assigning the swirl at the leading edges is expected to result in the specification of loading distribution which is approximately the same for the main and the splitter blades. 5.3 The Stacking Conditions As explained in chapter 2, the blade shapes are obtained iteratively from Eq.(2.28), which is again given below: W,+ =)+ -W()Va (5.1) r k=1l Now upon neglecting the last term on the RHS, we deduce that both the main blade and the splitter blade would have the same shape. This is so because the mean velocity is used on the LHS while the sum of rVo (not the rVo on each blade) is used on the RHS. Thus if the periodic velocity term is indeed small compared to the other terms in the equation, the blades will have approximately the same camber distributions for the same stacking conditions. It is for this reason that the same stacking conditions for the main and the splitter blades are chosen.PDF Image | Radial Inflow Splitter Blades in Three-Dimensional
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