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sin2 a2 =- 2 1 Page I3 The turning angle a2 - s is given by y + 1 (Y+1)/2(Y-l) %(2> (4Y-1 P2 Y-W 3 0PO1 I critical pressure sin2 where !tu 0p2 PO1 - PN p2 x-l-- PO1 [ exceeds the ratio The supersonic velocity c2 is obtained by application of the energy equation for isentropic flow. Thereafter the procedure is similar to that described in Section (a). m (Figures 7a and b) This is a form of casing frequently met on turbochargers. This analysis is intended primarily for unsteady flow studies, using the quasi steady approach, ie treating the flow as steady for short time intervals. Under such conditions inlet conditions at the 2 entries can differ widely and may be specified by ~01, Tel and ~02, Ts2. It is possible by the application of techniques similar to those already given to arrive at the common 'post shock' condition T2' (Figure 7b) in terms of the entry conditions pcI, To1 a-d ~02~ Toz. The general approach is to solve iteratively for the ccmmon interspace pressure p2 until mass flow compatibility between the sum of the nozzle flows (k)l and (rfiN)2 and the rotor flow l'k is obtained.PDF Image | Design of Radial Inflow and Mixed Flow Turbines 1971
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