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14 Proc IMechE Part A: J Power and Energy 0(0) the suction side of the blade. It also mix with the fluid deriving from the shroud and suction surface (Figure 17(a) and (c)). For stages 2 and 4, the fluid deriving from the hub is also mixed with the leakage vortex. As a result, the flow loss corresponding to the leakage vortex is much higher in the rotor. To further compare the internal flow in shrouded and unshrouded rotors, spanwise distribution of flow angle and isentropic efficiency distribution on the observe surface is provided in Figures 18 and 19. The definition for the efficiency at observation surface is shown below observ 1⁄4 h0 hobserv ð25Þ h0 hobserv,S Figure 18. The flow angle and efficiency distribution at outlet of shrouded rotor: (a) stage 1; (b) stage 2; (c) stage 3; (d) stage 4.PDF Image | radial turbine supercritical compressed air energy storage
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