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b7 bL bc b9 r9 Figure 3.11.: The impeller geometry with notations. Figure adapted from [2]. Table 3.4.: The geometry needed to run the performance analysis. ψ8 b8 r8 Inlet radius Inlet width Inlet axial coord. Inlet tangent angle Inlet blade angle Inlet blade thickness Throat blade to blade width Clearance r7 Mid passage radius r8 b7 Mid passage width b8 z7 Mid passage axial coord. z8 φ7 Mid tangent angle φ8 β7 Mid blade angle β8 t7 Mid blade thickness t8 o Throat passage width bth bc Clearance bL Outlet radius r9 Outlet width b9 Outlet axial coord. z9 Outlet tangent angle φ8 Outlet blade angle β9 Outlet blade thickness t9 Number of blades NR Surface finish erms (3.65) sources. Y =Yp +Yinc +YBL +YHS +YCL +YQ The profile loss, Yp, derived in chapter 3.2, is determined in a similar manner as the one for the nozzle blades. While the velocities used in expression for the nozzle blades profile loss are absolute, relative velocities are used when calculating the profile loss on the impeller. The meridional path length can be approximated using a third-order polynomial that matches the end-point coordinates and slopes. The is according to Aungier an accurate approximation. The mean surface curvature is then given by. κm = |φ9 − φ7| (3.66) m9 33PDF Image | A Detailed Analysis of Radial Turbines
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