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110 π. ππππ =2(1βπΎ )πππππΆ π΅4 4 4 4 π4 πΆπ4 = π4ππ‘π 2π£2 π πΌ = 10.8 + 14.2π2 4π (β5-10) (β5-11) Figure β5-2: Velocity triangles of the rotor inlet(left) and rotor exit(right). Given that π4 is now calculated, the radius of the rotor inlet can be obtained using equation (β5-12). The height of the rotor blade can be calculated using the mass continuity in equation (β5-13). πΎπ΅4 is the leading edge blockage factor calculated using equation (β5-14)[234]. π‘π4 is the blade thickness at the leading edge of the rotor and obtained using the default value [234] using equation (β5-15). ππ is the number of blades of the rotor obtained by the Glassman correlation [238], which is widely used in ideal gas turbines, as shown in equation (β5-16). π = π4 (β5-12) (β5-13) (β5-14) (β5-15) (β5-16) 4 π πΎπ΅4=1β πππ‘π4 π‘ =0.04π π4 4 ππ = π 110βπΌ4 tanπΌ4 30 2ππ π πππ½ 44 The number of blades of the rotor ππ can be obtained using different empirical correlations available in the open literature. An excessive number of blades will result in higher blade surface area and, hence, higher frictional loss [233]. Bycontrast, a flow reversal will take place when thePDF Image | Automotive Radial Turbine Expander Design WHR
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