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p01 ∆T0 m ̇√T01 N p ,η,T =f p ,√T 010 01 01 01 (3.5) The parameters on the left hand side of equation (3.5) are then plotted against m ̇ which is also known as the corrected mass flow, with N/ T01 as a parameter. N/ T01 is termed the corrected shaft speed. For a radial turbine such plots can look something like those in figure 3.1. Figure 3.1 shows that at a certain pressure ratio the turbine flow chokes and thereby makes it independent of the shaft speed. √ √√ T01/p01, Choking mass flow Shaft speed increasing Shaft speed increasing Figure 3.1.: The dimensional groups are plotted against each other. The figure shows, on the left hand side, p01/p010 as a function of m ̇ T01/p01 with √ N/ T01 as different parameters and, on the right hand side, the efficiency √√ η as a function of m ̇ T01/p01 with N/ T01 as different parameters. 16 √PDF Image | A Detailed Analysis of Radial Turbines
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