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π΄=ππ·2βπ·2 πππ π½ Eqn.3-10 1 4 1π 1π» 1 Here, W2 is the ideal relative velocity at impeller outlet, because outlet flow area A2 is defined by the backsweep angle. The relative velocity at the inlet, W1, represents the value at the RMS radius. The true relative velocity at the outlet is determined with the slip correlation described previously. Once the velocity triangle is determined, the enthalpy rise is calculated using the Euler turbomachinery equation. This enthalpy rise is then used to determine a new value for the fluid density at the outlet by calling the property subroutines with the calculated enthalpy as an input. The new value of density is then used to repeat the calculation until the density of the fluid converges. These calculations are contained in the subroutine OUTLET. Once the density converges, the velocity triangle and enthalpy rise are known for the current impeller outlet diameter. The process of determining the impellerβs performance is shown in Figure 3.10. The impeller will not be resized in the design portion of the code until the diffuser outlet static pressure is known, and therefore the entire compressor performance can be compared to the desired performance. Figure 3.10: The process for determining impeller performance. The outlet conditions of the impeller rely on the convergence of fluid density. Mass conservation determines the outlet triangle for each density iteration. 59PDF Image | Supercritical Carbon Dioxide Cycle Analysis
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