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86 6 Radial turbine design for a micro-ORC test setup 0.6 0.5 0.4 0.3 0.2 0.1 0 0 0.2 0.4 0.6 0.8 1 1.2 Lenght parameter, [−] k−ω SST k−ε Figure 6.6: The results of pressure distribution on the nozzle long wall by using k − ε-turbulence model and k − ω SST-Turbulence model. (a) (b) Figure 6.7: Velocity magnitude in the stator:(a) k − ε-turbulence model and (b) k − ω SST- turbulence model. shock waves and the viscous wake from the blade trailing edge affect the flow. The speed of sound of MDM increases near the throat section from 96 m/s to 132 m/s during the expansion. The increase in the speed of sound during the expansion, representing oppo- site behavior compared to an expansion when adopting ideal gas laws, can occur only for fluids having a high molecular complexity and if the expansion occurs in a certain thermodynamic region representing pressure or temperature relatively close to the fluids critical values (Harinck et al., 2009; Colonna and Guardone, 2006b). Similar results for the increase of the speed of sound of MDM were obtained by Colonna et al. (2006a) for expansion in a supersonic axial turbine stator with comparably similar turbine inlet state. p /p , [−] st tot,inPDF Image | WORKING FLUID SELECTION AND DESIGN OF SMALL-SCALE WASTE HEAT RECOVERY SYSTEMS BASED ON ORGANIC RANKINE CYCLES
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