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64 Model Details This is calculated as follows: m = ρ2vm2P ER2 = ρ2vm2πb2D2 ∴ b2 = m ρ2vm2πD2 (B-21) (B-22) (B-23) (B-24) where PER2 is the perimeter at the rotor inlet. Also, A3 = ρ3vm3 A2 ρ2 Mm2 a01 B-2-4 Turbine Outlet The subroutine TUOUTLET calculates the enthalpies, density and speed of sound of the fluid at this station. Furthermore, it determines the volumetric flow rate and temperature at the turbine exit. The stagnation enthalpy is determined by using the isentropic efficiency of the turbine given by the equation: h04 = h01 − ηi (h01 − h4s) (B-25) The optimum value of ηi is achieved when the value converges to the efficiency calculated using equation 3-13. The iterative Newton-Raphson method has been implemented to achieve the solution. B-3 Turbine Model Variable list Variables T1 V1 P1 H1 H01 S1 RHO1 M1 ETATS ETATSNOZ R VOLIN A1 A01 SPR SVR SDH Engineering Symbol\Physical Meaning Nozzle Inlet - Station 1 Temp at inlet of nozzle Velocity at nozzle inlet Pin at inlet to nozzle Enthalpy at inlet to nozzle Total Enthalpy at 1 Entropy at 1 Density at 1 Mass flow rate at 1 Total-Static efficiency Total-Static nozzle efficiency Degree of Reaction VolumeFlow Speed of sound Speed of sound in total conditions Static Pressure Ratio Static Volume Ratio Static enthalpy drop Units oC m/s bar kJ/kg kJ/kg kJ/kgK kg/m3 kg/s % % - m3/s m/s m/s - - kJ/kg Master of Science Thesis Akshay HattiangadiPDF Image | Working Fluid Design for Organic Rankine Cycle
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