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Isentropic process
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===Isentropic efficiencies of steady-flow devices in thermodynamic systems=== Most steady-flow devices operate under adiabatic conditions, and the ideal process for these devices is the isentropic process. The parameter that describes how efficiently a device approximates a corresponding isentropic device is called isentropic or adiabatic efficiency.<ref name="Cengel Boles 2012"/> Isentropic efficiency of turbines: : <math> \eta_\text{t} = \frac{\text{actual turbine work}}{\text{isentropic turbine work}} = \frac{W_a}{W_s} \cong \frac{h_1 - h_{2a}}{h_1 - h_{2s}}. </math> Isentropic efficiency of compressors: : <math> \eta_\text{c} = \frac{\text{isentropic compressor work}}{\text{actual compressor work}} = \frac{W_s}{W_a} \cong \frac{h_{2s} - h_1}{h_{2a} - h_1}. </math> Isentropic efficiency of nozzles: : <math> \eta_\text{n} = \frac{\text{actual KE at nozzle exit}}{\text{isentropic KE at nozzle exit}} = \frac{V_{2a}^2}{V_{2s}^2} \cong \frac{h_1 - h_{2a}}{h_1 - h_{2s}}. </math> For all the above equations: : <math> h_1 </math> is the specific [[enthalpy]] at the entrance state, : <math> h_{2a}</math> is the specific enthalpy at the exit state for the actual process, : <math> h_{2s}</math> is the specific enthalpy at the exit state for the isentropic process.
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