US CONSIDER combined cycle plants connected in series, One is the Gas turbine (Brayton cycle) and another is the Steam turbine (Rankine cycle) POWER plant.It is assumed that all the HEAT rejected by the topping cycle is ABSORBED by the bottoming cycle.\({{\rm{η }}_{{\rm{brayton}}}} = 1 - \frac{1}{{{\rm{r}}_{\rm{p}}^{\left( {\frac{{{\rm{\gamma }} - 1}}{{\rm{\gamma }}}} \right)}}}\)Topping cycle → Brayton cycle → Working fluid → HeliumBottoming cycle → Rankine cycle → Working fluid → WaterOverall efficiency,η0 = η1 + η2 - η1η2 η1 = efficiency of the Brayton cycleη2 = efficiency of the Rankine cycle η0 is always more than η1 and η2.

"> US CONSIDER combined cycle plants connected in series, One is the Gas turbine (Brayton cycle) and another is the Steam turbine (Rankine cycle) POWER plant.It is assumed that all the HEAT rejected by the topping cycle is ABSORBED by the bottoming cycle.\({{\rm{η }}_{{\rm{brayton}}}} = 1 - \frac{1}{{{\rm{r}}_{\rm{p}}^{\left( {\frac{{{\rm{\gamma }} - 1}}{{\rm{\gamma }}}} \right)}}}\)Topping cycle → Brayton cycle → Working fluid → HeliumBottoming cycle → Rankine cycle → Working fluid → WaterOverall efficiency,η0 = η1 + η2 - η1η2 η1 = efficiency of the Brayton cycleη2 = efficiency of the Rankine cycle η0 is always more than η1 and η2.

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If η­1 and η2 are the thermal efficiencies of two individual power plants. When they are coupled series, the overall thermal efficiency η0 of the combined plant is given by

Power Engineering Gas And Vapor Power Cycles in Power Engineering 8 months ago

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Explanation:Let US CONSIDER combined cycle plants connected in series, One is the Gas turbine (Brayton cycle) and another is the Steam turbine (Rankine cycle) POWER plant.It is assumed that all the HEAT rejected by the topping cycle is ABSORBED by the bottoming cycle.\({{\rm{η }}_{{\rm{brayton}}}} = 1 - \frac{1}{{{\rm{r}}_{\rm{p}}^{\left( {\frac{{{\rm{\gamma }} - 1}}{{\rm{\gamma }}}} \right)}}}\)Topping cycle → Brayton cycle → Working fluid → HeliumBottoming cycle → Rankine cycle → Working fluid → WaterOverall efficiency,η0 = η1 + η2 - η1η2 η1 = efficiency of the Brayton cycleη2 = efficiency of the Rankine cycle η0 is always more than η1 and η2.

Posted on 15 Nov 2024, this text provides information on Power Engineering related to Gas And Vapor Power Cycles in Power Engineering. Please note that while accuracy is prioritized, the data presented might not be entirely correct or up-to-date. This information is offered for general knowledge and informational purposes only, and should not be considered as a substitute for professional advice.

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