Informazioni sul documento
- Università
- Politecnico di Milano
- Corso di laurea
- Energy Engineering
- Materia
- Energy Conversion A
- Classificazione
- Altro materiale
- Formato originale
- Testo
- Testo ricercabile
Altro di Energy Conversion A per il corso di Energy Engineering presso Politecnico di Milano. Materiale proveniente dall’archivio storico Studwiz e classificato per la consultazione online.
Altro di Energy Conversion A per il corso di Energy Engineering presso Politecnico di Milano. Materiale proveniente dall’archivio storico Studwiz e classificato per la consultazione online.
Qualità dell’importazione: il testo è stato estratto direttamente dal documento originale.
Passaggi rappresentativi riconosciuti nelle diverse parti del materiale. Il testo completo resta presente nella pagina per la ricerca, mentre l’anteprima compatta rende più semplice la lettura.
Second project: analysis of a one-pressure level combined cycle power plant Simone Fedeli 892133 Luca Grippo 829683 Filippo Mecarelli 892120 Francesco Persico 893256 October 2017 1 The purpose of this analysis is to understand the main critical characteristics of a combined cycle power plant. We will investigate: • the power de cit of the gas turbine due to the presence of the HRSG at its outlet; • the optimal evaporation pressure for the steam cycle in the case of constant adiabatic isentropic e ciency of the steam turbine and with the presence of a correction for the e ciency at relatively low steam quality (below 0.98); • a complete and thorough II law analysis of the steam cycle in the second case (the one with the correction for the adiabatic isentropic e ciency of the turbine). 1 Gas turbine performance when coupled to the HRSG The presence of the HRSG means that the outlet pressure of the turbine is not atmospheric pressure anymore (101325 Pa , that is also the inlet pressure of the turbine, as we do not consider the presence of lters); the outlet pressure of the turbine is now increased of 3000 Pa , which is the value of the pressure drop of the exhaust gases inside the HRSG. The following diagram shows the new situation: As it is clear from the diagram, two key parameters change when the GT is 2 coupled to the HRSG: • the TOT becomes higher; • the power output of the gas turbine becomes lower. We assume the gas turbine to be a modern one, so to say, its blades are cooled by air bled from the compressor; this means that the actual path of the ex- pansion on the T −s diagram is not linear, and, more importantly, the usual isentropic relation T ·P 1−k k cannot be used, as the expansion process is clearly not adiabatic. We have to proceed in the opposite…
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