Thermodynamic cycles applied to gas turbines

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SUMMARY

The discussion focuses on the thermodynamic cycles applied to gas turbines, specifically the Brayton or Joule cycle, which includes adiabatic compression, heat addition at constant pressure, adiabatic expansion, and heat rejection at constant pressure. It highlights the inefficiencies in real gas turbine cycles that affect the temperature at the outlet of the compressor and turbine, leading to a scenario where the turbine work output equals the compressor input, resulting in no net work output. The user questions the validity of using Pressure-Volume (P-V) charts to represent net work output in gas turbines, particularly in comparison to Carnot cycles analyzed on Temperature-Entropy (T-s) charts.

PREREQUISITES
  • Understanding of Brayton cycle thermodynamics
  • Familiarity with Pressure-Volume (P-V) and Temperature-Entropy (T-s) charts
  • Knowledge of Carnot cycle principles
  • Basic concepts of turbomachinery, including compressors and turbines
NEXT STEPS
  • Research the impact of efficiency losses in gas turbines on performance metrics
  • Study the mathematical derivation of net work output in thermodynamic cycles
  • Explore advanced thermodynamic analysis techniques for real gas turbine cycles
  • Learn about the differences between ideal and real gas behavior in thermodynamic cycles
USEFUL FOR

Engineers, thermodynamics students, and professionals in the energy sector seeking to deepen their understanding of gas turbine performance and thermodynamic cycle analysis.

LaxeyT
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This is about the basic thermodynamic cycle of the gas turbine (i.e. Brayton or Joule cycle), consisting of adiabatic compression, heat addition at constant pressure, adiabatic expansion, and heat rejection at constant pressure, and the standard ways of analysing this through Pressure-Volume (P-V) and Temperature-Entropy (T-s) charts.

Real gas turbine cycles have inefficiencies in the compression and turbine expansion processes, which increase the temperatures at outlet from these components, compared with the same pressure rise (or fall) under isentropic conditions. I am trying to understand a contradiction - engineering consideration of a gas turbine would show that when the efficiencies of one or both components drops sufficiently that the turbine work output is equal to the compressor input, there is no net work output (the device would only just run).

However, if the same changes are shown on a P-V chart, there would still be positive net work output (based on the net work done around the cycle is ʃp.dv (the area under the P-V chart) around the cycle). Is it valid to use a P-V chart to show this?

Equivalently, and more straighforwardly, a Carnot cycle (a sequence of isothermal and adiabatic processes) produces positive net work output, but when analysed like a gas turbine on a T-s chart produces zero net work output..?
 
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Air standard Carnot cycle.

I would like to simplify my question:-

For the Carnot cycle:- Net work output =(ΔT)(ΔS), where ΔT = temp difference between source and sink temperatures and ΔS = entropy difference between adiabatic stages. This can be re-phrased in terms of Ps and Ts. Graphically, it is the area enclosed by the cycle on a T-S chart and also the area enclosed on a P-V chart.

In a 'real' implementation of a Carnot heat engine operating with air in a closed cycle, using turbomachinery (compressors and turbines), the net work would be extracted from the turbine, like in a Joule cycle gas turbine. However, if the net work is estimated like in a gas turbine, i.e. it is directly proportional to the difference in temperature differences across the compressor and turbine, this would be zero - no net work, but the cycle shows there is net work -can anyone explain this?

Thanks.
 

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