Abstract

The present paper describes the energy analysis of a regenerative vapour power system. The regenerative steam turbines based on the Rankine cycle and comprised of vapour extractions have been used industrially since the beginning of the 20th century, particularly regarding the processes of electrical production. After having performed worked in the first stages of the turbine, part of the vapour is directed toward a regenerative exchanger and heats feedwater coming from the condenser. This process is known as regeneration, and the heat exchanger where the heat is transferred from steam is called a regenerator (or a feedwater heater). The profit in the output brought by regenerative rakings is primarily enabled by the lack of exchange of the tapped vapour reheating water with the low-temperature reservoir. The economic optimum is often fixed at seven extractions. One knows the Carnot relation, which is the best possible theoretical yield of a dual-temperature cycle; in a Carnot cycle, one makes the assumption that both compressions and expansions are isentropic. This article studies an ideal theoretical machine comprised of vapour extractions in which each cycle partial of tapped vapour obeys these same compressions and isentropic expansions.

Highlights

  • The work output is maximised when the process between the two specified states is executed in a reversible manner

  • The present paper describes the energy analysis of a regenerative vapour power system

  • The Carnot factor, as is universally known, is a typical case limited to the cycles that do not involve feedwater heaters

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Summary

Alain DOI

Power plants that use steam as their working fluid operate on the basis of the Rankine cycle (1). The first stage in designing these power plants is performing the thermodynamic analysis of the Rankine cycle. Since the early 20th century, steam turbines have been most frequently used in regenerative cycles, e.g., in thermal and nuclear power plants. These steam engines are equipped with five to seven steam extractions. Part of the steam that performed work in the turbine is drawn off for use in heating the water. The drawn-off steam is proportional to the flow of water to be heated to conserve both mass and energy

Real Cycle
Ideal Carnot Cycle
Real Cycle with One Feedwater Heater
Ideal Cycle Comprised of One Feedwater Heater
Real Cycle with Two Feedwater Heaters
Ideal Cycle “n” Number of Feed Water Heaters
Conclusions

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