请输入您要查询的英文单词:

 

单词 carnot cycle
释义

Carnot cycle


Carnot cycle

n (General Engineering) an idealized reversible heat-engine cycle giving maximum efficiency and consisting of an isothermal expansion, an adiabatic expansion, an isothermal compression, and an adiabatic compression back to the initial state
Thesaurus
Noun1.Carnot cycle - a cycle (of expansion and compression) of an idealized reversible heat engine that does work without loss of heatCarnot's ideal cycleoscillation, cycle - a single complete execution of a periodically repeated phenomenon; "a year constitutes a cycle of the seasons"

Carnot cycle


Carnot cycle

[kär′nō ‚si·kəl] (thermodynamics) A hypothetical cycle consisting of four reversible processes in succession: an isothermal expansion and heat addition, an isentropic expansion, an isothermal compression and heat rejection process, and an isentropic compression.

Carnot Cycle

 

a reversible cyclic process in which heat is converted into work, or vice versa. It consists of two isothermal and two adiabatic processes that alternate.

The Carnot cycle was first examined by the French scientist N. L. S. Carnot (1824) as the ideal operating cycle of a heat engine. The conversion of heat into work is accompanied by the transfer of a certain amount of heat by the engine’s working substance from the hotter body (the heater) to the cooler.

The Carnot cycle proceeds as follows: at a temperature T1 the working substance (such as steam in a cylinder under a piston) is brought into contact with a heater that has a constant temperature T1 and isothermically acquires from it an amount of heat δQi (here the steam expands and performs work). In Figure 1 this process is represented by the segment AB of the isotherm. The working substance, expanding adiabatically (along the adiabatic curve BC ), then cools to temperature T2. At this temperature, as it becomes isothermically compressed (segment CD), it gives off a quantity of heat δQ2 to the cooler with temperature T2. The cycle ends with an adiabatic process (DA in Figure 1) that returns the working substance to its initial thermodynamic state. When the temperature difference (T1T2) between the heater and cooler is constant, the working substance performs the following amount of work in one cycle:

This work is numerically equal to the area ABCD (Figure 1) bounded by the segments of the isotherms and adiabatic curves forming Carnot’s cycle.

Figure 1. The Carnot cycle in a (p, V)(´Q1) quantity of heat received by the working substance from the heater, (´Q2) quantity of heat released by the working substance to the cooler. The area ABCD is numerically equal to the wor^k performed in the cycle.

The Carnot cycle is reversible and can be carried out in the reverse sequence (in the direction ADCBA). Here the quantity of heat ´Q2 is collected from the cooler and, together with the lost work ´A (which has been converted into heat), is transferred to the heater. A heat engine operates in this mode as an ideal cooler.

The Carnot cycle has the highest efficiency η = ´A/´Q1 = (T1T2)/T1 of all possible cycles accomplished in the same temperature interval (T1T2 ). In this sense the efficiency of the Carnot cycle serves as a measure of the efficiency of other working cycles.

Historically, the Carnot cycle played an important role in the development of thermodynamics and heat engineering. It was used to prove the equivalency of the formulations of the second law of thermodynamics given by R. Clausius and W. Thomson

(Lord Kelvin), to determine the absolute temperature scale, and frequently also to derive various thermodynamic relations (such as the Clausius-Clapeyron equation)

REFERENCES

Fermi, E. Termodinamika. Kharkov, 1969. (Translated from English.)
Putilov, K. A. Termodinamika. Moscow, 1971.

Carnot cycle

A hypothetical thermodynamic cycle used as a standard of comparison for actual cycles. The Carnot cycle shows that, even under ideal conditions, a heat engine cannot convert all the heat energy supplied to it into mechanical energy; some of the heat energy must be rejected.

In a Carnot cycle, an engine accepts heat energy from a high-temperature source, or hot body, converts part of the received energy into mechanical (or electrical) work, and rejects the remainder to a low-temperature sink, or cold body. The greater the temperature difference between the source and sink, the greater the efficiency of the heat engine.

The Carnot cycle (see illustration) consists first of an isentropic compression, then an isothermal heat addition, followed by an isentropic expansion, and concludes with an isothermal heat rejection process. In short, the processes are compression, addition of heat, expansion, and rejection of heat, all in a qualified and definite manner. The net effect of the cycle is that heat is added at a constant high temperature, somewhat less heat is rejected at a constant low temperature, and the algebraic sum of these heat quantities is equal to the work done by the cycle.

A name given to the cycle of operations of an internal combustion engine that would take place in an ideally perfect engine in which friction is nonexistent and heat losses are totally absent. A theoretical cycle derived by Nicoles Leonhard Sadi Carnot, who enunciated it in 1874. The four events that occur in a Carnot cycle are (i) an isothermal expansion, (ii) followed by an adiabatic expansion, (iii) an isothermal compression, and (iv) to an adiabatic compression. The cycle is depicted in the illustration.

Carnot cycle


Related to Carnot cycle: Rankine cycle, Refrigeration cycle
  • noun

Synonyms for Carnot cycle

noun a cycle (of expansion and compression) of an idealized reversible heat engine that does work without loss of heat

Synonyms

  • Carnot's ideal cycle

Related Words

  • oscillation
  • cycle
随便看

 

英语词典包含2567994条英英释义在线翻译词条,基本涵盖了全部常用单词的英英翻译及用法,是英语学习的有利工具。

 

Copyright © 2004-2022 Newdu.com All Rights Reserved
更新时间:2024/11/12 12:25:13