Classical thermodynamics, heat transfer Definition
Coefficient of performance
Builds on Thermodynamic cycleHeatThermodynamic workFirst law of thermodynamicsClausius statement of the second law
Definition
Consider a system that repeatedly performs a thermodynamic cycle. In each cycle it absorbs heat from a cold reservoir and receives work from its surroundings. It gives heat to a hot reservoir. When the purpose is cooling, the system is a refrigerator and its coefficient of performance is When the purpose is heating, the system is a heat pump and its coefficient of performance is
Remarks
By the first law of thermodynamics, , so . By the Clausius statement of the second law, heat cannot pass from cold to hot with no other effect, so the cycle needs work . For a reversible cycle between thermodynamic temperatures , the values are and , and no cycle between these reservoirs does better. Example: a reversible heat pump between and has . A non-example: an electric resistance heater turns work into heat but takes no heat from a cold reservoir, so the condition fails; its ratio is only .
Reading path
To understand this page from the ground up, read these 10 pages in order. The foundations come first.
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- no evidence level
- Heat concept
- Internal energy concept
- State function concept
- Temperature concept
- Thermodynamic cycle concept
- Thermodynamic system concept
- Thermodynamic work concept
- First law of thermodynamics statement
- Clausius statement of the second law statement
- Coefficient of performance definition
Further reading
About this page
| Tag | T65EB2RBR8 |
|---|---|
| URI | m2://T65EB2RBR8 |
| Kind | definition |
| Writing | W0 stub |
| MSC | 80A10, 80A05 |
| Defines | Coefficient of performance |
| Uses | Thermodynamic cycle, Heat, Thermodynamic work, First law of thermodynamics, Clausius statement of the second law |
| Changed | 3 November 2026 |
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