Week 4 Lecture 6 Flashcards
imposes restrictions on the direction of actual processes
second law of thermodynamics
Statements of the second law
- No apparatus can operate in such a way that it only effect is to convert heat absorbed by a system. It is impossible by a cyclic process to convert the heat absorbed by a system completely into work done by the system
- No process is possible which consists sole in the transfer of heat from one temperature level to a higher one
device that takes in energy by heat and operating in a cyclic process, expels a fraction of that energy by means of work
heat engine
A heat engine carries some working substance through a ____ process
cyclical
heat engine steps
- Working substance absorbs energy by heat from a higher temperature reservoir
- Work is done by the engine (Weng)
- Energy is expelled as heat to lower temperature reservoir (Qc)
First law equation
Qh =
Qh = Weng + Qc
efficiency equation
η =
net work output/heat input
efficiency equation
η =
|W eng|/|Qh|
efficiency equation
η =
|Qh|- |Qc|/|Qh|
efficiency equation
η =
1- (|Qc|/|Qh|)
High value of η meanings good conversion of …
Qh to Weng
Qc = 0
heat engine in inverse steps
- Energy is extracted from the cold reservoir (Qc) by work done on the heat pump (W)
- Energy is transferred to the hot reservoir (Qh)
- This process means the heat engine is running as a heat pump
Measured the performance of the heat pump running in cooling mode
Coefficient of performance (COP)
COP equation for cooling mode
|Qc|/W
COP equation for heating mode
|Qh|/W
depends only on the temperature between which it operates and is independent of the nature of the cyclic process
maximum efficiency