Academic Integrity: tutoring, explanations, and feedback — we don’t complete graded work or submit on a student’s behalf.

l: To understand that a heat engine run backward is a heat pump that can be used

ID: 1989326 • Letter: L

Question

l: To understand that a heat engine run backward is a heat pump that can be used as a refrigerator.

By now you should be familiar with heat engines--devices, theoretical or actual, designed to convert heat into work. You should understand the following:

Heat engines must be cyclical; that is, they must return to their original state some time after having absorbed some heat and done some work).
Heat engines cannot convert heat into work without generating some waste heat in the process.
The second characteristic is a rigorous result even for a perfect engine and follows from thermodynamics. A perfect heat engine is reversible, another result of the laws of thermodynamics.

If a heat engine is run backward (i.e., with every input and output reversed), it becomes a heat pump (as pictured schematically ). Work must be put into a heat pump, and it then pumps heat from a colder temperature to a hotter temperature , that is, against the usual direction of heat flow (which explains why it is called a "heat pump").

The heat coming out the hot side of a heat pump or the heat going in to the cold side of a refrigerator is more than the work put in; in fact it can be many times larger. For this reason, the ratio of the heat to the work in heat pumps and refrigerators is called the coefficient of performance, . In a refrigerator, this is the ratio of heat removed from the cold side to work put in:

.

In a heat pump the coefficient of performance is the ratio of heat exiting the hot side to the work put in:
.

Take , and to be the magnitudes of the heat emitted and absorbed respectively.

Explanation / Answer

 

KRefri  = Q C/Win

In a heat pump the coefficient of performance is the ratio of heat exiting the hot side Q h to the work put in:

KPump  = Q h/Win

Take ,Q C and Q h to be the magnitudes of the heat emitted and absorbed respectively.