The working fluid (say, water for a steam engine) of the heat engine receives heat Qh from the burning fuel (diesel oil, for example) which converts it to steam. The steam expands, pushing on the piston so that it does work W; as it expands, it cools and the pressure decreases. It then traverses a condenser, where it loses an amount of heat Qc to the coolant (cooling water or the atmosphere, for example), which returns it to the liquid state. The second law says that, if the working fluid (in this case the water) is to be returned to its original state so that the heat-work process could begin all over again, then some heat must be rejected to the coolant. Since the working fluid is returned to its original state, there is no change in its internal energy, so that the first law demands that Qh - Qc=W. The efficiency of the process is the amount of work obtained for a given cost in heat input: E = W/Qh. Thus, combining the two laws, E = (Qh-Qc)/Qh. It can be seen therefore that a heat engine can never run at 100% efficiency.
It is important to note that the laws of thermodynamics are of very great generality, and are of importance in understanding such diverse subjects as chemical reactions, very low temperature phenomena, and the changes in the internal structure of solids with changes in temperature, as well as engines of various kinds.
See also Gases, properties of.
Resources
Books
DiLavore, Philip, Energy: Insights from Physics. New York: Wiley, 1984.)
Goldstein, Martin, and Inge F. Goldstein. The Refrigerator and the Universe. Cambridge: Harvard University Press, Cambridge, 1993.
David Mintzer
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about 1 year ago
The calorie is the amount of heat to raise a certain volume of water 1 degree C. a "small" calorie raises a gram of water 1 degree, while a "large" calorie raises 1 kilogram of water 1 degree Celsius.