Treatise On the Mechanical Theory of Heat And Its Applications to the Steam Engi

Cover Treatise On the Mechanical Theory of Heat And Its Applications to the Steam Engi
Treatise On the Mechanical Theory of Heat And Its Applications to the Steam Engi
R S Richard Sears Mcculloh
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152 MECHANICAL THEORY OF HEAT.
Iii Ericsson s engine, (lie pressure is constant for J/JV, and its equation is p p Q = 0; hence for the equation of PQ, we have / np ; and botli arc straight lines parallel to the axis of v.
It is evident that the general equation of the line MN is arbi trary; and consequently, that the problem may have an infinite number of solutions.
Theoretically, a regenerator should absorb heat only from the hot air and give it back to it afterwards without loss ; practically
..., it is impossible to prevent waste; a large portion of the heat being always communicated by conduction and radiation to surroundiiur o bodies. The term economizer is, therefore, its appropriate name. And we see that for air and all other heat engines, loss by conduc tion and radiation must ever render it impracticable to make them dynamically perfect. Yet of such loss a regenerator may save quite a large part.
One of the greatest improvements made in furnaces for metal lurgy is that of Mr. Siemens, who, by attaching a regenerator composed of a mass of fire-brick, has introduced great economy of fuel united with other very important advantages.


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