complete cycle of operations is measured by the product of the volume of the vapor multiplied by the difference between the tensions that it possesses at the temperature of the body A and at that of the body B. As to the heat employed, that is to say, transported from the body A to the body B, it is evidently that which was necessary to turn the water into vapor, disregarding always the small quantity required to restore the temperature of the liquid water from that of B to that of A.
Suppose the temperature of the body A 100 degrees, and that of the body B 99 degrees: the difference of the tensions will be, according to the table of M. Dalton, 26 millimetres of mercury or 0m.36 head of water.
The volume of the vapor is 1700 times that of the water. If we operate on one kilogram, that will be 1700 litres, or 1mc.700.
Thus the value of the motive power developed is the product
1.700 × 0.36 = 0.611 units,
of the kind of which we have previously made use.
The quantity of heat employed is the quantity required to turn into vapor water already heated to 100°. This quantity is found by experiment. We
