be taken, as in the employment of different substances, or in the use of the same substance in two different states—for example, of a gas at two different densities.
This leads us naturally to those interesting researches on the aeriform fluids—researches which lead us also to new results in regard to the motive power of heat, and give us the means of verifying, in some particular cases, the fundamental proposition above stated.[1]
We readily see that our demonstration would have been simplified by supposing the temperatures of the bodies A and B to differ very little. Then the movements of the piston being slight during the periods 3 and 5, these periods might have been suppressed without influencing sensibly the production of motive power. A very little change of volume should suffice in fact to produce a very slight change of temperature, and this slight change of volume may be neglected in presence of that of the periods 4 and 6, of which the extent is unlimited.
If we suppress periods 3 and 5, in the series of
- ↑ We will suppose, in what follows, the reader to be au courant with the later progress of modern Physics in regard to gaseous substances and heat.
