seems to be due to the condensation of the watery vapor caused by the cooling of the air.
(2) The inflammation of German tinder in the so-called pneumatic tinder-boxes; which are, as we know, little pump-chambers in which the air is rapidly compressed.
(3) The fall of a thermometer placed in a space where the air has been first compressed and then allowed to escape by the opening of a cock.
(4) The results of experiments on the velocity of sound. M. de Laplace has shown that, in order to secure results accurately by theory and computation, it is necessary to assume the heating of the air by sudden compression.
The only fact which may be adduced in opposition to the above is an experiment of MM. Gay-Lussac and Welter, described in the Annales de Chimie et de Physique. A small opening having been made in a large reservoir of compressed air, and the ball of a thermometer having been introduced into the current of air which passes out through this opening, no sensible fall of the temperature denoted by the thermometer has been observed.
Two explanations of this fact may be given: (1) The striking of the air against the walls of the opening by which it escapes may develop heat in
