through a tin tube, 38 inches long, and 13⁄4 inch diameter, in the direction B A, the action of the sound being rendered manifest by its causing a sensitive flame placed at F' to become violently agitated.
"The invisible heated layer immediately above the luminous portion of an ignited coal-gas flame, issuing from an ordinary bat's-wing burner, was allowed to stream upward across the end A of the tin tube. A portion of the sound issuing from the tube was reflected at the limiting surfaces of the heated layer, the part transmitted being now only competent to slightly agitate the sensitive flame at F'.
"The heated layer was then placed at such an angle that the reflected portion of the sound was sent through a second tin tube, A F (of the same dimensions as B A). Its action was rendered visible by causing a second sensitive flame placed at the end of the tube F to become violently affected. This echo continued active so long as the heated layer intervened; but upon its withdrawal the sensitive flame placed at F' receiving the whole of the direct pulse, became again violently agitated, and at the same moment the sensitive flame at F, ceasing-to be affected by the echo, resumed its former tranquillity.
"Exactly the same action takes place when the luminous portion of a gas-flame is made the reflecting layer, but in the experiments above described the invisible layer above the flame only was used. By proper adjustment of the pressure of gas, the flame at F' can be rendered so moderately sensitive to the direct sound-wave that the portion transmitted through the reflecting layer shall be incompetent to affect the flame. Then by the introduction and withdrawal of the bat's-wing flame the two sensitive flames can be rendered alternately quiescent and strongly agitated.
"An illustration is here afforded of the perfect analogy between light and sound; for if a beam of light be projected from B to F', and a plate of glass be introduced at A in the exact position of the reflecting layer of gas, the beam will be divided, one portion being reflected in the direction A F, and the other portion transmitted through the glass toward F' exactly as the sound-wave is divided into a reflected and transmitted portion by the layer of heated gas or flame."
Thus far, therefore, we have placed our subject in the firm grasp of experiment; nor shall we find this test failing us further on.—Contemporary Review.
