On the figures obtained by strewing sand on vibrating surfaces, commonly called acoustic figures
Author(s) -
Charles Wheatstone
Publication year - 1837
Publication title -
abstracts of the papers printed in the philosophical transactions of the royal society of london
Language(s) - English
Resource type - Journals
eISSN - 2053-9142
pISSN - 0365-5695
DOI - 10.1098/rspl.1830.0101
Subject(s) - square (algebra) , vibration , superposition principle , line (geometry) , geometry , oscillation (cell signaling) , acoustics , physics , mathematics , mathematical analysis , biology , genetics
The author, after adverting to the imperfect notice taken by Galileo and by Hooke of the phenomena which form the subject of this paper, ascribes to Chladni exclusively the merit of the discovery of the symmetrical figures exhibited by plates of regular form when made to sound. He proposes a notation, by means of two numbers separated by a vertical line, for expressing the figures resulting from the vibrations of square or rectangular plates. He gives a table of the relative sounds expressed both by their musical names and by the number of their vibrations, of all the modes of vibration of a square plate, as ascertained by the experiments of Chladni. He then proceeds to class and analyse the various phenomena observed under these circumstances, and shows that all the figures of these vibrating surfaces are the resultants of very simple modes of oscillation, occurring isochronously, and superposed upon one another; the resultant figure varying with the component modes of the vibration, the number of the superpositions, and the angles at which they are superposed. In the present paper, which forms the first part of his investigation, he confines himself to the figures of square and other rectangular plates. The author finds that the principal results of the superposition of two similar modes of vibration are the following :—first, the points where the quiescent lines of each figure intersect each other remain quiescent points in the resultant figure; secondly, the quiescent lines of one figure are obliterated, when superposed, by the vibratory parts of the other; thirdly, new quiescent parts, which may be called points of compensation, are formed whenever the vibrations in opposite directions neutralize each other; and, lastly, at other points, the motion is as the sum of the concurring, or the differences of the opposing vibrations at these points. After considering various modes of binary superposition, the author examines the cases of four co-existing superpositions.
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