366 THE MATHEMATICAL PRINCIPLES [BoOK 11 in the ratio of the elastic force, and the matter to be moved is increased in the ratio of the density, the time which is necessary for producing the same motion as before will be increased in the subduplicate ratio of the density, and will be diminished in the subduplicate ratio of the elastic force. And therefore the velocity of the pulses will be in a ratio com pounded of the subduplicate ratio of the density of the medium inversely, and the subduplicate ratio of the elastic force directly. Q,.E.D. This Proposition will be made more clear from the construction of the following Problem. PROPOSITION XLIX. PROBLEM XL The. density and elastic force of a medium being given, to find the, ve locity of the pulses. Suppose the medium to be pressed by an incumbent weight after the manner of our air ; and let A be the height, of a homogeneous medium, whose weight is equal to the incumbent weight, and whose density is the same with the density of the compressed medium in which the pulses are propa gated. Suppose a pendulum to be constructed whose length between the point of suspension and the centre of oscillation is A : and in the time in which that pendulum will perform one entire oscillation composed of its going and returning, the pulse will be propagated right onwards through a space equal to the circumference of a circle described with the radius A. For, letting those things stand which were constructed in Prop. X.LV11, if any physical line, as EF, describing the space PS in each vibration, be acted on in the extremities P and S of every going and return that it makes by an elastic force that is equal to its weight, it will perform its several vibrations in the time in which the same might oscillate in a cy cloid whose whole perimeter is equal to the length PS ; and that because equal forces will impel equal corpuscles through equal spaces in the same or equal times. Therefore since the times of the oscillations are in the subduplicate ratio of the lengths of the pendulums, and the length of the pendulum is equal to half the arc of the whole cycloid, the time of one vi bration would be to the time of the oscillation of a pendulum whose length is A in the subduplicate ratio of the length ^PS or PO to the length A. But the elastic force with which the physical lineola EG is urged, when it Is found in its extreme places P, S, was (in the demonstration of Prop. XLVII) to its whole elastic force as HL — KN to V, that is (since the point K now falls upon P), as HK to V: and all that force, or which is the same thing, the incumbent weight by which the lineola EG is com pressed, is to the weight of the lineola as the altitude A of the incumbent weight to EG the length of the lineola ; and therefore, ex ctquo, the force