SEC. L\.] OF NATURAL PHILOSOPHY. 173 revolve with the point p in the curve line which the same point p, by the method just now explained, may be made to describe an immovable plane. Make the angle VC^ equal to the angle PC/?, and the line Cu equal to CV, and the figure uCp equal to the figure VCP; and the body being al ways in the point p} will move in the perimeter of the revolving figure nCp, and will describe its (revolving) arc up in the same time the* the other body P describes the similar and equal arc VP in the quiescov.t fig ure YPK. Find, then, by Cor. 5, Prop. VI., the centripetal force by which the body may be made to revolve in the curve line which the pom* p de scribes in an immovable plane, and the Problem will be solved. O/E.K. PROPOSITION XLIV. THEOREM XIV. The difference of the forces, by which two bodies may be madi, to KMVG equally, one in a quiescent, the other in the same orbit revolving, i 1 in a triplicate ratio of their common altitudes inversely. Let the parts of the quiescent or bit VP, PK be similar and equal to the parts of the revolving orbit up, pk ; and let the distance of the points P and K be supposed of the utmost smallness Let fall a perpendicular kr from the point k to the right line pC, and produce it to m, so that mr may be to kr as the angle VC/? to the /2\angle VCP. Because the altitudes of the bodies PC and pV, KG and kC} are always equal, it is manifest that the increments or decrements of the lines PC and pC are always equal ; and therefore if each of the several motions of the bodies in the places P and p be resolved into two (by Cor. 2 of the Laws of Motion), one of which is directed towards the centre, or according to the lines PC, pC, and the other, transverse to the former, hath a direction perpendicular to the lines PC and pC ; the mo tions towards the centre will be equal, and the transverse motion of the body p will be to the transverse motion of the body P as the angular mo tion of the line pC to the angular motion of the line PC ; that is, as the angle VC/? to the angle VCP. Therefore, at the same time that the bodv P, by both its motions, comes to the point K, the body p, having an equal motion towards the centre, will be equally moved from p towards C ; arid therefore that time being expired, it will be found somewhere in the line mkr, which, passing through the point k, is perpendicular to the line pC ; and by its transverse motion will acquire a distance from the line