163 THE MATHEMATICAL PRINCIPLES [BoOK I SECTION VIII. Of the invention of orbits wherein bodies will revolve, being acted upon by any sort of centripetal force. PROPOSITION XL. THEOREM XIII. //' a body, acted upon by any centripetal force, is any how moved, and another body ascends or descends in a right line, and their velocities be equal in amj one case of equal altitudes, t/ieir velocities will be also equal at all equal altitudes. Let a body descend from A through D and E, to the centre (j : and let another body move from V in the curve line VIK&. From the centre C, with any distances, describe the concentric circles DI, EK, meeting the right line AC in I) and E; and the curve VIK in I and K. Draw 1C meeting KE in N, and on IK let fall the perpendicular NT • and let the interval DE or IN between the circumferences of the circles be very small ; K/ and imagine the bodies in D and I to have equal velocities. Then because the distances CD and CI are equal, the centri petal forces in D and I will be also equal. Let those forces be k) expressed by the equal lineoke DE and IN ; and let the force IN (by Cor. 2 of the Laws of Motion) be resolved into two others, NT and IT. rl hen the force NT acting in the direction line NT perpendicular to the path ITK of the body will not at all affect or change the velocity of the body in that path, but only draw it aside from a rectilinear course, and make it deflect perpetually from the tangent of the orbit, and proceed in the curvilinear path ITK/j. That whole force, therefore, will be spent in producing this effect: but the other force IT, acting in the direction of the course of the body, will be all employed in accelerating it, and in the least given time will produce an acceleration proportional to itself. Therefore the accelerations of the bodies in D and I, produced in equal times, are as the lines DE, IT (if we take the first ratios of the nascent lines DE, IN, IK, IT, NT) ; and in unequal times as those lines and the times conjunctly. But the times in which DE and IK are described, are, by reason of the equal velocities (in D and I) as the spaces described DE and IK, and therefore the accelerations in the course of the bodies through the lines DE and IK are as DE and IT, and DE and IK conjunctly ; that is, as the square of DE to the rectangle IT into IK. But the rectangle IT X IK is equal to the square of IN, that is, equal to the square of DE ; and therefore the accelerations generated in the passage of the bodies from D and I to E and K are equal. Therefore the velocities of the holies in E and K are also equal, and by the same reasoning they will always be found equal in any subsequent equal dis tances. Q..E.D.