SEC. XIL] OF NATURAL PHILOSOPHY. 22\ tractions being destroyed by contrary attractions. There remains, there fore; only the attraction of the interior sphere PEQ,F. And (by Prop. LXXII) this is as the distance PS. Q.E.D. SCHOLIUM. By the superficies of which I here imagine the solids composed, I do not mean superficies purely mathematical, but orbs so extremely thin, that their thickness is as nothing; that is, the evanescent orbs of which the sphere will at last consist when the number of the orbs is increased, and their thickness diminished without end. In like manner, by the points of which lines, surfaces, and solids are said to be composed, are to be understood equal particles, whose magnitude is perfectly inconsiderable. PROPOSITION LXXIV. THEOREM XXXIV. The same things supposed, I say, that a corpuscle situate without the sphere is attracted with a force reciprocally proportional to the square of its distance from the centre. For suppose the sphere to be divided into innumerable concentric sphe rical superficies, and the attractions of the corpuscle arising from the sev eral superficies will be reciprocally proportional to the square of the dis tance of the corpuscle from the centre of the sphere (by Prop. LXXI). And, by composition, the sum of those attractions, that is, the attraction of the corpuscle towards the entire sphere, will be in the same ratio. Q.E.D. COR. 1. Hence the attractions of homogeneous spheres at equal distances from the centres will be as the spheres themselves. For (by Prop. LXXII) if the distances be proportional to the diameters of the spheres, the forces will be as the diameters. Let the greater distance be diminished in that ratio ; and the distances now being equal, the attraction will be increased in the duplicate of that ratio ; and therefore will be to the other attraction in the triplicate of that ratio ; that is, in the ratio of the spheres. COR. 2. At any distances whatever the attractions are as the spheres applied to the squares of the distances. COR. 3. If a corpuscle placed without an homogeneous sphere is attract ed by a force reciprocally proportional to the square of its distance from the centre, and the sphere consists of attractive particles, the force of ever y particle will decrease in a duplicate ratio of the distance from each particle. PROPOSITION LXXV. THEOREM XXXV. If to the several points of a given sphere there tend equal centripetal forces decreasing in a duplicate ratio of the distances from the points ; I say, that another similar sphere will be attracted by it with a force recip rocally proportional to the square of the distance of the centres. For the attraction of every particle is reciprocally as the square of its