SEC. Vll.J OF NATURAL PHILOSOPHY. 32S about its axis AB, moving in the before-mentioned rare medium from A towards B, will be less resisted than any other circular solid whatsoever, described of the same length and breadth. PROPOSITION XXXV. PROBLEM VII. If a rare medium consist of very small quiescent particles of equal mag nitudes, and freely disposed at equal distances from one another : to jind the resistance of a globe moving uniformly forward in this medium. CASE 1. Let a cylinder described with the same diameter and altitude be conceived to go forward with the same velocity in the direction of its axis through the same medium ; and let us suppose that the particles of the medium, on which the globe or cylinder falls, fly back with as great a force of reflexion as possible. Then since the resistance of the globe (by the last Proposition) is but half the resistance of the cylinder, and since the globe is to the cylinder as 2 to 3, and since the cylinder by falling perpendicu larly on the particles, and reflecting them with the utmost force, commu nicates to them a velocity double to its own; it follows that the cylinder. in moving forward uniformly half the length of its axis, will communicate a motion to the particles which is to the whole motion of the cylinder as the density of the medium to the density of the cylinder ; and that the globe, in the time it describes one length of its diameter in moving uni formly forward, will communicate the same motion to the particles ; and in the time that it describes twro thirds of its diameter, will communicate a motion to the particles which is to the whole motion of the globe as the density of the medium to the density of the globe. Arid therefore the globe meets with a resistance, which is to the force by which its whole mo tion may be either taken away or generated in the time in which it de scribes two thirds of its diameter moving uniformly forward, as the den sity of the medium to the density of the globe. CASE 2. Let us suppose that the particles of the medium incident on the globe or cylinder are not reflected ; and then the cylinder falling per pendicularly on the particles will communicate its own simple velocity to them, and therefore meets a resistance but half so great as in the former case, and the globe also meets with a resistance but half so great. CASE 3. Let us suppose the particles of the medium to fly back from the globe with a force which is neither the greatest, nor yet none at all, but with a certain mean force ; then the resistance of the globe will be in the same mean ratio between the resistance in the first case and the resistance in the second. Q.E.I. COR. 1. Hence if the globe and the particles are infinitely hard, and destitute of all elastic force, and therefore of all force of reflexion ; thf resistance of the globe will be to the force by which its whole motion may