EC. VII.] OF NATURAL PHILOSOPHY. 345 the ratio of the orifice of the canal to the excess of that orifice above half the greatest circle of the globe ; and the duplicate ratio of the orifice of the canal, to the excess of that orifice above the greatest circle of the globe ; and t/ie ratio of the density of the fluid to the density of the globe, nearly. This appears by Cor. 2, Prop. XXXVII, and the demonstration pro ceeds in the same manner as in the foregoing Proposition. SCHOLIUM. In the last two Propositions we suppose (as was done before in Lem. V) that all the water which precedes the globe, and whose fluidity increases the resistance of the same, is congealed. Now if that water becomes fluid, it will somewhat increase the resistance. But in these Propositions that increase is so small, that it may be neglected, because the convex superfi cies of the globe produces the very same effect almost as the congelation of the water. PROPOSITION XL. PROBLEM IX. To find by phenomena the resistance of a globe moving through a per fectly fluid compressed medium. Let A be the weight of the globe in vacua, B its weight in the resisting medium, D the diameter of the globe. F a space which is to f D as the den sity of the globe to the density of the medium, that is, as A to A — B, G the time in which the globe falling with the weight B without resistance describes the space P, and H the velocity which the body acquires by that fall. Then H will be the greatest velocity with which the globe can pos sibly descend with the weight B in the resisting medium, by Cor. 2, Prop XXXVIII ; and the resistance which the globe meets with, when descend ing with that velocity, will be equal to its weight B ; and the resistance it meets with in any other velocity will be to the weight B in the duplicate ra tio of that velocity to the greatest velocity H, by Cor. 1, Prop. XXXVIII. This is the resistance that arises from the inactivity of the matter of the fluid. That resistance which arises from the elasticity, tenacity, and friction of its parts, may be thus investigated. Let the globe be let fall so that it may descend in the fluid by the weight B ; and let P be the time of falling, and let that time be expressed in sec onds, if the time G be given in seconds. Find the absolute number N 2P agreeing to the logarithm 0,4342944819 —> and let L be the logarithm of N 4- 1 the number — — ' and *^e velocity acquired in falling will bf