434 THE MATHEMATICAL PRINCIPLES [BOOK III PROPOSITION XXXII. PROBLEM XIII. To find the mean motion of the nodes of the moon. The yearly mean motion is the sum of all the mean horary motions throughout the course of the year. Suppose that the node is in N, and that, after every hour is elapsed, it is drawn back again to its former place; so that, notwithstanding its proper motion, it may constantly re main in the same situation with respect to the fixed stars; while in the mean time the sun S, by the motion of the earth, is seen to leave the node, and to proceed till it completes its appa rent annual course by an uniform motion. Let Aa represent a given least arc, which the right line TS always drawn to the sun, by its intersection with the circle NA?/, describes in the least given moment of time; and the mean horary motion (from what we have above shewn) will be as A Z2, that is (because AZ and ZY are proportional), as the rectangle of AZ into ZY. that is, as the area AZYa ; and the sum of all the mean horary motions from the beginning will be as the sum of all the areas oYZA, that is, as the area NAZ. But the greatest AZYa is equal to the rectangle of the arc Aa into the radius of the circle ; and therefore the sum of all these rectangles in the whole circle will be to the like sum of all the greatest rectangles as the area of the whole circle to the rectangle of the whole circumference into the ra dius, that is, as 1 to 2. But the horary motion corresponding to that greatest rectangle was 16" 16'" 37iv. 42V. and this motion in the complete course of the sidereal year, 365d. 6". 9', amounts to 39° 38' 7" 50"', and therefore the half thereof, 19° 49' 3" 55"', is the mean motion of the nodes corresponding to the whole circle. And the motion of the nodes, in the time while the sun is carried from N to A, is to 19° 49' 3" 55"' as the area NAZ to the whole circle. Thus it would be if the node was after every hour drawn back again to its former place, that so, after a complete revolution, the sun at the year's end would be found again in the same node which it had left when the year begun. But, because of the motion of the node in the mean time, the sun must needs meet the node sooner ; and now it remains that we compute the abbreviation of the time Since, then, the sun, in the course of the year, travels 360 degrees, and the node in the same time by its greatest motion would be carried 39 > 38' 7" 50'", or 39,6355 degrees ; and the mean motion of the node in any place N is to its mean motion in its quadratures as AZ2 to AT- • the motion of the sun will be to the motion of the noda