Compound motion: the right triangle of fall and cross-motion
How a poured or thrown body's path forms the hypotenuse, with degrees halved along a f
Across folios 144v and 143r Leonardo analyses motion compounded of a 'natural' vertical fall and a 'transversal' horizontal drive, using a right triangle (ortogonio) whose hypotenuse is the path of the moving or poured body. When the two motions are equal the hypotenuse cuts the sides equally; doubling the weight or the cross-speed shifts where and how steeply it cuts, and the degrees of motion are laid off by repeated halving along the side a f into 2, 4, 8, 16 and 32 equal parts. A long note reasons that a continuous falling quantity, such as poured water, settles onto the same oblique hypotenuse as a stream of separate drops. A closing figure shows a weight n raised without added effort to its mover.
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Natural and transversal motion combine on a right triangle
The transversal motion of a pouring vessel and the natural fall of the poured matter form the two sides of a right angle whose hypotenuse is the falling stream. When the two motions are equal the hypotenuse cuts the sides of the right angle equally.
Doubling weight or cross-speed shifts the hypotenuse
If the natural motion doubles in weight it doubles in speed, so the natural side becomes double the transversal; and if the cross-speed doubles, the hypotenuse cuts the sides in double proportion, the upper side becoming double the natural.
The proportion of the sides equals the proportion of the motions
Such is the proportion of the transversal motion to the natural as that between the sides of the right angle they create, terminated at their hypotenuse.
Degrees of motion halved along the line a f
The degrees of the whole motion are measured on side a f, always halved at each cut, so that the 2 parts of e l match each of the 4 of d K, the 8 of c i, the 16 of b h and the 32, all equal in space.
A continuous poured stream falls like separate drops
Leonardo asks why a continuous quantity of water, lacking the piecewise fall of separate drops, still arranges itself along the same hypotenuse. He answers that its weight, uniformly distributed along the sustaining cord, keeps the same distances from the transversal motion as the disunited drops do.
A weight raised without added effort
Beside the central figure of a group of three at the lower right, a note states that the weight n is raised without any increase of effort to its mover.
