The mechanics of a pulley: weight, cord and 'excess'
Argument on how weight bears on two cords over a pulley, the balance, and air resistance
A densely written page reasoning about weights hung on the two cords of a pulley (carrucola), keyed to a small diagram at the upper right showing labelled points r, m, n. Leonardo argues, against an imagined adversary, that each cord feels the whole weight joined to it, proving the point with a balance, and that only the 'excess' (eccesso) of weight causes descent. He then treats how a falling weight penetrates the air, how air condenses above a fast-moving body, and why the cord breaks at the boundary between natural and accidental motion.
On this page
How weight bears on the two cords of a pulley
The lesser weight loads the whole cord r n and r m by the amount 4 of n, while m gives no more than 4 pounds, so the cord n r feels neither more nor less than 8. The excess of m falls as gravity without support, and only the cord r m feels it. Against the adversary, Leonardo holds that each cord hanging from the opposite sides of the pulley feels all the weight joined to it, proved by the balance whose right-arm weights do not load the left arm.
The 'excess', falling bodies and the resistance of air
Only the excess (eccesso) moves the body, and with greater velocity the greater it is; the falling thing has no support, so its cord seems not to feel it, yet were that so it would not descend. A body weighs more than air only because it penetrates the medium by its excess, and the air condenses above it the faster it moves. The cord therefore always breaks at the boundary between natural and accidental motion, beside the contact condensed by the pulley.
Diagram of the pulley with points r, m, n
A small figure at the upper right of the sheet shows the pulley (carrucola) with a weight and the two cords, labelled at the points r, m and n. The numbers 5, 4 and 8 in the text refer to weights carried on these cords. The drawing anchors the whole argument about the wheel and its cords.
