Power of Water Falling on Mill-Wheels at Various Obliquities
With a note on why water bubbles are hemispheres while air bubbles are perfect spheres
The sheet studies the driving force of water falling onto the paddles of a mill-wheel, comparing the weight and power of water delivered along different oblique paths from a single height. A large central diagram lettered K, v, f, e, S, i, x, y sets out the geometry of the falling streams and the paddles e a and f b, while a smaller drawing shows a wheel set half-submerged so its blades cut the water edge-on going down and meet it face-on coming up. In an upper-right note Leonardo asks why bubbles made by water are hemispherical whereas bubbles of air are perfectly round.
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Why water bubbles are hemispheres and air bubbles perfect spheres
Leonardo asks why the bubbles that water makes are half-round while those of air are perfectly round. He reasons that the base of the hemisphere meets the water in spherical right angles and the contact gives no projection above itself that the weight could bend and buckle.
A water-wheel set half-submerged, paddles turning edge-on then face-on
A note over a small wheel drawing directs that it stand half under the water, with the blades passing underwater edge-on (per taglio) and emerging face-on out of the water, so that the fall of water is fully exploited. The labels a and b mark the wheel.
Weighing the power of water K e against K f on the paddles
Taking the line Kv as 27 and vf as 20, Leonardo argues that the water Kv (that is Ke) weighs 27 pounds and acts on blade e a with all its power, while the water Kf of 47 pounds acts on blade f b with only half its power, 23 and 1/2 pounds. He concludes the power of K e exceeds that of K f by half a pound of water.
True power of falling water at obliquities K S, K i, K x, K y
The demonstration sets water falling from height K e onto the low point S t along oblique paths K S, K i, K x and K y. The perpendicular fall K S strikes paddle e a with all its weight at power 4; the oblique K i strikes paddle f b at f, falling one and a half times as far but losing half its weight, so that its effective power drops from a would-be 6 to 3, one degree less than the first wheel.
