Concave burning mirror: angle of incidence and the converging light pyramid
Reflection geometry, diminution of the pyramid of light, sun measurement and calculations of a mirror's focus
Both faces develop the optics of a concave (burning) mirror and the geometry of the light pyramid that converges toward it. On f. 78v Leonardo constructs the angle of incidence h f i between two equal opposite angles, reverses a light pyramid, and, in cancelled notes, proposes measuring the sun at the summer solstice to calculate what its rays contract to within one braccio, invoking the rule that circles are in proportion as the squares of their diameters. The upper half carries large multiplications (20736, 82944, 331776, 1327104) reckoning the potency of the diminishing pyramid, while f. 73r pursues the diminution of the pyramid with distance in braccia and argues from experience that the rays do not all intersect at the centre o, seeking the chord and sagitta of the mirror's concavity. A short expense list in another, non-mirror hand runs down the middle margin.
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Constructing the angle of incidence between equal opposite angles
From line a d a compass draws the curve d f e; lines a f and b f (parallel to a d) fix the point f, where a semicircle d h g is drawn. Carrying the measure d h onto the semicircle at i g yields the angle of incidence h f i, set between the two equal opposite angles d f h and g f i. The same procedure is then repeated with line a g and c g.
Measuring the sun to calculate the burning mirror's focus
A cancelled note proposes taking the measure of the sun at the summer solstice in June, placing its pyramid at the centre of the world and cutting it at the diameter of the mirror, to see what the parallels a b d f restrict within one braccio a d. Leonardo insists on first obtaining the sun's diameter and distance before making the calculation.
Circles in proportion as the squares of their diameters
A cancelled maxim, written upside down, states that the proportion from circle to circle is as that from square to square built on their diameters. It underpins the numerical estimates of how the light pyramid shrinks.
Calculating the potency of the one-oncia pyramid
Taking n as the base of a pyramid of one oncia, Leonardo tabulates its diminishing power down the pyramid: d 20736, c 82944, b 331776, a 1327104, worked out through columns of multiplication (144, 576, 20736, 41472, 82944, 165888). The smaller circle is reckoned 1/20736 of the larger and 20736 times more potent.
Rays do not intersect at the centre of the concave mirror
If the rays n m had to pass through the centre o they would end only at a b and would not fill the whole concavity c a b d. Since experience shows the contrary, Leonardo concludes that these rays do not intersect at the centre o.
Chord and sagitta of the mirror's concavity
The pyramid a b c is to be cut in the middle of its hypotenuse at o d; the semicircle b f a g c is half its base built on the semidiameter b d (or a d). Because the sought concavity has lips equal to the diameter b c, the line b c is the chord of the required arc, whose sagitta is o d (or m d).
