Lines of natural and accidental obliquity; descent and impetus
How a sloping line curves toward the center of the world, and the impetus gained in descent
Leonardo distinguishes the line of 'natural' obliquity, which curves ever more sharply as it nears the center of the world, from the straight line of 'mathematical' obliquity that gains equal nearness to the horizontal along its whole length. A body dragged up the natural slope meets constant resistance, while on the accidental slope its resistance varies with height. Descending, a body gains impetus at every degree along the natural obliquity, but on the accidental obliquity it gains impetus in one part, loses it in another, stops, and turns back. A large quarter-circle construction of radiating chords and nested arcs at lower center gives the geometry of these oblique lines.
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Natural versus mathematical obliquity
The line of natural obliquity is nowhere of equal curvature, growing more or less curved as it nears the center of the world; the line of mathematical obliquity is straight and gains one degree of nearness to the horizontal in every part of its length (labels e a - f b - g c).
Impetus gained in descent, and reversal on the accidental slope
A body descending the natural obliquity acquires power of impetus at every degree; but one descending the accidental obliquity gains impetus in one part of the motion, loses it in another, comes to rest, and in place of stopping turns back.
Fan of arcs constructing the oblique line
A large quarter-circle at lower center is filled with radiating chords and a family of overlapping arcs, the geometric construction underlying the lines of natural and mathematical obliquity discussed in the text.
