Bartlett, W. H. C. (William Holms Chambers), 1804-1893 · New York : Barnes · leaf 391
his point,take and retain the constant curvature of the wheel, tillit passes from the latter on the side of the power F.When, therefore, by*the motion of the wheel, the point mof the rope, now at the tangential point, passes to m, theworking point of the force #will have described in its ownpath… … AD R, and representing the quantity of work of the force S, by MECHANICS OF SOLIDS. 387 L, we get L = S.Rst; replacing Shy its value in Eqs. (127) to (130), K + I. W L = ItSjd, 2fi (131); work of thestiffness; in which di represents the quantity d2, d2, n, or d, m Eqs.(127), (128), (129), or (130),…
Mechanics · Acoustics · Optics
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