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Mechanics of engineering. Comprising statics and dynamics of solids: and the mechanics of the materials of constructions, or strength and elasticity of beams, columns, arches, shafts, etc (1888)

Church, Irving P[orter], 1851- [from old catalog] · New York, J. Wiley & sons · leaf 190

An illustration from Mechanics of engineering. Comprising statics and dynamics of solids: and the mechanics of the materials of constructions, or strength and elasticity of beams, columns, arches, shafts, etc, 1888, leaf 190
olved alongCA and CB, produces (nearly) equalpressures, each being i\T = P -f- 2 cos <*, at the two axles ofthe friction-wheels, which rub against their fixed plumber-blocks. R = P -\- Pi -f- 6r1? and .*. contains the unknown P,but approximately = G -\- 2P^ i.e., is nearly the same (in thiscase)… … Fig. 179. = 2fJV i2*r =a1 a, cos a fP27tr. Whereas, if C revolved in a fixed bearing, =fP27rr. Work lost per revol. without friction-wheels, Apparently, then, there is a saving of work in the ratio rx\ax cos a, but strictly the P is not quite the same in the two cases ;for with friction-wheels the…

Mechanics, Applied · Engineering · Strength of materials

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