Bartlett, W. H. C. (William Holms Chambers), 1804-1893 · New York : Barnes · leaf 197
almoments; Adding these equations together, and denoting themoment of inertia in reference to the axis 0 H by Ih andthat in reference to L M by I, we find 1 = Ix + D2 (m + m + m + &o.) + 2D(md + md+ m d + &c.); but m + m + m + &c.is the entire mass ofthe body, and md +md + md + &c.… … resulting value; I = Ix + MD (65); conclusion. whence we conclude that, the moment of inertia of a body,taken with reference to any axis, is equal to the moment ofinertia taken with reference to a parallel axis passing throughthe centre of gravity, increased by the product of the entiremass of the…
Mechanics · Acoustics · Optics
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