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Technical mechanics, statics and dynamics (1917)

Maurer, Edward R. (Edward Rose), b. 1869 · New York : John Wiley & sons, inc.; [etc., etc.] · leaf 98

An illustration from Technical mechanics, statics and dynamics, 1917, leaf 98
% Z2, the coordi-nates of B, etc. Also let W denote theweight of the whole body, Q its centerof gravity, and x, y, z, the coordinatesof Q. Since W is the resultant of Wi,W2, W3, etc., the moment of W aboutany Hne equals the algebraic sum of the moments of Wi, W2, W3, etc., about the same line (Art.… … Fig. 156 Thus, taking Wx = Wixi + W2X2 + W3X3 + •> from which equation x can be determined. Similarly, by taking momentsabout the x-axis we can get y. To get z, we imagine the body turned until they-axis is vertical, — the coordinate axes are assumed fixed to the body, — andthen take moments…

Mechanics

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