Maurer, Edward R. (Edward Rose), b. 1869 · New York : John Wiley & sons, inc.; [etc., etc.] · leaf 31
Pi, and P2 about that point; but F has no momentabout such point, and hence the moment of R equals the sum of the momentsof Pi and P2 (the moment of the couple). It follows from the foregoing that a force R can he resolved into a force equaland parallel to R, and a couple whose moment equals that… … Fig. 27 Let R (Fig. 27) be the force to be resolved, and O a point through whichthe line of action of the force component is to pass. First we resolve R into two concurrent components, one of whichpasses through 0; take any point on R (as a)for the point of concurrence and any direction(as ab) for…
Mechanics
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