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ads.harvard.eduThis is often defined to be that point where the force of gravity can be considered to be acting. Mathematically that would mean that all torques produced by gravity would vanish about that point so that ×∑ =∑ × =∫ [×ρ( ) ] = ii rg fi ri fi V r r g dV 0 r r r r r rr. (6.1.2) In a Cartesian coordinate frame this could be expressed in ...