The point and forces of interest are laid out as follows:
Taking clockwise as positive, the moment about the pulley center, O, is
which is the answer to part (a). We could do essentially the same thing to get the moment about point A, but just to throw in a bit of variety, we’ll start by taking the static equivalent of the forces at O
and transforming the moment to point A:
or 600\:\rm{lb}\cdot \rm{in} counterclockwise. This is the answer to part (b).
Last modified: January 22, 2009 at 8:32 PM.