Determine the moment of the force F in Fig. (a) about point A.
Determine the moment of the force F in Fig. (a) about point A.
The force F and point A lie in the xy-plane. Problems of this type may be solved using either the vector method (r × F) or the scalar method (Fd). For illustrative purposes, we use both methods.
Vector Solution
Recall that the three steps in the vector method are to write F in vector form, choose r and write it in vector form, and then evaluate the cross product r × F. Writing F in vector form, we get
F=-(\frac{4}{5} )1000i+(\frac{3}{5} )1000j=-800+600j NThere are several good choices for r in this problem, three of which are r_{AB}, r_{AC}, and r_{AD}. Choosing
r=r_{AB}= −120i + 180j
the moment about point A is
M_{A} =r × F=r_{AB} × F=\left|\begin{matrix} i & j & k \\ -120 & 180 & 0 \\ -800 & 600 & 0 \end{matrix} \right|Expanding this determinant, we obtain
M_{A} =k[(800)(−120) + (800)(180)]=72000k N · mm
The magnitude of M_{A} is 72000 N · mm. Note that the direction of M_{A} is the positive z direction, which by the right-hand rule means that the moment about point A is counterclockwise.
Scalar Solution
In Fig. (b), we have resolved the force into the rectangular components F_{1} and F_{2} at point B. The moment arm of each component about point A (the perpendicular distance between A and the line of action of the force) can be determined by inspection. The moment arms are d_{1} = 180mm for F_{1} and d_{2} = 120mm for F_{2}, as shown in Fig. (b).The moment of F about A now can be obtained by the principle of moments. Nothing that the moment of F_{1} is counterclockwise, whereas the moment of F_{2} is clockwise, we obtain
\underset{+}{\curvearrowleft } M_{A}=F_{1}d_{1}-F_{2}d_{2}=800(180) − 600(120) = 72000 N · mmNote that the sense of M_{A} is counterclockwise. Applying the right-hand rule, the vector representation of the moment is
M_{A}=72000k N·mm
Recall that a force, being a sliding vector, can be moved to any point on its line of action without changing its moment. In Fig. (c) we have moved F to point C. Now the moment arm of F_{1} about A is d_{1} = 90mm., and the moment arm of F_{2} is zero. Hence, the moment of F about A is
\underset{+}{\curvearrowleft } M_{A}=F_{1}d_{1}=800(90) = 72000 N · mmcounterclockwise, as before.Another convenient location for F would be point D in Fig. (c). Here the moment arm of F_{1} about A is zero, whereas the moment arm of F_{2} is 120 mm, which again yields M_{A} = 72000N · mm counterclockwise.