Since all the forces act in the same plane, there is a single force resultant for this problem. The resultant force is the same FR as before but it is located at a different point Q, which must satisfy the equation
MRo = rOQ × FR
Writing this equation in determinant form and substituting known vectors gives,
2.977k = [0
- rOQz (-0.007596)]i
- [0 - rOQz (-0.08682)]j +
+
[(rOQx (-0.007596) - rOQy(-0.08682)]k
From the i and j terms, rOQz must be zero. However, the k term gives
2.977 = -0.007596 rOQx + 0.08682 rOQy
From inspecting the diagram, it is noted that point Q was chosen to be directly vertical from O. Thus, the rOQx must be zero. This gives,
2.977 = 0.08682 rOQy
Therefore
rOQ = 0i + 34.29j
+ 0k in
Applying the single force FR at the point Q has the
same effect as the two original forces F1 and F2. |