Question 3.SP.6: Determine the components of the single couple equivalent to ......

Determine the components of the single couple equivalent to the two couples shown.

STRATEGY: Look for ways to add equal and opposite forces to the diagram that, along with already known perpendicular distances, will produce new couples with moments along the coordinate axes. These can be combined into a single equivalent couple.

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In this problem, we are given a system of forces and we want to find the equivalent single couple that can replace the original system.
Step 1:
We start by simplifying the computations. We attach two equal and opposite 20-lb forces at point A. This allows us to replace the original 20-lb-force couple with two new 20-lb-force couples: one lying in the zx plane and the other in a plane parallel to the xy plane.
Step 2:
Next, we represent these three couples using three couple vectors, denoted as Mx, My, and Mz, directed along the coordinate axes. These vectors represent the moments of the respective couples.
Step 3:
We calculate the moments of the given forces. The moment Mx is calculated by multiplying the magnitude of the force (-30 lb) with the perpendicular distance (18 in.) from the line of action of the force to the origin. Similarly, My is calculated by multiplying the magnitude of the force (20 lb) with the perpendicular distance (12 in.) from the line of action of the force to the origin. Finally, Mz is calculated by multiplying the magnitude of the force (20 lb) with the perpendicular distance (9 in.) from the line of action of the force to the origin.
Step 4:
We represent the equivalent single couple M by combining the moments Mx, My, and Mz. The vector M is given by -(540 lb·in.)i + (240 lb·in.)j + (180 lb·in.)k, where i, j, and k are unit vectors along the x, y, and z axes, respectively.
Step 5:
Alternatively, we can also obtain the components of the equivalent single couple M by computing the sum of the moments of the four given forces about an arbitrary point. Selecting point D, we calculate the moment MD. This can be done by taking the cross product of the position vector j with the force vector -30 lbk, and adding it to the cross product of the position vector (9 in.)j - (12 in.)k with the force vector -20 lbi.
Step 6:
After computing the cross products and simplifying the expression, we obtain the same result as before, which is -(540 lb·in.)i + (240 lb·in.)j + (180 lb·in.)k.
In summary, by attaching two equal and opposite 20-lb forces at point A, we can replace the original 20-lb-force couple with two new 20-lb-force couples. The moments of these couples can be represented by the vectors Mx, My, and Mz. By combining these moments, we obtain the equivalent single couple M, which can also be calculated by taking the sum of the moments of the four given forces about an arbitrary point.

Final Answer

MODELING: You can simplify the computations by attaching two equal and opposite 20-lb forces at A (Fig. 1). This enables you to replace the original 20-lb-force couple by two new 20-lb-force couples: one lying in the zx plane and the other in a plane parallel to the xy plane.

ANALYSIS: You can represent these three couples by three couple vectors \mathbf{M}_x, \mathbf{M}_y \text {, and } \mathbf{M}_z directed along the coordinate axes (Fig. 2). The corresponding moments are

\begin{array}{c}M_x=-(30 ~\mathrm{lb})(18 ~\mathrm{in} .)=-540 ~\mathrm{lb}\cdot \text { in. } \\M_y=+(20 ~\mathrm{lb})(12 ~\mathrm{in} .)=+240 ~\mathrm{lb}\cdot \text { in. } \\M_z=+(20 ~\mathrm{lb})(9 ~\mathrm{in} .)=+180 ~\mathrm{lb}\cdot \text { in. }\end{array}

These three moments represent the components of the single couple M equivalent to the two given couples. You can write M as

\mathbf{M}=-(540 ~\mathrm{lb} \cdot \text { in. }) \mathbf{i}+(240 ~\mathrm{lb} \cdot \mathrm{in} .) \mathbf{j}+(180 ~\mathrm{lb} \cdot \mathrm{in} .) \mathbf{k}

REFLECT and THINK: You can also obtain the components of the equivalent single couple M by computing the sum of the moments of the four given forces about an arbitrary point. Selecting point D, the moment is (Fig. 3)

\mathbf{M}=\mathbf{M}_D=(18 \text { in. }) \mathbf{j} \times(-30 ~\mathrm{lb}) \mathbf{k}+[(9 \text { in. }) \mathbf{j}-(12 \text { in. }) \mathbf{k}] \times(-20 ~\mathrm{lb}) \mathbf{i}

After computing the various cross products, you get the same result, as

\mathbf{M}=-(540 ~\mathrm{lb} \cdot \mathrm{in} .) \mathbf{i}+(240 ~\mathrm{lb} \cdot \mathrm{in} .) \mathbf{j}+(180 ~\mathrm{lb} \cdot \mathrm{in} .) \mathbf{k}

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