Reaction Forces 5897C6
1. **Problem Statement:**
Given lengths $L_1=2$ in, $L_2=3$ in, $L_3=6$ in, and $L_4=4$ in, and a downward force $F$ applied at point C, find the reactions at supports A and D for the structural system described.
2. **Understanding the Structure:**
- The top horizontal bar extends from A to C, with segments $L_1$ and $L_2$.
- The bottom bar extends vertically under B to D, with segments $L_3$ and $L_4$.
- Force $F$ acts downward at C.
- Supports at A and D provide reaction forces.
3. **Assumptions and Formulas:**
- Assume the structure is in static equilibrium.
- Sum of vertical forces must be zero: $$\sum F_y = 0$$
- Sum of moments about any point must be zero: $$\sum M = 0$$
4. **Define Reaction Forces:**
- Let $R_A$ be the vertical reaction at support A.
- Let $R_D$ be the vertical reaction at support D.
5. **Calculate Total Lengths:**
- Total length of top bar $AC = L_1 + L_2 = 2 + 3 = 5$ in.
- Total length of bottom bar $BD = L_3 + L_4 = 6 + 4 = 10$ in.
6. **Sum of Vertical Forces:**
$$R_A + R_D - F = 0 \implies R_A + R_D = F$$
7. **Sum of Moments about A:**
Taking moments about point A to eliminate $R_A$:
- Moment arm of $F$ is $L_1 + L_2 = 5$ in.
- Moment arm of $R_D$ is total horizontal distance from A to D. Since D is at the bottom bar end, horizontal distance is $L_1 + L_2 = 5$ in (assuming vertical bar under B does not affect horizontal distance).
Moment equilibrium:
$$-F \times 5 + R_D \times 5 = 0$$
8. **Solve for $R_D$:**
$$R_D \times 5 = F \times 5 \implies R_D = F$$
9. **Solve for $R_A$:**
From step 6:
$$R_A + R_D = F \implies R_A + F = F \implies R_A = 0$$
10. **Interpretation:**
- Reaction at A is zero.
- Reaction at D equals the applied force $F$.
**Final answer:**
$$R_A = 0, \quad R_D = F$$