Rod Wire Forces
1. **Stating the problem:**
We have a right triangle with a vertical side of 1.2 m, a horizontal base of 2.3 m, and a hypotenuse with a distributed load of 5 kN/m acting downward. There is a 6 kN horizontal force acting left at the top of the vertical side. The bottom-left corner has a pinned support with a vertical reaction force, and the bottom-right corner has a fixed support. Additionally, a rod extends from the bottom-left support at 25° and a wire from the top of the rod at 45°, with a 1 kN vertical load at the wire's joint. We need to find the forces in the rod and wire.
2. **Calculate the length of the hypotenuse:**
Using Pythagoras theorem:
$$\text{hypotenuse} = \sqrt{1.2^2 + 2.3^2} = \sqrt{1.44 + 5.29} = \sqrt{6.73} \approx 2.594 \, m$$
3. **Calculate total distributed load on hypotenuse:**
Distributed load = 5 kN/m over 2.594 m:
$$F_{dist} = 5 \times 2.594 = 12.97 \, kN$$
This acts downward at the midpoint of the hypotenuse.
4. **Resolve the 6 kN horizontal force:**
It acts left at the top of the vertical side.
5. **Analyze the rod and wire geometry:**
Rod angle = 25° from horizontal at bottom-left.
Wire angle = 45° from horizontal at top of rod.
6. **Set up equilibrium equations:**
Let $F_r$ be the force in the rod, $F_w$ the force in the wire.
- Horizontal equilibrium:
$$F_r \cos 25^\circ = F_w \cos 45^\circ + 6$$
- Vertical equilibrium:
$$F_r \sin 25^\circ + F_w \sin 45^\circ = 1 + R_v$$
where $R_v$ is the vertical reaction force at the pinned support.
7. **Moment equilibrium about bottom-left support:**
Sum moments to zero to solve for unknowns.
8. **Calculate components:**
$$\cos 25^\circ \approx 0.9063, \sin 25^\circ \approx 0.4226$$
$$\cos 45^\circ = \sin 45^\circ = \frac{\sqrt{2}}{2} \approx 0.7071$$
9. **From horizontal equilibrium:**
$$F_r \times 0.9063 = F_w \times 0.7071 + 6$$
10. **From vertical equilibrium (assuming $R_v$ balances remaining vertical forces):**
$$F_r \times 0.4226 + F_w \times 0.7071 = 1 + R_v$$
11. **Assuming $R_v$ is unknown, focus on rod and wire forces:**
Express $F_w$ from horizontal equation:
$$F_w = \frac{F_r \times 0.9063 - 6}{0.7071}$$
12. **Substitute into vertical equation:**
$$F_r \times 0.4226 + \left(\frac{F_r \times 0.9063 - 6}{0.7071}\right) \times 0.7071 = 1 + R_v$$
Simplify:
$$F_r \times 0.4226 + F_r \times 0.9063 - 6 = 1 + R_v$$
$$F_r (0.4226 + 0.9063) = 7 + R_v$$
$$F_r \times 1.3289 = 7 + R_v$$
13. **If $R_v$ is reaction force, to find $F_r$ and $F_w$ we need $R_v$ or additional info.**
14. **Summary:**
- Length hypotenuse = 2.594 m
- Distributed load total = 12.97 kN
- Rod force $F_r$ and wire force $F_w$ related by:
$$F_w = \frac{0.9063 F_r - 6}{0.7071}$$
- Vertical equilibrium relates $F_r$, $R_v$, and $F_w$.
Without $R_v$, exact $F_r$ and $F_w$ cannot be numerically determined.
**Final answer:**
The forces in the rod and wire satisfy:
$$F_w = \frac{0.9063 F_r - 6}{0.7071}$$
and
$$F_r \times 1.3289 = 7 + R_v$$
where $R_v$ is the vertical reaction force at the pinned support.
Further information about $R_v$ or additional constraints are needed for numeric values.