Introduction
This is a problem involving static equilibrium. The horizontal rod is supported at one end by a hinge and at the other end by a cable inclined at an angle. To solve this, we apply the conditions of equilibrium:
- Sum of all horizontal forces = 0
- Sum of all vertical forces = 0
- Sum of all torques (moments) = 0
Given Data
- Mass of rod, m = 10 kg
- Length of rod, L = 12 m
- Angle between cable and rod = 30º
- Acceleration due to gravity, g = 9.8 m/s²
- Weight of rod, W = mg = 10 × 9.8 = 98 N
Step 1: Torque Equation (About the Hinge)
Let T be the tension in the cable. The weight of the rod acts at its center (L/2 = 6 m from hinge). The tension provides a vertical component (Tsinθ) which produces torque in the opposite direction to the weight.
∑τ = 0 ⇒ T × L × sin(30º) = W × (L/2)
T × 12 × 0.5 = 98 × 6
T × 6 = 588
T = 588 / 6 = 98 N
Step 2: Vertical Force Balance
Let the vertical reaction at the hinge be Rv.
∑Fvertical = 0 ⇒ Rv + Tsin(30º) = W
Rv + 98 × 0.5 = 98
Rv + 49 = 98 ⇒ Rv = 49 N
Step 3: Horizontal Force Balance
Let the horizontal reaction at the hinge be Rh.
∑Fhorizontal = 0 ⇒ Rh = Tcos(30º)
Rh = 98 × cos(30º) = 98 × 0.866 ≈ 84.87 N
Step 4: Total Reaction Force at the Hinge
R = √(Rh² + Rv²) = √(84.87² + 49²) ≈ √(7201.6 + 2401) ≈ √9602.6 ≈ 98 N
Final Answers
- Tension in the cable: 98 N
- Horizontal force by hinge: 84.87 N
- Vertical force by hinge: 49 N
- Total hinge force: ~98 N
Conclusion
By applying the principles of static equilibrium, we determined that the tension in the supporting cable is 98 N and the hinge provides both horizontal and vertical support to maintain the system in balance. This problem illustrates the practical application of torque and force balance in real-world structures.