The body is subjected to three forces:
- The weight of the body (140 lb) acting downward.
- A force of 80 lb acting at an angle of 30° to the horizontal.
- The tension \( T \) acting at an angle \( \theta \) to the horizontal.
Resolve the 80 lb force into horizontal and vertical components:
- Horizontal component: \( 80 \cos(30°) \)
- Vertical component: \( 80 \sin(30°) \)
For the body to be in equilibrium, the sum of the forces in both the horizontal and vertical directions must be zero.
\[ T \cos(\theta) = 80 \cos(30°) \]
\[ T \sin(\theta) + 80 \sin(30°) = 140 \]
First, calculate the components of the 80 lb force:
- \( 80 \cos(30°) = 80 \times \frac{\sqrt{3}}{2} = 40\sqrt{3} \approx 69.28 \) lb
- \( 80 \sin(30°) = 80 \times \frac{1}{2} = 40 \) lb
Using the horizontal equilibrium equation:
\[ T \cos(\theta) = 69.28 \]
Using the vertical equilibrium equation:
\[ T \sin(\theta) + 40 = 140 \]
\[ T \sin(\theta) = 100 \]
Divide the vertical equation by the horizontal equation to find \( \theta \):
\[ \tan(\theta) = \frac{100}{69.28} \]
\[ \theta = \tan^{-1}\left(\frac{100}{69.28}\right) \approx 29.5° \]
Now, solve for \( T \) using \( \cos(\theta) \):
\[ T = \frac{69.28}{\cos(29.5°)} \approx 81.2 \text{ lb} \]
- Tension \( T \): 81.2 lb
- Angle \( \theta \): 29.5°