The tension in the left rope is approximately 120 N.
Analyze the forces:
There are three forces acting on the rod:
Tension in the left rope (T1)
Tension in the right rope (T2)
Weight of the monkey (W) acting downwards at 0.5 m from the right end.
2. Apply equilibrium conditions:
Since the rod is in static equilibrium (not moving or accelerating), the sum of forces and torques must be zero.
3. Sum of forces in the vertical direction:
T1y + T2y - W = 0
4. Sum of forces in the horizontal direction:
T1x = 0 (as the left rope makes an angle of 150° with the horizontal, its horizontal component is zero)
5. Sum of torques around the pivot point (right end of the rod):
(0.5 m)W - (3.00 m)T1y = 0 (counterclockwise torques are positive)
6. Solve the system of equations:
We have three equations and three unknowns (T1y, T2y, and T2x).
From equation 4, we know T1x = 0.
Substitute this into equation 3: T1y + T2y - W = 0.
From equation 5, we can express T1y as: T1y = (0.5 m * W) / (3.00 m).
Substitute this expression for T1y in the modified equation 3: (0.5 m * W) / (3.00 m) + T2y - W = 0.
Solve for T2y: T2y = (2/3)W.
7. Calculate the tension in the left rope (T1):
Use the trigonometric relationship for the left rope: sin(150°) = T1y / T1.
Since sin(150°) = -0.5, we have -0.5 = (2/3)W / T1.
Solve for T1: T1 = (2/3)W / (-0.5).
Substitute the weight of the monkey (W = 90 N): T1 = (2/3) * 90 N / (-0.5).
Calculate the tension: T1 ≈ 120 N.