Given:
- Weight of the bar \( W = 12 \, \text{kg} \),
- The bar makes an angle \( \theta = 60^\circ \) with the horizontal,
- Let \( N_1 \) be the normal force at the ground and \( N_2 \) be the force experienced by the man’s shoulder.
Condition for equilibrium about the pivot:
Torque about \( O = 0 \).
Taking moments about \( O \):
\(120 \left(\frac{L}{2} \cos 60^\circ \right) - N_2 L = 0\)
Simplifying:
\(N_2 = \frac{120}{2} \cdot \frac{1}{2} = 30 \, \text{N}.\)
Converting to weight experienced:
\(\text{Weight} = \frac{30 \, \text{N}}{10 \, \text{m/s}^2} = 3 \, \text{kg}.\)
The Correct answer is: 3 kg
A force \( \vec{f} = x^2 \hat{i} + y \hat{j} + y^2 \hat{k} \) acts on a particle in a plane \( x + y = 10 \). The work done by this force during a displacement from \( (0,0) \) to \( (4m, 2m) \) is Joules (round off to the nearest integer).
Let $ P_n = \alpha^n + \beta^n $, $ n \in \mathbb{N} $. If $ P_{10} = 123,\ P_9 = 76,\ P_8 = 47 $ and $ P_1 = 1 $, then the quadratic equation having roots $ \alpha $ and $ \frac{1}{\beta} $ is: