A heavy iron bar of weight 12 kg is having its one end on the ground and the other on the shoulder of a man. The rod makes an angle \(60^\circ\) with the horizontal, the weight experienced by the man is :
To calculate the weight experienced by the man, we need to consider the component of the weight of the iron bar that acts along the line touching the man's shoulder, because the other component will act against the support provided by the ground.
The weight of the bar is given as 12 kg. When the rod makes an angle \(60^\circ\) with the horizontal, the component of the weight acting along the direction of the man's shoulder can be found using the concept of resolving vectors.
The weight component along the vertical (which is relevant here as the force experienced by the bar due to gravity should be analyzed along its length) is given by:
\(W_{man} = W \cdot \sin(\theta)\)
Where:
Let's substitute the values:
\(W_{man} = 12 \cdot \sin(60^\circ) = 12 \cdot \frac{\sqrt{3}}{2}\)
Calculating this gives:
\(W_{man} = 12 \cdot 0.866 = 10.392 \text{ N}\)
However, since the weight experienced by the man is given in terms of mass under gravitational effect, convert Newtons back to mass equivalent in kg. Remember, 1 kg of force under Earth's gravity exerts approximately 9.8 N:
\(m_{man} = \frac{10.392}{9.8} \approx 1.06 \text{ kg}\)
Revisiting the problem, this approach simplifies as:
The component of weight contributing to the man's experienced load will be horizontally resolved and should be:
\(W_{effective} = W \cdot \cos(\theta) = 12 \cdot \cos(60^\circ) = 12 \cdot 0.5 = 6 \text{ kg}\) which breaks to a result for visualization directly as 3 kg horizontally actually lifting the reference weight converting equivalent experience lifting.
Thus, the weight experienced by the man is 3 kg. The correct answer is the option \(3 \text{ kg}\).
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).
A bob of mass \(m\) is suspended at a point \(O\) by a light string of length \(l\) and left to perform vertical motion (circular) as shown in the figure. Initially, by applying horizontal velocity \(v_0\) at the point ‘A’, the string becomes slack when the bob reaches at the point ‘D’. The ratio of the kinetic energy of the bob at the points B and C is: 
Two light beams fall on a transparent material block at point 1 and 2 with angle \( \theta_1 \) and \( \theta_2 \), respectively, as shown in the figure. After refraction, the beams intersect at point 3 which is exactly on the interface at the other end of the block. Given: the distance between 1 and 2, \( d = \frac{4}{3} \) cm and \( \theta_1 = \theta_2 = \cos^{-1} \left( \frac{n_2}{2n_1} \right) \), where \( n_2 \) is the refractive index of the block and \( n_1 \) is the refractive index of the outside medium, then the thickness of the block is …….. cm.

Let \( y^2 = 12x \) be the parabola and \( S \) its focus. Let \( PQ \) be a focal chord of the parabola such that \( (SP)(SQ) = \frac{147}{4} \). Let \( C \) be the circle described by taking \( PQ \) as a diameter. If the equation of the circle \( C \) is: \[ 64x^2 + 64y^2 - \alpha x - 64\sqrt{3}y = \beta, \] then \( \beta - \alpha \) is equal to: