Angle between the directions of motion of the two particles is 90Β°
To solve this problem, we need to analyze an elastic collision between two identical particles. Here's a detailed step-by-step solution to evaluate each given statement:
The collision is elastic, which means both momentum and kinetic energy are conserved. Initially, particle \( p_1 \) has mass \( m \) and velocity \( v \), while particle \( p_2 \) is stationary.
The vector components of momentum are conserved both in the x-direction and y-direction.
After the collision, particle \( p_1 \) is deflected at an angle \( \theta = 30^\circ \). The final speed of \( p_1 \) can be determined using trigonometric components:
\(v_{1f} = v \cos(30^\circ) = v \times \frac{\sqrt{3}}{2}\)
This matches the statement given as one of the options:
Speed of \( p_1 \) is \( \frac{\sqrt{3}}{2} V \)
Hence, this statement is true.
Using the conservation of kinetic energy:
\(\frac{1}{2}mv^2 = \frac{1}{2}m(v_{1f})^2 + \frac{1}{2}m(v_{2f})^2\)
Substituting \(v_{1f} = \frac{\sqrt{3}}{2}v\), we find:
\(\frac{1}{2}mv_{2f}^2 = \frac{1}{2}mv^2 - \frac{1}{2}m\left(\left(\frac{\sqrt{3}}{2}v\right)^2\right)\)
\( \Rightarrow \frac{1}{2}mv_{2f}^2 = \frac{1}{4}mv^2 \)
Thus, \( v_{2f}^2 = \frac{1}{2}v^2 \), meaning:
The kinetic energy of \( p_2 \) is 25% of the initial total energy, confirming:
Kinetic energy of \( p_2 \) is 25% of the total energy
Hence, this statement is true too.
Due to conservation of momentum in perpendicular directions, and since the initial momentum vector of \( p_2 \) was zero, the two particles move perpendicularly after the collision. Hence:
Angle between the directions of motion of the two particles is 90Β°
This statement is true as well.
The kinetic energy of the center of mass will not change because it depends on the system's total initial and final velocities, which remain the same for an isolated system.
This disproves the last statement:
The kinetic energy of the centre of mass of \( p_1 \) and \( p_2 \) decreases
This is false.
The correctly validated statements are:
In order to achieve the static equilibrium of the see-saw about the fulcrum \( P \), shown in the figure, the weight of Box B should be _________ kg, if the weight of Box A is 50 kg.

A particle of mass 1kg, initially at rest, starts sliding down from the top of a frictionless inclined plane of angle \(\frac{π}{6}\)\(\frac{\pi}{6}\) (as schematically shown in the figure). The magnitude of the torque on the particle about the point O after a time 2seconds is ______N-m. (Rounded off to nearest integer) 
(Take g = 10m/s2)

