To solve this problem, we need to analyze the collision between two particles of equal mass. Let's go through the solution step-by-step:
Prior to the collision, let the initial velocity of the moving particle be $v_0$. The stationary particle has an initial velocity of $0$.
The initial kinetic energy of the system is solely due to the moving particle. Thus,
Initial \ Kinetic \ Energy = \frac{1}{2}mv_0^2
After the collision, let the velocities of the two particles be $v_1$ and $v_2$, respectively.
The final kinetic energy is given to be 50\% greater than the initial kinetic energy. Therefore,
Final \ Kinetic \ Energy = 1.5 \times \frac{1}{2}mv_0^2 = \frac{3}{4}mv_0^2
The expression for the final kinetic energy is:
\frac{1}{2}m(v_1^2 + v_2^2) = \frac{3}{4}mv_0^2
Simplifying the equation:
v_1^2 + v_2^2 = \frac{3}{2}v_0^2
By the principle of conservation of momentum, the total momentum before and after the collision should remain constant. Therefore,
mv_0 = mv_1 + mv_2 \\ v_0 = v_1 + v_2
We have two equations:
To find the magnitude of the relative velocity between the two particles after the collision, calculate:
(v_1 - v_2)^2 = v_1^2 + v_2^2 - 2v_1v_2
Using the first equation, v_1 = v_0 - v_2 , substitute in the second equation:
(\frac{1}{2}v_0^2) + 2(v_0 - v_2)v_2 = (v_1 - v_2)^2 + \frac{3}{2}v_0^2 \\ \Rightarrow (v_1 - v_2)^2 = \frac{3}{2}v_0^2 - (v_1 - v_2)^2
Solving this gives:
v_1 - v_2 = \sqrt{4v_0^2 - \frac{3}{2}v_0^2} \\ v_1 - v_2 = \sqrt{2}v_0
The magnitude of the relative velocity between the two particles after the collision is therefore \sqrt{2}v_0.
Hence, the correct answer is \sqrt{2}v_0.

