To solve this problem, we need to apply the principles of elastic collision. Given that two particles collide elastically, we must ensure both conservation of momentum and conservation of kinetic energy.
Let's denote the masses of the particles as M and 2M. Their initial velocities are 10 \, \text{m/s} and 5 \, \text{m/s}, respectively. After the collision, their velocities are \upsilon_1 and \upsilon_2.
The total momentum before and after the collision must be equal.
The initial momentum \( p_{\text{initial}} \) is given by:
p_{\text{initial}} = M \cdot 10 + 2M \cdot 5 = 10M + 10M = 20M
The final momentum \( p_{\text{final}} \) is given by:
p_{\text{final}} = M \cdot \upsilon_1 + 2M \cdot \upsilon_2
Setting initial momentum equal to final momentum:
M \cdot \upsilon_1 + 2M \cdot \upsilon_2 = 20M
Dividing the entire equation by M, we get:
\upsilon_1 + 2\upsilon_2 = 20 \quad \text{(Equation 1)}
The total kinetic energy before and after the collision must also be equal.
The initial kinetic energy \( KE_{\text{initial}} \) is:
KE_{\text{initial}} = \frac{1}{2} M (10)^2 + \frac{1}{2} (2M) (5)^2 = 50M + 25M = 75M
The final kinetic energy \( KE_{\text{final}} \) is:
KE_{\text{final}} = \frac{1}{2} M \cdot \upsilon_1^2 + \frac{1}{2} (2M) \cdot \upsilon_2^2
= \frac{M}{2} \upsilon_1^2 + M \upsilon_2^2
Setting initial kinetic energy equal to final kinetic energy:
\frac{M}{2} \upsilon_1^2 + M \upsilon_2^2 = 75M
Dividing the entire equation by M, we get:
\frac{1}{2} \upsilon_1^2 + \upsilon_2^2 = 75 \quad \text{(Equation 2)}
From Equation 1: \upsilon_1 = 20 - 2\upsilon_2
Substitute \upsilon_1 in Equation 2:
\frac{1}{2} (20 - 2\upsilon_2)^2 + \upsilon_2^2 = 75
Simplify and solve the quadratic equation:
200 - 40\upsilon_2 + 2\upsilon_2^2 + \upsilon_2^2 = 75
3\upsilon_2^2 - 40\upsilon_2 + 125 = 0
Using the quadratic formula, we find the solution for \upsilon_2:
\upsilon_2 = \frac{-(-40) \pm \sqrt{(-40)^2 - 4 \cdot 3 \cdot 125}}{2 \cdot 3}
Calculate to get:
\upsilon_2 \approx 6.3 \, \text{m/s}
Substitute \upsilon_2 \approx 6.3 into Equation 1 to get \upsilon_1:
\upsilon_1 = 20 - 2 \times 6.3 = 20 - 12.6 = 7.4 \, \text{m/s}
As shown below, bob A of a pendulum having a massless string of length \( R \) is released from 60° to the vertical. It hits another bob B of half the mass that is at rest on a frictionless table in the center. Assuming elastic collision, the magnitude of the velocity of bob A after the collision will be (take \( g \) as acceleration due to gravity):

