v0/4
√2v0
v0/2
v0√2
Let m be the mass of each particle. The initial kinetic energy is given by:
KE_initial = (1/2)mv0^2
Since the second particle is stationary, its initial kinetic energy is 0. After the collision, the total kinetic energy is 50% of the initial kinetic energy:
KE_final = 0.5 * KE_initial = 0.5 * (1/2)mv0^2 = (1/4)mv0^2
Let v1 and v2 be the final velocities of the first and second particles, respectively. By conservation of momentum:
mv0 = mv1 + mv2
v0 = v1 + v2
By conservation of kinetic energy (in this case, 50% is retained):
(1/4)mv0^2 = (1/2)mv1^2 + (1/2)mv2^2
v0^2 = 2(v1^2 + v2^2)
We have a system of two equations with two unknowns:
From equation (1), v2 = v0 - v1. Substitute this into equation (2):
v0^2 = 2(v1^2 + (v0 - v1)^2)
v0^2 = 2(v1^2 + v0^2 - 2v0v1 + v1^2)
v0^2 = 4v1^2 - 4v0v1 + 2v0^2
0 = 4v1^2 - 4v0v1 + v0^2
This is a quadratic equation in v1. We can solve it using the quadratic formula:
v1 = [4v0 ± √(16v0^2 - 16v0^2)] / 8
v1 = [4v0 ± 0] / 8
v1 = v0/2
Therefore, the final speed of the first particle is v0/2.