Step 1: Understanding the Concept:
This problem involves a one-dimensional (head-on) collision. To solve it, we need to apply two fundamental principles: the conservation of linear momentum and the definition of the coefficient of restitution.
Step 2: Setting up the Equations:
Let the initial velocities be \(u_1 = v\) and \(u_2 = 0\).
Let the masses be \(m_1 = m\) and \(m_2 = 2m\).
Let the final velocities be \(v_1\) and \(v_2\).
Equation from Conservation of Momentum:
\[ m_1 u_1 + m_2 u_2 = m_1 v_1 + m_2 v_2 \]
\[ m(v) + 2m(0) = m(v_1) + 2m(v_2) \]
Dividing by \(m\):
\[ v = v_1 + 2v_2 \quad \cdots(1) \]
Equation from Coefficient of Restitution (e):
\[ e = \frac{\text{velocity of separation}}{\text{velocity of approach}} = \frac{v_2 - v_1}{u_1 - u_2} \]
\[ e = \frac{v_2 - v_1}{v - 0} \]
\[ ev = v_2 - v_1 \quad \cdots(2) \]
Step 3: Solving the Equations:
We have a system of two linear equations with two unknowns, \(v_1\) and \(v_2\). We need to find the ratio \(v_1/v_2\).
From equation (2), we can express \(v_1\) as \(v_1 = v_2 - ev\).
Substitute this expression for \(v_1\) into equation (1):
\[ v = (v_2 - ev) + 2v_2 \]
\[ v = 3v_2 - ev \]
\[ v + ev = 3v_2 \implies v(1+e) = 3v_2 \]
\[ v_2 = \frac{v(1+e)}{3} \]
Now, substitute this result for \(v_2\) back into the expression for \(v_1\):
\[ v_1 = v_2 - ev = \frac{v(1+e)}{3} - ev \]
\[ v_1 = \frac{v(1+e) - 3ev}{3} = \frac{v + ve - 3ev}{3} = \frac{v - 2ev}{3} = \frac{v(1-2e)}{3} \]
Step 4: Finding the Ratio:
Now we can find the ratio of the velocities, \(\frac{v_1}{v_2}\).
\[ \frac{v_1}{v_2} = \frac{\frac{v(1-2e)}{3}}{\frac{v(1+e)}{3}} \]
\[ \frac{v_1}{v_2} = \frac{1-2e}{1+e} \]
This matches option (D).