Concept:
Linear momentum is conserved during collision.
Since all masses are equal, we can work directly with velocity vectors.
Step 1: Find the initial resultant momentum.
The three particles move toward the centroid along the three medians of an equilateral triangle.
The angle between any two velocity vectors is
\[
120^\circ.
\]
Hence,
\[
\vec v_A+\vec v_B+\vec v_C=0.
\]
Therefore,
\[
\vec P_{\text{initial}}=0.
\]
Step 2: Apply conservation of momentum after collision.
After collision,
\[
\vec v_A'=0.
\]
Particle \(B\) retraces its path with speed \(v\).
Hence,
\[
\vec v_B'=-\vec v_B.
\]
Since total momentum must remain zero,
\[
\vec v_A'+\vec v_B'+\vec v_C'=0
\]
\[
0-\vec v_B+\vec v_C'=0.
\]
Thus,
\[
\vec v_C'=\vec v_B.
\]
Step 3: Interpret the result.
Initially \(B\) was moving from \(B\) toward \(G\).
Therefore,
\[
\vec v_C'
\]
has magnitude \(v\) and direction along \(BG\).
\[\begin{aligned}
\boxed{\text{Speed }=v,\ \text{direction along }BG}
\end{aligned}\]
Hence, option \(\mathbf{(B)}\) is correct.