Concept:
The acceleration of the centre of mass is given by
\[
\vec a_{cm} = \frac{\sum m_i \vec a_i}{\sum m_i}
\]
Similarly, velocity of centre of mass:
\[
\vec v_{cm} = \frac{\sum m_i \vec v_i}{\sum m_i}
\]
Step 1: {Find velocity of centre of mass.}
Since masses are equal:
\[
\vec v_{cm}=\frac{\vec v_1+\vec v_2}{2}
\]
\[
=\frac{4\hat{i}+4\hat{j}}{2}
\]
\[
=2\hat{i}+2\hat{j}
\]
Step 2: {Find acceleration of centre of mass.}
\[
\vec a_{cm}=\frac{\vec a_1+\vec a_2}{2}
\]
\[
=\frac{(6\hat{i}+6\hat{j})+0}{2}
\]
\[
=3\hat{i}+3\hat{j}
\]
Step 3: {Analyze the motion.}
Initial velocity:
\[
(2,2)
\]
Acceleration:
\[
(3,3)
\]
Thus both components vary linearly with time but acceleration is constant.
Hence trajectory satisfies a quadratic relation between \(x\) and \(y\), which represents a parabola.