Correct answer: −2î − ĵ + k̂
The position vector of the center of mass is given by \( \vec{R}_{cm} = \frac{m_1 \vec{r}_1 + m_2 \vec{r}_2}{m_1 + m_2} \). Substituting \( m_1 = 1 \), \( \vec{r}_1 = \hat{i} + 2\hat{j} + \hat{k} \), \( m_2 = 3 \), and \( \vec{r}_2 = -3\hat{i} - 2\hat{j} + \hat{k} \), we get \( \vec{R}_{cm} = \frac{(1)(\hat{i} + 2\hat{j} + \hat{k}) + (3)(-3\hat{i} - 2\hat{j} + \hat{k})}{1 + 3} = \frac{-8\hat{i} - 4\hat{j} + 4\hat{k}}{4} = -2\hat{i} - \hat{j} + \hat{k} \).