\[ \vec{d} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 1 & 1 & 1 \\ 2 & 2 & 1 \end{vmatrix} \] \[ \vec{d} = \hat{i}(1 \times 1 - 1 \times 2) - \hat{j}(1 \times 1 - 1 \times 2) + \hat{k}(1 \times 2 - 1 \times 2) \] \[ \vec{d} = \hat{i}(1 - 2) - \hat{j}(1 - 2) + \hat{k}(2 - 2) \] \[ \vec{d} = -\hat{i} + \hat{j} \]
\[ |\vec{d}| = \sqrt{(-1)^2 + 1^2} = \sqrt{1 + 1} = \sqrt{2} \]
Let \( \vec{c} = \alpha \vec{a} + \beta \vec{d} \). \[ \vec{a} \cdot \vec{c} = \alpha (\vec{a} \cdot \vec{a}) + \beta (\vec{a} \cdot \vec{d}) \] Since \( \vec{a} \perp \vec{d} \), \( \vec{a} \cdot \vec{d} = 0 \). \[ \vec{a} \cdot \vec{c} = \alpha (\vec{a} \cdot \vec{a}) = \alpha (1^2 + 1^2 + 1^2) = 3\alpha \] Also, \( \vec{a} \cdot \vec{c} = |\vec{c}| \). \[ 3\alpha = |\vec{c}| \]
\[ |\vec{c} - 2\vec{d}| = 8 \] \[ |\alpha \vec{a} + \beta \vec{d} - 2\vec{d}| = 8 \] \[ \vec{c} - 2\vec{d} = \alpha \vec{a} + (\beta - 2)\vec{d} \] \[ \|\vec{c} - 2\vec{d}\| = \sqrt{(3\alpha)^2 + (\beta - 2)^2 \times 2} \] \[ 9\alpha^2 + 2(\beta - 2)^2 = 64 \]
\[ \cos \frac{\pi}{4} = \frac{\vec{d} \cdot \vec{c}}{|\vec{d}||\vec{c}|} = \frac{\beta |\vec{d}|^2}{|\vec{d}||\vec{c}|} \] \[ \frac{\beta \times 2}{\sqrt{2} \times 3\alpha} = \frac{1}{\sqrt{2}} \] \[ \frac{2\beta}{3\alpha} = 1 \implies \beta = \frac{3\alpha}{2} \]
\[ 9\alpha^2 + 2\left( \frac{3\alpha}{2} - 2 \right)^2 = 64 \] Solving this equation will give us the final result.
The steam volatile compounds among the following are: