$\cos \theta=\left|\frac{n_1 \cdot n_2}{\left|n_1 \|\right| n_2 \mid}\right|$
$\ldots(1)$
Here, $\bar{n}_1=\hat{i}+\hat{j}+2 \hat{k}, \bar{n}_2=2 \vec{i}-\hat{j}+\vec{k}$
$\begin{aligned} \therefore \bar{n}_1 \cdot \bar{n}_2 & =(\hat{i}+\hat{j}+2 \hat{k}) \cdot(2 \hat{i}-\hat{j}+\hat{k}) \\ & =(1)(2)+(1)(-1)+(2)(1)\end{aligned}$
$=2-1+2=3$
Also, $\left|\bar{n}_1\right|=\sqrt{1^2+1^2+2^2}=\sqrt{6}$
$\left|\bar{n}_2\right|=\sqrt{2^2+(-1)^2+1^2}=\sqrt{6}$
$\therefore$ from (1), we have
$\cos \theta=\left|\frac{3}{\sqrt{6} \cdot \sqrt{6}}\right|=\frac{3}{6}=\frac{1}{2} \cos 60^{\circ}$
$\therefore \theta=60^{\circ}$.
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