plane $\bar{r} \cdot(2 \hat{i}-\hat{j}+\hat{k})=0$
plane $\bar{r} \cdot(2 \hat{i}-\hat{j}+\hat{k})=0$
$\sin \theta=\left|\frac{\bar{b} \cdot \bar{n}}{|b \vec{b}||n|}\right|$
$\ldots(1)$
$\begin{aligned} \text { Here, } \bar{b} & =2 \hat{i}+3 \hat{j}-6 \hat{k}, \bar{n}=2 \hat{i}-\hat{j}+\hat{k} \\ \therefore \bar{b} \cdot \bar{n} & =(2 \hat{i}+3 \hat{j}-6 \hat{k}) \cdot(2 \hat{i}-\hat{j}+\hat{k}) \\ & =(2)(2)+(3)(-1)+(-6)(1) \\ & =4-3-6=-5\end{aligned}$
Also, $|\bar{b}|=\sqrt{2^2+3^2+(-6)^2}=\sqrt{49}=7$
$|\bar{n}|=\sqrt{2^2+(-1)^2+1^2}=\sqrt{6}$
$\therefore$ from $(1)$, we have
$\begin{aligned} & \sin \theta=\left|\frac{-5}{7 \sqrt{6}}\right|=\frac{5}{7 \sqrt{6}} \\ & \therefore \theta=\sin ^{-1}\left(\frac{5}{7 \sqrt{6}}\right) .\end{aligned}$
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| Differential equation | Function |
| $\text{x}^3\frac{\text{d}{^2}\text{y}}{\text{dx}^2}=1$ | $\text{y}=\text{ax}+\text{b}+\frac{1}{2\text{x}}$ |
$\sqrt{\cos x}+\sqrt{\cos \sqrt{x}}$