Vectors in 3D are denoted $\mathbf{v} = \begin{pmatrix}v_1\\v_2\\v_3\end{pmatrix}$ or $v_1\mathbf{i} + v_2\mathbf{j} + v_3\mathbf{k}$. The fundamental operations are:
Magnitude: $|\mathbf{v}| = \sqrt{v_1^2 + v_2^2 + v_3^2}$
Unit vector: $\hat{\mathbf{v}} = \dfrac{\mathbf{v}}{|\mathbf{v}|}$
Dot product: $\mathbf{a} \cdot \mathbf{b} = a_1b_1 + a_2b_2 + a_3b_3 = |\mathbf{a}||\mathbf{b}|\cos\theta$
Cross product: $\mathbf{a} \times \mathbf{b} = \begin{vmatrix}\mathbf{i}&\mathbf{j}&\mathbf{k}\\a_1&a_2&a_3\\b_1&b_2&b_3\end{vmatrix}$, perpendicular to both $\mathbf{a}$ and $\mathbf{b}$, with $|\mathbf{a}\times\mathbf{b}| = |\mathbf{a}||\mathbf{b}|\sin\theta$
A line through point $A$ (position vector $\mathbf{a}$) with direction $\mathbf{b}$:
$$\mathbf{r} = \mathbf{a} + \lambda\mathbf{b}, \quad \lambda \in \mathbb{R}$$
Parametric form: $x = a_1 + \lambda b_1$, $y = a_2 + \lambda b_2$, $z = a_3 + \lambda b_3$
Symmetric form: $\dfrac{x-a_1}{b_1} = \dfrac{y-a_2}{b_2} = \dfrac{z-a_3}{b_3} = \lambda$
Normal vector form: $\mathbf{n}\cdot(\mathbf{r} - \mathbf{a}) = 0$, i.e., $ax + by + cz = d$ where $\mathbf{n} = (a,b,c)$
The normal vector $\mathbf{n}$ is perpendicular to every vector lying in the plane.
Distance from point $P$ to plane $ax+by+cz=d$: $$\text{dist} = \frac{|ax_P + by_P + cz_P - d|}{\sqrt{a^2+b^2+c^2}}$$
The angle $\phi$ between line (direction $\mathbf{d}$) and plane (normal $\mathbf{n}$) satisfies $\sin\phi = \dfrac{|\mathbf{d}\cdot\mathbf{n}|}{|\mathbf{d}||\mathbf{n}|}$.
$\mathbf{d} = (1,1,-1)$, $\mathbf{n} = (1,2,2)$. $\mathbf{d}\cdot\mathbf{n} = 1+2-2=1$. $|\mathbf{d}|=\sqrt{3}$, $|\mathbf{n}|=3$.
$\sin\phi = \dfrac{1}{3\sqrt{3}}$, so $\phi = \arcsin\!\left(\dfrac{1}{3\sqrt{3}}\right) \approx 11.0°$
$\text{dist} = \dfrac{|2(1)-2(1)+(1)-4|}{\sqrt{4+4+1}} = \dfrac{|2-2+1-4|}{3} = \dfrac{3}{3} = 1$
$\overrightarrow{AB} = (-1,2,0)$, $\overrightarrow{AC} = (-1,0,3)$.
$\mathbf{n} = \overrightarrow{AB}\times\overrightarrow{AC} = (6,3,2)$.
Using point $A$: $6(x-1)+3y+2z=0 \Rightarrow 6x+3y+2z=6$.