Skip to content
Family Table Math
Auto

Angles Between Lines and Planes

How steep is a roof? At what angle does a laser beam hit a mirror? Each of these questions asks for an angle between lines and planes in 3-D. You already know how to find the angle between two vectors with the scalar (dot) product. This page shows which two vectors to use in each case, and why the answer is always given as an acute angle.

This page writes vectors as columns, as IB does. The Ontario vector pages on this site write the same vectors in square brackets, so (2−12)\begin{pmatrix} 2 \\ -1 \\ 2 \end{pmatrix} there is [2,−1,2][2, -1, 2].

For non-zero vectors v⃗\vec{v} and w⃗\vec{w}, the angle θ\theta between them satisfies

cos⁡θ=v⃗⋅w⃗∣v⃗∣ ∣w⃗∣,0∘≤θ≤180∘\cos\theta = \frac{\vec{v} \cdot \vec{w}}{\lvert\vec{v}\rvert\,\lvert\vec{w}\rvert}, \qquad 0^\circ \le \theta \le 180^\circ

Everything on this page uses this formula with the right pair of vectors: direction vectors for lines, and normal vectors for planes.

Two lines r⃗=a⃗1+λb⃗1\vec{r} = \vec{a}_1 + \lambda\vec{b}_1 and r⃗=a⃗2+μb⃗2\vec{r} = \vec{a}_2 + \mu\vec{b}_2 meet at the same angle as their direction vectors b⃗1\vec{b}_1 and b⃗2\vec{b}_2. But crossing lines make two angles, θ\theta and 180∘−θ180^\circ - \theta, and the angle between the lines is the acute one. Taking the absolute value of the scalar product gives it straight away:

cos⁡θ=∣b⃗1⋅b⃗2∣∣b⃗1∣ ∣b⃗2∣\cos\theta = \frac{\lvert\vec{b}_1 \cdot \vec{b}_2\rvert}{\lvert\vec{b}_1\rvert\,\lvert\vec{b}_2\rvert}

If you forget the absolute value and get an obtuse angle, subtract it from 180∘180^\circ. The formula uses only directions, so it works for lines in 2-D or 3-D, and even for skew lines that never meet.

The position vectors a⃗1\vec{a}_1 and a⃗2\vec{a}_2 play no part. Don’t use them!

The angle between a line and a plane is the angle θ\theta between the line and its projection onto the plane (its “shadow” when light shines straight down onto the plane). It runs from 0∘0^\circ (line parallel to the plane) to 90∘90^\circ (line perpendicular to the plane).

A plane has no single direction vector, but it does have a normal n⃗\vec{n}. Let φ\varphi be the acute angle between the line’s direction b⃗\vec{b} and n⃗\vec{n}. In the figure, the normal is perpendicular to the projection, so

θ=90∘−φ\theta = 90^\circ - \varphi
A line meeting a plane: the angle θ with the plane and the angle φ with the normal add to 90 degrees. θ φ n b projection plane θ = 90° − φ
The angle θ\theta between the line and the plane and the angle φ\varphi between the line and the normal add to 90∘90^\circ.

Since cos⁡φ=sin⁡(90∘−φ)=sin⁡θ\cos\varphi = \sin(90^\circ - \varphi) = \sin\theta, you can go straight to θ\theta with sine:

sin⁡θ=∣b⃗⋅n⃗∣∣b⃗∣ ∣n⃗∣\sin\theta = \frac{\lvert\vec{b} \cdot \vec{n}\rvert}{\lvert\vec{b}\rvert\,\lvert\vec{n}\rvert}

Two special cases are worth spotting before you calculate:

  • b⃗⋅n⃗=0\vec{b} \cdot \vec{n} = 0: the line is parallel to the plane (or lies in it), so θ=0∘\theta = 0^\circ.
  • b⃗\vec{b} is a multiple of n⃗\vec{n}: the line is perpendicular to the plane, so θ=90∘\theta = 90^\circ.

Two planes that meet do so along a line. Look along that line, so each plane appears as a line seen edge-on: each normal is perpendicular to its own plane, so the angle between the normals equals the angle between the planes. Again, use the acute one:

cos⁡θ=∣n⃗1⋅n⃗2∣∣n⃗1∣ ∣n⃗2∣\cos\theta = \frac{\lvert\vec{n}_1 \cdot \vec{n}_2\rvert}{\lvert\vec{n}_1\rvert\,\lvert\vec{n}_2\rvert}

For a plane ax+by+cz=dax + by + cz = d, read the normal off the coefficients: n⃗=(abc)\vec{n} = \begin{pmatrix} a \\ b \\ c \end{pmatrix}. For a plane in vector form r⃗=a⃗+λb⃗+μc⃗\vec{r} = \vec{a} + \lambda\vec{b} + \mu\vec{c}, find the normal with the vector product: n⃗=b⃗×c⃗\vec{n} = \vec{b} \times \vec{c}.

Angle betweenVectors to useFormula for the acute angle
two linesdirections b⃗1\vec{b}_1, b⃗2\vec{b}_2cos⁡θ=∣b⃗1⋅b⃗2∣∣b⃗1∣∣b⃗2∣\cos\theta = \dfrac{\lvert\vec{b}_1 \cdot \vec{b}_2\rvert}{\lvert\vec{b}_1\rvert\lvert\vec{b}_2\rvert}
a line and a planedirection b⃗\vec{b}, normal n⃗\vec{n}sin⁡θ=∣b⃗⋅n⃗∣∣b⃗∣∣n⃗∣\sin\theta = \dfrac{\lvert\vec{b} \cdot \vec{n}\rvert}{\lvert\vec{b}\rvert\lvert\vec{n}\rvert}
two planesnormals n⃗1\vec{n}_1, n⃗2\vec{n}_2cos⁡θ=∣n⃗1⋅n⃗2∣∣n⃗1∣∣n⃗2∣\cos\theta = \dfrac{\lvert\vec{n}_1 \cdot \vec{n}_2\rvert}{\lvert\vec{n}_1\rvert\lvert\vec{n}_2\rvert}

Give angles in degrees to 3 significant figures unless the question asks for radians.

Find the acute angle between the lines

L1: r⃗=(102)+λ(2−12)andL2: r⃗=(03−1)+μ(12−2)L_1:\ \vec{r} = \begin{pmatrix} 1 \\ 0 \\ 2 \end{pmatrix} + \lambda\begin{pmatrix} 2 \\ -1 \\ 2 \end{pmatrix} \qquad\text{and}\qquad L_2:\ \vec{r} = \begin{pmatrix} 0 \\ 3 \\ -1 \end{pmatrix} + \mu\begin{pmatrix} 1 \\ 2 \\ -2 \end{pmatrix}

Solution. Use the direction vectors only:

b⃗1⋅b⃗2=2(1)+(−1)(2)+2(−2)=−4,∣b⃗1∣=4+1+4=3,∣b⃗2∣=1+4+4=3\vec{b}_1 \cdot \vec{b}_2 = 2(1) + (-1)(2) + 2(-2) = -4, \qquad \lvert\vec{b}_1\rvert = \sqrt{4 + 1 + 4} = 3, \qquad \lvert\vec{b}_2\rvert = \sqrt{1 + 4 + 4} = 3 cos⁡θ=∣−4∣3×3=49⇒θ=cos⁡−1 ⁣(49)≈63.6∘ (3 s.f.)\cos\theta = \frac{\lvert -4 \rvert}{3 \times 3} = \frac{4}{9} \quad\Rightarrow\quad \theta = \cos^{-1}\!\left(\frac{4}{9}\right) \approx 63.6^\circ \text{ (3 s.f.)}

Without the absolute value you’d get cos⁡−1 ⁣(−49)≈116.4∘\cos^{-1}\!\left(-\dfrac{4}{9}\right) \approx 116.4^\circ, the obtuse angle between the lines. Check: 180∘−116.4∘=63.6∘180^\circ - 116.4^\circ = 63.6^\circ. ✓

Find the angle between the line r⃗=(120)+t(112)\vec{r} = \begin{pmatrix} 1 \\ 2 \\ 0 \end{pmatrix} + t\begin{pmatrix} 1 \\ 1 \\ 2 \end{pmatrix} and the plane 2x−y+z=52x - y + z = 5.

Solution. The direction of the line is b⃗=(112)\vec{b} = \begin{pmatrix} 1 \\ 1 \\ 2 \end{pmatrix} and the normal to the plane is n⃗=(2−11)\vec{n} = \begin{pmatrix} 2 \\ -1 \\ 1 \end{pmatrix}.

b⃗⋅n⃗=2−1+2=3,∣b⃗∣=6,∣n⃗∣=6\vec{b} \cdot \vec{n} = 2 - 1 + 2 = 3, \qquad \lvert\vec{b}\rvert = \sqrt{6}, \qquad \lvert\vec{n}\rvert = \sqrt{6} sin⁡θ=∣3∣66=36=12⇒θ=30∘\sin\theta = \frac{\lvert 3 \rvert}{\sqrt{6}\sqrt{6}} = \frac{3}{6} = \frac{1}{2} \quad\Rightarrow\quad \theta = 30^\circ

Check with the normal. The angle between b⃗\vec{b} and n⃗\vec{n} satisfies cos⁡φ=12\cos\varphi = \dfrac{1}{2}, so φ=60∘\varphi = 60^\circ, and θ=90∘−60∘=30∘\theta = 90^\circ - 60^\circ = 30^\circ. ✓

Find the acute angle between the planes x+2y−2z=4x + 2y - 2z = 4 and −3x+4z=1-3x + 4z = 1.

Solution. The normals are n⃗1=(12−2)\vec{n}_1 = \begin{pmatrix} 1 \\ 2 \\ -2 \end{pmatrix} and n⃗2=(−304)\vec{n}_2 = \begin{pmatrix} -3 \\ 0 \\ 4 \end{pmatrix}. (The second plane has no yy term, so its yy-component is 00.)

n⃗1⋅n⃗2=−3+0−8=−11,∣n⃗1∣=3,∣n⃗2∣=5\vec{n}_1 \cdot \vec{n}_2 = -3 + 0 - 8 = -11, \qquad \lvert\vec{n}_1\rvert = 3, \qquad \lvert\vec{n}_2\rvert = 5 cos⁡θ=∣−11∣3×5=1115⇒θ≈42.8∘ (3 s.f.)\cos\theta = \frac{\lvert -11 \rvert}{3 \times 5} = \frac{11}{15} \quad\Rightarrow\quad \theta \approx 42.8^\circ \text{ (3 s.f.)}

The normals themselves are 137.2∘137.2^\circ apart; the planes meet at 42.8∘42.8^\circ and 137.2∘137.2^\circ, and the acute angle 42.8∘42.8^\circ is the answer.

Find the angle between the line x−12=y+3−1=z2\dfrac{x - 1}{2} = \dfrac{y + 3}{-1} = \dfrac{z}{2} and the plane

r⃗=(100)+λ(110)+μ(01−1)\vec{r} = \begin{pmatrix} 1 \\ 0 \\ 0 \end{pmatrix} + \lambda\begin{pmatrix} 1 \\ 1 \\ 0 \end{pmatrix} + \mu\begin{pmatrix} 0 \\ 1 \\ -1 \end{pmatrix}

Solution. Direction of the line. In Cartesian form, the direction vector is made of the denominators: b⃗=(2−12)\vec{b} = \begin{pmatrix} 2 \\ -1 \\ 2 \end{pmatrix}.

Normal to the plane. The two direction vectors lie in the plane, so their vector product is normal to it:

n⃗=(110)×(01−1)=((1)(−1)−(0)(1)(0)(0)−(1)(−1)(1)(1)−(1)(0))=(−111)\vec{n} = \begin{pmatrix} 1 \\ 1 \\ 0 \end{pmatrix} \times \begin{pmatrix} 0 \\ 1 \\ -1 \end{pmatrix} = \begin{pmatrix} (1)(-1) - (0)(1) \\ (0)(0) - (1)(-1) \\ (1)(1) - (1)(0) \end{pmatrix} = \begin{pmatrix} -1 \\ 1 \\ 1 \end{pmatrix}

Check: n⃗⋅(110)=−1+1+0=0\vec{n} \cdot \begin{pmatrix} 1 \\ 1 \\ 0 \end{pmatrix} = -1 + 1 + 0 = 0 and n⃗⋅(01−1)=0+1−1=0\vec{n} \cdot \begin{pmatrix} 0 \\ 1 \\ -1 \end{pmatrix} = 0 + 1 - 1 = 0. ✓

The angle.

b⃗⋅n⃗=−2−1+2=−1,∣b⃗∣=3,∣n⃗∣=3\vec{b} \cdot \vec{n} = -2 - 1 + 2 = -1, \qquad \lvert\vec{b}\rvert = 3, \qquad \lvert\vec{n}\rvert = \sqrt{3} sin⁡θ=∣−1∣33≈0.19245⇒θ≈11.1∘ (3 s.f.)\sin\theta = \frac{\lvert -1 \rvert}{3\sqrt{3}} \approx 0.19245 \quad\Rightarrow\quad \theta \approx 11.1^\circ \text{ (3 s.f.)}

The line is close to parallel to the plane, which matches the small value of b⃗⋅n⃗\vec{b} \cdot \vec{n}.

Using cosine for the angle between a line and a plane. ∣b⃗⋅n⃗∣∣b⃗∣∣n⃗∣\dfrac{\lvert\vec{b} \cdot \vec{n}\rvert}{\lvert\vec{b}\rvert\lvert\vec{n}\rvert} is the cosine of the angle with the normal. Either take sin⁡−1\sin^{-1} of it, or take cos⁡−1\cos^{-1} and subtract from 90∘90^\circ. In Example 2, cos⁡−1 ⁣(12)=60∘\cos^{-1}\!\left(\dfrac{1}{2}\right) = 60^\circ is the angle with the normal, not the answer.

Giving the obtuse angle. The angle between two lines, or two planes, is the acute one. Use the absolute value of the scalar product, or subtract an obtuse answer from 180∘180^\circ.

Using position vectors instead of direction vectors. The point a line passes through has nothing to do with its direction. Only b⃗1\vec{b}_1 and b⃗2\vec{b}_2 go into the formula, never a⃗1\vec{a}_1 or a⃗2\vec{a}_2.

Reading the wrong numbers from a Cartesian equation. For the line x−12=y+3−1=z2\dfrac{x - 1}{2} = \dfrac{y + 3}{-1} = \dfrac{z}{2}, the direction is the denominators (2−12)\begin{pmatrix} 2 \\ -1 \\ 2 \end{pmatrix}, while (1,−3,0)(1, -3, 0) is a point. For the plane x+2y−2z=4x + 2y - 2z = 4, the normal is the coefficients (12−2)\begin{pmatrix} 1 \\ 2 \\ -2 \end{pmatrix}, and a missing variable means a component of 00.

Using a direction vector of a plane as if it were the normal. For a plane in the form r⃗=a⃗+λb⃗+μc⃗\vec{r} = \vec{a} + \lambda\vec{b} + \mu\vec{c}, the vectors b⃗\vec{b} and c⃗\vec{c} lie in the plane. Find n⃗=b⃗×c⃗\vec{n} = \vec{b} \times \vec{c} first.

Calculator in radians. If cos⁡−1 ⁣(49)\cos^{-1}\!\left(\dfrac{4}{9}\right) comes out as 1.111.11, your calculator is in radian mode. That’s correct in radians, but give degrees unless the question asks otherwise.

1. (Warm-up) Find the acute angle between the lines r⃗=(01)+λ(34)\vec{r} = \begin{pmatrix} 0 \\ 1 \end{pmatrix} + \lambda\begin{pmatrix} 3 \\ 4 \end{pmatrix} and r⃗=(20)+μ(5−12)\vec{r} = \begin{pmatrix} 2 \\ 0 \end{pmatrix} + \mu\begin{pmatrix} 5 \\ -12 \end{pmatrix}.

Solutionb⃗1⋅b⃗2=15−48=−33,∣b⃗1∣=5,∣b⃗2∣=13\vec{b}_1 \cdot \vec{b}_2 = 15 - 48 = -33, \qquad \lvert\vec{b}_1\rvert = 5, \qquad \lvert\vec{b}_2\rvert = 13cos⁡θ=3365⇒θ≈59.5∘ (3 s.f.)\cos\theta = \frac{33}{65} \quad\Rightarrow\quad \theta \approx 59.5^\circ \text{ (3 s.f.)}

2. (Warm-up) Without finding any inverse cosines, decide whether each line is parallel or perpendicular to the plane x−2y+3z=1x - 2y + 3z = 1, and state the angle between them.

  • (a) A line with direction (2−46)\begin{pmatrix} 2 \\ -4 \\ 6 \end{pmatrix}.
  • (b) A line with direction (121)\begin{pmatrix} 1 \\ 2 \\ 1 \end{pmatrix}.
Solution

The normal is n⃗=(1−23)\vec{n} = \begin{pmatrix} 1 \\ -2 \\ 3 \end{pmatrix}.

(a) (2−46)=2n⃗\begin{pmatrix} 2 \\ -4 \\ 6 \end{pmatrix} = 2\vec{n}, so the line is parallel to the normal, which means it is perpendicular to the plane: the angle is 90∘90^\circ.

(b) (121)⋅n⃗=1−4+3=0\begin{pmatrix} 1 \\ 2 \\ 1 \end{pmatrix} \cdot \vec{n} = 1 - 4 + 3 = 0, so the line is perpendicular to the normal, which means it is parallel to the plane (or lies in it): the angle is 0∘0^\circ.

3. (Core) Line L1L_1 passes through A(1,2,3)A(1, 2, 3) and B(3,3,5)B(3, 3, 5). Line L2L_2 passes through C(0,1,−1)C(0, 1, -1) and D(4,−1,3)D(4, -1, 3). Find the acute angle between the lines.

Solution

Direction vectors: AB→=(212)\overrightarrow{AB} = \begin{pmatrix} 2 \\ 1 \\ 2 \end{pmatrix} and CD→=(4−24)\overrightarrow{CD} = \begin{pmatrix} 4 \\ -2 \\ 4 \end{pmatrix}, which is 2(2−12)2\begin{pmatrix} 2 \\ -1 \\ 2 \end{pmatrix}. A multiple doesn’t change the direction, so use (2−12)\begin{pmatrix} 2 \\ -1 \\ 2 \end{pmatrix}:

cos⁡θ=∣4−1+4∣3×3=79⇒θ≈38.9∘ (3 s.f.)\cos\theta = \frac{\lvert 4 - 1 + 4 \rvert}{3 \times 3} = \frac{7}{9} \quad\Rightarrow\quad \theta \approx 38.9^\circ \text{ (3 s.f.)}

4. (Core) A ski lift cable follows the line r⃗=(201)+t(304)\vec{r} = \begin{pmatrix} 2 \\ 0 \\ 1 \end{pmatrix} + t\begin{pmatrix} 3 \\ 0 \\ 4 \end{pmatrix}, where zz is the height. Find the angle the cable makes with the horizontal plane z=0z = 0.

Solution

The plane z=0z = 0 has normal n⃗=(001)\vec{n} = \begin{pmatrix} 0 \\ 0 \\ 1 \end{pmatrix}, and b⃗=(304)\vec{b} = \begin{pmatrix} 3 \\ 0 \\ 4 \end{pmatrix} has magnitude 55.

sin⁡θ=∣4∣5×1=0.8⇒θ≈53.1∘ (3 s.f.)\sin\theta = \frac{\lvert 4 \rvert}{5 \times 1} = 0.8 \quad\Rightarrow\quad \theta \approx 53.1^\circ \text{ (3 s.f.)}

Check: the cable rises 44 for every 33 across, and tan⁡−1 ⁣(43)≈53.1∘\tan^{-1}\!\left(\dfrac{4}{3}\right) \approx 53.1^\circ. ✓

5. (Core) Find the acute angle between the planes 2x+y−z=32x + y - z = 3 and x−y+2z=0x - y + 2z = 0.

Solution

n⃗1=(21−1)\vec{n}_1 = \begin{pmatrix} 2 \\ 1 \\ -1 \end{pmatrix} and n⃗2=(1−12)\vec{n}_2 = \begin{pmatrix} 1 \\ -1 \\ 2 \end{pmatrix}, each with magnitude 6\sqrt{6}.

n⃗1⋅n⃗2=2−1−2=−1,cos⁡θ=∣−1∣66=16⇒θ≈80.4∘ (3 s.f.)\vec{n}_1 \cdot \vec{n}_2 = 2 - 1 - 2 = -1, \qquad \cos\theta = \frac{\lvert -1 \rvert}{\sqrt{6}\sqrt{6}} = \frac{1}{6} \quad\Rightarrow\quad \theta \approx 80.4^\circ \text{ (3 s.f.)}

6. (Core) A flat roof panel contains the points (0,0,3)(0, 0, 3), (8,0,3)(8, 0, 3) and (0,4,6)(0, 4, 6), in metres, where zz is the height above the floor z=0z = 0. Find the angle between the roof panel and the floor.

Solution

Two vectors in the roof: (800)\begin{pmatrix} 8 \\ 0 \\ 0 \end{pmatrix} and (043)\begin{pmatrix} 0 \\ 4 \\ 3 \end{pmatrix}. A normal is

(800)×(043)=(0⋅3−0⋅40⋅0−8⋅38⋅4−0⋅0)=(0−2432)=8(0−34)\begin{pmatrix} 8 \\ 0 \\ 0 \end{pmatrix} \times \begin{pmatrix} 0 \\ 4 \\ 3 \end{pmatrix} = \begin{pmatrix} 0 \cdot 3 - 0 \cdot 4 \\ 0 \cdot 0 - 8 \cdot 3 \\ 8 \cdot 4 - 0 \cdot 0 \end{pmatrix} = \begin{pmatrix} 0 \\ -24 \\ 32 \end{pmatrix} = 8\begin{pmatrix} 0 \\ -3 \\ 4 \end{pmatrix}

Use n⃗1=(0−34)\vec{n}_1 = \begin{pmatrix} 0 \\ -3 \\ 4 \end{pmatrix} (magnitude 55) and the floor’s normal n⃗2=(001)\vec{n}_2 = \begin{pmatrix} 0 \\ 0 \\ 1 \end{pmatrix}:

cos⁡θ=∣4∣5×1=0.8⇒θ≈36.9∘ (3 s.f.)\cos\theta = \frac{\lvert 4 \rvert}{5 \times 1} = 0.8 \quad\Rightarrow\quad \theta \approx 36.9^\circ \text{ (3 s.f.)}

Check: the roof rises 33 m over a horizontal run of 44 m, and tan⁡−1 ⁣(34)≈36.9∘\tan^{-1}\!\left(\dfrac{3}{4}\right) \approx 36.9^\circ. ✓

7. (Core) A line has direction (1k2)\begin{pmatrix} 1 \\ k \\ 2 \end{pmatrix}, and Π\Pi is the plane 3x−y+z=43x - y + z = 4.

  • (a) Find the value of kk for which the line is parallel to Π\Pi.
  • (b) Show that there is no value of kk for which the line is perpendicular to Π\Pi.
Solution

The normal is n⃗=(3−11)\vec{n} = \begin{pmatrix} 3 \\ -1 \\ 1 \end{pmatrix}.

(a) Parallel to the plane means perpendicular to the normal: 3−k+2=03 - k + 2 = 0, so k=5k = 5.

(b) Perpendicular to the plane means (1k2)=c(3−11)\begin{pmatrix} 1 \\ k \\ 2 \end{pmatrix} = c\begin{pmatrix} 3 \\ -1 \\ 1 \end{pmatrix} for some cc. The first component gives c=13c = \dfrac{1}{3}, but the third gives c=2c = 2. These contradict each other, so no value of kk works.

8. (Challenge) The line through the origin with direction (11p)\begin{pmatrix} 1 \\ 1 \\ p \end{pmatrix} makes an angle of 45∘45^\circ with the plane z=0z = 0. Find the possible values of pp.

Solution

With n⃗=(001)\vec{n} = \begin{pmatrix} 0 \\ 0 \\ 1 \end{pmatrix}:

sin⁡45∘=∣p∣2+p2\sin 45^\circ = \frac{\lvert p \rvert}{\sqrt{2 + p^2}}

Square both sides, using sin⁡245∘=12\sin^2 45^\circ = \dfrac{1}{2}:

12=p22+p22+p2=2p2p2=2\begin{aligned} \frac{1}{2} &= \frac{p^2}{2 + p^2} \\ 2 + p^2 &= 2p^2 \\ p^2 &= 2 \end{aligned}

So p=2p = \sqrt{2} or p=−2p = -\sqrt{2}. (One line points upward and one downward; both make 45∘45^\circ with the plane.)

Check: 24=22=sin⁡45∘\dfrac{\sqrt{2}}{\sqrt{4}} = \dfrac{\sqrt{2}}{2} = \sin 45^\circ. ✓

9. (Challenge) The planes x+y+z=1x + y + z = 1 and x−y=0x - y = 0 meet in a line LL. Find the angle between LL and the plane 2x+y+z=72x + y + z = 7.

Solution

LL lies in both planes, so it is perpendicular to both normals. Its direction is their vector product:

b⃗=(111)×(1−10)=((1)(0)−(1)(−1)(1)(1)−(1)(0)(1)(−1)−(1)(1))=(11−2)\vec{b} = \begin{pmatrix} 1 \\ 1 \\ 1 \end{pmatrix} \times \begin{pmatrix} 1 \\ -1 \\ 0 \end{pmatrix} = \begin{pmatrix} (1)(0) - (1)(-1) \\ (1)(1) - (1)(0) \\ (1)(-1) - (1)(1) \end{pmatrix} = \begin{pmatrix} 1 \\ 1 \\ -2 \end{pmatrix}

With n⃗=(211)\vec{n} = \begin{pmatrix} 2 \\ 1 \\ 1 \end{pmatrix}:

b⃗⋅n⃗=2+1−2=1,∣b⃗∣=∣n⃗∣=6\vec{b} \cdot \vec{n} = 2 + 1 - 2 = 1, \qquad \lvert\vec{b}\rvert = \lvert\vec{n}\rvert = \sqrt{6}sin⁡θ=16⇒θ≈9.59∘ (3 s.f.)\sin\theta = \frac{1}{6} \quad\Rightarrow\quad \theta \approx 9.59^\circ \text{ (3 s.f.)}