Direction Cosines and Direction Ratios
If a line makes angles α , β , γ \alpha, \beta, \gamma α , β , γ with the positive x x x -, y y y -, z z z -axes, its direction cosines are
l = cos α , m = cos β , n = cos γ , l 2 + m 2 + n 2 = 1 l = \cos\alpha, \quad m = \cos\beta, \quad n = \cos\gamma, \qquad l^2 + m^2 + n^2 = 1 l = cos α , m = cos β , n = cos γ , l 2 + m 2 + n 2 = 1
Any triple a , b , c a, b, c a , b , c proportional to l , m , n l, m, n l , m , n gives direction ratios . To convert DRs to DCs, divide by a 2 + b 2 + c 2 \sqrt{a^2 + b^2 + c^2} a 2 + b 2 + c 2 :
l = a a 2 + b 2 + c 2 , m = b a 2 + b 2 + c 2 , n = c a 2 + b 2 + c 2 l = \frac{a}{\sqrt{a^2+b^2+c^2}}, \quad m = \frac{b}{\sqrt{a^2+b^2+c^2}}, \quad n = \frac{c}{\sqrt{a^2+b^2+c^2}} l = a 2 + b 2 + c 2 a , m = a 2 + b 2 + c 2 b , n = a 2 + b 2 + c 2 c
DCs are unique up to an overall sign (the two senses of the line); DRs are infinitely many. For the line through P ( x 1 , y 1 , z 1 ) P(x_1, y_1, z_1) P ( x 1 , y 1 , z 1 ) and Q ( x 2 , y 2 , z 2 ) Q(x_2, y_2, z_2) Q ( x 2 , y 2 , z 2 ) , one set of DRs is x 2 − x 1 , y 2 − y 1 , z 2 − z 1 x_2 - x_1,\ y_2 - y_1,\ z_2 - z_1 x 2 − x 1 , y 2 − y 1 , z 2 − z 1 .
Equations of a Line
Through a point with position vector a ⃗ \vec{a} a , parallel to b ⃗ \vec{b} b :
r ⃗ = a ⃗ + λ b ⃗ \vec{r} = \vec{a} + \lambda\vec{b} r = a + λ b
In cartesian form, through ( x 1 , y 1 , z 1 ) (x_1, y_1, z_1) ( x 1 , y 1 , z 1 ) with DRs a , b , c a, b, c a , b , c :
x − x 1 a = y − y 1 b = z − z 1 c \frac{x - x_1}{a} = \frac{y - y_1}{b} = \frac{z - z_1}{c} a x − x 1 = b y − y 1 = c z − z 1
Through two points a ⃗ \vec{a} a and b ⃗ \vec{b} b : r ⃗ = a ⃗ + λ ( b ⃗ − a ⃗ ) \vec{r} = \vec{a} + \lambda\left(\vec{b} - \vec{a}\right) r = a + λ ( b − a ) , i.e. use the joining vector as the direction.
Reading a cartesian equation: the standard form needs coefficient 1 1 1 on each of x , y , z x, y, z x , y , z — rewrite 1 − x 2 \frac{1 - x}{2} 2 1 − x as x − 1 − 2 \frac{x - 1}{-2} − 2 x − 1 before reading off the DRs. Rushing this step is the chapter's most common error.
Angle Between Two Lines
For lines with direction vectors b 1 ⃗ \vec{b_1} b 1 and b 2 ⃗ \vec{b_2} b 2 :
cos θ = ∣ b 1 ⃗ ⋅ b 2 ⃗ ∣ b 1 ⃗ ∣ ∣ b 2 ⃗ ∣ ∣ \cos\theta = \left\vert\frac{\vec{b_1}\cdot\vec{b_2}}{\vert\vec{b_1}\vert\vert\vec{b_2}\vert}\right\vert cos θ = ∣ b 1 ∣∣ b 2 ∣ b 1 ⋅ b 2
The modulus keeps θ \theta θ acute — the convention for the angle between lines. Consequences: perpendicular ⟺ a 1 a 2 + b 1 b 2 + c 1 c 2 = 0 \iff a_1a_2 + b_1b_2 + c_1c_2 = 0 ⟺ a 1 a 2 + b 1 b 2 + c 1 c 2 = 0 ; parallel ⟺ a 1 a 2 = b 1 b 2 = c 1 c 2 \iff \frac{a_1}{a_2} = \frac{b_1}{b_2} = \frac{c_1}{c_2} ⟺ a 2 a 1 = b 2 b 1 = c 2 c 1 .
Shortest Distance Between Two Lines
Skew lines — neither parallel nor intersecting — exist only in three dimensions, and the shortest distance is along the common perpendicular.
Skew lines r ⃗ = a 1 ⃗ + λ b 1 ⃗ \vec{r} = \vec{a_1} + \lambda\vec{b_1} r = a 1 + λ b 1 and r ⃗ = a 2 ⃗ + μ b 2 ⃗ \vec{r} = \vec{a_2} + \mu\vec{b_2} r = a 2 + μ b 2 :
d = ∣ ( b 1 ⃗ × b 2 ⃗ ) ⋅ ( a 2 ⃗ − a 1 ⃗ ) ∣ ∣ b 1 ⃗ × b 2 ⃗ ∣ d = \frac{\left\vert\left(\vec{b_1}\times\vec{b_2}\right)\cdot\left(\vec{a_2} - \vec{a_1}\right)\right\vert}{\vert\vec{b_1}\times\vec{b_2}\vert} d = ∣ b 1 × b 2 ∣ ( b 1 × b 2 ) ⋅ ( a 2 − a 1 )
Parallel lines (b 1 ⃗ = b 2 ⃗ = b ⃗ \vec{b_1} = \vec{b_2} = \vec{b} b 1 = b 2 = b ) make that formula collapse (b ⃗ × b ⃗ = 0 ⃗ \vec{b}\times\vec{b} = \vec{0} b × b = 0 ), so use
d = ∣ b ⃗ × ( a 2 ⃗ − a 1 ⃗ ) ∣ ∣ b ⃗ ∣ d = \frac{\left\vert\vec{b}\times\left(\vec{a_2} - \vec{a_1}\right)\right\vert}{\vert\vec{b}\vert} d = ∣ b ∣ b × ( a 2 − a 1 )
Test d = 0 d = 0 d = 0 : the lines intersect. The five-step routine for any shortest-distance question: extract a 1 ⃗ , b 1 ⃗ , a 2 ⃗ , b 2 ⃗ \vec{a_1}, \vec{b_1}, \vec{a_2}, \vec{b_2} a 1 , b 1 , a 2 , b 2 ; check parallel or not; compute the cross product; dot with a 2 ⃗ − a 1 ⃗ \vec{a_2} - \vec{a_1} a 2 − a 1 (skew case); divide by the right magnitude.
Worked Examples — Direction Cosines and Line Equations
Example 1 — DCs from the angles
A line makes angles 90 ∘ 90^\circ 9 0 ∘ , 60 ∘ 60^\circ 6 0 ∘ , 30 ∘ 30^\circ 3 0 ∘ with the x x x -, y y y -, z z z -axes. Find its direction cosines.
Step 1 — take cosines: l = cos 90 ∘ = 0 l = \cos 90^\circ = 0 l = cos 9 0 ∘ = 0 , m = cos 60 ∘ = 1 2 m = \cos 60^\circ = \dfrac{1}{2} m = cos 6 0 ∘ = 2 1 , n = cos 30 ∘ = 3 2 n = \cos 30^\circ = \dfrac{\sqrt{3}}{2} n = cos 3 0 ∘ = 2 3 .
Step 2 — verify: 0 + 1 4 + 3 4 = 1 0 + \dfrac{1}{4} + \dfrac{3}{4} = 1 0 + 4 1 + 4 3 = 1 .
Answer: ( 0 , 1 2 , 3 2 ) \left(0, \dfrac{1}{2}, \dfrac{\sqrt{3}}{2}\right) ( 0 , 2 1 , 2 3 ) — the identity check is a free mark, always show it.
Example 2 — DCs from DRs
Find the direction cosines of a line with direction ratios 2 , − 1 , 2 2, -1, 2 2 , − 1 , 2 .
Step 1 — the normaliser: 4 + 1 + 4 = 3 \sqrt{4 + 1 + 4} = 3 4 + 1 + 4 = 3 .
Answer: ( 2 3 , − 1 3 , 2 3 ) \left(\dfrac{2}{3}, -\dfrac{1}{3}, \dfrac{2}{3}\right) ( 3 2 , − 3 1 , 3 2 ) — or the same triple with all signs flipped; both describe the line.
Example 3 — DCs of a line through two points
Find the direction cosines of the line through A ( − 2 , 4 , − 5 ) A(-2, 4, -5) A ( − 2 , 4 , − 5 ) and B ( 1 , 2 , 3 ) B(1, 2, 3) B ( 1 , 2 , 3 ) .
Step 1 — DRs by subtraction: 3 , − 2 , 8 3, -2, 8 3 , − 2 , 8 .
Step 2 — normalise: 9 + 4 + 64 = 77 \sqrt{9 + 4 + 64} = \sqrt{77} 9 + 4 + 64 = 77 .
Answer: ( 3 77 , − 2 77 , 8 77 ) \left(\dfrac{3}{\sqrt{77}}, \dfrac{-2}{\sqrt{77}}, \dfrac{8}{\sqrt{77}}\right) ( 77 3 , 77 − 2 , 77 8 ) .
Example 4 — Line through a point, parallel to a vector
Find the vector and cartesian equations of the line through ( 5 , 2 , − 4 ) (5, 2, -4) ( 5 , 2 , − 4 ) parallel to 3 i ^ + 2 j ^ − 8 k ^ 3\hat{i} + 2\hat{j} - 8\hat{k} 3 i ^ + 2 j ^ − 8 k ^ .
Step 1 — vector form: r ⃗ = 5 i ^ + 2 j ^ − 4 k ^ + λ ( 3 i ^ + 2 j ^ − 8 k ^ ) \vec{r} = 5\hat{i} + 2\hat{j} - 4\hat{k} + \lambda\left(3\hat{i} + 2\hat{j} - 8\hat{k}\right) r = 5 i ^ + 2 j ^ − 4 k ^ + λ ( 3 i ^ + 2 j ^ − 8 k ^ ) .
Step 2 — cartesian form:
Answer: x − 5 3 = y − 2 2 = z + 4 − 8 \dfrac{x - 5}{3} = \dfrac{y - 2}{2} = \dfrac{z + 4}{-8} 3 x − 5 = 2 y − 2 = − 8 z + 4 — note z − ( − 4 ) z - (-4) z − ( − 4 ) becomes z + 4 z + 4 z + 4 ; sign slips here cost a full part.
Example 5 — Line through two points
Find the equations of the line through A ( − 1 , 0 , 2 ) A(-1, 0, 2) A ( − 1 , 0 , 2 ) and B ( 3 , 4 , 6 ) B(3, 4, 6) B ( 3 , 4 , 6 ) .
Step 1 — direction: A B → = 4 i ^ + 4 j ^ + 4 k ^ \overrightarrow{AB} = 4\hat{i} + 4\hat{j} + 4\hat{k} A B = 4 i ^ + 4 j ^ + 4 k ^ , and any proportional triple works — take 1 , 1 , 1 1, 1, 1 1 , 1 , 1 .
Step 2 — write both forms: r ⃗ = − i ^ + 2 k ^ + λ ( i ^ + j ^ + k ^ ) \vec{r} = -\hat{i} + 2\hat{k} + \lambda\left(\hat{i} + \hat{j} + \hat{k}\right) r = − i ^ + 2 k ^ + λ ( i ^ + j ^ + k ^ ) .
Answer: x + 1 1 = y 1 = z − 2 1 \dfrac{x + 1}{1} = \dfrac{y}{1} = \dfrac{z - 2}{1} 1 x + 1 = 1 y = 1 z − 2 — simplifying the DRs before writing the equation keeps everything clean.
Example 6 — Reading a cartesian equation correctly
Write the direction ratios and a point on the line 1 − x 2 = y + 3 5 = 2 z − 6 4 \dfrac{1 - x}{2} = \dfrac{y + 3}{5} = \dfrac{2z - 6}{4} 2 1 − x = 5 y + 3 = 4 2 z − 6 .
Step 1 — force standard form: 1 − x 2 = x − 1 − 2 \dfrac{1-x}{2} = \dfrac{x - 1}{-2} 2 1 − x = − 2 x − 1 and 2 z − 6 4 = z − 3 2 \dfrac{2z-6}{4} = \dfrac{z - 3}{2} 4 2 z − 6 = 2 z − 3 .
Step 2 — now read off:
x − 1 − 2 = y + 3 5 = z − 3 2 \frac{x - 1}{-2} = \frac{y + 3}{5} = \frac{z - 3}{2} − 2 x − 1 = 5 y + 3 = 2 z − 3
Answer: point ( 1 , − 3 , 3 ) (1, -3, 3) ( 1 , − 3 , 3 ) , DRs − 2 , 5 , 2 -2, 5, 2 − 2 , 5 , 2 — reading DRs before standardising would give the wrong triple 2 , 5 , 4 2, 5, 4 2 , 5 , 4 .
Example 7 — A line equally inclined to the axes
Find the direction cosines of a line equally inclined to the three coordinate axes.
Step 1 — set l = m = n l = m = n l = m = n : then 3 l 2 = 1 3l^2 = 1 3 l 2 = 1 .
Answer: l = m = n = ± 1 3 l = m = n = \pm\dfrac{1}{\sqrt{3}} l = m = n = ± 3 1 — the DRs are simply 1 , 1 , 1 1, 1, 1 1 , 1 , 1 .
Worked Examples — Angles and Shortest Distances
Example 8 — Angle between two lines (DRs given)
Find the angle between the lines with direction ratios 3 , 5 , 4 3, 5, 4 3 , 5 , 4 and 1 , 1 , 2 1, 1, 2 1 , 1 , 2 .
Step 1 — the three ingredients: b 1 ⃗ ⋅ b 2 ⃗ = 3 + 5 + 8 = 16 \vec{b_1}\cdot\vec{b_2} = 3 + 5 + 8 = 16 b 1 ⋅ b 2 = 3 + 5 + 8 = 16 , ∣ b 1 ⃗ ∣ = 50 = 5 2 \vert\vec{b_1}\vert = \sqrt{50} = 5\sqrt{2} ∣ b 1 ∣ = 50 = 5 2 , ∣ b 2 ⃗ ∣ = 6 \vert\vec{b_2}\vert = \sqrt{6} ∣ b 2 ∣ = 6 .
Step 2 — the formula: cos θ = 16 5 2 ⋅ 6 = 16 10 3 = 8 3 15 \cos\theta = \dfrac{16}{5\sqrt{2}\cdot\sqrt{6}} = \dfrac{16}{10\sqrt{3}} = \dfrac{8\sqrt{3}}{15} cos θ = 5 2 ⋅ 6 16 = 10 3 16 = 15 8 3 .
Answer: θ = cos − 1 8 3 15 \theta = \cos^{-1}\dfrac{8\sqrt{3}}{15} θ = cos − 1 15 8 3 — rationalise before boxing the answer.
Find the angle between r ⃗ = a 1 ⃗ + λ ( 3 i ^ + 2 j ^ + 6 k ^ ) \vec{r} = \vec{a_1} + \lambda\left(3\hat{i} + 2\hat{j} + 6\hat{k}\right) r = a 1 + λ ( 3 i ^ + 2 j ^ + 6 k ^ ) and r ⃗ = a 2 ⃗ + μ ( i ^ + 2 j ^ + 2 k ^ ) \vec{r} = \vec{a_2} + \mu\left(\hat{i} + 2\hat{j} + 2\hat{k}\right) r = a 2 + μ ( i ^ + 2 j ^ + 2 k ^ ) .
Step 1 — only the direction vectors matter: b 1 ⃗ ⋅ b 2 ⃗ = 3 + 4 + 12 = 19 \vec{b_1}\cdot\vec{b_2} = 3 + 4 + 12 = 19 b 1 ⋅ b 2 = 3 + 4 + 12 = 19 , ∣ b 1 ⃗ ∣ = 7 \vert\vec{b_1}\vert = 7 ∣ b 1 ∣ = 7 , ∣ b 2 ⃗ ∣ = 3 \vert\vec{b_2}\vert = 3 ∣ b 2 ∣ = 3 .
Answer: θ = cos − 1 19 21 \theta = \cos^{-1}\dfrac{19}{21} θ = cos − 1 21 19 — the points a 1 ⃗ , a 2 ⃗ \vec{a_1}, \vec{a_2} a 1 , a 2 play no role in the angle.
Example 10 — Perpendicularity check
Show that the lines with direction ratios 2 , 1 , − 2 2, 1, -2 2 , 1 , − 2 and 1 , 2 , 2 1, 2, 2 1 , 2 , 2 are perpendicular.
Step 1 — the dot-product test: 2 ( 1 ) + 1 ( 2 ) + ( − 2 ) ( 2 ) = 2 + 2 − 4 = 0 2(1) + 1(2) + (-2)(2) = 2 + 2 - 4 = 0 2 ( 1 ) + 1 ( 2 ) + ( − 2 ) ( 2 ) = 2 + 2 − 4 = 0 .
Answer: the sum vanishes, so the lines are perpendicular — one line of arithmetic, full marks.
Example 11 — Shortest distance between skew lines
Find the shortest distance between r ⃗ = i ^ + 2 j ^ + k ^ + λ ( i ^ − j ^ + k ^ ) \vec{r} = \hat{i} + 2\hat{j} + \hat{k} + \lambda\left(\hat{i} - \hat{j} + \hat{k}\right) r = i ^ + 2 j ^ + k ^ + λ ( i ^ − j ^ + k ^ ) and r ⃗ = 2 i ^ − j ^ − k ^ + μ ( 2 i ^ + j ^ + 2 k ^ ) \vec{r} = 2\hat{i} - \hat{j} - \hat{k} + \mu\left(2\hat{i} + \hat{j} + 2\hat{k}\right) r = 2 i ^ − j ^ − k ^ + μ ( 2 i ^ + j ^ + 2 k ^ ) .
Step 1 — extract the four vectors: a 1 ⃗ = ( 1 , 2 , 1 ) \vec{a_1} = (1,2,1) a 1 = ( 1 , 2 , 1 ) , b 1 ⃗ = ( 1 , − 1 , 1 ) \vec{b_1} = (1,-1,1) b 1 = ( 1 , − 1 , 1 ) , a 2 ⃗ = ( 2 , − 1 , − 1 ) \vec{a_2} = (2,-1,-1) a 2 = ( 2 , − 1 , − 1 ) , b 2 ⃗ = ( 2 , 1 , 2 ) \vec{b_2} = (2,1,2) b 2 = ( 2 , 1 , 2 ) .
Step 2 — cross product:
b 1 ⃗ × b 2 ⃗ = ∣ i ^ j ^ k ^ 1 − 1 1 2 1 2 ∣ = − 3 i ^ + 0 j ^ + 3 k ^ , ∣ b 1 ⃗ × b 2 ⃗ ∣ = 3 2 \vec{b_1}\times\vec{b_2} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 1 & -1 & 1 \\ 2 & 1 & 2 \end{vmatrix} = -3\hat{i} + 0\hat{j} + 3\hat{k}, \qquad \vert\vec{b_1}\times\vec{b_2}\vert = 3\sqrt{2} b 1 × b 2 = i ^ 1 2 j ^ − 1 1 k ^ 1 2 = − 3 i ^ + 0 j ^ + 3 k ^ , ∣ b 1 × b 2 ∣ = 3 2
Step 3 — dot with a 2 ⃗ − a 1 ⃗ = ( 1 , − 3 , − 2 ) \vec{a_2} - \vec{a_1} = (1, -3, -2) a 2 − a 1 = ( 1 , − 3 , − 2 ) : ( − 3 ) ( 1 ) + 0 ( − 3 ) + 3 ( − 2 ) = − 9 (-3)(1) + 0(-3) + 3(-2) = -9 ( − 3 ) ( 1 ) + 0 ( − 3 ) + 3 ( − 2 ) = − 9 .
Step 4 — divide: d = ∣ − 9 ∣ 3 2 = 3 2 d = \dfrac{\vert -9\vert}{3\sqrt{2}} = \dfrac{3}{\sqrt{2}} d = 3 2 ∣ − 9∣ = 2 3 .
Answer: 3 2 2 \dfrac{3\sqrt{2}}{2} 2 3 2 units.
Example 12 — Shortest distance, cartesian data
Find the shortest distance between x + 1 7 = y + 1 − 6 = z + 1 1 \dfrac{x + 1}{7} = \dfrac{y + 1}{-6} = \dfrac{z + 1}{1} 7 x + 1 = − 6 y + 1 = 1 z + 1 and x − 3 1 = y − 5 − 2 = z − 7 1 \dfrac{x - 3}{1} = \dfrac{y - 5}{-2} = \dfrac{z - 7}{1} 1 x − 3 = − 2 y − 5 = 1 z − 7 .
Step 1 — extract: a 1 ⃗ = ( − 1 , − 1 , − 1 ) \vec{a_1} = (-1,-1,-1) a 1 = ( − 1 , − 1 , − 1 ) , b 1 ⃗ = ( 7 , − 6 , 1 ) \vec{b_1} = (7,-6,1) b 1 = ( 7 , − 6 , 1 ) ; a 2 ⃗ = ( 3 , 5 , 7 ) \vec{a_2} = (3,5,7) a 2 = ( 3 , 5 , 7 ) , b 2 ⃗ = ( 1 , − 2 , 1 ) \vec{b_2} = (1,-2,1) b 2 = ( 1 , − 2 , 1 ) .
Step 2 — cross product: b 1 ⃗ × b 2 ⃗ = − 4 i ^ − 6 j ^ − 8 k ^ \vec{b_1}\times\vec{b_2} = -4\hat{i} - 6\hat{j} - 8\hat{k} b 1 × b 2 = − 4 i ^ − 6 j ^ − 8 k ^ , with magnitude 116 = 2 29 \sqrt{116} = 2\sqrt{29} 116 = 2 29 .
Step 3 — dot with a 2 ⃗ − a 1 ⃗ = ( 4 , 6 , 8 ) \vec{a_2} - \vec{a_1} = (4, 6, 8) a 2 − a 1 = ( 4 , 6 , 8 ) : − 16 − 36 − 64 = − 116 -16 - 36 - 64 = -116 − 16 − 36 − 64 = − 116 .
Step 4 — divide: d = 116 2 29 = 58 29 d = \dfrac{116}{2\sqrt{29}} = \dfrac{58}{\sqrt{29}} d = 2 29 116 = 29 58 .
Answer: 2 29 2\sqrt{29} 2 29 units — simplify the surd fully: 58 29 = 58 29 29 = 2 29 \frac{58}{\sqrt{29}} = \frac{58\sqrt{29}}{29} = 2\sqrt{29} 29 58 = 29 58 29 = 2 29 .
Example 13 — Distance between parallel lines
Find the distance between r ⃗ = i ^ + 2 j ^ − 4 k ^ + λ ( 2 i ^ + 3 j ^ + 6 k ^ ) \vec{r} = \hat{i} + 2\hat{j} - 4\hat{k} + \lambda\left(2\hat{i} + 3\hat{j} + 6\hat{k}\right) r = i ^ + 2 j ^ − 4 k ^ + λ ( 2 i ^ + 3 j ^ + 6 k ^ ) and r ⃗ = 3 i ^ + 3 j ^ − 5 k ^ + μ ( 2 i ^ + 3 j ^ + 6 k ^ ) \vec{r} = 3\hat{i} + 3\hat{j} - 5\hat{k} + \mu\left(2\hat{i} + 3\hat{j} + 6\hat{k}\right) r = 3 i ^ + 3 j ^ − 5 k ^ + μ ( 2 i ^ + 3 j ^ + 6 k ^ ) .
Step 1 — same b ⃗ \vec{b} b , so use the parallel formula: a 2 ⃗ − a 1 ⃗ = ( 2 , 1 , − 1 ) \vec{a_2} - \vec{a_1} = (2, 1, -1) a 2 − a 1 = ( 2 , 1 , − 1 ) .
Step 2 — cross product:
b ⃗ × ( a 2 ⃗ − a 1 ⃗ ) = ∣ i ^ j ^ k ^ 2 3 6 2 1 − 1 ∣ = − 9 i ^ + 14 j ^ − 4 k ^ , ∣ ⋅ ∣ = 293 \vec{b}\times\left(\vec{a_2} - \vec{a_1}\right) = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 2 & 3 & 6 \\ 2 & 1 & -1 \end{vmatrix} = -9\hat{i} + 14\hat{j} - 4\hat{k}, \qquad \vert\cdot\vert = \sqrt{293} b × ( a 2 − a 1 ) = i ^ 2 2 j ^ 3 1 k ^ 6 − 1 = − 9 i ^ + 14 j ^ − 4 k ^ , ∣ ⋅ ∣ = 293
Step 3 — divide by ∣ b ⃗ ∣ = 7 \vert\vec{b}\vert = 7 ∣ b ∣ = 7 :
Answer: 293 7 \dfrac{\sqrt{293}}{7} 7 293 units — spotting that the direction vectors match (and switching formulas) is the first mark of the question.