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Applications of vectors to 3-D geometryEdexcel A-Level Further Maths: Revision notes

Section 1

Equations of a line

A line through the point with position vector a\mathbf{a} with direction b\mathbf{b} has vector equation r=a+λb.\mathbf{r}=\mathbf{a}+\lambda\mathbf{b}. A line through two points AA and BB has direction AB→=b−a\overrightarrow{AB}=\mathbf{b}-\mathbf{a}. Writing r=xi+yj+zk\mathbf{r}=x\mathbf{i}+y\mathbf{j}+z\mathbf{k} and eliminating λ\lambda gives the Cartesian equations x−a1b1=y−a2b2=z−a3b3.\frac{x-a_1}{b_1}=\frac{y-a_2}{b_2}=\frac{z-a_3}{b_3}. For r=(i−2j+3k)+λ(2i+j−2k)\mathbf{r}=(\mathbf{i}-2\mathbf{j}+3\mathbf{k})+\lambda(2\mathbf{i}+\mathbf{j}-2\mathbf{k}) the Cartesian form is x−12=y+21=z−3−2\frac{x-1}{2}=\frac{y+2}{1}=\frac{z-3}{-2}. To test whether a point is on the line, find λ\lambda from one coordinate and check it gives the other two: (5,0,−1)(5,0,-1) has λ=2\lambda=2 in all three.

Key termsvector equationCartesian equationsparameter
Common mistake

Using the points as the direction: the direction is the difference of two position vectors, b−a\mathbf{b}-\mathbf{a}, not their sum.

Section 2

The form (r−a)×b=0(\mathbf{r}-\mathbf{a})\times\mathbf{b}=\mathbf{0}

The vector r−a\mathbf{r}-\mathbf{a} joins the fixed point AA to a general point on the line, and it is parallel to b\mathbf{b}. Two vectors are parallel exactly when their vector product is zero, so (r−a)×b=0(\mathbf{r}-\mathbf{a})\times\mathbf{b}=\mathbf{0} is another equation of the same line. To change from r=a+λb\mathbf{r}=\mathbf{a}+\lambda\mathbf{b}, subtract a\mathbf{a} and take the vector product with b\mathbf{b} on both sides, using b×b=0\mathbf{b}\times\mathbf{b}=\mathbf{0}. For the line above: (r−(i−2j+3k))×(2i+j−2k)=0\left(\mathbf{r}-(\mathbf{i}-2\mathbf{j}+3\mathbf{k})\right)\times(2\mathbf{i}+\mathbf{j}-2\mathbf{k})=\mathbf{0}.

Key termsparallel
Common mistake

Writing a scalar product: (r−a)⋅b=0(\mathbf{r}-\mathbf{a})\cdot\mathbf{b}=0 is a plane perpendicular to b\mathbf{b}, not a line.

Section 3

Direction ratios and direction cosines

The components l:m:nl:m:n of any vector along a line are direction ratios: the line with direction 2i+j−2k2\mathbf{i}+\mathbf{j}-2\mathbf{k} has ratios 2:1:−22:1:-2, and so does 4i+2j−4k4\mathbf{i}+2\mathbf{j}-4\mathbf{k}. The direction cosines are the cosines of the angles α,β,γ\alpha,\beta,\gamma the line makes with the xx-, yy- and zz-axes: cos⁡α=ll2+m2+n2, cos⁡β=ml2+m2+n2, cos⁡γ=nl2+m2+n2.\cos\alpha=\frac{l}{\sqrt{l^2+m^2+n^2}},\ \cos\beta=\frac{m}{\sqrt{l^2+m^2+n^2}},\ \cos\gamma=\frac{n}{\sqrt{l^2+m^2+n^2}}. They are the components of the unit vector along the line, so cos⁡2α+cos⁡2β+cos⁡2γ=1\cos^2\alpha+\cos^2\beta+\cos^2\gamma=1. For ratios 2:1:−22:1:-2 the magnitude is 33, so the direction cosines are 23,13,−23\frac23,\frac13,-\frac23. For 3:−4:123:-4:12 the magnitude is 1313, so the line makes an angle cos⁡−11213=22.6∘\cos^{-1}\frac{12}{13}=22.6^\circ with the zz-axis.

Key termsdirection ratiosdirection cosines
Common mistake

Giving the direction ratios when direction cosines are asked for: divide by the magnitude l2+m2+n2\sqrt{l^2+m^2+n^2}.

Section 4

Equations of a plane

A plane through the point with position vector a\mathbf{a} and perpendicular to a normal n\mathbf{n} has equation r⋅n=a⋅n.\mathbf{r}\cdot\mathbf{n}=\mathbf{a}\cdot\mathbf{n}. Writing n=n1i+n2j+n3k\mathbf{n}=n_1\mathbf{i}+n_2\mathbf{j}+n_3\mathbf{k} gives the Cartesian form n1x+n2y+n3z=dn_1x+n_2y+n_3z=d, with d=a⋅nd=\mathbf{a}\cdot\mathbf{n}. Example: through A(1,2,3)A(1,2,3) with n=2i−j+2k\mathbf{n}=2\mathbf{i}-\mathbf{j}+2\mathbf{k}: d=2−2+6=6d=2-2+6=6, so 2x−y+2z=62x-y+2z=6. A plane can also be written r=a+λb+μc\mathbf{r}=\mathbf{a}+\lambda\mathbf{b}+\mu\mathbf{c} for two non-parallel directions b\mathbf{b} and c\mathbf{c} in the plane. The normal is then b×c\mathbf{b}\times\mathbf{c}.

Key termsplanenormal
Common mistake

Forgetting the constant d=a⋅nd=\mathbf{a}\cdot\mathbf{n}, which describes a plane through the origin.

Section 5

Intersections and angles

To find where a line meets a plane, write a general point of the line in terms of λ\lambda, substitute it into the plane's equation, solve for λ\lambda, and substitute back. If the line has direction d\mathbf{d} and the plane has normal n\mathbf{n}, the acute angle θ\theta between the line and the plane satisfies sin⁡θ=∣d⋅n∣∣d∣∣n∣,\sin\theta=\frac{|\mathbf{d}\cdot\mathbf{n}|}{|\mathbf{d}||\mathbf{n}|}, because d⋅n\mathbf{d}\cdot\mathbf{n} gives the angle with the normal, which is 90∘−θ90^\circ-\theta. Example: d=2i+j−k\mathbf{d}=2\mathbf{i}+\mathbf{j}-\mathbf{k}, n=i+2j+2k\mathbf{n}=\mathbf{i}+2\mathbf{j}+2\mathbf{k}: sin⁡θ=236\sin\theta=\frac{2}{3\sqrt6}, so θ=15.8∘\theta=15.8^\circ. The angle between two planes is the angle between their normals: cos⁡ϕ=∣n1⋅n2∣∣n1∣∣n2∣\cos\phi=\frac{|\mathbf{n}_1\cdot\mathbf{n}_2|}{|\mathbf{n}_1||\mathbf{n}_2|}.

Key termsacute angle
Common mistake

Using cos⁡θ=∣d⋅n∣∣d∣∣n∣\cos\theta=\frac{|\mathbf{d}\cdot\mathbf{n}|}{|\mathbf{d}||\mathbf{n}|} for a line and a plane. That gives the angle between the line and the normal, so the formula for the line and plane uses sin⁡θ\sin\theta.

Section 6

Perpendicular distances

The distance from the point (x1,y1,z1)(x_1,y_1,z_1) to the plane n1x+n2y+n3z=dn_1x+n_2y+n_3z=d is ∣n1x1+n2y1+n3z1−d∣n12+n22+n32.\frac{|n_1x_1+n_2y_1+n_3z_1-d|}{\sqrt{n_1^2+n_2^2+n_3^2}}. For (4,3,−1)(4,3,-1) and 2x−y+2z=62x-y+2z=6: ∣8−3−2−6∣3=1\frac{|8-3-2-6|}{3}=1. To find the foot of the perpendicular, draw the line through the point in the direction n\mathbf{n} and find where it meets the plane. The distance from a point PP to a line through AA with direction d\mathbf{d} is ∣AP→×d∣∣d∣.\frac{|\overrightarrow{AP}\times\mathbf{d}|}{|\mathbf{d}|}. For A(1,−2,0)A(1,-2,0), d=3i−4j+12k\mathbf{d}=3\mathbf{i}-4\mathbf{j}+12\mathbf{k} and P(5,1,0)P(5,1,0): AP→×d=36i−48j−25k\overrightarrow{AP}\times\mathbf{d}=36\mathbf{i}-48\mathbf{j}-25\mathbf{k}, which has magnitude 6565, so the distance is 6513=5\frac{65}{13}=5.

Key termsfoot of the perpendicular
Exam tip

Divide by the magnitude of the normal (or direction) at the end, and take the modulus so the distance is positive.

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Exam questions on Applications of vectors to 3-D geometry

  1. The line ll has vector equation r=(i−2j+3k)+λ(2i+j−2k)\mathbf{r}=(\mathbf{i}-2\mathbf{j}+3\mathbf{k})+\lambda(2\mathbf{i}+\mathbf{j}-2\mathbf{k}).
    Find Cartesian equations for ll.2 marks
  2. The plane Π\Pi passes through the point A(1,2,3)A(1,2,3) and is perpendicular to the vector 2i−j+2k2\mathbf{i}-\mathbf{j}+2\mathbf{k}.
    The line mm passes through the origin and has direction i+j+k\mathbf{i}+\mathbf{j}+\mathbf{k}. Find the coordinates of the point where mm meets Π\Pi.2 marks
  3. The line ll has Cartesian equation x−13=y+2−4=z12\frac{x-1}{3}=\frac{y+2}{-4}=\frac{z}{12}, and the point PP has coordinates (5,1,0)(5,1,0).
    Find the direction cosines of ll, and the acute angle that ll makes with the zz-axis.3 marks
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Written by the Exaim team, led by Shaun Daswani (Head of Upper Secondary, Improve ME Institute; MSc Financial Mathematics, Imperial College London; BSc, UCL) and Jason Daswani (operational lead, Improve ME Institute; LSE).