Vectors (ME-V1)

NSWMaths Extension 1Syllabus dot point

How do we represent a line in the plane using vector equations?

Write parametric vector equations of lines and convert between vector and Cartesian forms

A focused answer to the HSC Maths Extension 1 dot point on parametric vector equations of lines. The point-direction form r=a+λd\mathbf{r} = \mathbf{a} + \lambda \mathbf{d}, conversion to Cartesian, intersection of lines, and the use of parametric form for collision and meeting-point problems.

Generated by Claude OpusReviewed by Better Tuition Academy7 min answer

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What this dot point is asking

NESA wants you to represent a line in the plane in vector form using a point on the line and a direction vector, convert between this and Cartesian form, and use the form to solve intersection and meeting problems.

The answer

Vector equation of a line

A line through point AA with direction vector d\mathbf{d} (non-zero) is the set of points

r=a+λd,λR,\mathbf{r} = \mathbf{a} + \lambda \mathbf{d}, \quad \lambda \in \mathbb{R},

where a\mathbf{a} is the position vector of AA and r\mathbf{r} is the position vector of a general point on the line.

In components,

(xy)=(a1a2)+λ(d1d2),\begin{pmatrix} x \\ y \end{pmatrix} = \begin{pmatrix} a_1 \\ a_2 \end{pmatrix} + \lambda \begin{pmatrix} d_1 \\ d_2 \end{pmatrix},

so x=a1+λd1x = a_1 + \lambda d_1 and y=a2+λd2y = a_2 + \lambda d_2.

Line through two points

A line through points AA and BB has direction vector AB=ba\mathbf{AB} = \mathbf{b} - \mathbf{a}. So

r=a+λ(ba),\mathbf{r} = \mathbf{a} + \lambda (\mathbf{b} - \mathbf{a}),

which can also be written as r=(1λ)a+λb\mathbf{r} = (1 - \lambda) \mathbf{a} + \lambda \mathbf{b}. At λ=0\lambda = 0 we are at AA, at λ=1\lambda = 1 we are at BB.

Converting to Cartesian form

From the parametric form, eliminate λ\lambda.

If d10d_1 \neq 0, from x=a1+λd1x = a_1 + \lambda d_1, solve for λ=xa1d1\lambda = \frac{x - a_1}{d_1}. Substitute into yy:

y=a2+xa1d1d2.y = a_2 + \frac{x - a_1}{d_1} \cdot d_2.

Rearranging, ya2=d2d1(xa1)y - a_2 = \frac{d_2}{d_1} (x - a_1), which is the point-slope form with slope d2d1\frac{d_2}{d_1}.

Vertical and horizontal lines

If d1=0d_1 = 0, the line is vertical: x=a1x = a_1 for all λ\lambda.

If d2=0d_2 = 0, the line is horizontal: y=a2y = a_2.

The parametric form handles these cleanly; Cartesian form needs a special case.

Intersection of two lines

Set the parametric equations of two lines equal:

a1+λd1=a2+μd2.\mathbf{a}_1 + \lambda \mathbf{d}_1 = \mathbf{a}_2 + \mu \mathbf{d}_2.

This is two equations (one for xx, one for yy) in two unknowns λ\lambda and μ\mu. Solve. If a unique solution exists, the lines meet at a single point; if the system is inconsistent, the lines are parallel and disjoint.

Two interpretations of IMATH_38

  • Geometric parameter: λ\lambda is just a real number indexing points along the line.
  • Time: if a particle moves with velocity d\mathbf{d} starting at a\mathbf{a} at time 00, then r(t)=a+td\mathbf{r}(t) = \mathbf{a} + t \mathbf{d} is the position at time tt.

The latter is useful for collision problems: do two particles meet, and if so when?

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