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Vector geometric proofs in HSC Mathematics Extension 2: proving collinearity, perpendicularity, midpoint and parallelogram properties, and properties of 3D figures using position vectors and the scalar product

Syllabus dot point

“Prove geometric results using vectors, including properties of triangles, parallelograms and the diagonals of quadrilaterals, by expressing points as position vectors”

HSCMaths Extension 2Further Work with Vectors (MEX-V1)14 min read

Quick answer

A point PP is represented by its position vector p\mathbf{p}, and the segment from AA to BB is AB→=b−a\overrightarrow{AB} = \mathbf{b} - \mathbf{a}. Parallel means one vector is a scalar multiple of another; collinear means AB→=λAC→\overrightarrow{AB} = \lambda\overrightarrow{AC}; perpendicular means scalar product zero; equal length means equal magnitude. The midpoint of ABAB is 12(a+b)\frac{1}{2}(\mathbf{a} + \mathbf{b}), and the point dividing ABAB in ratio m:nm:n is na+mbm+n\frac{n\mathbf{a} + m\mathbf{b}}{m + n}. These tools prove classical results directly.

Jump to a section
  1. What this dot point is asking
  2. Position vectors and segments
  3. The four-step tactic (use this every time)
  4. The midpoint and section formulas
  5. Collinearity
  6. Using the scalar product for angles and lengths
  7. Proofs about three-dimensional figures
  8. How exam questions ask about vector proofs
  9. Exam-style questions

What this dot point is asking

NESA wants you to prove geometric theorems using vectors rather than coordinate or Euclidean methods. You represent each point by a position vector, express segments as differences of position vectors, and translate geometric facts (parallel, collinear, equal length, perpendicular, midpoint) into vector statements. The proof then follows from vector algebra and the scalar product. The appeal is that one or two lines of algebra often replace a page of coordinate work, and the result holds for any configuration, including in three dimensions where coordinate geometry becomes unwieldy.

Position vectors and segments

Fix an origin OO. Every point PP then corresponds to a position vector p=OP→\mathbf{p} = \overrightarrow{OP}. The directed segment from AA to BB is

AB→=b−a.\overrightarrow{AB} = \mathbf{b} - \mathbf{a}.

This single identity is the engine of vector geometry. Two segments AB→\overrightarrow{AB} and CD→\overrightarrow{CD} are parallel exactly when b−a=λ(d−c)\mathbf{b} - \mathbf{a} = \lambda(\mathbf{d} - \mathbf{c}) for some scalar λ\lambda. They are equal in length when ∣b−a∣=∣d−c∣|\mathbf{b} - \mathbf{a}| = |\mathbf{d} - \mathbf{c}|, and perpendicular when (b−a)⋅(d−c)=0(\mathbf{b} - \mathbf{a}) \cdot (\mathbf{d} - \mathbf{c}) = 0.

The four-step tactic (use this every time)

Vector proofs all follow the same shape. Treat it as a fixed procedure:

  1. Assign a position vector to every labelled point (and, if it helps, put the origin at a useful vertex so one or more vectors become 0\mathbf{0}).
  2. Express the displacement vectors the question is about, using XY→=y−x\overrightarrow{XY} = \mathbf{y} - \mathbf{x}.
  3. Compute the algebraic relation that encodes the geometric claim: an equality, a scalar multiple, or a zero scalar product.
  4. Conclude by translating that relation back into the geometric statement, in words.

The skill is matching the geometric claim to the right algebraic relation in step 3. Here is the dictionary.

Key fact

Translate the geometry into algebra:

  • Parallel (XY→∥UV→\overrightarrow{XY} \parallel \overrightarrow{UV}): one is a scalar multiple of the other, XY→=λ UV→\overrightarrow{XY} = \lambda\,\overrightarrow{UV}.
  • Equal and parallel (XY→=UV→\overrightarrow{XY} = \overrightarrow{UV}): same direction and length, the test for a parallelogram.
  • Collinear (XX, YY, ZZ on a line): XY→=λ XZ→\overrightarrow{XY} = \lambda\,\overrightarrow{XZ} (parallel sharing a point).
  • Perpendicular (XY→⊥UV→\overrightarrow{XY} \perp \overrightarrow{UV}): XY→⋅UV→=0\overrightarrow{XY} \cdot \overrightarrow{UV} = 0.
  • Equal length (∣XY∣=∣UV∣|XY| = |UV|): ∣XY→∣2=∣UV→∣2|\overrightarrow{XY}|^2 = |\overrightarrow{UV}|^2, expanded with v⋅v=∣v∣2\mathbf{v}\cdot\mathbf{v} = |\mathbf{v}|^2.
  • Midpoint MM of ABAB: m=12(a+b)\mathbf{m} = \tfrac{1}{2}(\mathbf{a} + \mathbf{b}).

The midpoint and section formulas

The midpoint MM of segment ABAB has position vector

m=12(a+b).\mathbf{m} = \tfrac{1}{2}(\mathbf{a} + \mathbf{b}).

More generally, the point PP dividing ABAB internally in the ratio m:nm:n (so AP:PB=m:nAP:PB = m:n) has position vector

p=na+mbm+n.\mathbf{p} = \frac{n\mathbf{a} + m\mathbf{b}}{m + n}.

This follows because AP→=mm+nAB→\overrightarrow{AP} = \frac{m}{m+n}\overrightarrow{AB}, so p=a+mm+n(b−a)\mathbf{p} = \mathbf{a} + \frac{m}{m+n}(\mathbf{b} - \mathbf{a}), which simplifies to the stated form. The cross-over of the labels is worth memorising: the point nearer BB (large mm) carries the weight mm on b\mathbf{b}. The midpoint is just the case m:n=1:1m:n = 1:1.

Collinearity

Three points AA, BB, CC are collinear when one displacement is a scalar multiple of another and they share a point: AB→=λ AC→\overrightarrow{AB} = \lambda\,\overrightarrow{AC}. The shared vertex AA is what upgrades "parallel" to "on the same line", since two parallel vectors that share an endpoint must lie along one line through that endpoint.

Three collinear points Points A, B and C lie on one line. To prove this, show the vector AB is a scalar multiple of the vector AC; the shared point A then forces all three onto the same line. AC AB O A B C Collinear if AB = λ AC: the shared point A pins all three to one line.

Using the scalar product for angles and lengths

When perpendicularity or equal lengths appear, the scalar product is decisive. The key identities are

∣u+v∣2=∣u∣2+2 u⋅v+∣v∣2,u⋅v=0  ⟺  u⊥v.|\mathbf{u} + \mathbf{v}|^2 = |\mathbf{u}|^2 + 2\,\mathbf{u}\cdot\mathbf{v} + |\mathbf{v}|^2, \qquad \mathbf{u}\cdot\mathbf{v} = 0 \iff \mathbf{u} \perp \mathbf{v}.

The first turns a length statement into an algebraic one (expand the square with v⋅v=∣v∣2\mathbf{v}\cdot\mathbf{v} = |\mathbf{v}|^2); the second is the perpendicularity test. Together they prove, for example, that a triangle inscribed in a semicircle has a right angle at the circumference, by placing the centre at the origin and showing two radii-based vectors have zero scalar product.

Proofs about three-dimensional figures

In Extension 2 the same machinery proves properties of solids: cubes, rectangular boxes and pyramids. The move is identical, only now the position vectors are three-component. The natural setup for a box is to put one vertex at the origin and call the three edges from it a\mathbf{a}, b\mathbf{b}, c\mathbf{c}; every other vertex is then a sum of these, and the space diagonal is a+b+c\mathbf{a} + \mathbf{b} + \mathbf{c}.

A box for a vector proof A rectangular box with vertex O at the front-bottom-left. The three edges from O along the width, height and depth are the vectors a, b and c. The space diagonal OG equals a plus b plus c. OG = a + b + c O A B C G Edges OA = a, OB = b, OC = c; the space diagonal is a + b + c.

With the edges mutually perpendicular and equal in length (a cube), a⋅b=b⋅c=c⋅a=0\mathbf{a}\cdot\mathbf{b} = \mathbf{b}\cdot\mathbf{c} = \mathbf{c}\cdot\mathbf{a} = 0 and ∣a∣=∣b∣=∣c∣|\mathbf{a}| = |\mathbf{b}| = |\mathbf{c}|. These two facts collapse most cube proofs to a couple of lines, as the worked example shows.

How exam questions ask about vector proofs

  • "Show that XX, YY, ZZ are collinear": show XY→=λ XZ→\overrightarrow{XY} = \lambda\,\overrightarrow{XZ}, then state they share the point XX.
  • "Show that PP lies on the line through AA and BB": write OP→=OA→+t AB→\overrightarrow{OP} = \overrightarrow{OA} + t\,\overrightarrow{AB} for some scalar tt.
  • "Prove that PQRSPQRS is a parallelogram": show one pair of opposite sides are equal vectors, PQ→=SR→\overrightarrow{PQ} = \overrightarrow{SR}.
  • "Prove the diagonals bisect each other": show the midpoints of the two diagonals have the same position vector.
  • "PP divides ABAB in the ratio m:nm:n; find its position vector": apply the section formula na+mbm+n\frac{n\mathbf{a} + m\mathbf{b}}{m+n}.
  • "Show that the angle ... is a right angle" or "... edges are perpendicular": show the relevant scalar product is zero, expanding with v⋅v=∣v∣2\mathbf{v}\cdot\mathbf{v} = |\mathbf{v}|^2 where needed.
Exam technique

Always define your position vectors in the first line ("Let OA→=a\overrightarrow{OA} = \mathbf{a}, ..."); markers award a mark just for setting up the vectors cleanly. Choosing the origin at a vertex (so that vertex's position vector is 0\mathbf{0}) often halves the algebra, do it when you can. State the geometric conclusion in words after the algebra ("so PQ→=SR→\overrightarrow{PQ} = \overrightarrow{SR}, hence PQRSPQRS is a parallelogram"), because the final mark is usually for the interpretation. For a length or right-angle claim, square the magnitude with ∣v∣2=v⋅v|\mathbf{v}|^2 = \mathbf{v}\cdot\mathbf{v} rather than taking roots. For a 3D figure, write each vertex as a sum of the edge vectors a\mathbf{a}, b\mathbf{b}, c\mathbf{c} and use the perpendicular/equal-length conditions of the solid. To prove parallelism you must produce the explicit scalar multiple, not just assert that two segments look parallel.

Prove the angle in a semicircle is a right angle

Prove the angle in a semicircle is a right angle

We want to show that any point PP on a circle, when connected to the two endpoints of a diameter, forms a right angle at PP. The key is that two vectors are perpendicular exactly when their scalar product equals zero.

Set up the geometry with position vectors: Place the centre OO at the origin. Let ABAB be a diameter, so AA has position vector a\mathbf{a} and BB has position vector −a-\mathbf{a}, giving ∣a∣=r|\mathbf{a}| = r. Let PP be any other point on the circle, with ∣p∣=r|\mathbf{p}| = r.

Write the two vectors meeting at PP: The vectors from PP to AA and from PP to BB are found by subtracting the position vector of the tail from that of the head:

PA→=a−p,PB→=−a−p.\overrightarrow{PA} = \mathbf{a} - \mathbf{p}, \qquad \overrightarrow{PB} = -\mathbf{a} - \mathbf{p}.

Compute the scalar product: To test for a right angle, expand PA→⋅PB→\overrightarrow{PA}\cdot\overrightarrow{PB} using the distributive property of the scalar product:

PA→⋅PB→=(a−p)⋅(−a−p)=−a⋅a−a⋅p+p⋅a+p⋅p.\overrightarrow{PA}\cdot\overrightarrow{PB} = (\mathbf{a} - \mathbf{p})\cdot(-\mathbf{a} - \mathbf{p}) = -\mathbf{a}\cdot\mathbf{a} - \mathbf{a}\cdot\mathbf{p} + \mathbf{p}\cdot\mathbf{a} + \mathbf{p}\cdot\mathbf{p}.

The middle terms cancel because the scalar product is commutative (a⋅p=p⋅a\mathbf{a}\cdot\mathbf{p} = \mathbf{p}\cdot\mathbf{a}), leaving:

=−∣a∣2+∣p∣2=−r2+r2=0.= -|\mathbf{a}|^2 + |\mathbf{p}|^2 = -r^2 + r^2 = 0.

Conclude and verify: Since PA→⋅PB→=0\overrightarrow{PA}\cdot\overrightarrow{PB} = 0, the vectors are perpendicular, so the angle ∠APB\angle APB is a right angle. This holds for any point PP on the circle other than AA and BB.

To verify with a concrete example: take a=(1,0)\mathbf{a} = (1, 0), r=1r = 1, p=(0,1)\mathbf{p} = (0, 1). Then PA→=(1,−1)\overrightarrow{PA} = (1, -1) and PB→=(−1,−1)\overrightarrow{PB} = (-1, -1), giving scalar product =(1)(−1)+(−1)(−1)=−1+1=0= (1)(-1) + (-1)(-1) = -1 + 1 = 0. Confirmed.

Final answer: PA→⋅PB→=0\overrightarrow{PA}\cdot\overrightarrow{PB} = 0 for any PP on the circle, so the angle in a semicircle is always a right angle.

Prove the long diagonal and an edge of a cube are not perpendicular, then find the angle

Prove the long diagonal and an edge of a cube are not perpendicular, then find the angle

A cube has one vertex at OO with edges OA→=a\overrightarrow{OA} = \mathbf{a}, OB→=b\overrightarrow{OB} = \mathbf{b}, OC→=c\overrightarrow{OC} = \mathbf{c}, mutually perpendicular and each of length ss. The space diagonal is OG→=a+b+c\overrightarrow{OG} = \mathbf{a} + \mathbf{b} + \mathbf{c}. Find the angle between the space diagonal OG→\overrightarrow{OG} and the edge OA→\overrightarrow{OA}.

Record the cube conditions: Because the edges are mutually perpendicular, a⋅b=b⋅c=c⋅a=0\mathbf{a}\cdot\mathbf{b} = \mathbf{b}\cdot\mathbf{c} = \mathbf{c}\cdot\mathbf{a} = 0. Because they are equal in length, a⋅a=b⋅b=c⋅c=s2\mathbf{a}\cdot\mathbf{a} = \mathbf{b}\cdot\mathbf{b} = \mathbf{c}\cdot\mathbf{c} = s^2.

Compute the scalar product of diagonal and edge: Expand OG→⋅OA→\overrightarrow{OG}\cdot\overrightarrow{OA} and use the conditions:

OG→⋅OA→=(a+b+c)⋅a=a⋅a+b⋅a+c⋅a=s2+0+0=s2.\overrightarrow{OG}\cdot\overrightarrow{OA} = (\mathbf{a} + \mathbf{b} + \mathbf{c})\cdot\mathbf{a} = \mathbf{a}\cdot\mathbf{a} + \mathbf{b}\cdot\mathbf{a} + \mathbf{c}\cdot\mathbf{a} = s^2 + 0 + 0 = s^2.

Since this is s2≠0s^2 \neq 0, the space diagonal is not perpendicular to the edge.

Find the two magnitudes: The edge has length ∣OA→∣=s|\overrightarrow{OA}| = s. The diagonal has

∣OG→∣2=(a+b+c)⋅(a+b+c)=a⋅a+b⋅b+c⋅c=3s2,|\overrightarrow{OG}|^2 = (\mathbf{a} + \mathbf{b} + \mathbf{c})\cdot(\mathbf{a} + \mathbf{b} + \mathbf{c}) = \mathbf{a}\cdot\mathbf{a} + \mathbf{b}\cdot\mathbf{b} + \mathbf{c}\cdot\mathbf{c} = 3s^2,

where every cross term vanishes by perpendicularity, so ∣OG→∣=s3|\overrightarrow{OG}| = s\sqrt{3}.

Combine into the angle: Using cos⁡θ=OG→⋅OA→∣OG→∣∣OA→∣\cos\theta = \dfrac{\overrightarrow{OG}\cdot\overrightarrow{OA}}{|\overrightarrow{OG}||\overrightarrow{OA}|}:

cos⁡θ=s2(s3)(s)=13  ⟹  θ=arccos⁡13≈54.7∘.\cos\theta = \frac{s^2}{(s\sqrt{3})(s)} = \frac{1}{\sqrt{3}} \;\Longrightarrow\; \theta = \arccos\frac{1}{\sqrt{3}} \approx 54.7^\circ.

Final answer: the space diagonal and an edge meet at arccos⁡13≈54.7∘\arccos\dfrac{1}{\sqrt{3}} \approx 54.7^\circ, so they are not perpendicular.

Common traps
Choosing a poor origin
Placing the origin at a vertex or centre named in the problem often removes a whole vector and shortens the proof. A careless origin makes the algebra heavy.
Confusing "parallel" with "collinear"
Parallel only needs a scalar multiple; collinear also needs a shared point. State the common vertex when concluding collinearity.
Confusing the section ratio
In na+mbm+n\frac{n\mathbf{a} + m\mathbf{b}}{m+n} for ratio m:nm:n, the weight on a\mathbf{a} is nn, not mm. Mixing these places the point on the wrong side.
Treating the scalar product as a vector
u⋅v\mathbf{u}\cdot\mathbf{v} is a scalar. You cannot add it to a vector or take its direction.
Forgetting the cube conditions in 3D proofs
A box proof stalls until you write down a⋅b=0\mathbf{a}\cdot\mathbf{b} = 0 for perpendicular edges and ∣a∣=∣b∣=∣c∣|\mathbf{a}| = |\mathbf{b}| = |\mathbf{c}| for a cube. These collapse the cross terms.
Stopping at the algebra
After deriving the relation, state the geometric conclusion in words. The final mark is for the interpretation.

Exam-style questions

Questions in the style of NESA exam questions on this dot point, each with a worked answer. They are written by ExamExplained unless tagged "Past paper"; the year shows the paper a question is modelled on.

2023 HSC-style2 marks
The quadrilaterals ABCD and ABEF are parallelograms. By considering AB, show that CDFE is also a parallelogram.
Show worked answer →

Use the fact that in a parallelogram, opposite sides are equal and parallel as vectors.

In parallelogram ABCD, side AB equals side DC: AB = DC.

In parallelogram ABEF, side AB equals side FE: AB = FE.

Since both equal AB, transitivity gives DC = FE.

So in the quadrilateral CDFE the side DC is equal and parallel to the side FE. A quadrilateral with one pair of opposite sides equal and parallel is a parallelogram.

Therefore CDFE is a parallelogram.

Mark notes: 1 mark for expressing AB = DC and AB = FE from the two parallelograms, 1 mark for deducing DC = FE and concluding CDFE is a parallelogram.

2021 HSC-style4 marks
ABCDS is a pyramid where ABCD is a square whose diagonals bisect each other at H. (i) Show that HA + HB + HC + HD = 0. Let G be the point such that GA + GB + GC + GD + GS = 0. (ii) Using part (i), show that 4 GH + GS = 0. (iii) Find the value of L such that HG = L HS.
Show worked answer →

Part (i). H is the midpoint of both diagonals AC and BD, so HA = -HC and HB = -HD. Adding,
HA + HB + HC + HD = (HA + HC) + (HB + HD) = 0 + 0 = 0.

Part (ii). For any point X, GX = GH + HX. Sum over A, B, C, D:
GA + GB + GC + GD = 4 GH + (HA + HB + HC + HD) = 4 GH + 0 = 4 GH (using part (i)).
The defining condition is GA + GB + GC + GD + GS = 0, so 4 GH + GS = 0.

Part (iii). From 4 GH + GS = 0 we get GS = -4 GH = 4 HG (since GH = -HG).
Now HS = HG + GS = HG + 4 HG = 5 HG.
Therefore HG = (1/5) HS, so L = 1/5.

Mark notes: 1 mark for part (i); 2 marks for part (ii) (writing GX = GH + HX and using part (i)); 1 mark for part (iii) giving L = 1/5.

2024 HSC-style1 mark
Let a = OA, b = OB, where O is the origin and A, B are different from each other and the origin. The point M is such that (1/2)(a + b) = OM. Show that M lies on the line passing through A and B.
Show worked answer →

A point lies on the line through A and B if its position vector can be written as OA + t AB for some scalar t.

OM = (1/2)(a + b) = (1/2) a + (1/2) b.

Write this in terms of OA = a and AB = b - a:
OM = a + (1/2)(b - a) = OA + (1/2) AB.

This is of the form OA + t AB with t = 1/2, so M lies on the line through A and B (it is in fact the midpoint of AB).

Mark notes: 1 mark for expressing OM as OA + (1/2) AB, showing M is on line AB.

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