Borui Academy

Chapter 6

Plane Vectors

平面向量 · operations · dot product · collinearity · coordinate form

Unit 6 · Plane Vectors 平面向量

By the end of this chapter you can:

  1. Add, subtract, and scalar-multiply vectors using both the geometric (triangle/parallelogram) rule and coordinate arithmetic
  2. Compute the dot product a⃗⋅b⃗=∣a⃗∣∣b⃗∣cos⁡θ\vec{a} \cdot \vec{b} = |\vec{a}||\vec{b}|\cos\theta and apply the perpendicularity shortcut a⃗⋅b⃗=0\vec{a} \cdot \vec{b} = 0
  3. Determine whether two vectors are collinear using the scalar condition a⃗=λb⃗\vec{a} = \lambda \vec{b} or the coordinate cross-test x1y2=x2y1x_1 y_2 = x_2 y_1
  4. Solve exam problems that mix coordinate calculation, angle-finding, and geometric proof with vectors

Exam weight on past CSCA papers: ~8% (3–4 of 48 MCQs).


6.1 Vector Operations 向量的运算

A vector (向量) is a quantity with both magnitude (size) and direction. We write a⃗\vec{a} or AB→\overrightarrow{AB} (from point AA to point BB). A plain number with no direction is a scalar (标量).

Key vocabulary

Term Symbol Meaning
Magnitude (模) ∣a⃗∣|\vec{a}| length of the arrow; always ≥0\ge 0
Zero vector (零向量) 0⃗\vec{0} magnitude 00; direction undefined
Unit vector (单位向量) a^\hat{a} magnitude exactly 11
Opposite vector (反向量) −a⃗-\vec{a} same length, opposite direction
Equal vectors a⃗=b⃗\vec{a} = \vec{b} same magnitude and same direction (position doesn't matter)

Addition: triangle rule and parallelogram rule

Triangle rule (三角形法则): Place the tail of b⃗\vec{b} at the head of a⃗\vec{a}. The sum a⃗+b⃗\vec{a} + \vec{b} runs from the tail of a⃗\vec{a} to the head of b⃗\vec{b}.

Parallelogram rule (平行四边形法则): Place both vectors at the same tail point. The diagonal of the resulting parallelogram is a⃗+b⃗\vec{a} + \vec{b}.

a⃗+b⃗=b⃗+a⃗(commutative)\vec{a} + \vec{b} = \vec{b} + \vec{a} \qquad (\text{commutative})
(a⃗+b⃗)+c⃗=a⃗+(b⃗+c⃗)(associative)(\vec{a} + \vec{b}) + \vec{c} = \vec{a} + (\vec{b} + \vec{c}) \qquad (\text{associative})

⚠️ Direction matters. AB→+BC→=AC→\overrightarrow{AB} + \overrightarrow{BC} = \overrightarrow{AC} (the middle point cancels). But AB→+CB→≠AC→\overrightarrow{AB} + \overrightarrow{CB} \ne \overrightarrow{AC} — the arrow on CB→\overrightarrow{CB} runs the wrong way.

Subtraction

a⃗−b⃗=a⃗+(−b⃗)\vec{a} - \vec{b} = \vec{a} + (-\vec{b})

Geometrically: place both vectors at the same tail; the difference points from the head of b⃗\vec{b} to the head of a⃗\vec{a}.

Scalar multiplication (数乘)

For scalar λ∈R\lambda \in \mathbb{R}:

∣λa⃗∣=∣λ∣⋅∣a⃗∣|\lambda \vec{a}| = |\lambda| \cdot |\vec{a}|

  • λ>0\lambda > 0: same direction as a⃗\vec{a}
  • λ<0\lambda < 0: opposite direction
  • λ=0\lambda = 0: gives 0⃗\vec{0}

Distributive laws:
λ(a⃗+b⃗)=λa⃗+λb⃗,(λ+μ)a⃗=λa⃗+μa⃗\lambda(\vec{a} + \vec{b}) = \lambda \vec{a} + \lambda \vec{b}, \qquad (\lambda + \mu)\vec{a} = \lambda \vec{a} + \mu \vec{a}

Worked Example 6.1.A

In parallelogram ABCDABCD, let AB→=p⃗\overrightarrow{AB} = \vec{p} and AD→=q⃗\overrightarrow{AD} = \vec{q}. Express AC→\overrightarrow{AC} and BD→\overrightarrow{BD} in terms of p⃗\vec{p} and q⃗\vec{q}.

Solution.

By the parallelogram rule, diagonal AC→=AB→+AD→=p⃗+q⃗\overrightarrow{AC} = \overrightarrow{AB} + \overrightarrow{AD} = \vec{p} + \vec{q}.

For the other diagonal, use the triangle rule through AA:
BD→=BA→+AD→=−p⃗+q⃗=q⃗−p⃗.\overrightarrow{BD} = \overrightarrow{BA} + \overrightarrow{AD} = -\vec{p} + \vec{q} = \vec{q} - \vec{p}.

AC→=p⃗+q⃗,BD→=q⃗−p⃗\boxed{\overrightarrow{AC} = \vec{p} + \vec{q}, \quad \overrightarrow{BD} = \vec{q} - \vec{p}}

🔑 Cancellation trick: In any chain AB→+BC→+CD→=AD→\overrightarrow{AB} + \overrightarrow{BC} + \overrightarrow{CD} = \overrightarrow{AD}, intermediate points cancel like a telescoping sum. This is the fastest way to simplify multi-leg vector paths.


6.2 Dot Product 数量积(内积)

The dot product of two vectors is a scalar (number), not a vector:

a⃗⋅b⃗=∣a⃗∣∣b⃗∣cos⁡θ\vec{a} \cdot \vec{b} = |\vec{a}||\vec{b}|\cos\theta

where θ\theta is the angle between the vectors (0≤θ≤π0 \le \theta \le \pi).

Properties you must know

Property Formula
Commutative a⃗⋅b⃗=b⃗⋅a⃗\vec{a} \cdot \vec{b} = \vec{b} \cdot \vec{a}
Self-dot a⃗⋅a⃗=∣a⃗∣2\vec{a} \cdot \vec{a} = |\vec{a}|^{2}
Distributive a⃗⋅(b⃗+c⃗)=a⃗⋅b⃗+a⃗⋅c⃗\vec{a} \cdot (\vec{b} + \vec{c}) = \vec{a} \cdot \vec{b} + \vec{a} \cdot \vec{c}
Scalar pull-out (λa⃗)⋅b⃗=λ(a⃗⋅b⃗)(\lambda \vec{a}) \cdot \vec{b} = \lambda (\vec{a} \cdot \vec{b})

🔑 Perpendicularity shortcut: a⃗⊥b⃗  ⟺  a⃗⋅b⃗=0\vec{a} \perp \vec{b} \iff \vec{a} \cdot \vec{b} = 0. (Because cos⁡90°=0\cos 90° = 0.) This is the single most useful fact in this chapter — expect it on every exam.

Finding the angle between two vectors

Rearrange the dot product formula:

cos⁡θ=a⃗⋅b⃗∣a⃗∣∣b⃗∣\cos\theta = \frac{\vec{a} \cdot \vec{b}}{|\vec{a}||\vec{b}|}

The angle θ∈[0°,180°]\theta \in [0°, 180°], so check the sign of the dot product first:

  • a⃗⋅b⃗>0⇒θ\vec{a} \cdot \vec{b} > 0 \Rightarrow \theta is acute
  • a⃗⋅b⃗=0⇒θ=90°\vec{a} \cdot \vec{b} = 0 \Rightarrow \theta = 90° (perpendicular)
  • a⃗⋅b⃗<0⇒θ\vec{a} \cdot \vec{b} < 0 \Rightarrow \theta is obtuse

Projection formula

The scalar projection of b⃗\vec{b} onto a⃗\vec{a} (the component of b⃗\vec{b} in the direction of a⃗\vec{a}):

proja⃗b⃗=a⃗⋅b⃗∣a⃗∣\text{proj}_{\vec{a}} \vec{b} = \frac{\vec{a} \cdot \vec{b}}{|\vec{a}|}

Equivalently, ∣b⃗∣cos⁡θ|\vec{b}|\cos\theta.

Worked Example 6.2.A

Vectors a⃗\vec{a} and b⃗\vec{b} satisfy ∣a⃗∣=2|\vec{a}| = 2, ∣b⃗∣=3|\vec{b}| = 3, and the angle between them is 60°60°. Find a⃗⋅b⃗\vec{a} \cdot \vec{b} and ∣a⃗+b⃗∣|\vec{a} + \vec{b}|.

Solution.

Step 1 — dot product:
a⃗⋅b⃗=∣a⃗∣∣b⃗∣cos⁡60°=2⋅3⋅12=3.\vec{a} \cdot \vec{b} = |\vec{a}||\vec{b}|\cos 60° = 2 \cdot 3 \cdot \tfrac{1}{2} = 3.

Step 2 — magnitude of sum (expand using ∣v⃗∣2=v⃗⋅v⃗|\vec{v}|^{2} = \vec{v} \cdot \vec{v}):
∣a⃗+b⃗∣2=(a⃗+b⃗)⋅(a⃗+b⃗)=∣a⃗∣2+2a⃗⋅b⃗+∣b⃗∣2=4+6+9=19.|\vec{a} + \vec{b}|^{2} = (\vec{a} + \vec{b}) \cdot (\vec{a} + \vec{b}) = |\vec{a}|^{2} + 2\vec{a} \cdot \vec{b} + |\vec{b}|^{2} = 4 + 6 + 9 = 19.
∣a⃗+b⃗∣=19.|\vec{a} + \vec{b}| = \sqrt{19}.

a⃗⋅b⃗=3,∣a⃗+b⃗∣=19\boxed{\vec{a} \cdot \vec{b} = 3, \quad |\vec{a} + \vec{b}| = \sqrt{19}}

⚠️ Common mistake: Students write ∣a⃗+b⃗∣=∣a⃗∣+∣b⃗∣|\vec{a} + \vec{b}| = |\vec{a}| + |\vec{b}|. This is only true when both vectors point in exactly the same direction. Always expand ∣a⃗+b⃗∣2|\vec{a} + \vec{b}|^{2} using the dot product.


6.3 Collinear Vectors 共线向量(平行向量)

Two non-zero vectors are collinear (共线, also called parallel, 平行) if they lie along parallel lines — i.e., one is a scalar multiple of the other.

Scalar condition

a⃗∥b⃗  ⟺  ∃ λ∈R, a⃗=λb⃗(b⃗≠0⃗)\vec{a} \parallel \vec{b} \iff \exists\, \lambda \in \mathbb{R},\ \vec{a} = \lambda \vec{b} \qquad (\vec{b} \ne \vec{0})

The scalar λ\lambda can be positive (same direction) or negative (opposite direction).

Coordinate collinearity test

If a⃗=(x1,y1)\vec{a} = (x_1, y_1) and b⃗=(x2,y2)\vec{b} = (x_2, y_2), then:

a⃗∥b⃗  ⟺  x1y2−x2y1=0  ⟺  x1y2=x2y1\vec{a} \parallel \vec{b} \iff x_1 y_2 - x_2 y_1 = 0 \iff x_1 y_2 = x_2 y_1

🔑 Memory aid: This is the cross-product condition. Think of it as the determinant ∣x1y1x2y2∣=0\begin{vmatrix} x_1 & y_1 \\ x_2 & y_2 \end{vmatrix} = 0. If this determinant equals zero, the vectors are parallel.

⚠️ Don't confuse collinear vectors with collinear points. Three points AA, BB, CC are collinear iff AB→∥AC→\overrightarrow{AB} \parallel \overrightarrow{AC} — apply the vector collinearity test to the vectors, not the coordinates directly.

Worked Example 6.3.A

If a⃗=(2,−1)\vec{a} = (2, -1) and b⃗=(k,3)\vec{b} = (k, 3) are collinear, find kk.

Solution.

Apply the collinearity condition x1y2=x2y1x_1 y_2 = x_2 y_1:
2⋅3=k⋅(−1)  ⟹  6=−k  ⟹  k=−6.2 \cdot 3 = k \cdot (-1) \implies 6 = -k \implies k = -6.

Check: b⃗=(−6,3)=−3(2,−1)=−3a⃗\vec{b} = (-6, 3) = -3(2, -1) = -3\vec{a}. ✓

k=−6\boxed{k = -6}


6.4 Vectors in Coordinate Form 向量的坐标表示

In a coordinate plane with unit vectors e⃗1=(1,0)\vec{e}_1 = (1,0) and e⃗2=(0,1)\vec{e}_2 = (0,1), every vector can be written as:

a⃗=(a1, a2)=a1e⃗1+a2e⃗2\vec{a} = (a_1,\ a_2) = a_1 \vec{e}_1 + a_2 \vec{e}_2

The ordered pair (a1,a2)(a_1, a_2) is the component form of a⃗\vec{a}.

Point-to-vector conversion

If A=(x1,y1)A = (x_1, y_1) and B=(x2,y2)B = (x_2, y_2), then:

AB→=(x2−x1, y2−y1)\overrightarrow{AB} = (x_2 - x_1,\ y_2 - y_1)

⚠️ Order matters: AB→=B−A\overrightarrow{AB} = B - A (head minus tail). BA→=A−B=−AB→\overrightarrow{BA} = A - B = -\overrightarrow{AB}.

Coordinate arithmetic

Let a⃗=(a1,a2)\vec{a} = (a_1, a_2), b⃗=(b1,b2)\vec{b} = (b_1, b_2), scalar λ\lambda.

Operation Formula
Addition a⃗+b⃗=(a1+b1, a2+b2)\vec{a} + \vec{b} = (a_1 + b_1,\ a_2 + b_2)
Subtraction a⃗−b⃗=(a1−b1, a2−b2)\vec{a} - \vec{b} = (a_1 - b_1,\ a_2 - b_2)
Scalar multiplication λa⃗=(λa1, λa2)\lambda \vec{a} = (\lambda a_1,\ \lambda a_2)
Magnitude ∣a⃗∣=a12+a22|\vec{a}| = \sqrt{a_1^{2} + a_2^{2}}
Dot product a⃗⋅b⃗=a1b1+a2b2\vec{a} \cdot \vec{b} = a_1 b_1 + a_2 b_2

The coordinate dot product a⃗⋅b⃗=a1b1+a2b2\vec{a} \cdot \vec{b} = a_1 b_1 + a_2 b_2 follows directly from expanding ∣a⃗∣∣b⃗∣cos⁡θ|\vec{a}||\vec{b}|\cos\theta — this is the formula you use in all numerical calculations.

Worked Example 6.4.A

Let a⃗=(3,−2)\vec{a} = (3, -2) and b⃗=(−1,4)\vec{b} = (-1, 4).

(i) Find 2a⃗−b⃗2\vec{a} - \vec{b}.
(ii) Find a⃗⋅b⃗\vec{a} \cdot \vec{b}.
(iii) Find the angle θ\theta between a⃗\vec{a} and b⃗\vec{b}.

Solution.

(i) 2a⃗−b⃗=2(3,−2)−(−1,4)=(6,−4)−(−1,4)=(7, −8).2\vec{a} - \vec{b} = 2(3,-2) - (-1,4) = (6,-4) - (-1,4) = (7,\ -8).

(ii) a⃗⋅b⃗=(3)(−1)+(−2)(4)=−3−8=−11.\vec{a} \cdot \vec{b} = (3)(-1) + (-2)(4) = -3 - 8 = -11.

(iii)
∣a⃗∣=9+4=13,∣b⃗∣=1+16=17.|\vec{a}| = \sqrt{9 + 4} = \sqrt{13}, \qquad |\vec{b}| = \sqrt{1 + 16} = \sqrt{17}.
cos⁡θ=−1113⋅17=−11221.\cos\theta = \frac{-11}{\sqrt{13}\cdot\sqrt{17}} = \frac{-11}{\sqrt{221}}.

Since cos⁡θ<0\cos\theta < 0, the angle is obtuse.

θ=arccos⁡ ⁣(−11221)≈137.8°\boxed{\theta = \arccos\!\left(\frac{-11}{\sqrt{221}}\right) \approx 137.8°}

🔑 Perpendicularity in coordinates: a⃗⊥b⃗  ⟺  a1b1+a2b2=0\vec{a} \perp \vec{b} \iff a_1 b_1 + a_2 b_2 = 0. No magnitudes or trig needed — just multiply matching components and add.


6.5 Vector Applications 向量应用

Vectors let us solve geometric problems algebraically — lengths, angles, midpoints, and parallelism proofs all reduce to vector arithmetic.

Midpoint formula via vectors

If MM is the midpoint of segment ABAB, then:

OM→=12(OA→+OB→)\overrightarrow{OM} = \frac{1}{2}(\overrightarrow{OA} + \overrightarrow{OB})

In coordinates: M=(xA+xB2, yA+yB2)M = \left(\dfrac{x_A + x_B}{2},\ \dfrac{y_A + y_B}{2}\right).

Distance formula via vectors

∣AB∣=∣AB→∣=(xB−xA)2+(yB−yA)2|AB| = |\overrightarrow{AB}| = \sqrt{(x_B - x_A)^{2} + (y_B - y_A)^{2}}

Linear combination and basis

Any vector v⃗\vec{v} in the plane can be written as a linear combination of two non-collinear vectors e⃗1\vec{e}_1 and e⃗2\vec{e}_2:

v⃗=x e⃗1+y e⃗2\vec{v} = x\,\vec{e}_1 + y\,\vec{e}_2

where x,yx, y are unique scalars. This is frequently used to match coefficients in proof problems.

Worked Example 6.5.A

In triangle ABCABC, let AB→=m⃗\overrightarrow{AB} = \vec{m} and AC→=n⃗\overrightarrow{AC} = \vec{n}. Point DD is on BCBC such that BD:DC=1:2BD:DC = 1:2. Express AD→\overrightarrow{AD} in terms of m⃗\vec{m} and n⃗\vec{n}.

Solution.

DD divides BCBC in ratio 1:21:2, so:
BD→=11+2BC→=13BC→.\overrightarrow{BD} = \frac{1}{1+2}\overrightarrow{BC} = \frac{1}{3}\overrightarrow{BC}.

Now express BC→\overrightarrow{BC} using triangle law:
BC→=BA→+AC→=−m⃗+n⃗.\overrightarrow{BC} = \overrightarrow{BA} + \overrightarrow{AC} = -\vec{m} + \vec{n}.

Therefore:
AD→=AB→+BD→=m⃗+13(−m⃗+n⃗)=m⃗−13m⃗+13n⃗=23m⃗+13n⃗.\overrightarrow{AD} = \overrightarrow{AB} + \overrightarrow{BD} = \vec{m} + \frac{1}{3}(-\vec{m} + \vec{n}) = \vec{m} - \frac{1}{3}\vec{m} + \frac{1}{3}\vec{n} = \frac{2}{3}\vec{m} + \frac{1}{3}\vec{n}.

AD→=23m⃗+13n⃗\boxed{\overrightarrow{AD} = \tfrac{2}{3}\vec{m} + \tfrac{1}{3}\vec{n}}

🔑 Section formula: If DD divides BCBC in ratio m:nm:n (from BB to CC), then BD→=mm+nBC→\overrightarrow{BD} = \dfrac{m}{m+n}\overrightarrow{BC}. Memorise this — it appears in nearly every vector geometry question.

⚠️ Exam trap: When the problem asks "find the angle θ\theta between vectors a⃗\vec{a} and b⃗\vec{b}", the answer must satisfy 0≤θ≤180°0 \le \theta \le 180° (or 0≤θ≤π0 \le \theta \le \pi). Vectors do not have a "signed" angle like slopes do.


Try it! 自测练习

Q1. In parallelogram ABCDABCD, AB→=a⃗\overrightarrow{AB} = \vec{a} and BC→=b⃗\overrightarrow{BC} = \vec{b}. Express AC→−BD→\overrightarrow{AC} - \overrightarrow{BD} in terms of a⃗\vec{a} and b⃗\vec{b}.

Q2. Vectors ∣p⃗∣=5|\vec{p}| = 5, ∣q⃗∣=4|\vec{q}| = 4, and p⃗⋅q⃗=−10\vec{p} \cdot \vec{q} = -10. Find the angle between p⃗\vec{p} and q⃗\vec{q}.

Q3. a⃗=(1,t)\vec{a} = (1, t) and b⃗=(2,6)\vec{b} = (2, 6). For what value of tt are they collinear? For what value of tt are they perpendicular?

Q4. A=(1,2)A = (1, 2), B=(4,−1)B = (4, -1), C=(5,3)C = (5, 3). Find AB→⋅AC→\overrightarrow{AB} \cdot \overrightarrow{AC}.

Q5. In triangle OABOAB, let OA→=a⃗\overrightarrow{OA} = \vec{a} and OB→=b⃗\overrightarrow{OB} = \vec{b}. MM is the midpoint of ABAB. Show that OM→=12(a⃗+b⃗)\overrightarrow{OM} = \dfrac{1}{2}(\vec{a} + \vec{b}).

Answers & explanations

Q1. In parallelogram ABCDABCD: AC→=a⃗+b⃗\overrightarrow{AC} = \vec{a} + \vec{b} (diagonal via triangle rule). BD→=BC→+CD→=b⃗+(−a⃗)=b⃗−a⃗\overrightarrow{BD} = \overrightarrow{BC} + \overrightarrow{CD} = \vec{b} + (-\vec{a}) = \vec{b} - \vec{a} (since CD→=−AB→=−a⃗\overrightarrow{CD} = -\overrightarrow{AB} = -\vec{a}). Therefore:
AC→−BD→=(a⃗+b⃗)−(b⃗−a⃗)=2a⃗.\overrightarrow{AC} - \overrightarrow{BD} = (\vec{a} + \vec{b}) - (\vec{b} - \vec{a}) = 2\vec{a}.

Q2. cos⁡θ=p⃗⋅q⃗∣p⃗∣∣q⃗∣=−105×4=−1020=−12\cos\theta = \dfrac{\vec{p} \cdot \vec{q}}{|\vec{p}||\vec{q}|} = \dfrac{-10}{5 \times 4} = \dfrac{-10}{20} = -\dfrac{1}{2}. So θ=120°\theta = 120°.

Q3. Collinear: 1⋅6=2⋅t⇒t=31 \cdot 6 = 2 \cdot t \Rightarrow t = 3. Perpendicular: a⃗⋅b⃗=1⋅2+t⋅6=2+6t=0⇒t=−13\vec{a} \cdot \vec{b} = 1\cdot 2 + t \cdot 6 = 2 + 6t = 0 \Rightarrow t = -\tfrac{1}{3}.

Q4. AB→=(4−1, −1−2)=(3,−3)\overrightarrow{AB} = (4-1,\ -1-2) = (3,-3). AC→=(5−1, 3−2)=(4,1)\overrightarrow{AC} = (5-1,\ 3-2) = (4,1). AB→⋅AC→=3⋅4+(−3)⋅1=12−3=9\overrightarrow{AB} \cdot \overrightarrow{AC} = 3\cdot 4 + (-3)\cdot 1 = 12 - 3 = 9.

Q5. By the midpoint rule, M=12(A+B)M = \tfrac{1}{2}(A + B). In vector form:
OM→=OA→+AM→=a⃗+12AB→=a⃗+12(b⃗−a⃗)=12a⃗+12b⃗=12(a⃗+b⃗). □\overrightarrow{OM} = \overrightarrow{OA} + \overrightarrow{AM} = \vec{a} + \tfrac{1}{2}\overrightarrow{AB} = \vec{a} + \tfrac{1}{2}(\vec{b} - \vec{a}) = \tfrac{1}{2}\vec{a} + \tfrac{1}{2}\vec{b} = \tfrac{1}{2}(\vec{a} + \vec{b}).\ \square


📌 Chapter summary

Topic Key skill
6.1 Vector Operations Triangle/parallelogram rules; cancellation AB→+BC→=AC→\overrightarrow{AB}+\overrightarrow{BC}=\overrightarrow{AC}; scalar mult changes magnitude and direction
6.2 Dot Product a⃗⋅b⃗=∥a⃗∥∥b⃗∥cos⁡θ\vec{a}\cdot\vec{b}=\|\vec{a}\|\|\vec{b}\|\cos\theta; perpendicular ⇔\Leftrightarrow dot product =0=0; expand ∣a⃗+b⃗∣2|\vec{a}+\vec{b}|^{2} by dot product
6.3 Collinear Vectors a⃗=λb⃗\vec{a}=\lambda\vec{b} (scalar form); coordinate test x1y2=x2y1x_1 y_2 = x_2 y_1
6.4 Coordinate Form Component-wise +,−,×λ+,-,\times\lambda; ∣a⃗∣=a12+a22|\vec{a}|=\sqrt{a_1^2+a_2^2}; a⃗⋅b⃗=a1b1+a2b2\vec{a}\cdot\vec{b}=a_1 b_1+a_2 b_2
6.5 Applications Section formula for ratio division; midpoint =12(a⃗+b⃗)=\tfrac{1}{2}(\vec{a}+\vec{b}); match linear-combination coefficients in proofs

What's next → Unit 7 uses vector ideas directly: the slope of a line is related to a direction vector, and the perpendicular-line condition k1k2=−1k_1 k_2 = -1 mirrors the dot-product perpendicularity rule a⃗⋅b⃗=0\vec{a} \cdot \vec{b} = 0.