MathLabs

Grade 10

Vectors

Quantities with both magnitude and direction, added and scaled to describe displacement and force.

IntuitionWhat Is a Vector?

When you tell someone you walked three kilometers, they still do not know where you ended up: three kilometers east reaches a completely different place from three kilometers north. Many quantities in physics and geometry—displacement, velocity, acceleration, and force—carry both a magnitude (how much) and a direction (which way). A vector captures both pieces of information in a single mathematical object, drawn as a directed arrow whose length represents magnitude and whose arrowhead shows direction.

Interactive unit circle showing a rotating unit vector and its cosine and sine projections
Parallelogram law of vector addition: the two vectors u=(a11,a21)\mathbf{u} = (a_{11}, a_{21}) and v=(a12,a22)\mathbf{v} = (a_{12}, a_{22}) span a parallelogram whose diagonal is u+v\mathbf{u} + \mathbf{v}.

SchoolAdding and Scaling Vectors

Definition: Directed Segments, Magnitude, and Equality

A vector with initial point AA and terminal point BB is written AB→\overrightarrow{AB}, or by a single letter u⃗\vec{u}. Its magnitude (or length) is the distance between AA and BB, denoted ∣AB→∣|\overrightarrow{AB}| or ∣u⃗∣|\vec{u}|. The zero vector 0⃗=AA→\vec{0}=\overrightarrow{AA} has length 00 and arbitrary direction. Two vectors u⃗\vec{u} and v⃗\vec{v} are equal (u⃗=v⃗\vec{u}=\vec{v}) if and only if they have the same magnitude and the same direction, regardless of where their initial points are placed.

AB→+BC→=AC→,OA→+OB→=OC→(OACB parallelogram)\overrightarrow{AB} + \overrightarrow{BC} = \overrightarrow{AC}, \qquad \overrightarrow{OA} + \overrightarrow{OB} = \overrightarrow{OC} \quad (OACB \text{ parallelogram})

To add two vectors by the triangle rule, place the tail of the second vector at the tip of the first: going from AA to BB and then from BB to CC gives the net displacement AB→+BC→=AC→\overrightarrow{AB}+\overrightarrow{BC}=\overrightarrow{AC}. Equivalently, by the parallelogram rule, if OA→\overrightarrow{OA} and OB→\overrightarrow{OB} share the same initial point OO, their sum OA→+OB→\overrightarrow{OA}+\overrightarrow{OB} is the diagonal OC→\overrightarrow{OC} of the parallelogram OACBOACB. Subtracting vectors is adding the opposite vector: OB→−OA→=AB→\overrightarrow{OB}-\overrightarrow{OA}=\overrightarrow{AB}.

∣ku⃗∣=∣k∣ ∣u⃗∣,u⃗⋅v⃗=∣u⃗∣ ∣v⃗∣cos⁡θ|k\vec{u}| = |k|\,|\vec{u}|, \qquad \vec{u}\cdot\vec{v} = |\vec{u}|\,|\vec{v}|\cos\theta

Multiplying a vector u⃗\vec{u} by a real number kk (called scalar multiplication) produces a vector ku⃗k\vec{u} of length ∣k∣ ∣u⃗∣|k|\,|\vec{u}| that points in the same direction as u⃗\vec{u} when k>0k>0, in the opposite direction when k<0k<0, and equals 0⃗\vec{0} when k=0k=0. The dot product (or scalar product) u⃗⋅v⃗=∣u⃗∣ ∣v⃗∣cos⁡θ\vec{u}\cdot\vec{v}=|\vec{u}|\,|\vec{v}|\cos\theta, where θ\theta is the angle between u⃗\vec{u} and v⃗\vec{v} (0∘≤θ≤180∘0^\circ\le\theta\le 180^\circ), combines two vectors into a single real number that measures how strongly they align; in particular, two nonzero vectors are perpendicular (u⃗⊥v⃗\vec{u}\perp\vec{v}) if and only if u⃗⋅v⃗=0\vec{u}\cdot\vec{v}=0.

Core vector operations and their geometric meanings
OperationFormulaGeometric meaning
Triangle ruleAB→+BC→=AC→\overrightarrow{AB}+\overrightarrow{BC}=\overrightarrow{AC}Chaining displacements tip-to-tail
Subtraction ruleOB→−OA→=AB→\overrightarrow{OB}-\overrightarrow{OA}=\overrightarrow{AB}Vector pointing from tip AA to tip BB
Midpoint identityMA→+MB→=0⃗\overrightarrow{MA}+\overrightarrow{MB}=\vec{0}Midpoint MM of ABAB balances the two endpoints
Dot productu⃗⋅v⃗=∣u⃗∣ ∣v⃗∣cos⁡θ\vec{u}\cdot\vec{v}=|\vec{u}|\,|\vec{v}|\cos\thetaSigned projection of one vector onto another

UndergraduateKey Theorems

Point GG is the centroid of △ABC\triangle ABC if and only if GA→+GB→+GC→=0⃗\overrightarrow{GA}+\overrightarrow{GB}+\overrightarrow{GC}=\vec{0}, or equivalently, for every reference point OO in the plane, OG→=13(OA→+OB→+OC→)\overrightarrow{OG}=\dfrac{1}{3}(\overrightarrow{OA}+\overrightarrow{OB}+\overrightarrow{OC}).

Why is it true?

If equal unit masses are placed at the three vertices AA, BB, and CC, the vectors GA→\overrightarrow{GA}, GB→\overrightarrow{GB}, and GC→\overrightarrow{GC} represent the pulls toward each vertex from GG; their sum is 0⃗\vec{0} precisely when GG is the center of mass.

Proof

Let MM be the midpoint of side BCBC. Since MM bisects BCBC, the two vectors MB→\overrightarrow{MB} and MC→\overrightarrow{MC} have equal length and opposite directions, so MB→+MC→=0⃗\overrightarrow{MB}+\overrightarrow{MC}=\vec{0}. By the triangle rule from GG through MM, we have GB→+GC→=(GM→+MB→)+(GM→+MC→)=2GM→\overrightarrow{GB}+\overrightarrow{GC}=(\overrightarrow{GM}+\overrightarrow{MB})+(\overrightarrow{GM}+\overrightarrow{MC})=2\overrightarrow{GM}.

By the median property of △ABC\triangle ABC, the centroid GG lies on the median AMAM and divides it in a 2:12:1 ratio from the vertex, meaning GA→=−2GM→\overrightarrow{GA}=-2\overrightarrow{GM}.

Adding the two relations yields GA→+GB→+GC→=−2GM→+2GM→=0⃗\overrightarrow{GA}+\overrightarrow{GB}+\overrightarrow{GC}=-2\overrightarrow{GM}+2\overrightarrow{GM}=\vec{0}. Finally, for any point OO, writing GA→=OA→−OG→\overrightarrow{GA}=\overrightarrow{OA}-\overrightarrow{OG} (and similarly for BB and CC) gives (OA→+OB→+OC→)−3OG→=0⃗(\overrightarrow{OA}+\overrightarrow{OB}+\overrightarrow{OC})-3\overrightarrow{OG}=\vec{0}, or OG→=13(OA→+OB→+OC→)\overrightarrow{OG}=\dfrac{1}{3}(\overrightarrow{OA}+\overrightarrow{OB}+\overrightarrow{OC}).

For any two vectors u⃗=(x1,y1)\vec{u}=(x_1,y_1) and v⃗=(x2,y2)\vec{v}=(x_2,y_2) forming an angle θ\theta, the geometric dot product u⃗⋅v⃗=∣u⃗∣ ∣v⃗∣cos⁡θ\vec{u}\cdot\vec{v}=|\vec{u}|\,|\vec{v}|\cos\theta equals the coordinate expression x1x2+y1y2x_1x_2+y_1y_2.

Why is it true?

Expanding ∣u⃗−v⃗∣2|\vec{u}-\vec{v}|^2 in coordinates and comparing it with the Law of Cosines on the triangle formed by u⃗\vec{u}, v⃗\vec{v}, and u⃗−v⃗\vec{u}-\vec{v} cancels the squared lengths and isolates the cross-term x1x2+y1y2x_1x_2+y_1y_2.

Proof

Place u⃗=OA→\vec{u}=\overrightarrow{OA} and v⃗=OB→\vec{v}=\overrightarrow{OB} at the origin OO so that AB→=v⃗−u⃗=(x2−x1,y2−y1)\overrightarrow{AB}=\vec{v}-\vec{u}=(x_2-x_1,y_2-y_1). By the Law of Cosines in △OAB\triangle OAB, the squared side length opposite angle θ\theta is ∣v⃗−u⃗∣2=∣u⃗∣2+∣v⃗∣2−2∣u⃗∣ ∣v⃗∣cos⁡θ|\vec{v}-\vec{u}|^2=|\vec{u}|^2+|\vec{v}|^2-2|\vec{u}|\,|\vec{v}|\cos\theta.

On the other hand, computing the squared lengths in coordinates gives ∣u⃗∣2=x12+y12|\vec{u}|^2=x_1^2+y_1^2, ∣v⃗∣2=x22+y22|\vec{v}|^2=x_2^2+y_2^2, and ∣v⃗−u⃗∣2=(x2−x1)2+(y2−y1)2=x12+y12+x22+y22−2(x1x2+y1y2)|\vec{v}-\vec{u}|^2=(x_2-x_1)^2+(y_2-y_1)^2=x_1^2+y_1^2+x_2^2+y_2^2-2(x_1x_2+y_1y_2).

Equating the two expressions for ∣v⃗−u⃗∣2|\vec{v}-\vec{u}|^2 and subtracting x12+y12+x22+y22x_1^2+y_1^2+x_2^2+y_2^2 from both sides yields −2∣u⃗∣ ∣v⃗∣cos⁡θ=−2(x1x2+y1y2)-2|\vec{u}|\,|\vec{v}|\cos\theta=-2(x_1x_2+y_1y_2). Dividing by −2-2 gives u⃗⋅v⃗=∣u⃗∣ ∣v⃗∣cos⁡θ=x1x2+y1y2\vec{u}\cdot\vec{v}=|\vec{u}|\,|\vec{v}|\cos\theta=x_1x_2+y_1y_2.

UndergraduateReal-World Applications and Worked Examples

In mechanics, aviation, and computer graphics, vectors are the standard language for combining motions and forces. An airplane flying through a crosswind moves along the vector sum of its airspeed vector and the wind velocity vector; a physics engine computes mechanical work and surface lighting by taking dot products between force, displacement, and normal vectors.

Example: Resultant of Two Tugboat Forces

Two tugboats pull a barge with forces F⃗1\vec{F}_1 of magnitude ∣F⃗1∣=300|\vec{F}_1|=300 kN due east and F⃗2\vec{F}_2 of magnitude ∣F⃗2∣=400|\vec{F}_2|=400 kN due north. Find the magnitude ∣F⃗∣|\vec{F}| of the resultant force F⃗=F⃗1+F⃗2\vec{F}=\vec{F}_1+\vec{F}_2.

Solution

Choose a coordinate system with the positive first axis pointing east and the positive second axis pointing north, so F⃗1=(300,0)\vec{F}_1=(300,0) and F⃗2=(0,400)\vec{F}_2=(0,400).

Adding the two vectors component-wise gives the resultant force F⃗=F⃗1+F⃗2=(300,400)\vec{F}=\vec{F}_1+\vec{F}_2=(300,400). Its magnitude is ∣F⃗∣=3002+4002=90000+160000=250000=500|\vec{F}|=\sqrt{300^2+400^2}=\sqrt{90000+160000}=\sqrt{250000}=500 kN.

Example: Mechanical Work via the Dot Product

A crate is pulled along a horizontal floor by a rope exerting a force F⃗\vec{F} of magnitude ∣F⃗∣=50|\vec{F}|=50 N at an angle θ=60∘\theta=60^\circ above the horizontal over a displacement d⃗\vec{d} of length ∣d⃗∣=10|\vec{d}|=10 m. Compute the mechanical work W=F⃗⋅d⃗W=\vec{F}\cdot\vec{d}.

Solution

By definition of mechanical work as the dot product of force and displacement, we have W=F⃗⋅d⃗=∣F⃗∣ ∣d⃗∣cos⁡θW=\vec{F}\cdot\vec{d}=|\vec{F}|\,|\vec{d}|\cos\theta.

Substituting ∣F⃗∣=50|\vec{F}|=50, ∣d⃗∣=10|\vec{d}|=10, and cos⁡60∘=12\cos 60^\circ=\dfrac{1}{2} gives W=50×10×12=250W=50\times 10\times\dfrac{1}{2}=250 J. Only the horizontal component ∣F⃗∣cos⁡60∘=25|\vec{F}|\cos 60^\circ=25 N along d⃗\vec{d} performs work.

What is the magnitude ∣u⃗∣|\vec{u}| of the vector u⃗=(6,−8)\vec{u}=(6,-8)?

Let GG be the centroid of △ABC\triangle ABC. If GA→=(2,−1)\overrightarrow{GA}=(2,-1) and GB→=(−5,4)\overrightarrow{GB}=(-5,4), what is GC→\overrightarrow{GC}?

For which value of mm are the vectors u⃗=(3,4)\vec{u}=(3,4) and v⃗=(m,−6)\vec{v}=(m,-6) perpendicular?

A delivery drone flies 1212 km due east from AA to BB and then 55 km due north from BB to CC. What is the magnitude ∣AC→∣|\overrightarrow{AC}| of its net displacement?

References

  1. H. S. M. Coxeter, S. L. Greitzer (1967). Geometry Revisited
  2. Murray R. Spiegel (1959). Schaum's Outline of Vector Analysis