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3.12 Vectors: concepts and algebraIB Maths: Analysis and Approaches HL: Revision notes

Section 1

What is a vector?

A vector has both magnitude (size) and direction; a scalar has only magnitude. A vector can be shown as a directed line segment AB→\overrightarrow{AB}, from AA to BB. Two vectors are equal if they have the same magnitude and direction, wherever they are drawn.

  • A position vector OA→=a\overrightarrow{OA}=\mathbf{a} gives the position of AA relative to the origin OO.
  • A displacement vector AB→\overrightarrow{AB} describes the move from AA to BB: AB→=b−a\overrightarrow{AB}=\mathbf{b}-\mathbf{a}.
Key termsvectorposition vectordisplacement vector
Common mistake

AB→\overrightarrow{AB} is b−a\mathbf{b}-\mathbf{a} (end minus start), not a−b\mathbf{a}-\mathbf{b}.

Section 2

Components and base vectors

In three dimensions the base vectors i\mathbf{i}, j\mathbf{j}, k\mathbf{k} are unit vectors along the xx-, yy- and zz-axes. Any vector can be written in component form v=(v1v2v3)=v1i+v2j+v3k.\mathbf{v}=\begin{pmatrix}v_1\\ v_2\\ v_3\end{pmatrix}=v_1\mathbf{i}+v_2\mathbf{j}+v_3\mathbf{k}. The point A(2,−1,3)A(2,-1,3) has position vector a=2i−j+3k\mathbf{a}=2\mathbf{i}-\mathbf{j}+3\mathbf{k}.

Key termsbase vectorscomponents

Section 3

Adding, subtracting and scaling

Work component by component. Geometrically, u+v\mathbf{u}+\mathbf{v} is "u\mathbf{u} then v\mathbf{v}" (the triangle law), and u−v=u+(−v)\mathbf{u}-\mathbf{v}=\mathbf{u}+(-\mathbf{v}).

  • The zero vector 0\mathbf{0} has every component 0; v+(−v)=0\mathbf{v}+(-\mathbf{v})=\mathbf{0}.
  • −v-\mathbf{v} has the same magnitude as v\mathbf{v} but the opposite direction.
  • kvk\mathbf{v} is parallel to v\mathbf{v}, with magnitude ∣k∣∣v∣|k||\mathbf{v}|; it points the opposite way if k<0k<0.

Two non-zero vectors are parallel exactly when one is a scalar multiple of the other. For example (m,2,n)(m,2,n) is parallel to (2,−1,2)(2,-1,2) only if it equals −2(2,−1,2)-2(2,-1,2).

Key termszero vectorparallel vectors
Exam tip

To test parallel, find kk from one component, then check it works for every component.

Section 4

Magnitude, unit vectors and distance

The magnitude of v\mathbf{v} is ∣v∣=v12+v22+v32|\mathbf{v}|=\sqrt{v_1^2+v_2^2+v_3^2}. A unit vector has magnitude 1; the unit vector in the direction of v\mathbf{v} is v∣v∣\frac{\mathbf{v}}{|\mathbf{v}|}.

The distance between AA and BB is ∣AB→∣=∣b−a∣|\overrightarrow{AB}|=|\mathbf{b}-\mathbf{a}|. For A(2,−1,3)A(2,-1,3) and B(5,3,3)B(5,3,3): AB→=(3,4,0)\overrightarrow{AB}=(3,4,0) and AB=5AB=5.

To get a vector of magnitude 6 in the direction of p\mathbf{p}, use 6p∣p∣6\frac{\mathbf{p}}{|\mathbf{p}|}.

Key termsmagnitudeunit vector
Common mistake

Forgetting to square negative components: ∣(−3,1,4)∣=9+1+16=26|(-3,1,4)|=\sqrt{9+1+16}=\sqrt{26}.

Section 5

Proving geometric properties with vectors

Useful facts:

  • The midpoint of PQPQ has position vector 12(p+q)\frac12(\mathbf{p}+\mathbf{q}).
  • A point dividing ABAB in the ratio m:nm:n has position vector a+mm+n(b−a)\mathbf{a}+\frac{m}{m+n}(\mathbf{b}-\mathbf{a}).
  • KL→=NM→\overrightarrow{KL}=\overrightarrow{NM} means KLKL and NMNM are parallel and equal, so KLMNKLMN is a parallelogram.
  • Points OO, DD, FF are collinear if OF→=kOD→\overrightarrow{OF}=k\overrightarrow{OD}: parallel vectors sharing a point.

Example: joining the midpoints of the sides of any quadrilateral gives a parallelogram, because both KL→\overrightarrow{KL} and NM→\overrightarrow{NM} equal 12(r−p)\frac12(\mathbf{r}-\mathbf{p}).

Key termscollinearmidpoint
Common mistake

Parallel is not enough for collinear: you must also state the common point.

Must know

  • AB→=b−a\overrightarrow{AB}=\mathbf{b}-\mathbf{a}; distance AB=∣b−a∣AB=|\mathbf{b}-\mathbf{a}|.
  • ∣v∣=v12+v22+v32|\mathbf{v}|=\sqrt{v_1^2+v_2^2+v_3^2}; unit vector v∣v∣\frac{\mathbf{v}}{|\mathbf{v}|}.
  • u∥v  ⟺  u=kv\mathbf{u}\parallel\mathbf{v}\iff\mathbf{u}=k\mathbf{v}.
  • Midpoint 12(p+q)\frac12(\mathbf{p}+\mathbf{q}); ratio m:nm:n point a+mm+n(b−a)\mathbf{a}+\frac{m}{m+n}(\mathbf{b}-\mathbf{a}).
  • Collinear: parallel vectors and a common point.

That's the notes covered.

Carry on to the next subtopic.