13. Vectors in two dimensions
- Syllabus
- 0606–2028–2029
- Topic
- 13
- Level
- —
A vector records both magnitude and direction. Different notations can describe the same vector, but the notation must show that the quantity is a vector rather than an ordinary number.
| Form | What it identifies |
|---|---|
| a or p | a named vector |
| AB | the directed displacement from A to B |
| (xy) | horizontal and vertical components |
| xi+yj | the same components in unit-vector form |
If A=(2,−1) and B=(7,3), then AB=(7−23−(−1))=(54)=5i+4j. These are three descriptions of the same directed displacement.
AB and BA point in opposite directions, so BA=−AB. By contrast, AB without an arrow normally denotes the scalar distance between the points. Do not drop bold type or the arrow when a vector is required.
A position vector locates a point from a fixed origin. If R=(x,y) relative to origin O, then OR=(xy). A unit vector keeps a direction but has magnitude 1.
|\mathbf{a}|=\sqrt{x^2+y^2},\qquad \widehat{\mathbf{a}}=\frac{\mathbf{a}}{|\mathbf{a}|}\quad(\mathbf{a}\ne\mathbf{0})
Find the magnitude first, then divide every component by that same positive magnitude. This scales the vector without changing its direction.
For a=(5−12), ∣a∣=52+(−12)2=13. The unit vector in the same direction is 131(5−12)=(5/13−12/13). Its magnitude checks as 1.
The zero vector has no direction, so it cannot be normalized. Dividing by a negative number would reverse the direction; the denominator in the unit-vector formula is the non-negative magnitude ∣a∣.
Vector calculations are component-wise: combine horizontal components together and vertical components together. Equality of two vectors therefore gives one equation from each component.
| Operation | Component rule |
|---|---|
| addition | (ab)+(cd)=(a+cb+d) |
| subtraction | (ab)−(cd)=(a−cb−d) |
| scalar multiplication | k(ab)=(kakb) |
| magnitude | (ab)=a2+b2 |
For example, (41)+k(−23)=r(−105) gives 4−2k=−10r and 1+3k=5r. Solving the two scalar equations gives k=−3/2 and r=−7/10.
In vector geometry, build a route using directed segments. If OA=a, OB=b and P divides AB with AP:PB=1:3, then AB=b−a and OP=a+41(b−a)=43a+41b.
To prove points are collinear, show that two directed vectors with a common point are scalar multiples. A positive scalar gives the same direction and a negative scalar gives the opposite direction, but both lie on the same straight line. Equal magnitudes alone do not prove parallelism or collinearity.
A velocity vector combines speed with direction. Resolve every velocity into components on the same axes; resultant velocities are then found by component-wise addition, and position changes linearly when velocity is constant.
\mathbf p(t)=\mathbf p_0+t\mathbf v
With i east and j north, a speed s on bearing θ has velocity ssinθi+scosθj, because a bearing is measured clockwise from north. If an angle α is measured above the positive horizontal axis instead, use scosαi+ssinαj.
A cyclist travelling at 4ms−1 on bearing 015∘ has velocity 4sin15∘i+4cos15∘j. If another velocity acts at the same time, add its i and j components separately to obtain the resultant.
For two particles, write both position vectors using the same time variable. They collide only if both component equations give the same admissible time. For instance, if the x-components meet at one time but the y-components meet at another, the paths may cross geometrically but the particles do not collide.
Keep displacement, velocity and speed distinct: displacement and velocity are vectors, while speed is the scalar magnitude of velocity. Include the initial position p0 unless the particle starts at the origin.