Adding Vectors: Two Equivalent Laws
Triangle law
A vector is a displacement. If a girl walks from to and then from to , her net displacement is from straight to :
This is the triangle law of vector addition: to add and , slide (a free vector!) so its initial point sits on the terminal point of ; the sum runs from the tail of to the tip of — the third side of the triangle, taken from start to finish.

Two immediate consequences:
- Sides of a triangle taken in order sum to zero: — the walk returns to its starting point.
- Subtraction is addition of the negative: , built by reversing and then applying the triangle law.
Parallelogram law
If and are drawn from a common initial point as two adjacent sides of a parallelogram, their sum is the diagonal through that common point — think of a boat crossing a river: engine velocity one side, stream velocity the other, actual motion along the diagonal.
Key Point: the two laws are the same fact drawn differently. In parallelogram : (since ) — triangle law on one half of the parallelogram is the parallelogram law.
Properties of vector addition
- Commutative: (walk the parallelogram's two triangle-halves).
- Associative: — so needs no brackets.
- Additive identity: — the zero vector changes nothing.
- Additive inverse: .
Multiplying a Vector by a Scalar
For a vector and a scalar , the product is a vector collinear with :
- Direction: same as when ; opposite when .
- Magnitude: — note the absolute value of : , never .
Special values of tell the whole story:
- gives , the additive inverse: same length, opposite direction.
- (for ) gives a vector of magnitude in the direction of — the unit vector
- For any scalar , .
Key Point (the workhorse recipe): to produce a vector of magnitude in the direction of , compute . Normalise first, then scale — this two-step is behind half the 2-mark questions in this chapter.
How big can a sum be?
From the triangle picture, the resultant's length is bounded by the triangle inequality:
Equality on the right holds when and point the same way; on the left when they point opposite ways. With and , the sum's magnitude can be anything in — and nothing outside it.
Solved Examples
Example 1: Net displacement
A girl walks km due west and then km due north. Find the magnitude of her net displacement.
Solution:
- Set up the triangle: the two legs are perpendicular, with the net displacement as the third side (tail of the first to tip of the second).
- Pythagoras: km.
Answer: km, pointing north of west. Note that the distance walked is km — displacement (vector) and distance (scalar) part ways exactly here.
Example 2: Magnitude under scaling
If , find and describe the direction of .
Solution:
- Magnitude rule: .
- Direction rule: , so the direction is opposite to .
Answer: magnitude , direction opposite to . A magnitude is never negative — has the absolute value built in for exactly this reason.
Example 3: Building a vector of prescribed length
Given , write a vector of magnitude in the direction of , in terms of .
Solution:
- Normalise: .
- Scale: the required vector is .
Answer: . Check: . ✓
Example 4: A closed walk
Prove that for any triangle , and state the generalisation for a polygon.
Solution:
- Triangle law twice: .
- Add the last side: .
Answer: the sum is — and the same telescoping shows the directed sides of any closed polygon, taken in order, sum to the zero vector: every closed walk ends where it began.
Example 5: Diagonals of a parallelogram
In parallelogram , let and . Express both diagonals in terms of and .
Solution:
- Diagonal from : (since ).
- Diagonal from : .
Answer: , — the two diagonals are the sum and the difference. This picture is worth memorising: it turns many geometry proofs into two-line vector computations.
Example 6: The boat and the stream
A boat's engine drives it at km/h straight across a river whose current flows at km/h parallel to the banks. Find the boat's actual speed.
Solution:
- Parallelogram (rectangle) law: the two velocity vectors are perpendicular adjacent sides; the actual velocity is the diagonal.
- Magnitude: km/h.
- Direction: downstream of straight-across by the angle with .
Answer: km/h, tilted downstream at from the crossing direction — the classic physical picture behind the parallelogram law.