Adding Vectors: Two Equivalent Laws

Triangle law

A vector is a displacement. If a girl walks from AA to BB and then from BB to CC, her net displacement is from AA straight to CC:

AB→+BC→=AC→\overrightarrow{AB} + \overrightarrow{BC} = \overrightarrow{AC}

This is the triangle law of vector addition: to add a⃗\vec{a} and b⃗\vec{b}, slide b⃗\vec{b} (a free vector!) so its initial point sits on the terminal point of a⃗\vec{a}; the sum runs from the tail of a⃗\vec{a} to the tip of b⃗\vec{b} — the third side of the triangle, taken from start to finish.

Triangle law tail to tip and parallelogram law with diagonal sum

Two immediate consequences:

  1. Sides of a triangle taken in order sum to zero: AB→+BC→+CA→=AC→+CA→=0⃗\overrightarrow{AB} + \overrightarrow{BC} + \overrightarrow{CA} = \overrightarrow{AC} + \overrightarrow{CA} = \vec{0} — the walk returns to its starting point.
  2. Subtraction is addition of the negative: a⃗−b⃗=a⃗+(−b⃗)\vec{a} - \vec{b} = \vec{a} + \left(-\vec{b}\right), built by reversing b⃗\vec{b} and then applying the triangle law.

Parallelogram law

If a⃗\vec{a} and b⃗\vec{b} are drawn from a common initial point as two adjacent sides of a parallelogram, their sum a⃗+b⃗\vec{a} + \vec{b} 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 ABCDABCD: AC→=AB→+BC→=AB→+AD→\overrightarrow{AC} = \overrightarrow{AB} + \overrightarrow{BC} = \overrightarrow{AB} + \overrightarrow{AD} (since BC→=AD→\overrightarrow{BC} = \overrightarrow{AD}) — triangle law on one half of the parallelogram is the parallelogram law.

Properties of vector addition

  1. Commutative: a⃗+b⃗=b⃗+a⃗\vec{a} + \vec{b} = \vec{b} + \vec{a} (walk the parallelogram's two triangle-halves).
  2. Associative: (a⃗+b⃗)+c⃗=a⃗+(b⃗+c⃗)\left(\vec{a} + \vec{b}\right) + \vec{c} = \vec{a} + \left(\vec{b} + \vec{c}\right) — so a⃗+b⃗+c⃗\vec{a} + \vec{b} + \vec{c} needs no brackets.
  3. Additive identity: a⃗+0⃗=a⃗\vec{a} + \vec{0} = \vec{a} — the zero vector changes nothing.
  4. Additive inverse: a⃗+(−a⃗)=0⃗\vec{a} + \left(-\vec{a}\right) = \vec{0}.

Multiplying a Vector by a Scalar

For a vector a⃗\vec{a} and a scalar λ\lambda, the product λa⃗\lambda\vec{a} is a vector collinear with a⃗\vec{a}:

  • Direction: same as a⃗\vec{a} when λ>0\lambda > 0; opposite when λ<0\lambda < 0.
  • Magnitude: ∣λa⃗∣=∣λ∣ ∣a⃗∣\left|\lambda\vec{a}\right| = |\lambda|\,|\vec{a}| — note the absolute value of λ\lambda: ∣−2a⃗∣=2∣a⃗∣\left|-2\vec{a}\right| = 2|\vec{a}|, never −2∣a⃗∣-2|\vec{a}|.

Special values of λ\lambda tell the whole story:

  1. λ=−1\lambda = -1 gives −a⃗-\vec{a}, the additive inverse: same length, opposite direction.
  2. λ=1∣a⃗∣\lambda = \dfrac{1}{|\vec{a}|} (for a⃗≠0⃗\vec{a} \neq \vec{0}) gives a vector of magnitude 11 in the direction of a⃗\vec{a} — the unit vector

a^=a⃗∣a⃗∣\hat{a} = \frac{\vec{a}}{|\vec{a}|}

  1. For any scalar kk, k0⃗=0⃗k\vec{0} = \vec{0}.

Key Point (the workhorse recipe): to produce a vector of magnitude MM in the direction of a⃗\vec{a}, compute Ma^=M∣a⃗∣a⃗M\hat{a} = \dfrac{M}{|\vec{a}|}\vec{a}. 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:

∣ ∣a⃗∣−∣b⃗∣ ∣  ≤  ∣a⃗+b⃗∣  ≤  ∣a⃗∣+∣b⃗∣\bigl|\,|\vec{a}| - |\vec{b}|\,\bigr| \;\leq\; \left|\vec{a} + \vec{b}\right| \;\leq\; |\vec{a}| + |\vec{b}|

Equality on the right holds when a⃗\vec{a} and b⃗\vec{b} point the same way; on the left when they point opposite ways. With ∣a⃗∣=3|\vec{a}| = 3 and ∣b⃗∣=5|\vec{b}| = 5, the sum's magnitude can be anything in [2,8][2, 8] — and nothing outside it.

Solved Examples

Example 1: Net displacement

A girl walks 44 km due west and then 33 km due north. Find the magnitude of her net displacement.

Solution:

  1. 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).
  2. Pythagoras: ∣net∣=42+32=25=5\left|\text{net}\right| = \sqrt{4^2 + 3^2} = \sqrt{25} = 5 km.

Answer: 55 km, pointing north of west. Note that the distance walked is 77 km — displacement (vector) and distance (scalar) part ways exactly here.


Example 2: Magnitude under scaling

If ∣a⃗∣=3|\vec{a}| = 3, find ∣−2a⃗∣\left|-2\vec{a}\right| and describe the direction of −2a⃗-2\vec{a}.

Solution:

  1. Magnitude rule: ∣−2a⃗∣=∣−2∣⋅∣a⃗∣=2×3=6\left|-2\vec{a}\right| = |-2| \cdot |\vec{a}| = 2 \times 3 = 6.
  2. Direction rule: λ=−2<0\lambda = -2 < 0, so the direction is opposite to a⃗\vec{a}.

Answer: magnitude 66, direction opposite to a⃗\vec{a}. A magnitude is never negative — ∣λa⃗∣=∣λ∣∣a⃗∣|\lambda\vec{a}| = |\lambda||\vec{a}| has the absolute value built in for exactly this reason.


Example 3: Building a vector of prescribed length

Given ∣a⃗∣=4|\vec{a}| = 4, write a vector of magnitude 1010 in the direction of a⃗\vec{a}, in terms of a⃗\vec{a}.

Solution:

  1. Normalise: a^=a⃗4\hat{a} = \dfrac{\vec{a}}{4}.
  2. Scale: the required vector is 10a^=104a⃗=52a⃗10\hat{a} = \dfrac{10}{4}\vec{a} = \dfrac{5}{2}\vec{a}.

Answer: 52a⃗\dfrac{5}{2}\vec{a}. Check: ∣52a⃗∣=52×4=10\left|\dfrac{5}{2}\vec{a}\right| = \dfrac{5}{2} \times 4 = 10. ✓


Example 4: A closed walk

Prove that AB→+BC→+CA→=0⃗\overrightarrow{AB} + \overrightarrow{BC} + \overrightarrow{CA} = \vec{0} for any triangle ABCABC, and state the generalisation for a polygon.

Solution:

  1. Triangle law twice: AB→+BC→=AC→\overrightarrow{AB} + \overrightarrow{BC} = \overrightarrow{AC}.
  2. Add the last side: AC→+CA→=AA→=0⃗\overrightarrow{AC} + \overrightarrow{CA} = \overrightarrow{AA} = \vec{0}.

Answer: the sum is 0⃗\vec{0} — 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 ABCDABCD, let AB→=a⃗\overrightarrow{AB} = \vec{a} and AD→=b⃗\overrightarrow{AD} = \vec{b}. Express both diagonals in terms of a⃗\vec{a} and b⃗\vec{b}.

Solution:

  1. Diagonal from AA: AC→=AB→+BC→=a⃗+b⃗\overrightarrow{AC} = \overrightarrow{AB} + \overrightarrow{BC} = \vec{a} + \vec{b} (since BC→=AD→=b⃗\overrightarrow{BC} = \overrightarrow{AD} = \vec{b}).
  2. Diagonal from BB: BD→=BA→+AD→=−a⃗+b⃗=b⃗−a⃗\overrightarrow{BD} = \overrightarrow{BA} + \overrightarrow{AD} = -\vec{a} + \vec{b} = \vec{b} - \vec{a}.

Answer: AC→=a⃗+b⃗\overrightarrow{AC} = \vec{a} + \vec{b}, BD→=b⃗−a⃗\overrightarrow{BD} = \vec{b} - \vec{a} — 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 88 km/h straight across a river whose current flows at 66 km/h parallel to the banks. Find the boat's actual speed.

Solution:

  1. Parallelogram (rectangle) law: the two velocity vectors are perpendicular adjacent sides; the actual velocity is the diagonal.
  2. Magnitude: 82+62=100=10\sqrt{8^2 + 6^2} = \sqrt{100} = 10 km/h.
  3. Direction: downstream of straight-across by the angle θ\theta with tan⁡θ=68=34\tan\theta = \dfrac{6}{8} = \dfrac{3}{4}.

Answer: 1010 km/h, tilted downstream at tan⁡−134\tan^{-1}\dfrac{3}{4} from the crossing direction — the classic physical picture behind the parallelogram law.