Given a rectangle ABCD . Express the side vectors in terms…
Given a rectangle $ABCD$. Express the side vectors in terms of the diagonal vectors.
Explanation of Method
Expressing side vectors of a rectangle through its diagonal vectors.
Step 1: Setup
Denote the diagonal vectors by
\[ \vec{p} = \overrightarrow{AC}, \qquad \vec{q} = \overrightarrow{BD}. \]
By the triangle rule, \[\overrightarrow{AC} = \overrightarrow{AB} + \overrightarrow{BC}, \qquad \overrightarrow{BD} = \overrightarrow{BA} + \overrightarrow{AD},\] so \[\vec{p} = \overrightarrow{AB} + \overrightarrow{BC}, \qquad \vec{q} = -\overrightarrow{AB} + \overrightarrow{AD}.\]
In a rectangle opposite sides are equal and parallel, hence $\overrightarrow{BC} = \overrightarrow{AD}$, and both equations become
\[ \vec{p} = \overrightarrow{AB} + \overrightarrow{AD}, \qquad \vec{q} = -\overrightarrow{AB} + \overrightarrow{AD}. \]
- $\vec p=\overrightarrow{AC}$
- $\vec q=\overrightarrow{BD}$
Step 2: Solve for the side vectors
Adding the two equations: $\vec{p} + \vec{q} = 2\,\overrightarrow{AD}$.
\[\overrightarrow{AD} = \frac{1}{2}(\vec{p} + \vec{q})\]
Subtracting the second equation from the first: $\vec{p} - \vec{q} = 2\,\overrightarrow{AB}$.
\[\overrightarrow{AB} = \frac{1}{2}(\vec{p} - \vec{q})\]
Step 3: Remaining sides
Along the traversal $A \to B \to C \to D$, opposite sides are equal in length and point in opposite directions: $\overrightarrow{BC} = \overrightarrow{AD} = \frac{1}{2}(\vec{p} + \vec{q})$.
\[\overrightarrow{CD} = -\overrightarrow{AB} = \frac{1}{2}(\vec{q} - \vec{p})\]
Result
All four side vectors expressed through $\vec{p} = \overrightarrow{AC}$ and $\vec{q} = \overrightarrow{BD}$:
| Side vector | Expression |
|---|---|
| $\overrightarrow{AB}$ | $\dfrac{1}{2}(\vec{p} - \vec{q})$ |
| $\overrightarrow{BC}$ | $\dfrac{1}{2}(\vec{p} + \vec{q})$ |
| $\overrightarrow{CD}$ | $\dfrac{1}{2}(\vec{q} - \vec{p})$ |
| $\overrightarrow{DA}$ | $-\dfrac{1}{2}(\vec{p} + \vec{q})$ |
Remark
Check. The four side vectors must add up to the zero vector, since the polygon is closed:
\[ \overrightarrow{AB}+\overrightarrow{BC}+\overrightarrow{CD}+\overrightarrow{DA} = \tfrac12\big[(\vec p-\vec q)+(\vec p+\vec q)+(\vec q-\vec p)-(\vec p+\vec q)\big]=\vec 0. \]