Given a regular hexagon $ABCDEF$, with $\vec{AB} = p$ and $\vec{BC} = q$, express the vectors $\vec{CD}, \vec{DE}, \vec{EF}, \vec{FA}, \vec{AD}, \vec{EA}, \vec{AC}$ in terms of $p$ and $q$.

GeometryVectorsHexagonGeometryVector AdditionGeometric Proof
2025/3/30

1. Problem Description

Given a regular hexagon ABCDEFABCDEF, with AB=p\vec{AB} = p and BC=q\vec{BC} = q, express the vectors CD,DE,EF,FA,AD,EA,AC\vec{CD}, \vec{DE}, \vec{EF}, \vec{FA}, \vec{AD}, \vec{EA}, \vec{AC} in terms of pp and qq.

2. Solution Steps

In a regular hexagon, all sides are of equal length, and all interior angles are 120120^\circ.
The opposite sides are parallel.
AB=p\vec{AB} = p
BC=q\vec{BC} = q
Since ABCDEFABCDEF is a regular hexagon, we have:
AB=BC=CD=DE=EF=FA|AB| = |BC| = |CD| = |DE| = |EF| = |FA|.
Also, ABC=120\angle ABC = 120^\circ.
CD\vec{CD}: Since CDCD is parallel to FAFA, we can say that CD\vec{CD} is equivalent to a rotation of AB\vec{AB} by 120120^\circ clockwise from AB\vec{AB}, which is a rotation of BC=q\vec{BC}=q by 6060^\circ. We can also say that it is p+q-p+q.
CD=p+q\vec{CD} = -p+q
DE\vec{DE}: Since DEDE is parallel to ABAB but in the opposite direction, with length DE=AB|DE|=|AB|, DE=p\vec{DE} = -p
EF\vec{EF}: Since EFEF is parallel to BCBC but in the opposite direction, with length EF=BC|EF|=|BC|, EF=q\vec{EF} = -q
FA\vec{FA}: Since FAFA is parallel to CDCD but in the opposite direction, with length FA=CD|FA|=|CD|, FA=pq\vec{FA} = p - q.
AD\vec{AD}: We can write AD=AB+BC+CD=p+q+(p+q)=2q+0p=p+q+p+q+(p+q)=p+q+(p+q)=p+qp+q=2q+0p\vec{AD} = \vec{AB} + \vec{BC} + \vec{CD} = p + q + (-p+q) = 2q+0p = -p + q+p +q +(-p+q)=p+q+(-p+q)=p+q-p+q = 2q+0p, also AD=BC+EF=2q\vec{AD} = \vec{BC} + \vec{EF}=2q. AD=2q\vec{AD}=2q
EA\vec{EA}: We can write EA=AE\vec{EA} = - \vec{AE}. Also, AE=AD+DE=2q+(p)=p+2q\vec{AE} = \vec{AD} + \vec{DE} = 2q + (-p) = -p + 2q. So, EA=p2q\vec{EA} = p - 2q
AC\vec{AC}: AC=AB+BC=p+q\vec{AC} = \vec{AB} + \vec{BC} = p + q

3. Final Answer

CD=p+q\vec{CD} = -p+q
DE=p\vec{DE} = -p
EF=q\vec{EF} = -q
FA=pq\vec{FA} = p-q
AD=p+q+CD=p+q+(p+q)=2q\vec{AD} = p + q + \vec{CD} = p + q + (-p + q) = 2q
EA=p2q\vec{EA} = p - 2q
AC=p+q\vec{AC} = p + q

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