J5 - Vector proofs and contextual problems

J5 - Vector proofs and contextual problems

Use directed-vector relationships to prove geometric claims and locate constrained intersections. Apply the same component reasoning to forces and planar motion, stating what the model assumes and checking that the answer describes the physical event asked for.

Vector geometry proofs

If two particles follow paths that cross, must they collide? A shared location is only part of the answer: we will need a shared time too. First, learn how vector relationships establish exactly what a geometric diagram suggests.

You already know

Joining vectors are end position minus start position. Scalar multiples describe parallel directions; signed sine and cosine projections resolve a magnitude and angle into perpendicular components.

Keep the points and the arrow directions explicit when turning these calculations into a proof.

For A=(1,−1,2)A=(1,-1,2), B=(3,2,1)B=(3,2,1) and C=(7,8,−1)C=(7,8,-1), the joining vectors are AB→=(2,3,−1)\overrightarrow{AB}=(2,3,-1) and AC→=(6,9,−3)\overrightarrow{AC}=(6,9,-3). The second is three times the first. Since both start at AA, the three points lie on one line.

Parallel and collinear

Two nonzero vectors are parallel when one is a scalar multiple of the other. Distinct points A,B,CA,B,C are collinear when they lie on one line; equivalently, AC→=λAB→\overrightarrow{AC}=\lambda\overrightarrow{AB} for some real λ\lambda. Equal magnitudes alone establish neither condition.

The shared point matters. Two parallel arrows placed far apart do not make all their endpoints collinear. These parallelism and collinearity criteria are not in the formula booklet: learn them. A proof must finish by translating the scalar-multiple relationship into the geometric claim asked for.

Worked example 1: collinearity in space

Question. Prove that A=(1,−1,2)A=(1,-1,2), B=(3,2,1)B=(3,2,1), C=(7,8,−1)C=(7,8,-1) are collinear, and find AB:BCAB:BC.

Plan. Form two vectors starting at AA, compare their components, then locate CC on the line.

AB→=(3−1,2−(−1),1−2)=(2,3,−1)AC→=(7−1,8−(−1),−1−2)=(6,9,−3)=3AB→one multiplier in every componentBC→=AC→−AB→=2AB→\begin{aligned} \overrightarrow{AB}&=(3-1,2-(-1),1-2)=(2,3,-1)\\ \overrightarrow{AC}&=(7-1,8-(-1),-1-2)=(6,9,-3)\\ &=3\overrightarrow{AB} && \text{one multiplier in every component}\\ \overrightarrow{BC}&=\overrightarrow{AC}-\overrightarrow{AB}=2\overrightarrow{AB} \end{aligned}

Why this step? Comparing vectors with a common starting point establishes one common line, rather than only parallel directions.

Answer. A,B,CA,B,C are collinear. The multiplier 3>13>1 places CC beyond BB, and AB:BC=1:2AB:BC=1:2.

Check. Starting at BB, adding 2(2,3,−1)2(2,3,-1) gives (7,8,−1)=C(7,8,-1)=C.

Change only the multiplier locating the third point, from 33 to −2-2. This time the point is on the other side of AA.

Worked example 2: a point beyond the other endpoint

Question. Prove that A=(1,−1,2)A=(1,-1,2), B=(3,2,1)B=(3,2,1), D=(−3,−7,4)D=(-3,-7,4) are collinear, and find AB:BDAB:BD.

Plan. Compare AD→\overrightarrow{AD} with the unchanged AB→\overrightarrow{AB}, then use nonnegative lengths for the ratio.

AD→=(−4,−6,2)=−2(2,3,−1)=−2AB→BD→=AD→−AB→=−3AB→BD=3ABmagnitude of multiplier\begin{aligned} \overrightarrow{AD}&=(-4,-6,2)=-2(2,3,-1)=-2\overrightarrow{AB}\\ \overrightarrow{BD}&=\overrightarrow{AD}-\overrightarrow{AB}=-3\overrightarrow{AB}\\ BD&=3AB && \text{magnitude of multiplier} \end{aligned}

Why this step? A negative scalar reverses direction; it does not make a length negative.

Answer. A,B,DA,B,D are collinear, with DD beyond AA away from BB. The length ratio is AB:BD=1:3AB:BD=1:3.

Check. Starting at AA, the position becomes (1,−1,2)−2(2,3,−1)=(−3,−7,4)(1,-1,2)-2(2,3,-1)=(-3,-7,4), the coordinates of DD.

Vector proofs also work with arbitrary positions. Let a,b,c\mathbf a,\mathbf b,\mathbf c denote the vertices of a nondegenerate triangle: they are not collinear. Keeping the letters general proves a result for every such triangle, including one tilted in three-dimensional space.

Worked example 3: the midpoint theorem

Question. In a nondegenerate triangle ABCABC, M,NM,N are the midpoints of AB,ACAB,AC. Prove that MNMN is parallel to BCBC and has half its length.

Plan. Write both midpoint positions, subtract, and recognise a multiple of BC→\overrightarrow{BC}.

m=a+b2n=a+c2midpointsMN→=n−mend minus start=a+c−a−b2=12(c−b)=12BC→\begin{aligned} \mathbf m&=\frac{\mathbf a+\mathbf b}{2}\qquad \mathbf n=\frac{\mathbf a+\mathbf c}{2} && \text{midpoints}\\ \overrightarrow{MN}&=\mathbf n-\mathbf m && \text{end minus start}\\ &=\frac{\mathbf a+\mathbf c-\mathbf a-\mathbf b}{2}\\ &=\frac12(\mathbf c-\mathbf b)=\frac12\overrightarrow{BC} \end{aligned}

Why this step? Subtraction cancels the shared vertex position a\mathbf a, leaving the opposite side vector.

Answer. Since BC→≠0\overrightarrow{BC}\ne\mathbf0, the scalar multiple proves MN∥BCMN\parallel BC, and MN=BC/2MN=BC/2.

Check. The positive multiplier gives the same direction from MM to NN as from BB to CC, consistent with the two midpoint positions.

Change only the fraction travelled along both sides, from one half to one third. The cancellation is the same.

Worked example 4: a different common fraction

Question. In a nondegenerate triangle ABCABC, points P,QP,Q satisfy AP:PB=AQ:QC=1:2AP:PB=AQ:QC=1:2. Prove that PQ∥BCPQ\parallel BC and PQ=BC/3PQ=BC/3.

Plan. Use a travelled fraction of 1/31/3 on each side and subtract the resulting positions.

p=a+13(b−a)=2a+b3q=a+13(c−a)=2a+c3PQ→=q−p=c−b3=13BC→\begin{aligned} \mathbf p&=\mathbf a+\frac13(\mathbf b-\mathbf a)=\frac{2\mathbf a+\mathbf b}{3}\\ \mathbf q&=\mathbf a+\frac13(\mathbf c-\mathbf a)=\frac{2\mathbf a+\mathbf c}{3}\\ \overrightarrow{PQ}&=\mathbf q-\mathbf p=\frac{\mathbf c-\mathbf b}{3}=\frac13\overrightarrow{BC} \end{aligned}

Why this step? The fractions must match on the two sides for the shared a\mathbf a terms to cancel.

Answer. PQ∥BCPQ\parallel BC and PQ=BC/3PQ=BC/3, as required.

Check. More generally, equal travelled fractions tt give PQ→=tBC→\overrightarrow{PQ}=t\overrightarrow{BC}; t=1/2t=1/2 recovers the midpoint theorem.

Medians and diagonals

A median joins a triangle vertex to the midpoint of the opposite side. All three medians meet at one point, two thirds of the way from each vertex, however uneven the triangle looks. To see why, let m=(b+c)/2\mathbf m=(\mathbf b+\mathbf c)/2 be the midpoint of BCBC, and put g=(a+b+c)/3\mathbf g=(\mathbf a+\mathbf b+\mathbf c)/3. Then

AG→=g−a=b+c−2a3=23(m−a)=23AM→\begin{aligned} \overrightarrow{AG}&=\mathbf g-\mathbf a=\frac{\mathbf b+\mathbf c-2\mathbf a}{3}\\ &=\frac23(\mathbf m-\mathbf a)=\frac23\overrightarrow{AM} \end{aligned}

Thus GG is on median AMAM, with AG:GM=2:1AG:GM=2:1. The same calculation starting at BB and CC reaches exactly the same GG; the three medians therefore meet there. This point is the centroid.

A nondegenerate triangle with its three medians meeting at the centroid

For a parallelogram ABCDABCD in vertex order, the side relation AD→=BC→\overrightarrow{AD}=\overrightarrow{BC} gives d=a+c−b\mathbf d=\mathbf a+\mathbf c-\mathbf b. Hence the midpoint of BDBD is (b+d)/2=(a+c)/2(\mathbf b+\mathbf d)/2=(\mathbf a+\mathbf c)/2, also the midpoint of ACAC. This proves that its diagonals bisect one another without assuming that property at the start. The midpoint, common-fraction, centroid and parallelogram results here are not in the formula booklet: learn how to derive them from positions.

Watch out

Wrong: “(2,4,7)=2(1,2,3)(2,4,7)=2(1,2,3), so the vectors are parallel.” The third component would have to be 66. Right: one scalar must work in every component, so these two vectors are not parallel.

Apply the shared-fraction proof with a new ratio, keeping the vertices general.

Intersections and segment constraints

A geometric intersection is a position reached by two routes. Build each route with its own parameter, then ask whether the two positions can agree.

Positions on the line through distinct points A,BA,B can be written a+λ(b−a)\mathbf a+\lambda(\mathbf b-\mathbf a), with real λ\lambda; its segment requires 0≤λ≤10\le\lambda\le1. A second line through C,DC,D has positions c+μ(d−c)\mathbf c+\mu(\mathbf d-\mathbf c). These are position constructions from fractions of joining vectors, not an instruction to assume λ=μ\lambda=\mu.

A common position

At an intersection,

a+λ(b−a)=c+μ(d−c)\mathbf a+\lambda(\mathbf b-\mathbf a)=\mathbf c+\mu(\mathbf d-\mathbf c)

All corresponding components must agree. For intersection of the closed segments, also require 0≤λ≤10\le\lambda\le1 and 0≤μ≤10\le\mu\le1. Not in the formula booklet: learn it.

In three dimensions, two component equations may give candidate parameters, but the third still has to agree. For example, positions (s,s,0)(s,s,0) and (t,1−t,1)(t,1-t,1) give s=t=1/2s=t=1/2 from their first two coordinates, but their third coordinates differ for every choice. Those lines have no common point. Parallel lines may likewise be distinct or may be the same line; inspect the actual positions.

Worked example 5: crossing segments

Question. A=(1,0)A=(1,0), B=(7,6)B=(7,6), C=(1,5)C=(1,5), D=(7,−1)D=(7,-1). Find the intersection of the extended lines and decide whether both segments contain it.

Plan. Equate two independently parameterised positions and check both parameter ranges.

(1+6λ,6λ)=(1+6μ,5−6μ)6λ=6μhorizontal coordinates6λ=5−6μvertical coordinatesλ=μ=512solve both conditionsp=(1+6⋅5/12,6⋅5/12)=(7/2,5/2)\begin{aligned} (1+6\lambda,6\lambda)&=(1+6\mu,5-6\mu)\\ 6\lambda&=6\mu && \text{horizontal coordinates}\\ 6\lambda&=5-6\mu && \text{vertical coordinates}\\ \lambda=\mu&=\frac5{12} && \text{solve both conditions}\\ \mathbf p&=(1+6\cdot5/12,6\cdot5/12)=(7/2,5/2) \end{aligned}

Why this step? The two parameters turn out equal because of the horizontal equation; equality was not assumed beforehand.

Answer. The lines meet at (7/2,5/2)(7/2,5/2). Both parameters lie in [0,1][0,1], so both segments contain the intersection.

Check. The second route gives (1+6⋅5/12,5−6⋅5/12)=(7/2,5/2)(1+6\cdot5/12,5-6\cdot5/12)=(7/2,5/2) too.

Translate only the second segment upwards by eight units in the next example. Its direction stays the same, but the intersection moves beyond the endpoints.

Worked example 6: intersection outside a segment

Question. A=(1,0)A=(1,0), B=(7,6)B=(7,6), C=(1,13)C=(1,13), D=(7,7)D=(7,7). Find the line intersection and determine whether the segments intersect.

Plan. Use the same direction vectors, with the new starting position for the second route.

(1+6λ,6λ)=(1+6μ,13−6μ)λ=μhorizontal equation12λ=13vertical equationλ=μ=1312p=(15/2,13/2)\begin{aligned} (1+6\lambda,6\lambda)&=(1+6\mu,13-6\mu)\\ \lambda&=\mu && \text{horizontal equation}\\ 12\lambda&=13 && \text{vertical equation}\\ \lambda=\mu&=\frac{13}{12}\\ \mathbf p&=(15/2,13/2) \end{aligned}

Why this step? Solving the line equations does not automatically enforce the endpoint restrictions.

Answer. The extended lines meet at (15/2,13/2)(15/2,13/2). Both parameters exceed 11, so this point is beyond BB and beyond DD; the segments do not intersect.

Check. From D=(7,7)D=(7,7), an extra 1/121/12 of (6,−6)(6,-6) reaches (7.5,6.5)(7.5,6.5), the same point.

An endpoint itself is allowed for a closed segment, because the parameter bounds include equality.

Watch out

Wrong: “The equations have a solution, so the segments intersect.” That proves a common point of the extended lines only. Right: check both parameters against [0,1][0,1]; a value 5/45/4 lies beyond the ending point by a further quarter of the full joining vector.

Try one new endpoint translation with the same directions.

Planar force models

Forces combine like directed movements: add their components, not their magnitudes. A 6 N6\,\mathrm N force east and an 8 N8\,\mathrm N force northwest do not pull with a resultant of 14 N14\,\mathrm N, because their directions differ.

Resultant and equilibrium

The resultant force on a model particle is the vector sum of all forces acting on it. In equilibrium, that sum is zero. A balancing force is the negative of the resultant of the other forces, so it has equal magnitude and opposite direction.

The particle model treats the forces as acting at one point. Zero resultant gives translational equilibrium; these calculations do not test the rotational equilibrium of an extended object. Equilibrium need not mean that the particle is stationary: constant velocity is also compatible with zero resultant.

A force FF at angle θ\theta anticlockwise from the positive i\mathbf i direction has components Fcos⁡θF\cos\theta, Fsin⁡θF\sin\theta. With a bearing from north, east and north components use Fsin⁡bF\sin b, Fcos⁡bF\cos b instead. These are the projections already used for displacement.

Vector balance

For concurrent planar forces,

R=∑Fequilibrium: ∑F=0\mathbf R=\sum\mathbf F\qquad \text{equilibrium: }\sum\mathbf F=\mathbf0

Thus, for three forces, F3=−(F1+F2)\mathbf F_3=-(\mathbf F_1+\mathbf F_2). Not in the formula booklet: learn it.

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