Three non-zero vectors p\mathbf{p}, q\mathbf{q} and r\mathbf{r} are such that 3p×q=r×p3\mathbf{p} \times \mathbf{q} = \mathbf{r} \times \mathbf{p}. Find a linear relationship between p\mathbf{p}, q\mathbf{q} and r\mathbf{r}. Referred to the origin OO, the points AA and BB have position vectors a\mathbf{a} and b\mathbf{b}. It is given that a\mathbf{a} and b\mathbf{b} are non-parallel unit vectors. The point BB divides ACAC in the ratio 1:31:3. The point DD lies on OBOB produced such that OB:OD=1:mOB : OD = 1 : m, where m∈Zm \in \mathbb{Z}, m≥2m \ge 2. Given that AB→\overrightarrow{AB} is perpendicular to CD→\overrightarrow{CD}, find the numerical value of mm.

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Worked solution

7(a)

1. Rearrange the given equation and apply the anti-commutative property of the vector product.

3p×q−r×p=03\mathbf{p} \times \mathbf{q} - \mathbf{r} \times \mathbf{p} = \mathbf{0}
3p×q−(−p×r)=03\mathbf{p} \times \mathbf{q} - (-\mathbf{p} \times \mathbf{r}) = \mathbf{0}

2. Factorise the expression using the distributive property of the vector product.

3p×q+p×r=03\mathbf{p} \times \mathbf{q} + \mathbf{p} \times \mathbf{r} = \mathbf{0}
p×(3q+r)=0\mathbf{p} \times (3\mathbf{q} + \mathbf{r}) = \mathbf{0}

3. Deduce the geometrical relationship between the vectors to form a linear relationship.

Since p\mathbf{p} is a non-zero vector, the zero cross product implies that the vector 3q+r3\mathbf{q} + \mathbf{r} must be parallel to p\mathbf{p}.
Therefore,
3q+r=kp3\mathbf{q} + \mathbf{r} = k\mathbf{p}
for some scalar k∈Rk \in \mathbb{R}.

Answer

3q+r=kp3\mathbf{q} + \mathbf{r} = k\mathbf{p} for some scalar k∈Rk \in \mathbb{R}

7(b)

1. Express the position vector $\mathbf{c}$ in terms of $\mathbf{a}$ and $\mathbf{b}$ using the ratio theorem.

Since BB divides ACAC in the ratio 1:31:3, by the ratio theorem:
b=3a+1c1+3\mathbf{b} = \frac{3\mathbf{a} + 1\mathbf{c}}{1 + 3}
4b=3a+c4\mathbf{b} = 3\mathbf{a} + \mathbf{c}
c=4b−3a\mathbf{c} = 4\mathbf{b} - 3\mathbf{a}

2. Express the vectors $\overrightarrow{AB}$ and $\overrightarrow{CD}$ in terms of $\mathbf{a}$ and $\mathbf{b}$.

Since DD lies on OBOB produced and OB:OD=1:mOB : OD = 1 : m, we have d=mb\mathbf{d} = m\mathbf{b}.

AB→=b−a\overrightarrow{AB} = \mathbf{b} - \mathbf{a}

CD→=d−c\overrightarrow{CD} = \mathbf{d} - \mathbf{c}
CD→=mb−(4b−3a)\overrightarrow{CD} = m\mathbf{b} - (4\mathbf{b} - 3\mathbf{a})
CD→=(m−4)b+3a\overrightarrow{CD} = (m - 4)\mathbf{b} + 3\mathbf{a}

3. Apply the condition for perpendicular vectors and expand the dot product.

Since AB→\overrightarrow{AB} is perpendicular to CD→\overrightarrow{CD}, their scalar (dot) product is zero:
AB→⋅CD→=0\overrightarrow{AB} \cdot \overrightarrow{CD} = 0
(b−a)⋅((m−4)b+3a)=0(\mathbf{b} - \mathbf{a}) \cdot ((m - 4)\mathbf{b} + 3\mathbf{a}) = 0
Expanding the expression:
(m−4)(b⋅b)+3(b⋅a)−(m−4)(a⋅b)−3(a⋅a)=0(m - 4)(\mathbf{b} \cdot \mathbf{b}) + 3(\mathbf{b} \cdot \mathbf{a}) - (m - 4)(\mathbf{a} \cdot \mathbf{b}) - 3(\mathbf{a} \cdot \mathbf{a}) = 0

4. Use the properties of unit vectors to simplify and solve for $m$.

Given that a\mathbf{a} and b\mathbf{b} are unit vectors, ∣a∣=1  ⟹  a⋅a=1|\mathbf{a}| = 1 \implies \mathbf{a} \cdot \mathbf{a} = 1 and ∣b∣=1  ⟹  b⋅b=1|\mathbf{b}| = 1 \implies \mathbf{b} \cdot \mathbf{b} = 1.
(m−4)(1)+3(a⋅b)−(m−4)(a⋅b)−3(1)=0(m - 4)(1) + 3(\mathbf{a} \cdot \mathbf{b}) - (m - 4)(\mathbf{a} \cdot \mathbf{b}) - 3(1) = 0
m−7+(7−m)(a⋅b)=0m - 7 + (7 - m)(\mathbf{a} \cdot \mathbf{b}) = 0
Factorising the expression:
(m−7)(1−a⋅b)=0(m - 7)(1 - \mathbf{a} \cdot \mathbf{b}) = 0
Since a\mathbf{a} and b\mathbf{b} are non-parallel unit vectors, the angle θ\theta between them is not 00, so a⋅b=∣a∣∣b∣cos⁡θ=cos⁡θ≠1\mathbf{a} \cdot \mathbf{b} = |\mathbf{a}||\mathbf{b}|\cos\theta = \cos\theta \neq 1.
Therefore, 1−a⋅b≠01 - \mathbf{a} \cdot \mathbf{b} \neq 0, which means:
m−7=0m - 7 = 0
m=7m = 7

Answer

m=7m = 7

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