Referred to the origin O, let P, Q and R be distinct points with position vectors p\mathbf{p}, q\mathbf{q} and r\mathbf{r} respectively.

  1. (a)

    Show that (r−p)×(r−q)=p×q+q×r+r×p(\mathbf{r}-\mathbf{p})\times(\mathbf{r}-\mathbf{q}) = \mathbf{p}\times\mathbf{q} + \mathbf{q}\times\mathbf{r} + \mathbf{r}\times\mathbf{p}.

  2. (b)

    Give the geometrical meaning of 12 ∣p×q+q×r+r×p∣\tfrac{1}{2}\,|\mathbf{p}\times\mathbf{q} + \mathbf{q}\times\mathbf{r} + \mathbf{r}\times\mathbf{p}|.

  3. (c)

    Given that p×q+q×r+r×p=0\mathbf{p}\times\mathbf{q} + \mathbf{q}\times\mathbf{r} + \mathbf{r}\times\mathbf{p} = \mathbf{0}, PR=3QRPR = 3QR, and that PQ>PRPQ > PR, express r\mathbf{r} in terms of p\mathbf{p} and q\mathbf{q}.

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Worked solution

4(a)

1. Expand the vector product on the left-hand side using the distributive law.

LHS=(r−p)×(r−q)=r×r−r×q−p×r+p×q\begin{aligned} \text{LHS} &= (\mathbf{r}-\mathbf{p})\times(\mathbf{r}-\mathbf{q}) \\ &= \mathbf{r}\times\mathbf{r} - \mathbf{r}\times\mathbf{q} - \mathbf{p}\times\mathbf{r} + \mathbf{p}\times\mathbf{q} \end{aligned}

2. Apply the properties of vector products to simplify the expression to the right-hand side.

Since r×r=0,  r×q=−q×r and p×r=−r×p,LHS=0−(−q×r)−(−r×p)+p×q=q×r+r×p+p×q=p×q+q×r+r×p=RHS (shown)\begin{aligned} &\text{Since } \mathbf{r}\times\mathbf{r} = \mathbf{0}, \; \mathbf{r}\times\mathbf{q} = -\mathbf{q}\times\mathbf{r} \text{ and } \mathbf{p}\times\mathbf{r} = -\mathbf{r}\times\mathbf{p}, \\ \text{LHS} &= \mathbf{0} - (-\mathbf{q}\times\mathbf{r}) - (-\mathbf{r}\times\mathbf{p}) + \mathbf{p}\times\mathbf{q} \\ &= \mathbf{q}\times\mathbf{r} + \mathbf{r}\times\mathbf{p} + \mathbf{p}\times\mathbf{q} \\ &= \mathbf{p}\times\mathbf{q} + \mathbf{q}\times\mathbf{r} + \mathbf{r}\times\mathbf{p} \\ &= \text{RHS (shown)} \end{aligned}

Answer

(r−p)×(r−q)=p×q+q×r+r×p(\mathbf{r}-\mathbf{p})\times(\mathbf{r}-\mathbf{q}) = \mathbf{p}\times\mathbf{q} + \mathbf{q}\times\mathbf{r} + \mathbf{r}\times\mathbf{p} (shown)

4(b)

1. Substitute the identity proved in part (a) into the given expression.

From part (a), we know that p×q+q×r+r×p=(r−p)×(r−q)\mathbf{p}\times\mathbf{q} + \mathbf{q}\times\mathbf{r} + \mathbf{r}\times\mathbf{p} = (\mathbf{r}-\mathbf{p})\times(\mathbf{r}-\mathbf{q}).

Substituting this into the given expression, we get:
12 ∣p×q+q×r+r×p∣=12 ∣(r−p)×(r−q)∣\frac{1}{2}\,|\mathbf{p}\times\mathbf{q} + \mathbf{q}\times\mathbf{r} + \mathbf{r}\times\mathbf{p}| = \frac{1}{2}\,|(\mathbf{r}-\mathbf{p})\times(\mathbf{r}-\mathbf{q})|

2. Interpret the vectors geometrically to find the meaning of the expression.

The vectors can be written in terms of the points PP, QQ, and RR:
r−p=PR⃗\mathbf{r}-\mathbf{p} = \vec{PR}
r−q=QR⃗\mathbf{r}-\mathbf{q} = \vec{QR}

The expression becomes 12 ∣PR⃗×QR⃗∣\frac{1}{2}\,|\vec{PR}\times\vec{QR}|.
The magnitude of the cross product of two vectors representing adjacent sides of a triangle gives the area of the parallelogram formed by them. Multiplying by 12\frac{1}{2} gives the area of the triangle.

Therefore, the expression represents the area of triangle PQRPQR.

Answer

Area of triangle PQRPQR

4(c)

1. Establish that points P, Q, and R are collinear.

From the result shown in (a), we substitute the given condition p×q+q×r+r×p=0\mathbf{p}\times\mathbf{q} + \mathbf{q}\times\mathbf{r} + \mathbf{r}\times\mathbf{p} = \mathbf{0} to obtain:
(r−p)×(r−q)=0(\mathbf{r}-\mathbf{p})\times(\mathbf{r}-\mathbf{q}) = \mathbf{0}
PR⃗×QR⃗=0\vec{PR} \times \vec{QR} = \mathbf{0}
Since the cross product of these two vectors is the zero vector, PR⃗\vec{PR} and QR⃗\vec{QR} are parallel. As they share the common point RR, the points PP, QQ and RR are collinear.

2. Set up the vector equations for the two possible cases and eliminate the invalid one.

Since the points are collinear and their lengths relate by PR=3QRPR = 3QR, the vectors must satisfy either PR⃗=3QR⃗\vec{PR} = 3\vec{QR} or PR⃗=−3QR⃗\vec{PR} = -3\vec{QR}.

Consider Case 1 where PR⃗=3QR⃗\vec{PR} = 3\vec{QR}:
r−p=3(r−q)\mathbf{r} - \mathbf{p} = 3(\mathbf{r} - \mathbf{q})
2r=3q−p  ⟹  r=32q−12p2\mathbf{r} = 3\mathbf{q} - \mathbf{p} \implies \mathbf{r} = \frac{3}{2}\mathbf{q} - \frac{1}{2}\mathbf{p}
We check the magnitude condition PQ>PRPQ > PR for this case:
PR⃗=(32q−12p)−p=32(q−p)=32PQ⃗\vec{PR} = \left(\frac{3}{2}\mathbf{q} - \frac{1}{2}\mathbf{p}\right) - \mathbf{p} = \frac{3}{2}(\mathbf{q} - \mathbf{p}) = \frac{3}{2}\vec{PQ}
Taking magnitudes gives PR=32PQPR = \frac{3}{2}PQ, meaning PQ<PRPQ < PR. This contradicts the given condition PQ>PRPQ > PR, so we reject this case.

3. Solve the valid case to find $\mathbf{r}$ in terms of $\mathbf{p}$ and $\mathbf{q}$.

Consider Case 2 where PR⃗=−3QR⃗\vec{PR} = -3\vec{QR}:
r−p=−3(r−q)\mathbf{r} - \mathbf{p} = -3(\mathbf{r} - \mathbf{q})
r−p=−3r+3q\mathbf{r} - \mathbf{p} = -3\mathbf{r} + 3\mathbf{q}
4r=p+3q4\mathbf{r} = \mathbf{p} + 3\mathbf{q}
r=14p+34q\mathbf{r} = \frac{1}{4}\mathbf{p} + \frac{3}{4}\mathbf{q}

(Self-check for this case: PR⃗=r−p=34q−34p=34PQ⃗\vec{PR} = \mathbf{r} - \mathbf{p} = \frac{3}{4}\mathbf{q} - \frac{3}{4}\mathbf{p} = \frac{3}{4}\vec{PQ}, so PR=34PQPR = \frac{3}{4}PQ, which correctly satisfies PQ>PRPQ > PR.)

Answer

r=14p+34q\mathbf{r} = \frac{1}{4}\mathbf{p} + \frac{3}{4}\mathbf{q}

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