Question 1 Report
Figure 2 shows the parallelogram \(OACB\), in which \(\overrightarrow{OA} = \mathbf{a}\) and \(\overrightarrow{OB} = \mathbf{b}\). The point \(M\) is the midpoint of \(BC\). The line \(OM\) meets the diagonal \(AB\) at the point \(X\).
Twelve marks of vector geometry in a parallelogram. Figure 2 shows \(OACB\) with \(\overrightarrow{OA} = \mathbf{a}\) and \(\overrightarrow{OB} = \mathbf{b}\), \(M\) the midpoint of \(BC\), and \(X\) the point where \(OM\) crosses the diagonal \(AB\). The whole question turns on one powerful idea: if \(\mathbf{a}\) and \(\mathbf{b}\) are not parallel, then any point of the plane has exactly one expression as \(\lambda\mathbf{a} + \mu\mathbf{b}\). Writing the same point two ways therefore forces the coefficients to match, and that gives simultaneous equations.
In the parallelogram \(OACB\), the side \(AC\) is equal and parallel to \(OB\), so travelling \(O\) to \(A\) to \(C\) is \(\mathbf{a}\) followed by \(\mathbf{b}\): \[\overrightarrow{OC} = \mathbf{a} + \mathbf{b} \quad \textbf{B1}\]
Since the result is given, the marks are for the route. First find the side \(BC\): \[\overrightarrow{BC} = \overrightarrow{OC} - \overrightarrow{OB} = (\mathbf{a} + \mathbf{b}) - \mathbf{b} = \mathbf{a}, \ \text{so} \ \overrightarrow{BM} = \tfrac{1}{2}\mathbf{a} \quad \textbf{M1}\] Then travel \(O\) to \(B\) to \(M\): \[\overrightarrow{OM} = \overrightarrow{OB} + \overrightarrow{BM} = \mathbf{b} + \tfrac{1}{2}\mathbf{a} = \tfrac{1}{2}\mathbf{a} + \mathbf{b} \quad \textbf{A1}\]
Along \(OM\), \(X\) is a fraction \(t\) of the way: \[\overrightarrow{OX} = t\left(\tfrac{1}{2}\mathbf{a} + \mathbf{b}\right) = \tfrac{1}{2}t\,\mathbf{a} + t\,\mathbf{b} \quad \textbf{B1}\] Along \(AB\), start at \(A\) and move a fraction \(s\) of the way towards \(B\). The direction is \[\overrightarrow{AB} = \overrightarrow{OB} - \overrightarrow{OA} = \mathbf{b} - \mathbf{a} \quad \textbf{B1}\] so \[\overrightarrow{OX} = \overrightarrow{OA} + s\,\overrightarrow{AB} = \mathbf{a} + s(\mathbf{b} - \mathbf{a}) = (1 - s)\mathbf{a} + s\,\mathbf{b} \quad \textbf{B1}\] Three independent B marks. Both expressions must be written purely in terms of \(\mathbf{a}\), \(\mathbf{b}\) and the single parameter, with the brackets expanded ready for comparison.
The two expressions describe the same point, and \(\mathbf{a}\) and \(\mathbf{b}\) are non-parallel, so the coefficients may be equated: \[\text{Coefficients may be compared because } \mathbf{a} \ \text{and} \ \mathbf{b} \ \text{are not parallel.} \quad \textbf{M1}\] \[\mathbf{a}: \ \tfrac{1}{2}t = 1 - s; \qquad \mathbf{b}: \ t = s \quad \textbf{A1}\] Substituting \(t = s\) into the first equation: \[\tfrac{1}{2}s = 1 - s \ \Rightarrow\ \tfrac{3}{2}s = 1 \ \Rightarrow\ s = \tfrac{2}{3}, \qquad t = \tfrac{2}{3} \quad \textbf{A1}\] The M1 rewards the justification as well as the act of comparing; it is the mathematical content of the part. The final A1 needs both values.
Since \(\overrightarrow{AX} = s\,\overrightarrow{AB} = \tfrac{2}{3}\overrightarrow{AB}\), the point \(X\) is two thirds of the way from \(A\) to \(B\), leaving one third: \[AX : XB = 2 : 1 \quad \textbf{B1}\] Read from \(s\) directly as \(s : (1 - s)\). Quoting \(1 : 2\) reverses the segments.
Use either expression with \(s = t = \tfrac{2}{3}\). Taking the second gives \(\overrightarrow{OX} = \tfrac{1}{3}\mathbf{a} + \tfrac{2}{3}\mathbf{b}\): \[\overrightarrow{OX} = \tfrac{1}{3}(4\mathbf{i} + \mathbf{j}) + \tfrac{2}{3}(-2\mathbf{i} + 5\mathbf{j}) = \left(\tfrac{4}{3} - \tfrac{4}{3}\right)\mathbf{i} + \left(\tfrac{1}{3} + \tfrac{10}{3}\right)\mathbf{j} = \tfrac{11}{3}\mathbf{j} \quad \textbf{M1}\] The \(\mathbf{i}\) components cancel exactly, so \(\overrightarrow{OX}\) points straight up the \(\mathbf{j}\) direction and its modulus is simply the size of that one component: \[\left|\overrightarrow{OX}\right| = \tfrac{11}{3} \quad \textbf{A1}\] Using the first expression is an equally good check: \(\tfrac{2}{3}\left(\tfrac{1}{2}\mathbf{a} + \mathbf{b}\right) = \tfrac{1}{3}\mathbf{a} + \tfrac{2}{3}\mathbf{b}\), the same vector.
With the given components, \(\overrightarrow{OM} = \tfrac{1}{2}(4\mathbf{i} + \mathbf{j}) + (-2\mathbf{i} + 5\mathbf{j}) = 0\mathbf{i} + \tfrac{11}{2}\mathbf{j}\), so \(OM\) itself lies along the \(\mathbf{j}\)-axis and \(\tfrac{2}{3}\) of it is \(\tfrac{11}{3}\mathbf{j}\), confirming part (f) independently. The ratio in part (e) is also verifiable numerically: \(A\) is at \((4, 1)\), \(B\) at \((-2, 5)\), and the point two thirds of the way along is \(\left(4 - \tfrac{2}{3}(6),\ 1 + \tfrac{2}{3}(4)\right) = \left(0,\ \tfrac{11}{3}\right)\), exactly the \(X\) found.
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