· H2 Mathematics — Ten-Year Series, worked ← All 11 questions

2018 A-Level · Paper 1 · Question 6

2018 H2 Maths Paper 1, Question 6

Vectors 7 marks vector product
Download Paper 1 solutions (PDF)

Part (i)

2 marks

Since a×3b=2a×c\mathbf{a} \times 3\mathbf{b} = 2\mathbf{a} \times \mathbf{c},

3(a×b)=2(a×c)3\left( \mathbf{a} \times \mathbf{b} \right) = 2\left( \mathbf{a} \times \mathbf{c} \right)
3(a×b)−2(a×c)=03\left( \mathbf{a} \times \mathbf{b} \right) - 2\left( \mathbf{a} \times \mathbf{c} \right) = \mathbf{0}
a×(3b−2c)=0.\mathbf{a} \times \left( 3\mathbf{b} - 2\mathbf{c} \right) = \mathbf{0}.

Since a≠0\mathbf{a} \neq \mathbf{0}, a vector cross product a×v=0\mathbf{a} \times \mathbf{v} = \mathbf{0} means v\mathbf{v} is parallel to a\mathbf{a} (or v=0\mathbf{v} = \mathbf{0}, the degenerate case of parallel). So 3b−2c3\mathbf{b} - 2\mathbf{c} is parallel to a\mathbf{a}, i.e.

3b−2c=λa3\mathbf{b} - 2\mathbf{c} = \lambda\mathbf{a}

for some constant λ\lambda.  (shown)

Part (ii)

5 marks

Approach

We are given magnitudes and an angle, which is scalar-product information, so we turn the vector equation from (i) into a scalar one by taking the modulus of both sides and squaring — this brings in ∣b∣\left| \mathbf{b} \right|, ∣c∣\left| \mathbf{c} \right| and b⋅c\mathbf{b} \cdot \mathbf{c}, all of which we know, and ∣a∣=1\left| \mathbf{a} \right| = 1.

Since a\mathbf{a} and c\mathbf{c} are unit vectors, ∣a∣=1\left| \mathbf{a} \right| = 1 and ∣c∣=1\left| \mathbf{c} \right| = 1; also ∣b∣=4\left| \mathbf{b} \right| = 4 and the angle between b\mathbf{b} and c\mathbf{c} is 60∘60^{\circ}, so

b⋅c=∣b∣∣c∣cos⁡60∘=4(1)(12)=2.\mathbf{b} \cdot \mathbf{c} = \left| \mathbf{b} \right|\left| \mathbf{c} \right|\cos 60^{\circ} = 4(1)\left( \frac{1}{2} \right) = 2.

Taking the modulus squared of both sides of 3b−2c=λa3\mathbf{b} - 2\mathbf{c} = \lambda\mathbf{a},

∣3b−2c∣2=λ2∣a∣2\left| 3\mathbf{b} - 2\mathbf{c} \right|^{2} = \lambda^{2}\left| \mathbf{a} \right|^{2}
(3b−2c)⋅(3b−2c)=λ2\left( 3\mathbf{b} - 2\mathbf{c} \right) \cdot \left( 3\mathbf{b} - 2\mathbf{c} \right) = \lambda^{2}
9∣b∣2−12(b⋅c)+4∣c∣2=λ29\left| \mathbf{b} \right|^{2} - 12\left( \mathbf{b} \cdot \mathbf{c} \right) + 4\left| \mathbf{c} \right|^{2} = \lambda^{2}
9(16)−12(2)+4(1)=λ29(16) - 12(2) + 4(1) = \lambda^{2}
124=λ2.124 = \lambda^{2}.

Solving,

λ=±124=±231.\lambda = \pm \sqrt{124} = \pm 2\sqrt{31}.

∴λ=231\therefore\lambda = 2\sqrt{31} or λ=−231\lambda = - 2\sqrt{31}.

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