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2023 A-Level · Paper 1 · Question 3

2023 H2 Maths Paper 1, Question 3

Vectors 6 marks Scalar and Vector Products
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Part (a)

3 marks

Approach

We let c=a×b\mathbf{c} = \mathbf{a} \times \mathbf{b} and use the fact that c\mathbf{c} is perpendicular to both a\mathbf{a} and b\mathbf{b}, together with the given perpendicularity condition written as a dot product equal to zero.

Since c=a×b\mathbf{c} = \mathbf{a} \times \mathbf{b} is perpendicular to both a\mathbf{a} and b\mathbf{b}:

c⋅a=0,c⋅b=0\mathbf{c} \cdot \mathbf{a} = 0,\quad\mathbf{c} \cdot \mathbf{b} = 0

Since (a×b+a)\left( \mathbf{a} \times \mathbf{b} + \mathbf{a} \right) is perpendicular to (a×b+b)\left( \mathbf{a} \times \mathbf{b} + \mathbf{b} \right):

(c+a)⋅(c+b)=0\left( \mathbf{c} + \mathbf{a} \right) \cdot \left( \mathbf{c} + \mathbf{b} \right) = 0
⇒c⋅c+c⋅b+a⋅c+a⋅b=0\Rightarrow \mathbf{c} \cdot \mathbf{c} + \mathbf{c} \cdot \mathbf{b} + \mathbf{a} \cdot \mathbf{c} + \mathbf{a} \cdot \mathbf{b} = 0

Substituting c⋅b=0\mathbf{c} \cdot \mathbf{b} = 0 and a⋅c=0\mathbf{a} \cdot \mathbf{c} = 0:

⇒∣c∣2+a⋅b=0\Rightarrow \left| \mathbf{c} \right|^{2} + \mathbf{a} \cdot \mathbf{b} = 0

Rearranging, and using a⋅b=−1\mathbf{a} \cdot \mathbf{b} = - 1:

∣a×b∣2=−a⋅b\left| \mathbf{a} \times \mathbf{b} \right|^{2} = - \mathbf{a} \cdot \mathbf{b}
=−(−1)= - ( - 1)
=1= 1
To check your answer: ∣a×b∣2=1≥0\left| \mathbf{a} \times \mathbf{b} \right|^{2} = 1 \geq 0, consistent with a magnitude squared, and the derivation used only a×b⊥a\mathbf{a} \times \mathbf{b}\bot\mathbf{a} and a×b⊥b\mathbf{a} \times \mathbf{b}\bot\mathbf{b}, which hold for any vectors a,b\mathbf{a},\mathbf{b} ✓

Since ∣a×b∣2=1\left| \mathbf{a} \times \mathbf{b} \right|^{2} = 1 and ∣a×b∣≥0\left| \mathbf{a} \times \mathbf{b} \right| \geq 0:

∴\therefore ∣a×b∣=1\left| \mathbf{a} \times \mathbf{b} \right| = 1 (shown).

Part (b)

3 marks

Let θ\theta be the angle between the directions of a\mathbf{a} and b\mathbf{b}, so 0∘≤θ≤180∘0^{\circ} \leq \theta \leq 180^{\circ}. Using the standard results a⋅b=∣a∣∣b∣cos⁡θ\mathbf{a} \cdot \mathbf{b} = \left| \mathbf{a} \right|\left| \mathbf{b} \right|\cos\theta and ∣a×b∣=∣a∣∣b∣sin⁡θ\left| \mathbf{a} \times \mathbf{b} \right| = \left| \mathbf{a} \right|\left| \mathbf{b} \right|\sin\theta, dividing eliminates the factor ∣a∣∣b∣\left| \mathbf{a} \right|\left| \mathbf{b} \right|, so the magnitudes of a\mathbf{a} and b\mathbf{b} are never needed:

tan⁡θ=∣a×b∣a⋅b\tan\theta = \frac{\left| \mathbf{a} \times \mathbf{b} \right|}{\mathbf{a} \cdot \mathbf{b}}
=1−1= \frac{1}{- 1}
=−1= - 1
To check your answer: since 0∘≤θ≤180∘0^{\circ} \leq \theta \leq 180^{\circ}, sin⁡θ≥0\sin\theta \geq 0 always; here a⋅b<0\mathbf{a} \cdot \mathbf{b} < 0 so cos⁡θ<0\cos\theta < 0, meaning θ\theta is obtuse — consistent with the second-quadrant solution below ✓

Since tan⁡θ=−1\tan\theta = - 1 with θ\theta obtuse:

∴\therefore θ=135∘\theta = 135^{\circ}.

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