The vectors a\mathbf{a} and b\mathbf{b} are given by a=i+(sin⁡θ)j+(cos⁡θ)kandb=i+(sin⁡ϕ)j+(cos⁡ϕ)k, where 0≤θ≤ϕ≤π.\mathbf{a} = \mathbf{i} + (\sin\theta)\mathbf{j} + (\cos\theta)\mathbf{k} \quad \text{and} \quad \mathbf{b} = \mathbf{i} + (\sin\phi)\mathbf{j} + (\cos\phi)\mathbf{k} \text{, where } 0 \le \theta \le \phi \le \pi .

  1. (a)

    Find an expression for ∣a×b∣|\mathbf{a} \times \mathbf{b}| in terms of δ\delta, where δ=12(ϕ−θ)\delta = \frac{1}{2}(\phi - \theta).

  2. (b)

    Deduce that the angle α\alpha between a\mathbf{a} and b\mathbf{b} is given by sin⁡α=sin⁡δ1+cos⁡2δ\sin\alpha = \sin\delta \sqrt{1 + \cos^2\delta}.

Work through it with AI →

It won't just hand you the answer — it asks where you're stuck.How the checker works

Worked solution

2(a)

1. Compute the cross product of vectors $\mathbf{a}$ and $\mathbf{b}$ and simplify the x-component.

a×b=(1sin⁡θcos⁡θ)×(1sin⁡ϕcos⁡ϕ)\mathbf{a} \times \mathbf{b} = \begin{pmatrix} 1 \\ \sin\theta \\ \cos\theta \end{pmatrix} \times \begin{pmatrix} 1 \\ \sin\phi \\ \cos\phi \end{pmatrix}
=(sin⁡θcos⁡ϕ−cos⁡θsin⁡ϕcos⁡θ(1)−cos⁡ϕ(1)1(sin⁡ϕ)−1(sin⁡θ))= \begin{pmatrix} \sin\theta\cos\phi - \cos\theta\sin\phi \\ \cos\theta(1) - \cos\phi(1) \\ 1(\sin\phi) - 1(\sin\theta) \end{pmatrix}
=(sin⁡(θ−ϕ)cos⁡θ−cos⁡ϕsin⁡ϕ−sin⁡θ)= \begin{pmatrix} \sin(\theta - \phi) \\ \cos\theta - \cos\phi \\ \sin\phi - \sin\theta \end{pmatrix}

2. Set up the equation for the square of the magnitude and expand the terms.

∣a×b∣2=sin⁡2(θ−ϕ)+(cos⁡θ−cos⁡ϕ)2+(sin⁡ϕ−sin⁡θ)2|\mathbf{a} \times \mathbf{b}|^2 = \sin^2(\theta - \phi) + (\cos\theta - \cos\phi)^2 + (\sin\phi - \sin\theta)^2
=sin⁡2(θ−ϕ)+cos⁡2θ−2cos⁡θcos⁡ϕ+cos⁡2ϕ+sin⁡2ϕ−2sin⁡θsin⁡ϕ+sin⁡2θ= \sin^2(\theta - \phi) + \cos^2\theta - 2\cos\theta\cos\phi + \cos^2\phi + \sin^2\phi - 2\sin\theta\sin\phi + \sin^2\theta

3. Group terms and apply Pythagorean and compound angle identities to simplify the expression.

Grouping the terms:
∣a×b∣2=sin⁡2(θ−ϕ)+(cos⁡2θ+sin⁡2θ)+(cos⁡2ϕ+sin⁡2ϕ)−2(cos⁡θcos⁡ϕ+sin⁡θsin⁡ϕ)|\mathbf{a} \times \mathbf{b}|^2 = \sin^2(\theta - \phi) + (\cos^2\theta + \sin^2\theta) + (\cos^2\phi + \sin^2\phi) - 2(\cos\theta\cos\phi + \sin\theta\sin\phi)
Using cos⁡2x+sin⁡2x=1\cos^2 x + \sin^2 x = 1 and the cosine difference identity cos⁡(θ−ϕ)=cos⁡θcos⁡ϕ+sin⁡θsin⁡ϕ\cos(\theta - \phi) = \cos\theta\cos\phi + \sin\theta\sin\phi:
∣a×b∣2=sin⁡2(θ−ϕ)+1+1−2cos⁡(θ−ϕ)|\mathbf{a} \times \mathbf{b}|^2 = \sin^2(\theta - \phi) + 1 + 1 - 2\cos(\theta - \phi)
Since sin⁡2(θ−ϕ)=sin⁡2(ϕ−θ)\sin^2(\theta - \phi) = \sin^2(\phi - \theta) and cos⁡(θ−ϕ)=cos⁡(ϕ−θ)\cos(\theta - \phi) = \cos(\phi - \theta):
∣a×b∣2=sin⁡2(ϕ−θ)+2−2cos⁡(ϕ−θ)|\mathbf{a} \times \mathbf{b}|^2 = \sin^2(\phi - \theta) + 2 - 2\cos(\phi - \theta)

4. Substitute $\delta = \frac{1}{2}(\phi - \theta)$ and factorise the expression completely using double-angle identities.

Given δ=12(ϕ−θ)\delta = \frac{1}{2}(\phi - \theta), we have ϕ−θ=2δ\phi - \theta = 2\delta. Substituting this in:
∣a×b∣2=sin⁡2(2δ)+2−2cos⁡(2δ)|\mathbf{a} \times \mathbf{b}|^2 = \sin^2(2\delta) + 2 - 2\cos(2\delta)
Using the double-angle identities sin⁡(2δ)=2sin⁡δcos⁡δ\sin(2\delta) = 2\sin\delta\cos\delta and cos⁡(2δ)=1−2sin⁡2δ\cos(2\delta) = 1 - 2\sin^2\delta:
∣a×b∣2=(2sin⁡δcos⁡δ)2+2−2(1−2sin⁡2δ)|\mathbf{a} \times \mathbf{b}|^2 = (2\sin\delta\cos\delta)^2 + 2 - 2(1 - 2\sin^2\delta)
=4sin⁡2δcos⁡2δ+4sin⁡2δ= 4\sin^2\delta\cos^2\delta + 4\sin^2\delta
=4sin⁡2δ(cos⁡2δ+1)= 4\sin^2\delta (\cos^2\delta + 1)

5. Take the positive square root and justify the sign of $\sin\delta$ based on the given angle range.

Taking the square root gives:
∣a×b∣=2∣sin⁡δ∣1+cos⁡2δ|\mathbf{a} \times \mathbf{b}| = 2|\sin\delta| \sqrt{1 + \cos^2\delta}
We are given 0≤θ≤ϕ≤π0 \le \theta \le \phi \le \pi, which means 0≤ϕ−θ≤π0 \le \phi - \theta \le \pi.
Since δ=12(ϕ−θ)\delta = \frac{1}{2}(\phi - \theta), it follows that 0≤δ≤π20 \le \delta \le \frac{\pi}{2}.
In this principal range, sin⁡δ≥0\sin\delta \ge 0, so ∣sin⁡δ∣=sin⁡δ|\sin\delta| = \sin\delta.
∴∣a×b∣=2sin⁡δ1+cos⁡2δ\therefore |\mathbf{a} \times \mathbf{b}| = 2\sin\delta \sqrt{1 + \cos^2\delta}

Answer

2sin⁡δ1+cos⁡2δ2\sin\delta \sqrt{1 + \cos^2\delta}

2(b)

1. Concisely re-derive the expression for $|\mathbf{a} \times \mathbf{b}|$ from part (a).

From part (a), we first determine ∣a×b∣.\text{From part (a), we first determine } |\mathbf{a} \times \mathbf{b}|.
a×b=(1sin⁡θcos⁡θ)×(1sin⁡ϕcos⁡ϕ)=(sin⁡θcos⁡ϕ−cos⁡θsin⁡ϕcos⁡ϕ−cos⁡θsin⁡ϕ−sin⁡θ)\mathbf{a} \times \mathbf{b} = \begin{pmatrix} 1 \\ \sin\theta \\ \cos\theta \end{pmatrix} \times \begin{pmatrix} 1 \\ \sin\phi \\ \cos\phi \end{pmatrix} = \begin{pmatrix} \sin\theta\cos\phi - \cos\theta\sin\phi \\ \cos\phi - \cos\theta \\ \sin\phi - \sin\theta \end{pmatrix}
Using trigonometric factor formulae and ϕ−θ=2δ:\text{Using trigonometric factor formulae and } \phi - \theta = 2\delta:
a×b=(−sin⁡(2δ)−2sin⁡(ϕ+θ2)sin⁡δ2cos⁡(ϕ+θ2)sin⁡δ)\mathbf{a} \times \mathbf{b} = \begin{pmatrix} -\sin(2\delta) \\ -2\sin\left(\frac{\phi+\theta}{2}\right)\sin\delta \\ 2\cos\left(\frac{\phi+\theta}{2}\right)\sin\delta \end{pmatrix}
∣a×b∣2=sin⁡2(2δ)+4sin⁡2δ(sin⁡2(ϕ+θ2)+cos⁡2(ϕ+θ2))|\mathbf{a} \times \mathbf{b}|^2 = \sin^2(2\delta) + 4\sin^2\delta\left(\sin^2\left(\frac{\phi+\theta}{2}\right) + \cos^2\left(\frac{\phi+\theta}{2}\right)\right)
∣a×b∣2=(2sin⁡δcos⁡δ)2+4sin⁡2δ(1)=4sin⁡2δ(1+cos⁡2δ)|\mathbf{a} \times \mathbf{b}|^2 = (2\sin\delta\cos\delta)^2 + 4\sin^2\delta(1) = 4\sin^2\delta(1+\cos^2\delta)
∣a×b∣=2sin⁡δ1+cos⁡2δ|\mathbf{a} \times \mathbf{b}| = 2\sin\delta\sqrt{1+\cos^2\delta}

2. Calculate the magnitudes of vectors $\mathbf{a}$ and $\mathbf{b}$.

∣a∣=12+sin⁡2θ+cos⁡2θ=1+1=2|\mathbf{a}| = \sqrt{1^2 + \sin^2\theta + \cos^2\theta} = \sqrt{1 + 1} = \sqrt{2}
∣b∣=12+sin⁡2ϕ+cos⁡2ϕ=1+1=2|\mathbf{b}| = \sqrt{1^2 + \sin^2\phi + \cos^2\phi} = \sqrt{1 + 1} = \sqrt{2}

3. Relate the cross product magnitude to the angle $\alpha$ to deduce the given expression.

By definition, ∣a×b∣=∣a∣∣b∣sin⁡α.\text{By definition, } |\mathbf{a} \times \mathbf{b}| = |\mathbf{a}||\mathbf{b}|\sin\alpha.
Substitute the values obtained:\text{Substitute the values obtained:}
2sin⁡δ1+cos⁡2δ=(2)(2)sin⁡α2\sin\delta\sqrt{1+\cos^2\delta} = (\sqrt{2})(\sqrt{2})\sin\alpha
2sin⁡δ1+cos⁡2δ=2sin⁡α2\sin\delta\sqrt{1+\cos^2\delta} = 2\sin\alpha
sin⁡α=sin⁡δ1+cos⁡2δ(shown)\sin\alpha = \sin\delta\sqrt{1+\cos^2\delta} \quad \text{(shown)}

Answer

sin⁡α=sin⁡δ1+cos⁡2δ\sin\alpha = \sin\delta \sqrt{1 + \cos^2\delta}

AI analysis — may contain mistakes.

Worked this one out on paper? Snap your steps and Gigle's AI math checker will circle the step where it went wrong.

More questions on this topic

  1. 1The lines l1l_1 and l2l_2 have equations r=(4110)+λ(1−1−6),λ∈R\mathbf{r} = \begin{pmatrix} 4 \\ 1 \\ 10 \end{pmatrix} + \lambda \begin{pmatrix} 1 \\ -1 \\ -6 \end{pmatrix}, \lambda \in \mathbb{R}…
  2. 2The vectors a\mathbf{a} and b\mathbf{b} are given by a=i+(sin⁡θ)j+(cos⁡θ)k\mathbf{a}=\mathbf{i}+(\sin\theta)\mathbf{j}+(\cos\theta)\mathbf{k}\quad…
  3. 3With reference to the origin OO, the points AA, PP and QQ have position vectors a\mathbf{a}, p\mathbf{p} and q\mathbf{q}…
  4. 4A plane Π1\Pi_1 has equation x+y+z=3x + y + z = 3. A line passes through the points PP and QQ with position vectors i+j+2k\mathbf{i} + \mathbf{j} + 2\mathbf{k}…
  5. 5The planes Π1\Pi_1 and Π2\Pi_2 have vector equations r=λ1(i+j−k)+μ1(2i−j+k)andr=λ2(i+2j+k)+μ2(3i+j−k)\mathbf{r} = \lambda_1(\mathbf{i} + \mathbf{j} - \mathbf{k}) + \mu_1(2\mathbf{i} - \mathbf{j} + \mathbf{k}) \quad \text{and} \quad \mathbf{r} = \lambda_2(\mathbf{i} + 2\mathbf{j} + \mathbf{k}) + \mu_2(3\mathbf{i} + \mathbf{j} - \mathbf{k})…