向量 a\mathbf{a} 和 b\mathbf{b} 分别由下式给出: a=i+(sin⁡θ)j+(cos⁡θ)k且b=i+(sin⁡ϕ)j+(cos⁡ϕ)k,其中 0≤θ≤ϕ≤π.\mathbf{a} = \mathbf{i} + (\sin\theta)\mathbf{j} + (\cos\theta)\mathbf{k} \quad \text{且} \quad \mathbf{b} = \mathbf{i} + (\sin\phi)\mathbf{j} + (\cos\phi)\mathbf{k} \text{,其中 } 0 \le \theta \le \phi \le \pi .

  1. (a)

    用 δ\delta 的表达式表示 ∣a×b∣|\mathbf{a} \times \mathbf{b}|,其中 δ=12(ϕ−θ)\delta = \frac{1}{2}(\phi - \theta)。

  2. (b)

    由此推导,a\mathbf{a} 和 b\mathbf{b} 之间的夹角 α\alpha 满足 sin⁡α=sin⁡δ1+cos⁡2δ\sin\alpha = \sin\delta \sqrt{1 + \cos^2\delta}。

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完整解法

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}

答案

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)}

答案

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

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