证明 eiθ1−eiθ\frac{\text{e}^{\text{i}\theta}}{1 - \text{e}^{\text{i}\theta}} 可以表示为 k(icot⁡θ2−1)k\left(\text{i}\cot\frac{\theta}{2} - 1\right) 的形式,其中 kk 是一个待确定的实常数。 将复数 i\text{i} 表示为三种等价的 reiθr\text{e}^{\text{i}\theta} 形式,其中 r>0r > 0 且 −3π<θ≤3π-3\pi < \theta \le 3\pi。 由此求方程 (ww+1)3−i=0\left(\frac{w}{w+1}\right)^3 - \text{i} = 0 的根,并将你的答案表示为 k(icot⁡ϕ−1)k(\text{i}\cot\phi - 1) 的形式,其中 −π2<ϕ≤π2-\frac{\pi}{2} < \phi \le \frac{\pi}{2}。

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完整解法

6(i)

1. Factor out the half-angle exponential $\text{e}^{\text{i}\frac{\theta}{2}}$ from both the numerator and the denominator.

eiθ1−eiθ=eiθ2⋅eiθ2eiθ2(e−iθ2−eiθ2)\frac{\text{e}^{\text{i}\theta}}{1 - \text{e}^{\text{i}\theta}} = \frac{\text{e}^{\text{i}\frac{\theta}{2}} \cdot \text{e}^{\text{i}\frac{\theta}{2}}}{\text{e}^{\text{i}\frac{\theta}{2}} \left(\text{e}^{-\text{i}\frac{\theta}{2}} - \text{e}^{\text{i}\frac{\theta}{2}}\right)}\n=eiθ2e−iθ2−eiθ2= \frac{\text{e}^{\text{i}\frac{\theta}{2}}}{\text{e}^{-\text{i}\frac{\theta}{2}} - \text{e}^{\text{i}\frac{\theta}{2}}}

2. Apply Euler's formula to convert the exponential terms into trigonometric form.

Numerator:
eiθ2=cos⁡θ2+isin⁡θ2\text{e}^{\text{i}\frac{\theta}{2}} = \cos\frac{\theta}{2} + \text{i}\sin\frac{\theta}{2}
Denominator:
e−iθ2−eiθ2=(cos⁡θ2−isin⁡θ2)−(cos⁡θ2+isin⁡θ2)=−2isin⁡θ2\text{e}^{-\text{i}\frac{\theta}{2}} - \text{e}^{\text{i}\frac{\theta}{2}} = \left(\cos\frac{\theta}{2} - \text{i}\sin\frac{\theta}{2}\right) - \left(\cos\frac{\theta}{2} + \text{i}\sin\frac{\theta}{2}\right) = -2\text{i}\sin\frac{\theta}{2}
Substitute these back into the fraction:
eiθ1−eiθ=cos⁡θ2+isin⁡θ2−2isin⁡θ2\frac{\text{e}^{\text{i}\theta}}{1 - \text{e}^{\text{i}\theta}} = \frac{\cos\frac{\theta}{2} + \text{i}\sin\frac{\theta}{2}}{-2\text{i}\sin\frac{\theta}{2}}

3. Separate the fraction and simplify to obtain the required format and determine $k$.

=cos⁡θ2−2isin⁡θ2+isin⁡θ2−2isin⁡θ2= \frac{\cos\frac{\theta}{2}}{-2\text{i}\sin\frac{\theta}{2}} + \frac{\text{i}\sin\frac{\theta}{2}}{-2\text{i}\sin\frac{\theta}{2}}
Since 1i=−i\frac{1}{\text{i}} = -\text{i} and cos⁡xsin⁡x=cot⁡x\frac{\cos x}{\sin x} = \cot x:
=i2cot⁡θ2−12= \frac{\text{i}}{2}\cot\frac{\theta}{2} - \frac{1}{2}
=12(icot⁡θ2−1)= \frac{1}{2}\left(\text{i}\cot\frac{\theta}{2} - 1\right)
By comparing with the given form k(icot⁡θ2−1)k\left(\text{i}\cot\frac{\theta}{2} - 1\right), we have k=12k = \frac{1}{2}.

答案

k=12k = \frac{1}{2}

6(ii)

1. Determine the modulus and principal argument of $\text{i}$.

r=∣i∣=1r = |\text{i}| = 1
arg⁡(i)=π2\arg(\text{i}) = \frac{\pi}{2}

2. Find all valid arguments within the specified range $-3\pi < \theta \le 3\pi$.

The general argument is θ=π2+2kπ\theta = \frac{\pi}{2} + 2k\pi, where k∈Zk \in \mathbb{Z}.
For k=−1k = -1: θ=π2−2π=−3π2\theta = \frac{\pi}{2} - 2\pi = -\frac{3\pi}{2}
For k=0k = 0: θ=π2\theta = \frac{\pi}{2}
For k=1k = 1: θ=π2+2π=5π2\theta = \frac{\pi}{2} + 2\pi = \frac{5\pi}{2}
(Checking boundaries: −3π<−3π2,π2,5π2≤3π-3\pi < -\frac{3\pi}{2}, \frac{\pi}{2}, \frac{5\pi}{2} \le 3\pi)

3. Write the three equivalent exponential forms.

The three forms reiθr\text{e}^{\text{i}\theta} are:
e−i3π2,eiπ2,ei5π2\text{e}^{-\text{i}\frac{3\pi}{2}}, \text{e}^{\text{i}\frac{\pi}{2}}, \text{e}^{\text{i}\frac{5\pi}{2}}

答案

e−i3π2,eiπ2,ei5π2\text{e}^{-\text{i}\frac{3\pi}{2}}, \text{e}^{\text{i}\frac{\pi}{2}}, \text{e}^{\text{i}\frac{5\pi}{2}}

6(iii)

1. Briefly establish the results from parts (i) and (ii) required to solve the target.

From (i), finding kk:
eiθ1−eiθ=eiθ/2e−iθ/2−eiθ/2=eiθ/2−2isin⁡(θ2)=12(icot⁡θ2−1)\frac{\text{e}^{\text{i}\theta}}{1 - \text{e}^{\text{i}\theta}} = \frac{\text{e}^{\text{i}\theta/2}}{\text{e}^{-\text{i}\theta/2} - \text{e}^{\text{i}\theta/2}} = \frac{\text{e}^{\text{i}\theta/2}}{-2\text{i}\sin(\frac{\theta}{2})} = \frac{1}{2}\left(\text{i}\cot\frac{\theta}{2} - 1\right)
Thus, k=12k = \frac{1}{2}.

From (ii), expressing i\text{i} in reiθr\text{e}^{\text{i}\theta} form within −3π<θ≤3π-3\pi < \theta \le 3\pi:
i=e−i3π2,eiπ2,ei5π2\text{i} = \text{e}^{-\text{i}\frac{3\pi}{2}}, \text{e}^{\text{i}\frac{\pi}{2}}, \text{e}^{\text{i}\frac{5\pi}{2}}

2. Take the cube root of both sides to find the possible expressions for the base.

Given the equation:
(ww+1)3=i\left(\frac{w}{w+1}\right)^3 = \text{i}

Taking the cube root using the three forms of i\text{i} from (ii):
ww+1=eiθ\frac{w}{w+1} = \text{e}^{\text{i}\theta}
where θ=13(−3π2),13(π2),13(5π2)\theta = \frac{1}{3}\left(-\frac{3\pi}{2}\right), \frac{1}{3}\left(\frac{\pi}{2}\right), \frac{1}{3}\left(\frac{5\pi}{2}\right)
So θ=−π2,π6,5π6\theta = -\frac{\pi}{2}, \frac{\pi}{6}, \frac{5\pi}{6}

3. Solve for w algebraically.

w=weiθ+eiθw = w\text{e}^{\text{i}\theta} + \text{e}^{\text{i}\theta}
w(1−eiθ)=eiθw(1 - \text{e}^{\text{i}\theta}) = \text{e}^{\text{i}\theta}
w=eiθ1−eiθw = \frac{\text{e}^{\text{i}\theta}}{1 - \text{e}^{\text{i}\theta}}

Using the identity proven in part (i), we can rewrite this as:
w=12(icot⁡θ2−1)w = \frac{1}{2}\left(\text{i}\cot\frac{\theta}{2} - 1\right)

4. Substitute the angles into the expression to find the final roots and check the domain of phi.

Letting ϕ=θ2\phi = \frac{\theta}{2}:
For θ=−π2\theta = -\frac{\pi}{2}, ϕ=−π4\phi = -\frac{\pi}{4}, so w=12(icot⁡(−π4)−1)w = \frac{1}{2}\left(\text{i}\cot\left(-\frac{\pi}{4}\right) - 1\right)
For θ=π6\theta = \frac{\pi}{6}, ϕ=π12\phi = \frac{\pi}{12}, so w=12(icot⁡(π12)−1)w = \frac{1}{2}\left(\text{i}\cot\left(\frac{\pi}{12}\right) - 1\right)
For θ=5π6\theta = \frac{5\pi}{6}, ϕ=5π12\phi = \frac{5\pi}{12}, so w=12(icot⁡(5π12)−1)w = \frac{1}{2}\left(\text{i}\cot\left(\frac{5\pi}{12}\right) - 1\right)

All ϕ\phi values {−π4,π12,5π12}\left\{-\frac{\pi}{4}, \frac{\pi}{12}, \frac{5\pi}{12}\right\} strictly satisfy −π2<ϕ≤π2-\frac{\pi}{2} < \phi \le \frac{\pi}{2}.

答案

12(icot⁡(−π4)−1)\frac{1}{2}\left(\text{i}\cot\left(-\frac{\pi}{4}\right) - 1\right), 12(icot⁡(π12)−1)\frac{1}{2}\left(\text{i}\cot\left(\frac{\pi}{12}\right) - 1\right), 12(icot⁡(5π12)−1)\frac{1}{2}\left(\text{i}\cot\left(\frac{5\pi}{12}\right) - 1\right)

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