Given that z1=r1(cos⁡θ1+isin⁡θ1)z_1 = r_1(\cos\theta_1 + \mathrm{i}\sin\theta_1) and z2=r2(cos⁡θ2+isin⁡θ2)z_2 = r_2(\cos\theta_2 + \mathrm{i}\sin\theta_2), prove, using a trigonometric method, that z1z2=r1r2[cos⁡(θ1−θ2)+isin⁡(θ1−θ2)]\frac{z_1}{z_2} = \frac{r_1}{r_2}[\cos(\theta_1 - \theta_2) + \mathrm{i}\sin(\theta_1 - \theta_2)]. Hence state arg⁡(z1z2)\arg\left(\frac{z_1}{z_2}\right) in terms of θ1\theta_1 and θ2\theta_2. Let wr=r+iw_r = r + \mathrm{i}, where rr is a real constant, r≥0r \ge 0. Use the method of differences to express ∑r=1n(arg⁡(wr−1)−arg⁡(wr))\sum_{r=1}^{n} (\arg(w_{r-1}) - \arg(w_r)) in the form k−arg⁡(n+i)k - \arg(n + \mathrm{i}), where kk is an exact real constant to be determined. Explain why ∑r=1∞(arg⁡(wr−1)−arg⁡(wr))\sum_{r=1}^{\infty} (\arg(w_{r-1}) - \arg(w_r)) converges and state its limit. Hence, or otherwise, find the exact value of
arg⁡(1+i2+i)3+arg⁡(2+i3+i)3+arg⁡(3+i4+i)3+…\arg\left(\frac{1+\mathrm{i}}{2+\mathrm{i}}\right)^3 + \arg\left(\frac{2+\mathrm{i}}{3+\mathrm{i}}\right)^3 + \arg\left(\frac{3+\mathrm{i}}{4+\mathrm{i}}\right)^3 + \dots

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Worked solution

3(a)

1. Set up the quotient and rationalise the denominator by multiplying the numerator and denominator by the conjugate of $\cos\theta_2 + \mathrm{i}\sin\theta_2$.

z1z2=r1(cos⁡θ1+isin⁡θ1)r2(cos⁡θ2+isin⁡θ2)\frac{z_1}{z_2} = \frac{r_1(\cos\theta_1 + \mathrm{i}\sin\theta_1)}{r_2(\cos\theta_2 + \mathrm{i}\sin\theta_2)}
z1z2=r1r2[(cos⁡θ1+isin⁡θ1)(cos⁡θ2−isin⁡θ2)(cos⁡θ2+isin⁡θ2)(cos⁡θ2−isin⁡θ2)]\frac{z_1}{z_2} = \frac{r_1}{r_2} \left[ \frac{(\cos\theta_1 + \mathrm{i}\sin\theta_1)(\cos\theta_2 - \mathrm{i}\sin\theta_2)}{(\cos\theta_2 + \mathrm{i}\sin\theta_2)(\cos\theta_2 - \mathrm{i}\sin\theta_2)} \right]

2. Expand the numerator and simplify the denominator using the Pythagorean identity.

z1z2=r1r2[(cos⁡θ1cos⁡θ2+sin⁡θ1sin⁡θ2)+i(sin⁡θ1cos⁡θ2−cos⁡θ1sin⁡θ2)cos⁡2θ2+sin⁡2θ2]\frac{z_1}{z_2} = \frac{r_1}{r_2} \left[ \frac{(\cos\theta_1\cos\theta_2 + \sin\theta_1\sin\theta_2) + \mathrm{i}(\sin\theta_1\cos\theta_2 - \cos\theta_1\sin\theta_2)}{\cos^2\theta_2 + \sin^2\theta_2} \right]
Since cos⁡2θ2+sin⁡2θ2=1\cos^2\theta_2 + \sin^2\theta_2 = 1,
z1z2=r1r2[(cos⁡θ1cos⁡θ2+sin⁡θ1sin⁡θ2)+i(sin⁡θ1cos⁡θ2−cos⁡θ1sin⁡θ2)]\frac{z_1}{z_2} = \frac{r_1}{r_2} [(\cos\theta_1\cos\theta_2 + \sin\theta_1\sin\theta_2) + \mathrm{i}(\sin\theta_1\cos\theta_2 - \cos\theta_1\sin\theta_2)]

3. Apply trigonometric compound angle identities to complete the proof.

Using the compound angle identities cos⁡(A−B)=cos⁡Acos⁡B+sin⁡Asin⁡B\cos(A-B) = \cos A\cos B + \sin A\sin B and sin⁡(A−B)=sin⁡Acos⁡B−cos⁡Asin⁡B\sin(A-B) = \sin A\cos B - \cos A\sin B,
z1z2=r1r2[cos⁡(θ1−θ2)+isin⁡(θ1−θ2)](shown)\frac{z_1}{z_2} = \frac{r_1}{r_2} [\cos(\theta_1 - \theta_2) + \mathrm{i}\sin(\theta_1 - \theta_2)] \quad \text{(shown)}

4. State the argument of the quotient.

From the polar form shown above, the argument is the angle of the complex number.
arg⁡(z1z2)=θ1−θ2\arg\left(\frac{z_1}{z_2}\right) = \theta_1 - \theta_2

Answer

arg⁡(z1z2)=θ1−θ2\arg\left(\frac{z_1}{z_2}\right) = \theta_1 - \theta_2

3(b)

1. List the first few terms and the last term of the series to apply the method of differences.

∑r=1n(arg⁡(wr−1)−arg⁡(wr))\sum_{r=1}^{n} (\arg(w_{r-1}) - \arg(w_r))\n=(arg⁡(w0)−arg⁡(w1))= (\arg(w_0) - \arg(w_1))\n=+(arg⁡(w1)−arg⁡(w2))\phantom{= } + (\arg(w_1) - \arg(w_2))\n=+(arg⁡(w2)−arg⁡(w3))\phantom{= } + (\arg(w_2) - \arg(w_3))\n=+…\phantom{= } + \dots\n=+(arg⁡(wn−1)−arg⁡(wn))\phantom{= } + (\arg(w_{n-1}) - \arg(w_n))

2. Cancel out the intermediate terms to simplify the sum.

=arg⁡(w0)−arg⁡(wn)= \arg(w_0) - \arg(w_n)

3. Evaluate the remaining terms using the given definition of $w_r$ to find the constant $k$.

Given wr=r+iw_r = r + \mathrm{i}.\nWhen r=0r = 0, w0=0+i=iw_0 = 0 + \mathrm{i} = \mathrm{i}.\narg⁡(w0)=arg⁡(i)=π2\arg(w_0) = \arg(\mathrm{i}) = \frac{\pi}{2}\nWhen r=nr = n, wn=n+iw_n = n + \mathrm{i}.\nSubstituting these back into the simplified sum:\n∑r=1n(arg⁡(wr−1)−arg⁡(wr))=π2−arg⁡(n+i)\sum_{r=1}^{n} (\arg(w_{r-1}) - \arg(w_r)) = \frac{\pi}{2} - \arg(n + \mathrm{i})\nComparing this to k−arg⁡(n+i)k - \arg(n + \mathrm{i}), we find:\nk=π2k = \frac{\pi}{2}

Answer

π2−arg⁡(n+i)\frac{\pi}{2} - \arg(n + \mathrm{i}), so k=π2k = \frac{\pi}{2}

3(c)

1. Deduce the expression for the partial sum from part (b).

From the method of differences in part (b), the sum telescopes to arg⁡(w0)−arg⁡(wn)\arg(w_0) - \arg(w_n).
Since w0=0+i=iw_0 = 0 + \mathrm{i} = \mathrm{i}, its argument is arg⁡(i)=π2\arg(\mathrm{i}) = \frac{\pi}{2}.
Thus, the partial sum to nn terms is Sn=π2−arg⁡(n+i)S_n = \frac{\pi}{2} - \arg(n+\mathrm{i}).

2. Set up the limit of the partial sum and explain the behaviour of $\arg(n+\mathrm{i})$ as $n \to \infty$.

To find the sum to infinity, we consider lim⁡n→∞Sn=lim⁡n→∞(π2−arg⁡(n+i))\lim_{n \to \infty} S_n = \lim_{n \to \infty} \left( \frac{\pi}{2} - \arg(n+\mathrm{i}) \right).
For n>0n > 0, the complex number n+in+\mathrm{i} is in the first quadrant, so we can express its argument as arg⁡(n+i)=tan⁡−1(1n)\arg(n+\mathrm{i}) = \tan^{-1}\left(\frac{1}{n}\right).
As n→∞n \to \infty, 1n→0\frac{1}{n} \to 0, which means arg⁡(n+i)→tan⁡−1(0)=0\arg(n+\mathrm{i}) \to \tan^{-1}(0) = 0.
Since the limit of the sequence of partial sums exists and is finite, the infinite series converges.

3. State the limit of the infinite series.

Evaluating the limit gives:
lim⁡n→∞Sn=π2−0=π2\lim_{n \to \infty} S_n = \frac{\pi}{2} - 0 = \frac{\pi}{2}

Answer

The series converges because the partial sum approaches a finite limit as n→∞n \to \infty. Its limit is π2\frac{\pi}{2}.

3(d)

1. Express the given series in sigma notation and simplify using properties of arguments.

Let the given sum be SS. We can write SS as:
S=∑r=1∞arg⁡((r+ir+1+i)3)S = \sum_{r=1}^{\infty} \arg\left( \left(\frac{r+\mathrm{i}}{r+1+\mathrm{i}}\right)^3 \right)
Using the property arg⁡(z3)=3arg⁡(z)\arg(z^3) = 3\arg(z) and the result from part (a) that arg⁡(z1z2)=arg⁡(z1)−arg⁡(z2)\arg\left(\frac{z_1}{z_2}\right) = \arg(z_1) - \arg(z_2):
S=3∑r=1∞arg⁡(r+ir+1+i)S = 3 \sum_{r=1}^{\infty} \arg\left( \frac{r+\mathrm{i}}{r+1+\mathrm{i}} \right)
S=3∑r=1∞[arg⁡(r+i)−arg⁡(r+1+i)]S = 3 \sum_{r=1}^{\infty} \left[ \arg(r+\mathrm{i}) - \arg(r+1+\mathrm{i}) \right]
Using the definition wr=r+iw_r = r + \mathrm{i} from part (b):
S=3∑r=1∞[arg⁡(wr)−arg⁡(wr+1)]S = 3 \sum_{r=1}^{\infty} \left[ \arg(w_r) - \arg(w_{r+1}) \right]

2. Use the method of differences to evaluate the infinite sum and apply the limit.

Consider the partial sum for the first nn terms:
∑r=1n[arg⁡(wr)−arg⁡(wr+1)]\sum_{r=1}^{n} \left[ \arg(w_r) - \arg(w_{r+1}) \right]
=(arg⁡(w1)−arg⁡(w2))+(arg⁡(w2)−arg⁡(w3))+⋯+(arg⁡(wn)−arg⁡(wn+1))= (\arg(w_1) - \arg(w_2)) + (\arg(w_2) - \arg(w_3)) + \dots + (\arg(w_n) - \arg(w_{n+1}))
=arg⁡(w1)−arg⁡(wn+1)= \arg(w_1) - \arg(w_{n+1})
Taking the limit as n→∞n \to \infty:
lim⁡n→∞∑r=1n[arg⁡(wr)−arg⁡(wr+1)]=arg⁡(w1)−lim⁡n→∞arg⁡(wn+1)\lim_{n \to \infty} \sum_{r=1}^{n} \left[ \arg(w_r) - \arg(w_{r+1}) \right] = \arg(w_1) - \lim_{n \to \infty} \arg(w_{n+1})
Similar to part (c), as n→∞n \to \infty, wn+1=n+1+i→∞w_{n+1} = n+1+\mathrm{i} \to \infty along the real axis, so lim⁡n→∞arg⁡(wn+1)=0\lim_{n \to \infty} \arg(w_{n+1}) = 0.

3. Substitute the argument of the first term to find the exact value of the series.

We need to evaluate arg⁡(w1)\arg(w_1). Since w1=1+iw_1 = 1+\mathrm{i}, its argument is:
arg⁡(1+i)=π4\arg(1+\mathrm{i}) = \frac{\pi}{4}
Substituting this back into our expression for SS:
S=3(π4−0)=3π4S = 3 \left( \frac{\pi}{4} - 0 \right) = \frac{3\pi}{4}

Answer

3π4\frac{3\pi}{4}

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