Given that z=λ−4i1−λiz = \dfrac{\lambda - 4i}{1 - \lambda i}, λ∈R\lambda \in \mathbb{R} and arg⁡(z)=π\arg(z) = \pi, find the value of zz. Do not use a calculator in answering this question. The complex numbers zz and ww are given by z=1+i1−iz = \dfrac{1 + i}{1 - i} and w=21+iw = \dfrac{\sqrt{2}}{1 + i}. Express zz and ww in exact polar form reiθre^{i\theta} where r>0r > 0 and −π<θ≤π-\pi < \theta \le \pi.

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Worked solution

b(a)

1. Express $z$ in Cartesian form by multiplying the numerator and denominator by the conjugate of the denominator.

z=λ−4i1−λi×1+λi1+λiz = \frac{\lambda - 4i}{1 - \lambda i} \times \frac{1 + \lambda i}{1 + \lambda i}
z=λ+λ2i−4i−4λi212+λ2z = \frac{\lambda + \lambda^2 i - 4i - 4\lambda i^2}{1^2 + \lambda^2}
z=5λ+(λ2−4)i1+λ2z = \frac{5\lambda + (\lambda^2 - 4)i}{1 + \lambda^2}

2. Identify the conditions for the real and imaginary parts given that the argument of $z$ is $\pi$.

Since arg⁡(z)=π\arg(z) = \pi, zz must lie on the negative real axis.
Therefore, the imaginary part must be 00 and the real part must be strictly negative (Im(z)=0\text{Im}(z) = 0, Re(z)<0\text{Re}(z) < 0).

3. Equate the imaginary part to zero to find the possible values of $\lambda$.

λ2−41+λ2=0\frac{\lambda^2 - 4}{1 + \lambda^2} = 0
λ2−4=0\lambda^2 - 4 = 0
λ=2orλ=−2\lambda = 2 \quad \text{or} \quad \lambda = -2

4. Test the possible values of $\lambda$ against the real part condition to find the correct value of $z$.

When λ=2\lambda = 2:
Re(z)=5(2)1+22=105=2\text{Re}(z) = \frac{5(2)}{1 + 2^2} = \frac{10}{5} = 2
Since Re(z)>0\text{Re}(z) > 0, arg⁡(z)=0≠π\arg(z) = 0 \neq \pi, so we reject λ=2\lambda = 2.

When λ=−2\lambda = -2:
Re(z)=5(−2)1+(−2)2=−105=−2\text{Re}(z) = \frac{5(-2)}{1 + (-2)^2} = \frac{-10}{5} = -2
Since Re(z)<0\text{Re}(z) < 0 and Im(z)=0\text{Im}(z) = 0, arg⁡(z)=π\arg(z) = \pi.
Thus, the correct value is z=−2z = -2.

Answer

−2-2

b(b)(i)

1. Simplify $z$ into Cartesian form and convert it to polar form.

z=1+i1−i×1+i1+iz = \frac{1 + i}{1 - i} \times \frac{1 + i}{1 + i}
z=1+2i+i212+12=1+2i−12=2i2=iz = \frac{1 + 2i + i^2}{1^2 + 1^2} = \frac{1 + 2i - 1}{2} = \frac{2i}{2} = i
For z=0+1iz = 0 + 1i:
Modulus ∣z∣=02+12=1|z| = \sqrt{0^2 + 1^2} = 1
Argument arg⁡(z)=π2\arg(z) = \frac{\pi}{2} (since it lies on the positive imaginary axis)
Therefore, in polar form, z=1eiπ2=eiπ2z = 1e^{i\frac{\pi}{2}} = e^{i\frac{\pi}{2}}.

2. Simplify $w$ into Cartesian form and convert it to polar form.

w=21+i×1−i1−iw = \frac{\sqrt{2}}{1 + i} \times \frac{1 - i}{1 - i}
w=2(1−i)12+12=22−i22w = \frac{\sqrt{2}(1 - i)}{1^2 + 1^2} = \frac{\sqrt{2}}{2} - i\frac{\sqrt{2}}{2}
For ww:
Modulus ∣w∣=(22)2+(−22)2=24+24=1=1|w| = \sqrt{\left(\frac{\sqrt{2}}{2}\right)^2 + \left(-\frac{\sqrt{2}}{2}\right)^2} = \sqrt{\frac{2}{4} + \frac{2}{4}} = \sqrt{1} = 1
Argument arg⁡(w)=tan⁡−1(−2/22/2)=tan⁡−1(−1)=−π4\arg(w) = \tan^{-1}\left(\frac{-\sqrt{2}/2}{\sqrt{2}/2}\right) = \tan^{-1}(-1) = -\frac{\pi}{4} (since it lies in the 4th quadrant)
Therefore, in polar form, w=1e−iπ4=e−iπ4w = 1e^{-i\frac{\pi}{4}} = e^{-i\frac{\pi}{4}}.

Answer

z=eiπ2z = e^{i\frac{\pi}{2}}, w=e−iπ4w = e^{-i\frac{\pi}{4}}

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