To solve the given problem, we start by examining the equation:
\(\frac{|z_1 - 2z_2|}{\left| \frac{1}{2} - z_1 \overline{z_2} \right|} = 2\)
This equation essentially represents a condition involving the distances between two points on the complex plane.
First, let's simplify the equation:
\(|z_1 - 2z_2| = 2 \left| \frac{1}{2} - z_1 \overline{z_2} \right|\)
Consider \(|z_1 - 2z_2|\)as the distance from \(z_1\) to \(2z_2\):
- If we assume that \(z_1\) lies on a circle of radius 1, then we have:
\(|z_1| = 1 \ \text{or} \ |z_2 - 0| = \frac{1}{2}\)
Similarly, consider the absolute value:
\(\left| \frac{1}{2} - z_1 \overline{z_2} \right|\)represents the modulus of a complex number.
- If we assume \(z_2\) lies on a circle of radius \(\frac{1}{2}\), this satisfies the equation provided since both sides could balance out to remain equal.
Therefore, the correct interpretation is that either:
Conclusion: The correct answer is that either \(z_1\) lies on a circle of radius 1 or \(z_2\) lies on a circle of radius \(\frac{1}{2}\).
\[ \frac{z_1 - 2z_2}{\frac{1}{2} - 2z_1z_2} \times \frac{\overline{z_1} - 2\overline{z_2}}{\frac{1}{2} - z_1z_2} = 4 \]
\[ \lvert z_1 \rvert^2 \left\lvert 2z_1z_2 - 2z_2\overline{z_1} + 4\lvert z_2 \rvert^2 \right\rvert^2 \]
\[ = 4 \left( \frac{1}{4}(z_1\overline{z_2} - z_2\overline{z_1})^2 + \lvert z_1 \rvert^2 \lvert z_2 \rvert^2 \right) \]
\[ z_1\overline{z_1} + 2z_2 \cdot 2\overline{z_2} - z_1z_2 \cdot z_2\overline{z_2} - 1 = 0 \]
\[ (z_1\overline{z_1} - 1)(1 - 2z_2\overline{z_2}) = 0 \]
\[ (\lvert z_1 \rvert^2 - 1)\left((2\lvert z_2 \rvert^2 - 1)\right) = 0 \]
If \( z \) is a complex number and \( k \in \mathbb{R} \), such that \( |z| = 1 \), \[ \frac{2 + k^2 z}{k + \overline{z}} = kz, \] then the maximum distance from \( k + i k^2 \) to the circle \( |z - (1 + 2i)| = 1 \) is:
Consider the following sequence of reactions : 
Molar mass of the product formed (A) is ______ g mol\(^{-1}\).
In a Young's double slit experiment, three polarizers are kept as shown in the figure. The transmission axes of \( P_1 \) and \( P_2 \) are orthogonal to each other. The polarizer \( P_3 \) covers both the slits with its transmission axis at \( 45^\circ \) to those of \( P_1 \) and \( P_2 \). An unpolarized light of wavelength \( \lambda \) and intensity \( I_0 \) is incident on \( P_1 \) and \( P_2 \). The intensity at a point after \( P_3 \), where the path difference between the light waves from \( S_1 \) and \( S_2 \) is \( \frac{\lambda}{3} \), is:
