Step 1: Analyzing (S1).
Consider the equation \( \frac{z - i}{z + i} \) being purely real.
This means the imaginary part of \( \frac{z - i}{z + i} \) must be zero.
We know that if \( z = x + iy \), then for this fraction to be real, we have the condition that the imaginary part of the quotient vanishes. Using algebra, we can rewrite the equation in terms of real and imaginary parts and find that there are exactly two solutions that satisfy the condition \( |z| = 1 \).
Hence, \( \{ z \in \mathbb{C} - \{-i\} : |z| = 1 \text{ and } \frac{z - i}{z + i} \text{ is purely real} \} \) contains exactly two elements, so statement (S1) is correct.
Step 2: Analyzing (S2).
Consider the equation \( \frac{z - 1}{z + 1} \) being purely imaginary.
This means the real part of \( \frac{z - 1}{z + 1} \) must be zero. Again, using algebra, we find that there are infinitely many solutions to this equation when \( |z| = 1 \), as there are infinitely many points on the unit circle where the real part of the quotient vanishes.
Therefore, statement (S2) is also correct.
Step 3: Conclusion.
Thus, the correct answer is: \[ \text{Only (S2) is correct}. \]
Given: \[ S_1 : |z| = 1, \quad \frac{z - i}{z + i} = \frac{\bar{z} + i}{\bar{z} - i} \] \[ \Rightarrow (z - i)(\bar{z} - i) = (z + i)(\bar{z} + i) \] \[ |z|^2 - i(z + \bar{z}) - 1 = |z|^2 + i(z + \bar{z}) - 1 \] \[ i(z + \bar{z}) = 0 \] \[ z + \bar{z} = 2\cos\theta = 0 \Rightarrow \cos\theta = 0 \] \[ z = 0 + 0i, \quad |z| \ne 1 \] Now consider: \[ S_1 : \frac{z - 1}{z + 1} + \frac{\bar{z} - 1}{\bar{z} + 1} = 0 \] \[ (z - 1)(\bar{z} + 1) + (z + 1)(\bar{z} - 1) = 0 \] \[ \Rightarrow |z|^2 + (z - \bar{z}) - 1 + |z|^2 + (\bar{z} - z) - 1 = 0 \] \[ \Rightarrow 2|z|^2 - 2 = 0 \] \[ \boxed{|z|^2 = 1} \]
A thin transparent film with refractive index 1.4 is held on a circular ring of radius 1.8 cm. The fluid in the film evaporates such that transmission through the film at wavelength 560 nm goes to a minimum every 12 seconds. Assuming that the film is flat on its two sides, the rate of evaporation is:

In the first configuration (1) as shown in the figure, four identical charges \( q_0 \) are kept at the corners A, B, C and D of square of side length \( a \). In the second configuration (2), the same charges are shifted to mid points C, E, H, and F of the square. If \( K = \frac{1}{4\pi \epsilon_0} \), the difference between the potential energies of configuration (2) and (1) is given by: