To solve this complex number problem, we need to find the locus of the complex number \( z \) such that:
\(\text{Re} \left( \frac{z - 1}{2z + i} \right) + \text{Re} \left( \frac{ \bar{z} - 1}{2 \bar{z} - i} \right) = 2.\)
Let's break this down step-by-step. Given that \( z \) is a complex number, we assume \( z = x + yi \) where \( x, y \) are real numbers. The conjugate \( \bar{z} = x - yi \).
First, calculate:
Perform similar calculations for these terms and use the symmetry that will help to simplify it.
When you add the two real parts for given expression, due to the calculated symmetry:
This simplifies to: \(x - 1 = 5 \quad \rightarrow \quad x = 6\).
The solution indicates a circle equation centered at point \((x, y)\) with known conditions, indicating:
Finally, compute:
\(\frac{15ab}{r^2} = \frac{15 \times \frac{5}{2} \times 0}{2} = 18\)
Thus, the correct solution is 18.
A substance 'X' (1.5 g) dissolved in 150 g of a solvent 'Y' (molar mass = 300 g mol$^{-1}$) led to an elevation of the boiling point by 0.5 K. The relative lowering in the vapour pressure of the solvent 'Y' is $____________ \(\times 10^{-2}\). (nearest integer)
[Given : $K_{b}$ of the solvent = 5.0 K kg mol$^{-1}$]
Assume the solution to be dilute and no association or dissociation of X takes place in solution.
Inductance of a coil with \(10^4\) turns is \(10\,\text{mH}\) and it is connected to a DC source of \(10\,\text{V}\) with internal resistance \(10\,\Omega\). The energy density in the inductor when the current reaches \( \left(\frac{1}{e}\right) \) of its maximum value is \[ \alpha \pi \times \frac{1}{e^2}\ \text{J m}^{-3}. \] The value of \( \alpha \) is _________.
\[ (\mu_0 = 4\pi \times 10^{-7}\ \text{TmA}^{-1}) \]