The given quadratic equation is:
\( x^2 - (3 - 2i)x - (2i - 2) = 0 \)
Using the quadratic formula:
\[
x = \frac{(3 - 2i) \pm \sqrt{(3 - 2i)^2 - 4(1)(-(2i - 2))}}{2(1)}
\]
Expanding the terms inside the square root:
\[
x = \frac{(3 - 2i) \pm \sqrt{9 - 4i^2 - 4(1)(-2i + 2)}}{2}
\]
\[
= \frac{3 - 2i \pm \sqrt{9 - 4(-1) - 12i + 8i - 8}}{2}
\]
\[
= \frac{3 - 2i \pm \sqrt{-3 - 4i}}{2}
\]
Breaking the square root term into a solvable form:
\[
= 3 - 2i \pm \sqrt{(1)^2 + (2i)^2 - 2(1)(2i)}
\]
\[
= 3 - 2i \pm (1)^{2} + (2i)^{2} - 2(1)(2i)
\]
The final roots are:
\( x = 2 - 2i \quad \text{or} \quad x = 1 + 0i \)
From the roots obtained, we have:
\( \alpha \beta = 2(1) \cdot (-2)(0) = 2 \)
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 _________.
\[ (\mu_0 = 4\pi \times 10^{-7}\ \text{TmA}^{-1}) \]