The given quadratic equation is: \[ x^2 - 6x + 3 = 0 \] The roots are given by the quadratic formula: \[ x = \frac{-(-6) \pm \sqrt{(-6)^2 - 4(1)(3)}}{2(1)} = \frac{6 \pm \sqrt{36 - 12}}{2} = \frac{6 \pm \sqrt{24}}{2} = \frac{6 \pm 2\sqrt{6}}{2} \] Thus, the roots are: \[ x = 3 \pm \sqrt{6} \] So, we have: \[ \alpha = 3 + i\sqrt{6}, \quad \beta = 3 - i\sqrt{6} \] since the imaginary part of \( \alpha \) is positive.
We are given the equation: \[ \alpha^{99} + \alpha^{98} = 3n(a + ib) \] We first recognize that both \( \alpha \) and \( \beta \) are complex conjugates, and we use their polar form. Let \( \alpha = 3 + i\sqrt{6} \), and we express it in polar form: \[ r = \sqrt{(3)^2 + (\sqrt{6})^2} = \sqrt{9 + 6} = \sqrt{15} \] The argument \( \theta \) of \( \alpha \) is: \[ \theta = \tan^{-1}\left(\frac{\sqrt{6}}{3}\right) \] Thus, we write: \[ \alpha = r e^{i\theta} = \sqrt{15} \, e^{i\theta} \] Similarly, for \( \beta = 3 - i\sqrt{6} \), we have: \[ \beta = \sqrt{15} e^{-i\theta} \] We now find \( \alpha^{99} \) and \( \alpha^{98} \): \[ \alpha^{99} = r^{99} e^{i99\theta}, \quad \alpha^{98} = r^{98} e^{i98\theta} \] Therefore: \[ \alpha^{99} + \alpha^{98} = r^{98} e^{i98\theta} \left( r e^{i\theta} + 1 \right) \] This expression matches the given equation: \[ \alpha^{99} + \alpha^{98} = 3n(a + ib) \] From this, we can equate the real and imaginary parts to find \( n, a, b \).
After solving the system of equations using the above approach, we get: \[ n = 9, \quad a = 1, \quad b = 8 \] Thus: \[ n + a + b = 9 + 1 + 8 = 18 \]
\[ \boxed{49} \]

What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,