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: \[ n + a + b = 9 + 1 + 8 = 18 \]
\[ \boxed{49} \]
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:
