Given:
\[ (a^2 + b^2)x^2 - 2b(a + c)x + b^2 + c^2 = 0 \]
\[ (ax - b)^2 + (bx - c)^2 = 0 \]
\[ x = \frac{b \pm \sqrt{b^2 - ac}}{a^2 + b^2} \]
Step 1:
Consider the triangle with sides \( a, b, c \): \[ |h - k| < c < (a + b) \]
Since \( b^2 = ac \), \[ |a - c| < b < a + c \] Substituting \( b^2 = ac \): \[ |1 - \xi| < \xi < 1 + \xi \]
Hence, \[ |1 - \xi| < \xi < 1 + \xi \] \[ |1 - x^2| < x < 1 + x^2 \]
Case 1: \( b < x < 1 + x^2 \)
This is always positive.
Case 2: \( |1 - x^2| < x \)
\[ -x < 1 - x^2 < x \]
Now:
\[ 1 - x^2 < x \] \[ x^2 + x - 1 > 0 \]
Solving: \[ x = \frac{-1 \pm \sqrt{5}}{2} \]
\[ -x < 1 - x^2 \] \[ x^2 - x - 1 < 0 \]
Hence, \[ x = \frac{1 \pm \sqrt{5}}{2} \]
Now:
\[ \alpha = \frac{-1 + \sqrt{5}}{2}, \quad \beta = \frac{-1 - \sqrt{5}}{2} \]
Step 2:
\[ 12(a^2 + b^2) = 12 \left[\left(\frac{-1 + \sqrt{5}}{2}\right)^2 + \left(\frac{-1 - \sqrt{5}}{2}\right)^2\right] \]
\[ = 12 \left(\frac{(1 + \sqrt{5})^2 + (1 - \sqrt{5})^2}{4}\right) \]
\[ = 12 \times \frac{12}{4} = 36 \]
∴ Final Answer:
\[ \boxed{36} \]
The given quadratic equation in \( x \) is:
\[ (a^2 + b^2)x^2 - 2b(a + c)x + (b^2 + c^2) = 0. \]
This can be written in the form:
\[ (ax - b)^2 + (bx - c)^2 = 0. \]
Thus, we deduce that the discriminant must satisfy conditions related to triangle inequalities, leading us to intervals of \( x \) values.
By evaluating the possible values of \( x \), we find that the interval \((\alpha, \beta)\) corresponds to:
\[ \alpha = \frac{1 - \sqrt{5}}{2}, \quad \beta = \frac{1 + \sqrt{5}}{2}. \]
Then, calculate \(12(\alpha^2 + \beta^2)\):
\[ 12(\alpha^2 + \beta^2) = 36. \]
Thus, the answer is:
\[ 36. \]
If the roots of the quadratic equation \( ax^2 + bx + c = 0 \) are real and equal, then:
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:
