Let \( \alpha, \beta \) be the roots of the equation \( x^2 - ax - b = 0 \) with \( \text{Im}(\alpha) < \text{Im}(\beta) \). Let \( P_n = \alpha^n - \beta^n \). If \[ P_3 = -5\sqrt{7}, \quad P_4 = -3\sqrt{7}, \quad P_5 = 11\sqrt{7}, \quad P_6 = 45\sqrt{7}, \] then \( |\alpha^4 + \beta^4| \) is equal to:
Given the roots \( \alpha \) and \( \beta \) of the quadratic equation \( x^2 - ax - b = 0 \), we define \( P_n = \alpha^n - \beta^n \). We aim to calculate \( |\alpha^4 + \beta^4| \).
Recall the properties of roots of quadratic equations:
Using the identities:
Given:
For the sequence \( P_n \) defined by:
\( P_n = (\alpha + \beta)P_{n-1} - \alpha\beta P_{n-2} \)
Starting with \(P_3, P_4\):
\( P_5 = (\alpha + \beta)P_4 - \alpha\beta P_3 \)
Substituting the values:
\( 11\sqrt{7} = a(-3\sqrt{7}) - b(-5\sqrt{7}) \)
\( 11 = -3a + 5b \)
Using \(P_4, P_5\):
\( P_6 = (\alpha + \beta)P_5 - \alpha\beta P_4 \)
\( 45\sqrt{7} = a(11\sqrt{7}) - b(-3\sqrt{7}) \)
\( 45 = 11a + 3b \)
We solve the system of equations:
\( -3a + 5b = 11 \) (i)
\( 11a + 3b = 45 \) (ii)
Multiply (i) by 3, (ii) by 5, and add:
\(-9a + 15b = 33\)
\( 55a + 15b = 225\)
Adding yields:
\(46a = 258 \Rightarrow a = \frac{129}{23} = 3\)
Substitute \( a = 3 \) in (i):
\(-3(3) + 5b = 11\)
\(-9 + 5b = 11\)
\(5b = 20 \Rightarrow b = 4\)
Now calculate:
\(\alpha^4 + \beta^4 = (\alpha^2 + \beta^2)^2 - 2(\alpha\beta)^2\)
Where \( \alpha^2 + \beta^2 = (\alpha+\beta)^2 - 2\alpha\beta = 3^2 - 2 \cdot 4 = 9 - 8 = 1 \)
Hence:
\(\alpha^4 + \beta^4 = 1^2 - 2 \cdot 4^2 = 1 - 2 \cdot 16 = 1 - 32 = -31\)
Finally, \(|\alpha^4 + \beta^4| = 31\)
A small point of mass \(m\) is placed at a distance \(2R\) from the center \(O\) of a big uniform solid sphere of mass \(M\) and radius \(R\). The gravitational force on \(m\) due to \(M\) is \(F_1\). A spherical part of radius \(R/3\) is removed from the big sphere as shown in the figure, and the gravitational force on \(m\) due to the remaining part of \(M\) is found to be \(F_2\). The value of the ratio \( F_1 : F_2 \) is: 
A transparent block A having refractive index $ \mu_2 = 1.25 $ is surrounded by another medium of refractive index $ \mu_1 = 1.0 $ as shown in figure. A light ray is incident on the flat face of the block with incident angle $ \theta $ as shown in figure. What is the maximum value of $ \theta $ for which light suffers total internal reflection at the top surface of the block ?