Given that \( f(x) \) is a polynomial of degree 2, let \( f(x) = ax^2 + bx + c \) where \( a \neq 0 \).
Step 1: Apply the given condition to find \( f(x) \). From the given condition, we have: \[ f(x)f\left( \frac{1}{x} \right) = f(x) + f\left( \frac{1}{x} \right) \] Substitute the expression for \( f(x) \) into this: \[ (ax^2 + bx + c) \left( a\frac{1}{x^2} + b\frac{1}{x} + c \right) = (ax^2 + bx + c) + \left( a\frac{1}{x^2} + b\frac{1}{x} + c \right) \]
Step 2: Simplify the equation. From this, we simplify and solve to find the constant values. Based on the given condition \( f(K) = -2K \), the equation becomes: \[ 1 - K^2 = -2K \quad \Rightarrow \quad 1 - K^2 + 2K = 0 \]
Step 3: Solve for \( K \). This is a quadratic equation in \( K \): \[ K^2 - 2K - 1 = 0 \] The roots of this equation are: \[ K = \alpha \quad {and} \quad K = \beta \]
Step 4: Find the sum of squares of the roots. We use the formula for the sum of squares of the roots of a quadratic equation: \[ \alpha^2 + \beta^2 = (\alpha + \beta)^2 - 2\alpha\beta \] From Vieta’s formulas, we know: \[ \alpha + \beta = 2 \quad {and} \quad \alpha\beta = -1 \] Thus: \[ \alpha^2 + \beta^2 = 2^2 - 2(-1) = 4 + 2 = 6 \]
The value of current \( I \) in the electrical circuit as given below, when the potential at \( A \) is equal to the potential at \( B \), will be _____ A.
Two light beams fall on a transparent material block at point 1 and 2 with angle \( \theta_1 \) and \( \theta_2 \), respectively, as shown in the figure. After refraction, the beams intersect at point 3 which is exactly on the interface at the other end of the block. Given: the distance between 1 and 2, \( d = \frac{4}{3} \) cm and \( \theta_1 = \theta_2 = \cos^{-1} \left( \frac{n_2}{2n_1} \right) \), where \( n_2 \) is the refractive index of the block and \( n_1 \) is the refractive index of the outside medium, then the thickness of the block is …….. cm.