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: \[ \alpha^2 + \beta^2 = 2^2 - 2(-1) = 4 + 2 = 6 \]
\(\text{The number of solutions of the equation}\)\(\left(\frac{9}{x}-\frac{9}{\sqrt{x}}+2\right)\left(\frac{2}{x}-\frac{7}{\sqrt{x}}+3\right)=0\mathrm \; {is:}\)
If the set of all values of \( a \), for which the equation \( 5x^3 - 15x - a = 0 \) has three distinct real roots, is the interval \( (\alpha, \beta) \), then \( \beta - 2\alpha \) is equal to
If the equation \( a(b - c)x^2 + b(c - a)x + c(a - b) = 0 \) has equal roots, where \( a + c = 15 \) and \( b = \frac{36}{5} \), then \( a^2 + c^2 \) is equal to .
A conducting bar moves on two conducting rails as shown in the figure. A constant magnetic field \( B \) exists into the page. The bar starts to move from the vertex at time \( t = 0 \) with a constant velocity. If the induced EMF is \( E \propto t^n \), then the value of \( n \) is _____. 