Step 1: Using the given equation. We are given that \( x = 2 \) is a root of the equation: \[ x^2 + px + q = 0. \] Substitute \( x = 2 \) into this equation: \[ 2^2 + 2p + q = 0 \quad \Rightarrow \quad 4 + 2p + q = 0 \quad \Rightarrow \quad q = -2p - 4. \quad \cdots (1) \] Step 2: Substituting into the function \( f(x) \). The function is given as: \[ f(x) = \frac{1 - \cos(x^2 - 4px + q^2 + 8q + 16)}{(x - 2p)^4}. \] Substitute \( q = -2p - 4 \) from equation (1): \[ f(x) = \frac{1 - \cos(x^2 - 4px + (-2p - 4)^2 + 8(-2p - 4) + 16)}{(x - 2p)^4}. \] Simplify the expression inside the cosine: \[ q^2 + 8q + 16 = (-2p - 4)^2 + 8(-2p - 4) + 16. \] Expanding this gives: \[ q^2 + 8q + 16 = 4p^2 + 16p + 16 - 16p - 32 + 16 = 4p^2 + 0p + 0 = 4p^2. \] Now the function becomes: \[ f(x) = \frac{1 - \cos(x^2 - 4px + 4p^2)}{(x - 2p)^4}. \] Step 3: Apply L'Hôpital's Rule.
Since the expression is in the form \( \frac{0}{0} \) as \( x \to 2p \), we can apply L'Hôpital's Rule. First, differentiate the numerator and denominator with respect to \( x \).
Numerator: \[ \frac{d}{dx} \left[ 1 - \cos(x^2 - 4px + 4p^2) \right] = \sin(x^2 - 4px + 4p^2) \cdot (2x - 4p). \] Denominator: \[ \frac{d}{dx} \left[ (x - 2p)^4 \right] = 4(x - 2p)^3. \] Thus, the limit becomes: \[ \lim_{x \to 2p} \frac{\sin(x^2 - 4px + 4p^2) \cdot (2x - 4p)}{4(x - 2p)^3}. \] Step 4: Simplifying the limit.
At \( x = 2p \), the numerator becomes \( \sin(0) \cdot 0 = 0 \) and the denominator also becomes \( 0 \), so we apply L'Hôpital's Rule again. The limit simplifies to: \[ \lim_{x \to 2p} f(x) = 0. \] Step 5: Conclusion.
Thus, the correct value of the limit is \( 0 \), and the correct answer is option (3).
What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,