To solve the problem, we need to evaluate the following limit:
\[\lim_{x \to 0} \frac{\int_{0}^{x} f(t) \, dt}{e^{x^2} - 1} = \alpha\]Given that \(f(0) = \frac{1}{2}\) and \(f(x)\) is differentiable, we will use L'Hôpital's Rule. L'Hôpital's Rule is applicable since both the numerator and the denominator approach 0 as \(x \to 0\).
First, we differentiate the numerator and the denominator with respect to \(x\):
Using L'Hôpital's Rule, we have:
\[\lim_{x \to 0} \frac{f(x)}{2x e^{x^2}} = \alpha\]Substituting \(f(0) = \frac{1}{2}\), we focus on the expression at \(x = 0\):
\[\lim_{x \to 0} \frac{f(x)}{2x e^{x^2}} = \lim_{x \to 0} \frac{\frac{1}{2} + \frac{d}{dx}(f(x) - \frac{1}{2})}{2x e^{x^2}}\]Notice that the higher order terms vanish faster than \(x\), hence:
\[\lim_{x \to 0} \frac{\frac{1}{2}}{2x} = \frac{1}{4}\]Thus, \(\alpha = \frac{1}{4}\).
Next, we find \(8\alpha^{2}\):
\[8 \alpha^2 = 8 \left(\frac{1}{4}\right)^2 = 8 \times \frac{1}{16} = \frac{1}{2} \times 2 = 2\]Hence, the correct answer is 2.
Rewrite the limit as follows:
\[ \lim_{x \to 0} \frac{\int_0^x f(t) \, dt}{e^{x^2} - 1} = \lim_{x \to 0} \left( \frac{\int_0^x f(t) \, dt}{x} \times \frac{x}{e^{x^2} - 1} \right) \]
Evaluate each part separately:
For the first part, use L'Hôpital's Rule:
\[ \lim_{x \to 0} \frac{\int_0^x f(t) \, dt}{x} = \lim_{x \to 0} f(x) = f(0) = \frac{1}{2} \]
For the second part, apply the Taylor series expansion \( e^{x^2} \approx 1 + x^2 \) near \( x = 0 \):
\[ \lim_{x \to 0} \frac{x}{e^{x^2} - 1} = \lim_{x \to 0} \frac{x}{x^2} = \lim_{x \to 0} \frac{1}{x} = 1 \]
So, \( \alpha = \frac{1}{2} \). Then,
\[ 8\alpha^2 = 8 \times \left( \frac{1}{2} \right)^2 = 2 \]
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,