To solve the integral, we note that it is an even function due to the symmetric limits and the even nature of \( \cos(\alpha x) \). Therefore, we can simplify by doubling the integral from 0 to 1:
\[ \int_{-1}^1 \frac{\cos \alpha x}{1 + 3^x} \, dx = 2 \int_0^1 \frac{\cos \alpha x}{1 + 3^x} \, dx. \]
Given that the value of this integral equals \( \frac{2}{\pi} \), we proceed by testing values of \( \alpha \) to match this result.
Through evaluation, it turns out that setting \( \alpha = \frac{\pi}{2} \) satisfies this condition, yielding:
\[ \int_{-1}^1 \frac{\cos \left( \frac{\pi}{2} x \right)}{1 + 3^x} \, dx = \frac{\pi}{2}. \]
Therefore, the value of \( \alpha \) is \( \frac{\pi}{2} \).
\(\lim_{x \to 0} \frac{e - (1 + 2x)^{\frac{1}{2x}}}{x} \quad \text{is equal to:}\)
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,