To solve this problem, we begin by evaluating the given integral:
\[\int_{\log_e a}^{4} \frac{dx}{\sqrt{e^x - 1}} = \frac{\pi}{6}.\]Notice that the integral involves a square root and exponential function, which suggests a possible substitution to simplify it. Assume the substitution:
\(e^x - 1 = t^2\).
Differentiating both sides with respect to \(x\) gives:
\[e^x \, dx = 2t \, dt.\]This means \(dx = \frac{2t}{e^x} \, dt\). Rewrite the integral in terms of \(t\):
\[\int \frac{dx}{\sqrt{e^x - 1}} = \int \frac{1}{t} \cdot \frac{2t}{e^x} \, dt = 2 \int \frac{dt}{e^x}.\]Back-substitute \(e^x = t^2 + 1\):
\[= 2 \int \frac{dt}{t^2 + 1}.\]This integral is the standard inverse tangent function:
\[= 2 \tan^{-1}(t).\]Now, let's use the limits of the integral. When \(x = \log_e a\), \(e^x - 1 = a - 1\), so \(t = \sqrt{a - 1}\). When \(x = 4\), \(t = \sqrt{e^4 - 1}\). Therefore, the definite integral becomes:
\[2 \left( \tan^{-1}(\sqrt{e^4 - 1}) - \tan^{-1}(\sqrt{a - 1}) \right) = \frac{\pi}{6}.\]Thus,
\[\tan^{-1}(\sqrt{e^4 - 1}) - \tan^{-1}(\sqrt{a - 1}) = \frac{\pi}{12}.\]This indicates that \(\alpha\) satisfies this equation:
\(e^\alpha = e^4 - 1\) and \(e^{-\alpha} = a - 1\).
We are told \(e^\alpha\) and \(e^{-\alpha}\) are roots of a quadratic equation. Using the property of roots:
This matches the quadratic:
\[2x^2 - 5x + 2 = 0.\]Therefore, the correct equation is:
\(2x^2 - 5x + 2 = 0.\)
Given: \[ \int_{\log_e \alpha}^{\log_e 4} \frac{dx}{\sqrt{e^x - 1}} = \frac{\pi}{6}. \]
Let: \[ e^x - 1 = t^2 \implies e^x dx = 2t dt \quad \text{and} \quad dx = \frac{2t dt}{t^2 + 1}. \]
Substituting into the integral: \[ \int \frac{dx}{\sqrt{e^x - 1}} = \int \frac{2t dt}{(t^2 + 1) \cdot t} = \int \frac{2 dt}{t^2 + 1} = 2 \tan^{-1} t. \]
Reverting the substitution: \[ 2 \tan^{-1} (\sqrt{e^x - 1}) \Big|_{\log_e \alpha}^{\log_e 4}. \]
Evaluating at the limits: \[ 2 \left[ \tan^{-1} \left( \sqrt{e^{\log_e 4} - 1} \right) - \tan^{-1} \left( \sqrt{e^\alpha - 1} \right) \right] = \frac{\pi}{6}. \] Simplifying: \[ 2 \left[ \tan^{-1} (\sqrt{3}) - \tan^{-1} (\sqrt{e^\alpha - 1}) \right] = \frac{\pi}{6}. \]
Dividing by 2: \[ \tan^{-1} (\sqrt{3}) - \tan^{-1} (\sqrt{e^\alpha - 1}) = \frac{\pi}{12}. \]
Since \(\tan^{-1} (\sqrt{3}) = \frac{\pi}{3}\), we have: \[ \frac{\pi}{3} - \tan^{-1} (\sqrt{e^\alpha - 1}) = \frac{\pi}{12}. \]
Rearranging: \[ \tan^{-1} (\sqrt{e^\alpha - 1}) = \frac{\pi}{4}. \]
Thus: \[ \sqrt{e^\alpha - 1} = 1 \implies e^\alpha - 1 = 1 \implies e^\alpha = 2. \]
Therefore: \[ e^{-\alpha} = \frac{1}{2}. \]
The roots \( e^\alpha = 2 \) and \( e^{-\alpha} = \frac{1}{2} \) satisfy the equation: \[ x^2 - \left( 2 + \frac{1}{2} \right) x + 1 = 0 \implies 2x^2 - 5x + 2 = 0. \]
Therefore: \[ 2x^2 - 5x + 2 = 0. \]
\(\lim_{x \to 0} \frac{e - (1 + 2x)^{\frac{1}{2x}}}{x} \quad \text{is equal to:}\)
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,