To solve, begin by analyzing the differential equation: \((1 + y^2)(1 + \log_e x) \, dx + x \, dy = 0\). Rewrite it in standard form: \(\frac{dy}{dx} = -\frac{(1 + y^2)(1 + \log_e x)}{x}\).
The problem describes an implicit differential equation separable via substitution: let \(v = 1 + \log_e x\), then \(dv = \frac{dx}{x}\). The equation transforms to:
\(\frac{dy}{dy} = -v(1 + y^2) \Rightarrow \frac{dy}{1 + y^2} = -v \, dv\).
Integrate both sides:
\(\int \frac{dy}{1 + y^2} = \int -v \, dv\).
Using integration formulas, \(\int \frac{dy}{1 + y^2} = \tan^{-1}(y)\) and \(\int -v \, dv = -\frac{v^2}{2}\), the integrated equation becomes:
\(\tan^{-1}(y) = -\frac{(1 + \log_e x)^2}{2} + C\).
Substitute initial condition \((x, y) = (1, 1)\):
\(\tan^{-1}(1) = -\frac{(1 + \log_e 1)^2}{2} + C = \frac{\pi}{4} = C\).
The equation becomes:
\(\tan^{-1}(y) = -\frac{(1 + \log_e x)^2}{2} + \frac{\pi}{4}\).
For \(x = e\), \(v = 1 + \log_e e = 2\). At this point, \(y(e) = \frac{\alpha - \tan\left(\frac{3}{2}\right)}{\beta + \tan\left(\frac{3}{2}\right)}\), replaced in our derived equation:
\(\tan^{-1}\left(\frac{\alpha - \tan\left(\frac{3}{2}\right)}{\beta + \tan\left(\frac{3}{2}\right)}\right) = -2 + \frac{\pi}{4} = \frac{\pi}{4} - 2\).
Inverting \(\tan^{-1}\), we solve for \(\alpha\) and \(\beta\):
\(\frac{\alpha - \tan\left(\frac{3}{2}\right)}{\beta + \tan\left(\frac{3}{2}\right)} = \tan\left(\frac{\pi}{4} - 2\right)\).
Assume \(A = \tan\left(\frac{3}{2}\right)\), simplify using the tangent subtraction identity, \(\tan(x - y) = \frac{\tan x - \tan y}{1 + \tan x \tan y}\):
\(T = \tan\left(\frac{\pi}{4} - 2\right)\). Find \(T\), equate and solve for \(\alpha\) and \(\beta\) in terms of known values and ensure expressions balance.
Finally, calculate \(\alpha + 2\beta\) = 3.
\[ \int \left( \frac{1}{x} + \frac{\ln x}{x} \right) dx + \int \frac{dy}{1 + y^2} = 0 \]
Integrating, we get:
\[ \ln x + \frac{(\ln x)^2}{2} + \tan^{-1} y = C \]
Substitute \(x = 1\) and \(y = 1\) to find \(C\):
\[ \ln 1 + \frac{(\ln 1)^2}{2} + \tan^{-1}(1) = C \Rightarrow C = \frac{\pi}{4} \]
\[ \ln x + \frac{(\ln x)^2}{2} + \tan^{-1} y = \frac{\pi}{4} \]
Substitute \(x = e\) into the equation:
\[ \ln e + \frac{(\ln e)^2}{2} + \tan^{-1} y = \frac{\pi}{4} \]
\[ 1 + \frac{1}{2} + \tan^{-1} y = \frac{\pi}{4} \]
Solving for \(y\), we get:
\[ y = \tan \left( \frac{\pi}{4} - \frac{3}{2} \right) = \frac{1 - \tan \frac{3}{2}}{1 + \tan \frac{3}{2}} \]
Comparing with the given expression for \(y(e)\), we find \(\alpha = 1\) and \(\beta = 1\).
\[ \alpha + 2\beta = 1 + 2 \cdot 1 = 3 \]
So, the correct answer is: 3
Let $y=y(x)$ be the solution of the differential equation $\left(x^2-3 y^2\right) d x+3 x y d y=0, y(1)=1$.Then $6 y^2( e )$ 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,