We are given the equation:
\[
a|x| = |y| e^{xy - \beta}, \quad a, b \in \mathbb{N}
\]
Step 1: Differentiate both sides
\[
x dy - y dx + xy(x dy + y dx) = 0
\]
Dividing throughout by \(x y\):
\[
\frac{dy}{y} - \frac{dx}{x} + (x dy + y dx) = 0
\]
Step 2: Integrate both sides
\[
\ln|y| - \ln|x| + xy = c
\]
Step 3: Using the condition \( y(1) = 2 \)
Substitute \(x = 1, y = 2\):
\[
\ln|2| - 0 + 2 = c
\]
\[
c = 2 + \ln 2
\]
Step 4: Substituting the value of \( c \)
\[
\ln|y| - \ln|x| + xy = 2 + \ln 2
\]
\[
\ln|x| = \ln\left|\frac{y}{2}\right| - 2 + xy
\]
Step 5: Simplifying the equation
\[
|x| = \left|\frac{y}{2}\right| e^{xy - 2}
\]
\[
2|x| = |y| e^{xy - 2}
\]
Step 6: Comparing with the given form
\[
a|x| = |y| e^{xy - \beta}
\]
Thus, comparing both sides:
\[
a = 2, \quad \beta = 2
\]
Step 7: Final result
\[
\alpha + \beta = 2 + 2 = 4
\]
Final Answer:
\[
\boxed{\alpha + \beta = 4}
\]
Consider the given differential equation:
\[xdy - ydx + xy(xdy + ydx) = 0.\]
Rearranging terms:
\[(x + xy)dy = (y - xy)dx.\]
Dividing both sides by \(xy\):
\[\frac{dy}{dx} = \frac{y - xy}{x + xy}.\]
Given that \(\alpha|x| = |y|e^{xy - \beta}\), substituting the initial condition \(y(1) = 2\) into the expression:
\[\alpha|1| = |2|e^{1 \cdot 2 - \beta}.\]
Simplifying:
\[\alpha = 2e^{2 - \beta}.\]
Since \(\alpha, \beta \in \mathbb{N}\), assume values for \(\beta\) such that \(\alpha\) is an integer. Let \(\beta = 2\):
\[\alpha = 2e^0 = 2.\]
Calculating \(\alpha + \beta\):
\[\alpha + \beta = 2 + 2 = 4.\]
Answer: 4.
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,