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.
A conducting bar moves on two conducting rails as shown in the figure. A constant magnetic field \( B \) exists into the page. The bar starts to move from the vertex at time \( t = 0 \) with a constant velocity. If the induced EMF is \( E \propto t^n \), then the value of \( n \) is _____. 