Let αx=exp(xβyγ) be the solution of the differential equation 2x2ydy−(1−xy2) dx = 0, x>0 , y(2)=\(\sqrt {log_e2}\). Then α+β−γ equals :
When solving differential equations involving substitution, always verify the boundary conditions to determine the constant of integration.
The given differential equation is:
\[2x^2y \, dy - (1 - xy^2) \, dx = 0.\]
Rearranging:
\[2x^2y \, dy = (1 - xy^2) \, dx.\]
\[\frac{dy}{dx} = \frac{1 - xy^2}{2x^2y}.\]
Substitute \(y^2 = t\), so that:
\[2y \, dy = dt.\]
The equation becomes:
\[x^2 \frac{dt}{dx} = 1 - xt.\]
\[\frac{dt}{dx} + \frac{t}{x} = \frac{1}{x^2}.\]
This is a first-order linear differential equation with integrating factor (I.F.):
\[\text{I.F.} = e^{\int \frac{1}{x} dx} = e^{\ln x} = x.\]
Multiplying through by the integrating factor:
\[x \frac{dt}{dx} + t = \frac{1}{x}.\]
\[\frac{d}{dx}(t \cdot x) = \frac{1}{x}.\]
Integrating both sides:
\[t \cdot x = \int \frac{1}{x} dx = \ln x + C.\]
\[t = \frac{\ln x + C}{x}.\]
Substituting back \(t = y^2\):
\[y^2 \cdot x = \ln x + C.\]
Using the condition \(y(2) = \sqrt{\ln 2}\):
\[(\ln 2) \cdot 2 = \ln 2 + C.\]
\[C = \ln 2.\]
Thus:
\[y^2 \cdot x = \ln x + \ln 2.\]
\[y^2 = \frac{\ln(2x)}{x}.\]
From \(\alpha x = \exp(x^\beta y^\gamma)\):
\[\alpha x = \exp(x \cdot y^2).\]
\[\alpha x = \exp(x \cdot \frac{\ln(2x)}{x}).\]
\[\alpha x = \exp(\ln(2x)).\]
\[\alpha x = 2x.\]
Comparing with the given form \(\alpha x = \exp(x^\beta y^\gamma)\), we find:
\[\alpha = 2, \, \beta = 1, \, \gamma = 2.\]
Step 5: Calculate \(\alpha + \beta - \gamma\):
\[\alpha + \beta - \gamma = 2 + 1 - 2 = 1.\]
Conclusion: \(\alpha + \beta - \gamma = 1\) .

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A relation between involved variables, which satisfy the given differential equation is called its solution. The solution which contains as many arbitrary constants as the order of the differential equation is called the general solution and the solution free from arbitrary constants is called particular solution.
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