The problem involves solving a differential equation given in series form as:
\(x = 1 + xy\frac{dy}{dx} + \frac{(xy)^2}{2!}\left(\frac{dy}{dx}\right)^2 + \frac{(xy)^3}{3!}\left(\frac{dy}{dx}\right)^3 + \ldots\)
We can observe that this series resembles the Taylor expansion of the exponential function \(e^u\), where:
\(e^u = 1 + u + \frac{u^2}{2!} + \frac{u^3}{3!} + \ldots\)
Comparing this with the given series, we find:
\(u = xy \left(\frac{dy}{dx}\right)\)
Therefore, the differential equation can be rewritten as the exponential equation:
\(e^{xy\frac{dy}{dx}} = x\)
Taking natural logarithms on both sides, we get:
\(xy \frac{dy}{dx} = \ln x\)
Separating variables, we have:
\(y \, dy = \frac{\ln x}{x} \, dx\)
Integrating both sides, the left side becomes:
\(\int y \, dy = \frac{y^2}{2} + C_1\)
For the right side, the integral of \(\frac{\ln x}{x}\) is a known result:
\(\int \frac{\ln x}{x} \, dx = \frac{(\ln x)^2}{2} + C_2\)
Equating the integrals gives:
\(\frac{y^2}{2} = \frac{(\ln x)^2}{2} + C\)
where \(C = C_2 - C_1\).
After simplifying and solving for \(y\), we get:
\(y^2 = (\ln x)^2 + 2C\)
This implies:
\(y = \pm \sqrt{(\ln x)^2 + 2C}\)
Renaming \(2C\) as y = \pm e^{\frac{(\ln x)^2}{2}} + C, which matches the correct answer.
Thus, the solution is:
\( y = \pm e^{\frac{(\log x)^2}{2}} + C \)