Problem 171
Medium Nonhomogeneous Equations

Find the general integral of the third-order equation y' = x…

Find the general integral of the third-order equation $y' = x y'' - \frac{(y'')^2}{2}$.

Explanation of Method

Setting $p=y'$, $q=y''$ reveals a Clairaut equation in $(x,p)$, yielding both a two-parameter general solution and a singular solution that is its envelope.

Step 1: Recognizing the Clairaut structure

Set $p=y'$ and $q=y''=\dfrac{dp}{dx}$. The equation becomes

\[ p = xq - \frac{q^2}{2}, \]

which is a Clairaut equation in the pair $(x,p)$, with $q=dp/dx$ playing the role of the "slope" variable. It has exactly the form $p = x q - \varphi(q)$ with $\varphi(q)=q^2/2$.

Step 2: Differentiating with respect to $x$

Differentiate $p=xq-q^2/2$ with respect to $x$, using $dp/dx=q$: \[\frac{dp}{dx} = q + x\frac{dq}{dx} - q\frac{dq}{dx} \;\Longrightarrow\; q = q + (x-q)\frac{dq}{dx} \;\Longrightarrow\; (x-q)\frac{dq}{dx} = 0.\]

As with any Clairaut equation, this factored condition splits the problem into two independent cases.

Step 3: Case I — the general (two-parameter) solution

Case I: General Solution.

Take $dq/dx=0$, i.e. $q=C_1$, a constant. Substituting this constant value back into $p=xq-q^2/2$: $p = C_1x - \frac{C_1^2}{2}, \qquad \text{i.e.} \qquad y' = C_1x - \frac{C_1^2}{2}.$

Integrating once more in $x$:

$y = \frac{C_1$.

This is the general integral: a two-parameter family of parabolas, one parameter ($C_1$) coming from the Clairaut structure and the other ($C_3$) from the final integration.

Step 4: Case II — the singular solution (envelope)

Case II: Singular Solution.

Take instead $x-q=0$, i.e. $q=x$, so that $y''=x$. Substitute $q=x$ back into $p=xq-q^2/2$: \[p = x\cdot x - \frac{x^2}{2} = \frac{x^2}{2}, \qquad \text{i.e.} \qquad y' = \frac{x^2}{2}.\]

Integrating:

$y = \frac{x^3$.

Unlike Case I, this branch carries only a single free constant $C$ — it is the singular solution of the Clairaut equation.

Step 5: Verification

Case II directly: with $y'=x^2/2$ and $y''=x$, check $y'=xy''-\tfrac12(y'')^2$: \[xy'' - \frac{(y'')^2}{2} = x\cdot x - \frac{x^2}{2} = \frac{x^2}{2} = y'.\ \checkmark\]

Case I: with $y'=C_1x-C_1^2/2$ and $y''=C_1$, the same substitution gives $xy''-\tfrac12(y'')^2=xC_1-C_1^2/2=y'$ identically, for every $C_1$ and $C_3. $\checkmark$


Result

Final answer:

\[\boxed{\,y = \frac{C_1}{2}x^2 - \frac{C_1^2}{2}x + C_3\,}\]

Final answer:

\[\boxed{\,y = \frac{x^3}{6} + C\,}\]

Remark

Geometric remark. The general-solution family of Case I is tangent to the singular solution of Case II — it is the envelope of the family. Comparing the two slope conditions $p=C_1x-C_1^2/2$ and $p=x^2/2$ at fixed $C_1$:

\[ \frac{x^2}{2} - C_1x + \frac{C_1^2}{2} = \frac{(x-C_1)^2}{2} = 0 \]

has the double root $x=C_1$, confirming that each member of the Case I family touches the Case II curve tangentially at $x=C_1$, which is exactly the envelope property expected of the singular solution of a Clairaut equation.