$$y'(x)=\frac{1}{x'(y)}\\
\frac{dy'}{dy}=-\frac{x''}{(x')^2}\\
y''=\frac{dy'}{dy}\frac{dy}{dx}=-\frac{x''}{(x')^3}$$
Now, substitute this into the DE:
$$(x')^2=x'-yx''-y(x')^3\\
x'(y)=r(y)\\
r^2=r-yr'-yr^3\\
r'=\frac{r-r^2-yr^3}{y}\\
r(y)=z(y)y\\
z'=-z^2-y^2z^3\\
\frac{z'}{z^3}=-\frac{1}{z}-y^2\\
w(y)=\frac{1}{z(y)}\\
ww'=w+y^2$$
As pointed out by @Eli Bartlett, this is an Abel DE of the second kind and doesn't have an elementary solution and I don't think it is even analytically solvable.
Edit: The DE can also be reduced to an Abel DE of the first kind:
$$27y^6e^yu^3+27y^4e^{y/3}u'+3y^2+18y+1=0$$
where $u(y)=\left(z(y)+\frac{1}{3y^2}\right)e^{-y/3}$ which is motivated by completing the cube on the RHS to get $\left(z(y)+\frac{1}{3y^2}\right)^3=\ldots-\frac{z'(y)}{y^2}$ and making the substitution $f(y)=z(y)+\frac{1}{3y^2}$ and then making another substitution $f(y)=g(y)h(y)$ and choosing $g(y)$ to eliminate the $f^1(y)$ term by solving a DE in $g(y)$ that gives $g(y)=e^{y/3}$.
This DE is of the form:
$$u_y'=P(y)u^3(y)+Q(y)$$
Letting $s=\int P(y)dy$ puts the DE in canonical form.
$$u_s'=u^3(s)+\frac{Q(s)}{P(s)}\\
u_s'=u^3(s)+\phi(s)$$
which can be solved analytically as per Wikipedia and I found this paper that states the solution method.
If practical, after solving this DE,
we would get:
$u=f(s)$ and substitute $s=\int P(y)dy$ to get $u=f\left(\int P(y)dy\right)$ and then substitute $u=\left(\frac{x'(y)}{y}+\frac{1}{3y^2}\right)e^{-y/3}$ to get $x'(y)=yf\left(\int P(y)dy\right)e^{y/3}-\frac{1}{3y}$ and integrate to get $x(y)$, then invert using series reversion to solve for $y(x)$.