Consider the Emden equation y'' + (2)/(x)y' + y^α = 0 , (E)…
Consider the Emden equation $y'' + \dfrac{2}{x}y' + y^\alpha = 0$, (E), with $\alpha\in\mathbb{R}$. 1° Show that if $f(x)$ solves (E), then so does $g(x)=A^{2/(\alpha-1)}f(Ax)$, for any $A\gt 0$. 2° For $\alpha=5$, find a particular solution of $y''+\dfrac{2}{x}y'+y^5=0$.
Explanation of Method
The Emden equation $y''+\tfrac2xy'+y^\alpha=0$ carries a scaling symmetry $g(x)=A^{2/(\alpha-1)}f(Ax)$, which motivates the exact solution $y=(x^2+\tfrac13)^{-1/2}$ at $\alpha=5$.
Step 1: 1° — Setting up the scaling ansatz
Suppose $f$ solves (E). Seek a rescaled solution of the form $g(x)=\lambda f(Ax)$, with $\lambda$ to be determined, and write $\xi=Ax$. Then
\[ g'(x) = \lambda A f'(\xi), \qquad g''(x) = \lambda A^2 f''(\xi). \]
Step 2: Substituting into (E)
Substituting into $g''+\dfrac{2}{x}g'+g^\alpha$ and using $\dfrac{2}{x}=\dfrac{2A}{\xi}$: \[g''+\frac{2}{x}g'+g^\alpha = \lambda A^2 f''(\xi) + \lambda A\cdot\frac{2A}{\xi}f'(\xi) + \lambda^\alpha f(\xi)^\alpha = \lambda A^2\left[f''(\xi)+\frac{2}{\xi}f'(\xi)\right] + \lambda^\alpha f(\xi)^\alpha.\]
Since $f$ solves (E) at $\xi$, the bracket equals $-f(\xi)^\alpha$, so this reduces to
\[ g''+\frac{2}{x}g'+g^\alpha = \bigl(\lambda^\alpha - \lambda A^2\bigr)f(\xi)^\alpha. \]
Step 3: Determining $\lambda$
For $g$ to solve (E) for every $x$, the coefficient must vanish: $\lambda^\alpha = \lambda A^2$, i.e. $\lambda^{\alpha-1}=A^2$, i.e.
\[ \lambda = A^{2/(\alpha-1)}. \]
Hence $g(x) = A^{2/(\alpha-1)}f(Ax)$ is again a solution of (E), for any $A\gt 0$.
\[f \text{ solves (E)} \ \Longrightarrow\ g(x) = A^{2/(\alpha-1)}f(Ax) \text{ solves (E), for every } A\gt 0\]
Step 4: 2° — A particular solution for $\alpha=5$
For $\alpha=5$ the scaling law gives $\lambda=A^{2/4}=A^{1/2}$: a solution rescales as $x\mapsto Ax$, $y\mapsto A^{1/2}y$. Guided by this symmetry, try the two-parameter ansatz
\[ y = (ax^2+c)^{-1/2}, \qquad D := ax^2+c. \]
Then \[y' = -\frac{ax}{D^{3/2}}, \qquad y'' = \frac{2a^2x^2-ac}{D^{5/2}}, \qquad \frac{2}{x}y' = -\frac{2a}{D^{3/2}} = -\frac{2aD}{D^{5/2}}.\]
Step 5: Substituting into the equation
Combining the first two terms over the common denominator $D^{5/2}$: \[y''+\frac{2}{x}y' = \frac{2a^2x^2-ac-2aD}{D^{5/2}} = \frac{2a^2x^2-ac-2a^2x^2-2ac}{D^{5/2}} = \frac{-3ac}{D^{5/2}}.\]
Also $y^5=D^{-5/2}$, so the full equation $y''+\frac{2}{x}y'+y^5=0$ becomes
\[ \frac{-3ac+1}{D^{5/2}} = 0 \quad\Longrightarrow\quad ac = \frac{1}{3}. \]
So $y=(ax^2+c)^{-1/2}$ solves the $\alpha=5$ Emden equation for any $a,c$ with $ac=\tfrac13$. The simplest choice, $a=1$, $c=\tfrac13$, gives
\[ y = \left(x^2+\frac13\right)^{-1/2}. \]
Step 6: Verification
Substituting $y=(x^2+\tfrac13)^{-1/2}$ directly into $y''+\dfrac{2}{x}y'+y^5$ confirms the residual is exactly $0$. The general symbolic argument was checked independently in two ways: (i) for arbitrary $\alpha$, expanding $g''+2g'/x+g^\alpha$ and confirming that $\lambda=A^{2/(\alpha-1)}$ makes the exponents $2\alpha/(\alpha-1)$ and $2+2/(\alpha-1)$ exactly equal, forcing the bracket $\lambda^\alpha-\lambda A^2$ to vanish identically; (ii) at $\alpha=5$ specifically, using the explicit family $f(x)=(ax^2+c)^{-1/2}$, confirming that $g(x)=A^{1/2}f(Ax)$ also solves the $\alpha=5$ equation exactly, for symbolic $A$.
\[y = \left(x^2+\frac13\right)^{-1/2}\]
Result
Final answer:
\[\boxed{\,f \text{ solves (E)} \ \Longrightarrow\ g(x) = A^{2/(\alpha-1)}f(Ax) \text{ solves (E), for every } A\gt 0\,}\]
Final answer:
\[\boxed{\,y = \left(x^2+\frac13\right)^{-1/2}\,}\]
Remark
Remark. The scaling symmetry of Part 1° is what makes the ansatz $y=(ax^2+c)^{-1/2}$ natural: since a solution must rescale as $y\mapsto A^{1/2}y$ under $x\mapsto Ax$ for $\alpha=5$, a solution built purely from $x^2$ via a fixed negative half-power is exactly the right shape to absorb that scaling, leaving only the algebraic constraint $ac=\tfrac13$ to be fixed by substitution.