The motion of a mass is described by $\frac{d^2 x}{dt^2} + x+x^3 = 0$. Determine how solutions of this equation behave.

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So far this is what I have:

First off, let $\dot x = y$ and $\dot y = -x-x^3$. Then the DE can be written as $$\frac{y^2}{2}+\frac{x^2}{2}+\frac{x^4}{4} = H(x,y)$$

This is Newtonian, so consider the following:

$$U(x) = \frac{x^2}{2} + \frac{x^4}{4}$$ $$U'(x) = x+x^3$$

This shows that $U'(x) = 0$ means that $x = 0$. Now

$$U''(x) = 1 + 3x^2$$

So $U''(0) = 1 > 0$ which implies that we have a min at $x = 0$. This implies that we have a center at $x =0$.

Is there more that I can add to this without explicitly using software? This is a question from a former PhD qualifying exam, so I'm trying to figure out what they may be expecting.

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As additional information you can approximate the period of small oscillatins. Consider the solution curve through $(x,y)=(x_0,0)$, $x_0$ small. Then with the Hamiltionian we get $$ y^2+x^2+\frac12x^4=x_0^2+\frac12x_0^4 \\ \dot x^2=y^2=(x_0^2-x^2)\left(1+\frac12(x_0^2+x^2)\right). $$ One quarter of the period can be computed as the integral \begin{align} \frac{T}4&=\int_0^{x_0}\frac{dx}{\sqrt{x_0^2-x^2}\sqrt{1+\frac12(x_0^2+x^2)}}\\ &=\int_0^1\frac{dz}{\sqrt{1-z^2}\sqrt{1+\frac{x_0^2}2(1+z^2)}} \\[1em] &=\int_0^1\frac{dz}{\sqrt{1-z^2}\sqrt{1+x_0^2}\sqrt{1-\frac{x_0^2(1-z^2)}{2(1+x_0^2)}}} \\ &=\sum_{k=0}^\infty\binom{2k}{k}\frac{x_0^{2k}}{8^k(1+x_0^2)^{k+\frac12}}\int_0^1(1-z^2)^{k-\frac12}\,dz \\ &=\frac1{\sqrt{1+x_0^2}}\int_0^1\frac{dz}{\sqrt{1-z^2}} +\frac{x_0^2}{4(1+x_0^2)^{\frac32}}\int_0^1\sqrt{1-z^2}\,dz+O(x_0^4)\\[1em] &=\frac\pi{2\sqrt{1+x_0^2}}+\frac{\pi x_0^2}{16(1+x_0^2)^{\frac32}}+O(x_0^4). \end{align} The series expansion was done using the binomial series $$ (1-u)^{-1/2}=\sum\binom{-1/2}k(-u)^k=\sum\binom{2k}{k}\left(\frac u4\right)^k $$