First of all, this is by no means a trivial problem. The usual method goes something like the following. The force from mass 2 on mass 1 is:
$$F_{21} = G\frac{m_1 m_2}{(x_2 - x_1)^2} = m_1 \ddot{x}_1$$
Similarly:
$$F_{12} = -F_{21} = -G\frac{m_1 m_2}{(x_2 - x_1)^2} = m_2 \ddot{x}_2$$
Canceling masses and subtracting the equations from each other gives:
$$\ddot{x}_2 - \ddot{x}_1 = \frac{d^2}{dt^2}(x_2 - x_1) = -G\frac{m_1 + m_2}{(x_2 - x_1)^2}$$
If we define $~r=x_2-x_1$ as the separation between the masses, then our equation becomes:
$$\ddot{r} = -G\frac{m_1 + m_2}{r^2}$$
Now it gets a bit trickier. We use the fact that $\ddot{r}=\dot{r}~d\dot{r}/dr$ to separate the differential equation:
$$\dot{r}~d\dot{r}=-G\frac{m_1 + m_2}{r^2}~dr$$
For $\dot{r}=0$ at $r_0$ (they're initially at rest), the integral of the above yields:
$$\frac{dr}{dt} = \sqrt{ \frac{2 G (m_1 + m_2)}{r} - \frac{2 G (m_1 + m_2)}{r_0}} = \sqrt{ \frac{2 G r_0 (m_1 + m_2) - 2 G r (m_1 + m_2)} {r\ r_0}}$$
So then:
$$\Delta t=\sqrt{\frac{r_0}{2 G (m_1 + m_2)}}~\int_{r_0}^{r} \sqrt{\frac{r}{r_0 - r}}~dr $$
In your case you've set $G=10$, $r_0=10$, and the masses each to one. When they've each traveled four meters, $r=2$. So you need to integrate the above from 10 to 2.