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Verlet algorithm

The Nose-Hoover temperature and pressure controls are incorporated in the equations of motion as friction coefficients in the time integration which is performed using the Verlet algorithm [1],[17].

$\displaystyle \mathbf{r}(t+\delta t)$ $\textstyle =$ $\displaystyle 2 \mathbf{r}(t) - \mathbf{r}(t-\delta t) + \delta t^2 \mathbf{a}(t)$ (4)
$\displaystyle \mathbf{v}(t)$ $\textstyle =$ $\displaystyle \frac{\mathbf{r}(t+\delta t) - \mathbf{r}(t-\delta t)}{2\delta t}$  

The first step of the integration was computed with ordinary Taylor expansion:

\begin{displaymath}
\mathbf{r}(t+\delta t) = \mathbf{r}(t) + \delta t \mathbf(v)(t)
+ \frac{1}{2} \delta t^2 \mathbf{a}(t)
\end{displaymath}