Skip to main content
. 2019 Jul 10;9:10002. doi: 10.1038/s41598-019-46449-5

Figure 1.

Figure 1

(a) Time evolution of the collective water re-orientation at different electric field-strengths. The angle θ is between the water molecular bisector and the electric field. For the strongest considered field, the average of 20 independent trajectories is plotted, while each of the other two traces is based on a single MD trajectory. (b) Time evolution of the average angle between the molecular bisector and the three Cartesian axes for the strongest field at 4.3 × 109 Vm−1. The shaded region marks the duration of the electric field pulse. (c) Average time evolution of the temperature for the system plotted in (b).