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. Author manuscript; available in PMC: 2015 Jan 1.
Published in final edited form as: Commun Comput Phys. 2014 Jan;15(1):10.4208/cicp.101112.100413a. doi: 10.4208/cicp.101112.100413a

Figure 12.

Figure 12

Profiles of the non-electrostatic potential U (left) and the Péclet number (right) for the system investigated in Experiment 3. The schematics of the system is shown in Fig. 2(b). Both profiles were computed along a line parallel to the z-axis and passing through x = y = 1.5 nm. In these profiles, the surface of the nanopore, which separates the solvent region from the membrane, is located at z = 2 nm. The sharp repulsive gradients in the potential U cause spurious modes in the Galerkin approximation.

(a) Profile of U (kT units)

(b) Péclet number