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A conservative finite difference scheme for Poisson–Nernst–Planck equations

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Figure

Fig. 1 Comparing our steady-state solution (the dashed lines) usingTR-BDF2 method with that of the Poisson–Boltzmann equation (thesolid lines) obtained in [21]
Figure =timestion (negative charges toward the left boundary and the no-fluxboundary condition (accumulate at the boundary
Fig. 4 (time from the simulations using the mass-conservative (conservative (a) The total ion concentration for species 2 as a function ofsolid) and non–dashed) schemes
Fig. 5 (using the mass-conservative (a) The total energy as a function of time from the simulationssolid) and non-conservative (dashed)schemes
+3

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