c c c ################################################################ c ## COPYRIGHT (C) 2006 by Michael Schnieders & Jay W. Ponder ## c ## All Rights Reserved ## c ################################################################ c c ################################################################ c ## ## c ## pbstuf.i -- parameters for Poisson-Boltzmann solvation ## c ## ## c ################################################################ c c c pbe Poisson-Boltzmann permanent multipole solvation energy c apbe Poisson-Boltzmann permanent multipole energy over atoms c pbr Poisson-Boltzmann cavity radii for atom types c pbep Poisson-Boltzmann energies on permanent multipoles c pbfp Poisson-Boltzmann forces on permanent multipoles c pbtp Poisson-Boltzmann torques on permanent multipoles c pbeuind Poisson-Boltzmann field due to induced dipoles c pbeuinp Poisson-Boltzmann field due to non-local induced dipoles c c APBS configuration parameters (see APBS documentation for details) c In the column on the right are possible values for each variable, c with default values given in brackets. Only a subset of the APBS c options are supported and/or are appropriate for use with AMOEBA c c pbtyp lpbe c c At some point AMOEBA with the non-linear PBE could be supported, c but there is only have theory for energies (no gradients) c c pbsoln mg-auto, [mg-manual] c c Currently there is only limited support for focusing calculations, c which is a powerful feature of APBS. At present, all energies and c forces must all be calculated using the finest solution c c bcfl boundary conditions zero, sdh, [mdh] c chgm multipole discretization spl4 c c other charge discretization methods are not appropriate for AMOEBA c c srfm surface method mol, smol, [spl4] c c spl4 is required for forces calculations, although mol is useful c for comparison with generalized Kirkwood c c dime number of grid points [65, 65, 65] c grid grid spacing (mg-manual) fxn of "dime" c cgrid coarse grid spacing fxn of "dime" c fgrid fine grid spacing cgrid / 2 c c stable results require grid spacing to be fine enough to keep c multipoles inside the dielectric boundary (2.5 * grid < PBR) c c gcent grid center (mg-manual) center of mass c cgcent coarse grid center center of mass c fgcent fine grid center center of mass c pdie solute/homogeneous dieletric [1.0] c sdie solvent dieletric [78.3] c ionn number of ion species [0] c ionc ion concentration (M) [0.0] c ionq ion charge (electrons) [1.0] c ionr ion radius (A) [2.0] c srad solvent probe radius (A) [1.4] c swin surface spline window width [0.3] c sdens density of surface points [10.0] c c additional parameter to facilitate default grid setup c c smin minimum distance between an [10.0] c atom and the grid boundary (A) c c integer maxion parameter (maxion=10) integer ionn,dime,ionq real*8 pbe,apbe,pbr real*8 pbep,pbfp,pbtp real*8 pbeuind,pbeuinp real*8 grid,gcent real*8 cgrid,cgcent real*8 fgrid,fgcent real*8 ionr,ionc real*8 pdie,sdie real*8 srad,swin real*8 sdens,smin character*20 pbtyp,pbsoln character*20 bcfl,srfm,chgm common /pbstuf/ pbe,apbe(maxatm),pbr(maxatm),pbep(3,maxatm), & pbfp(3,maxatm),pbtp(3,maxatm),pbeuind(3,maxatm), & pbeuinp(3,maxatm),grid(3),gcent(3),cgrid(3), & cgcent(3),fgrid(3),fgcent(3),ionr(maxion), & ionc(maxion),pdie,sdie,srad,swin,sdens,smin,ionn, & dime(3),ionq(maxion),pbtyp,pbsoln,bcfl,srfm,chgm