# # Input parameters for mm_pbsa.pl # This example uses snapshots from ../01_GenerateSnapshots, and computes # continuum free energy estimates, using both GB and PB models # # Holger Gohlke # 08.01.2002 # ################################################################################ @GENERAL # # General parameters # 0: means NO; >0: means YES # # mm_pbsa allows to calculate (absolute) free energies for one molecular # species or a free energy difference according to: # # Receptor + Ligand = Complex, # DeltaG = G(Complex) - G(Receptor) - G(Ligand). # # PREFIX - To the prefix, "{_com, _rec, _lig}.crd.Number" is added during # generation of snapshots as well as during mm_pbsa calculations. # PATH - Specifies the location where to store or get snapshots. # # COMPLEX - Set to 1 if free energy difference is calculated. # RECEPTOR - Set to 1 if either (absolute) free energy or free energy # difference are calculated. # LIGAND - Set to 1 if free energy difference is calculated. # # COMPT - parmtop file for the complex (not necessary for option GC). # RECPT - parmtop file for the receptor (not necessary for option GC). # LIGPT - parmtop file for the ligand (not necessary for option GC). # # GC - Snapshots are generated from trajectories (see below). # AS - Residues are mutated during generation of snapshots from trajectories. # DC - Decompose the free energies into individual contributions # (only works with MM and GB). # # MM - Calculation of gas phase energies using sander. # GB - Calculation of desolvation free energies using the GB models in sander # (see below). # PB - Calculation of desolvation free energies using delphi (see below). # MS - Calculation of nonpolar contributions to desolvation using molsurf # (see below). # If MS == 0, nonpolar contributions are calculated with the LCPO method # in sander. # NM - Calculation of entropies with nmode. # PREFIX 2zni PATH ./ # COMPLEX 0 RECEPTOR 1 LIGAND 0 # COMPT XXX RECPT rec.prm.top LIGPT XXX # GC 0 AS 0 DC 0 # MM 1 GB 1 PB 1 MS 1 # NM 0 # ################################################################################ @PB # # PB parameters (this section is only relevant if PB = 1 above) # # The following parameters are passed to the PB solver. # Additional parameters (e.g. SALT) may be added here. # For further details see the delphi and pbsa documentation. # # PROC - Determines which method is used for solving the PB equation: # If PROC = 1, the delphi program is applied. If PROC = 2, # the pbsa program of the AMBER suite is used. # REFE - Determines which reference state is taken for PB calc: # If REFE = 0, reaction field energy is calculated with EXDI/INDI. # Here, INDI must agree with DIELC from MM part. # If REFE > 0 && INDI > 1.0, the difference of total energies for # combinations EXDI,INDI and 1.0,INDI is calculated. # The electrostatic contribution is NOT taken from sander here. # INDI - Dielectric constant for the molecule. # EXDI - Dielectric constant for the surrounding solvent. # SCALE - Lattice spacing in no. of grids per Angstrom. # LINIT - No. of iterations with linear PB equation. # PRBRAD - Solvent probe radius in A (e.g. use 1.4 with the PARSE parameter set # and 1.6 with the radii optimized by R. Luo) # # Parameters for pbsa only # # RADIOPT - Option to set up atomic avity radii for molecular surface calculation # and dielectric assignment. A value of 0 uses the cavity radii from the prmtop file. # A value of 1 sets up optimized cavity radii at the pbsa initialization phase. # The latter radii are optimized for model compounds of proteins only; use cautions # when applying these radii to nucleic acids. # # Parameters for delphi only # # FOCUS - If FOCUS > 0, subsequent (multiple) PERFIL and SCALE parameters are # used for multiple delphi calculations using the focussing technique. # The # of _focussing_ delphi calculations thus equals the value of FOCUS. # PERFIL - Percentage of the lattice that the largest linear dimension of the # molecule will fill. # CHARGE - Name of the charge file. # SIZE - Name of the size (radii) file. # # SURFTEN / SURFOFF - Values used to compute the nonpolar contribution Gnp to # the desolvation according to Gnp = SURFTEN * SASA + SURFOFF. # # PROC 2 REFE 0 INDI 1.0 EXDI 80.0 SCALE 2.0 LINIT 500 PRBRAD 1.6 # RADIOPT 1 # FOCUS 0 PERFIL 80.0 CHARGE ./my_amber94_delphi.crg SIZE ./my_parse_delphi.siz # SURFTEN 0.005 SURFOFF 0.0 # ################################################################################ @MM # # MM parameters (this section is only relevant if MM = 1 above) # # The following parameters are passed to sander. # For further details see the sander documentation. # # DIELC - Dielectricity constant for electrostatic interactions. # Note: This is not related to GB calculations. # DIELC 1.0 # ################################################################################ @GB # # GB parameters (this section is only relevant if GB = 1 above) # # The first group of the following parameters are passed to sander. # For further details see the sander documentation. # # IGB - Switches between Tsui's GB (1), Onufriev's GB (2, 5). # GBSA - Switches between LCPO (1) and ICOSA (2) method for SASA calc. # Decomposition only works with ICOSA. # SALTCON - Concentration (in M) of 1-1 mobile counterions in solution. # EXTDIEL - Dielectricity constant for the solvent. # INTDIEL - Dielectricity constant for the solute # # SURFTEN / SURFOFF - Values used to compute the nonpolar contribution Gnp to # the desolvation according to Gnp = SURFTEN * SASA + SURFOFF. # IGB 2 GBSA 1 SALTCON 0.00 EXTDIEL 80.0 INTDIEL 1.0 # SURFTEN 0.0072 SURFOFF 0.00 # ################################################################################ @MS # # Molsurf parameters (this section is only relevant if MS = 1 above) # # PROBE - Radius of the probe sphere used to calculate the SAS. # Since Bondi radii are already augmented by 1.4A, PROBE should be 0.0 # PROBE 0.0 # ################################################################################# @PROGRAMS # # Program executables # DELPHI /home/gohlke/src/delphi.98/exe/delphi # ################################################################################