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Add PTMA_GBNO2_IBI/example_run
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ricalessandri committed Aug 27, 2023
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41,906 changes: 41,906 additions & 0 deletions PTMA_GBNO2_IBI/example_run/conf-conect.pdb

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132 changes: 132 additions & 0 deletions PTMA_GBNO2_IBI/example_run/grompp-NPT.mdp
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; VARIOUS PREPROCESSING OPTIONS
; Preprocessor - specify a full path if necessary.
include =
define =

; RUN CONTROL PARAMETERS
integrator = sd
; Start time and timestep in ps
tinit = 0
dt = 0.020
nsteps = 1000000
; For exact run continuation or redoing part of a run
init_step = 0
; mode for center of mass motion removal
comm-mode = Linear
; number of steps for center of mass motion removal
nstcomm = 10
; group(s) for center of mass motion removal
comm_grps =
;system

; LANGEVIN DYNAMICS OPTIONS
; Friction coefficient (amu/ps) and random seed
ld-seed = -1

; OUTPUT CONTROL OPTIONS
; Output frequency for coords (x), velocities (v) and forces (f)
nstxout = 0
nstvout = 0
nstfout = 0
; Output frequency for energies to log file and energy file
nstlog = 100
nstenergy = 100
; Output frequency and precision for xtc file
nstxout-compressed = 100
compressed-x-precision = 1000
; This selects the subset of atoms for the xtc file. You can
; select multiple groups. By default all atoms will be written.
compressed-x-grps = System ;Protein
; Selection of energy groups
energygrps = VNL EST C1 NO

; NEIGHBORSEARCHING PARAMETERS
; nblist update frequency
nstlist = 10
; ns algorithm (simple or grid)
ns_type = grid
; Periodic boundary conditions: xyz (default), no (vacuum)
; or full (infinite systems only)
pbc = xyz
; nblist cut-off
rlist = 1.5


; OPTIONS FOR ELECTROSTATICS AND VDW
; Method for doing electrostatics
coulombtype = Cut-off
rcoulomb-switch = 0
rcoulomb = 1.5
; Relative dielectric constant for the medium and the reaction field
epsilon_r = 1
epsilon_rf = 1
; Method for doing Van der Waals
vdwtype = user
; cut-off lengths
rvdw-switch = 0
rvdw = 1.5
; Apply long range dispersion corrections for Energy and Pressure
DispCorr = EnerPres
; Extension of the potential lookup tables beyond the cut-off
table-extension = 1.0
; Seperate tables between energy group pairs
energygrp_table = VNL VNL VNL EST VNL C1 VNL NO EST EST EST C1 EST NO C1 C1 C1 NO NO NO
; Spacing for the PME/PPPM FFT grid
fourierspacing = 0.12
; FFT grid size, when a value is 0 fourierspacing will be used
fourier_nx = 0
fourier_ny = 0
fourier_nz = 0
; EWALD/PME/PPPM parameters
pme_order = 4
ewald_rtol = 1e-05
ewald_geometry = 3d
epsilon_surface = 0

; OPTIONS FOR WEAK COUPLING ALGORITHMS
; Temperature coupling
tcoupl = berendsen
; Groups to couple separately
tc-grps = System
; Time constant (ps) and reference temperature (K)
tau_t = 1.0
ref_t = 300
; Pressure coupling
Pcoupl = berendsen
pcoupltype = isotropic
; Time constant (ps), compressibility (1/bar) and reference P (bar)
tau_p = 2.0
compressibility = 4.5e-5
ref_p = 1.0


; GENERATE VELOCITIES FOR STARTUP RUN
gen_vel = yes
gen_temp = 300
gen_seed = -1

; OPTIONS FOR BONDS
constraints = none
; Type of constraint algorithm
constraint_algorithm = LINCS
; Use successive overrelaxation to reduce the number of shake iterations
Shake-SOR = no
; Relative tolerance of shake
shake-tol = 1e-04
; Highest order in the expansion of the constraint coupling matrix
lincs-order = 4
; Number of iterations in the final step of LINCS. 1 is fine for
; normal simulations, but use 2 to conserve energy in NVE runs.
; For energy minimization with constraints it should be 4 to 8.
lincs_iter = 2
; Lincs will write a warning to the stderr if in one step a bond
; rotates over more degrees than
lincs-warnangle = 30
; Convert harmonic bonds to morse potentials
morse = no

; ENERGY GROUP EXCLUSIONS
; Pairs of energy groups for which all non-bonded interactions are excluded
energygrp_excl =

cutoff-scheme = Group
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