-
Notifications
You must be signed in to change notification settings - Fork 18
Main Input Commands
Douglas M Franz edited this page Nov 30, 2018
·
38 revisions
All of these commands would go in the mcmd input file, which would be run by, e.g.
./mcmd myinput.inp
Command | Description | Default |
---|---|---|
jobname [string] |
The job's name. | default_jobname |
restart |
Automatically restarts a previously halted job by replacing the input atoms file with the existing restart.pdb , and saving directory files to saved_dataX where X automatically counts from 1. YOU MUST USE THE input_atoms command if you plan to restart a job. |
off |
mode [mc | md | sp | opt] |
mc for Monte Carlo; md for Molecular Dynamics. sp for classical single-point energy and multipoles. opt for classical optimization. |
NONE |
omp [int] |
Enables OpenMP parallelization for faster simulation. Argument is number of threads. 0 will disable OpenMP. Requires compilation with OpenMP enabled. |
0 |
checkpoints_option [on | off] |
Displays checkpoints from code with relevant timing info (for debugging). | off |
ensemble [nve|nvt|npt|uvt] |
Thermodynamic ensemble. nve = Microcanonical; nvt = Canonical; npt = Isobaric,Isothermal (Gibbs); uvt = Grand Canonical. |
NONE |
input_atoms [string] |
Takes the filename of input atoms in .pdb form (see examples). Not required for uVT simulation. |
NONE |
input_atoms_xyz [string] |
Option to use an XYZ file for input atoms. The string is the filename. This assumes all atoms are Frozen (e.g. part of a MOF) and uses periodic-table mass, UFF LJ params, and van Duijnen polarizabilities by default. Point-charges (in e) are optional and can be placed in the 5th column. Default parameters are only read for element names that match the standard names (e.g. "Na", not "NA" or "Na1"). | NONE |
output_traj_xyz [string] |
Takes the filename in which to write .xyz trajectory file every corrtime. Especially useful if you view trajectories for uVT simulation using VMD. |
traj.xyz . |
output_traj_pdb [string] |
Takes the filename in which to write .pdb trajectory file every corrtime. |
traj.pdb . |
draw_box_option [on|off] |
Enables creation of the simulation box in the restart_pdb and output_traj_pdb files. |
on |
restart_pdb [string] |
Filename for the restart input_atoms file generated at each corrtime. |
restart.pdb . |
thermo_output [string] |
Takes the filename in which to write thermodynamic data at each corrtime: energy, temperature, pressure, etc. | thermo.dat |
potential_form [lj | ljes | ljespolar | ljpolar | tt | ttes | ttespolar | commy | commyes | commyespolar] |
Dictates which functions to use for potential energy and force (MD only) calculations: lj=Lennard-Jones repulsion-dispersion; tt=Tang-Toennies RD; es=Ewald electrostatics; polar=polarization energy; commy=a VDW RD potential which is a hybrid of LJ and a form from a 1961 paper linked in commy.cpp. | lj |
rd_lrc [on|off] |
Enables Lennard-Jones long-range corrections to the potential energy. | on |
ewald_es [on|off] |
Enables Ewald-method calculation of electrostatic energy (including long-range). | on |
ewald_kmax [int] |
Specifies the maximum k-space vector for Ewald energy/force computation. >3 is generally good. Can be very expensive for large systems if >=5. | 7 |
polar_max_iter [int] |
Change the max number of iterations for dipole solver in polarization energy calculation. | 4 |
dipole_precision [double] |
Turns dipole-convergence-by-dipole-precision on (instead of fixed maximum iterations). Expressed in Debye. (the iteration-cap is the default method). A good value is between 10e-7 and 10e-4. | NONE |
full_A_matrix [on|off] |
Option to enable the full Thole Polarization A matrix -- takes more (~double) memory but runs faster. | on |
pdb_traj_option [on|off] |
Enables PDB trajectory output in output_traj_pdb filename. |
off |
xyz_traj_option [on|off] |
Option to (also) write .xyz trajectory output. | on |
big_pdb_traj [on|off] |
Forces frozen atoms to be (re-)written in trajectory steps in PDB. | off |
big_xyz_traj [on|off] |
Forces frozen atoms to be (re-)written in trajectory steps in XYZ. | off |
com_option [on|off] |
Enables on-the-fly center-of-mass calculation which adds a COM atom to the output files in each frame. |
off |
pdb_long [on|off] |
Enables long (%8.6f instead of %8.3f) output for greater precision on atom coordinates. Do NOT enable if you plan to view .pdb output in VMD. | off |
dist_within [on|off] |
Enables on-the-fly counter of atoms within a specified radius from the origin at each corrtime. | off |
dist_within_target [string] |
Takes the (PDB input label) name of the atom to calculate for dist_within . |
NONE |
dist_within_radius [double] |
Takes the radius from the origin in which to count occurrences of selected atom. | NONE |
auto_center [on|off] |
Enables automatic centering of all atoms to the origin (0,0,0) before beginning simulation. Important to make sure atoms fit in periodic box. | on |
temperature [double] |
Temperature in K for fixed-T simulations. | NONE |
pressure [double] |
Pressure in atm for fixed-P simulations (including uVT because chemical potential is auto-generated from pressure using equations-of-state). | 1.0 |
sig_override [string] [double] |
Manually changes the LJ sigma parameter for atoms by name. For multiple, issue this command in multiple lines. (Units = Angstrom) | NONE |
eps_override [string] [double] |
Does likewise for LJ epsilon parameter. (Units = Kelvin) | NONE |
charge_override [string] [double] |
Does likewise for the partial charge of this site. (Units = elementary charge) | NONE |
radial_dist [on|off] |
Enables radial-distribution calculation, which updates every corrtime. | off |
radial_bin_size [double] |
Specifies the bin size for g(r) in A. | 0.1 |
radial_max_dist [double] |
Sets the cutoff for relevant g(r) distance calculations between atoms. | 10.0 |
radial_centroid [string] |
Supplies name of atom (site) to calculate as the the center of g(r) interactions. | NONE |
radial_counterpart [string] |
Supplies the other atom to calculate distance from radial_centroid . |
NONE |
radial_file [string] |
Specifies name of output file for g(r). Supplies bin-counts as a function of pair-distance. |
radial_distribution.datX (X = pair id for multiple) |
radial_exclude_molecules [on|off] |
Option to exclude intramolecular distances in g(r) pair calculations. | off |
histogram [on|off] |
Option for histogram output (which can be viewed in VMD). | off |
histogram_output [string] |
Filename for histogram output. | histogram.dx |
histogram_resolution [double] |
Resolution of histogram bins in Angstroms. | 0.7 |
lj_uff [on|off] |
Option to set all atoms' Lennard-Jones sigma and epsilon to UFF (Rappe et al.) values (overrides other input) | off |
vand_polar [on|off] |
Option to set all atoms' point-polarizability parameters to van Duijnen values (overrides other input) | off |
manual_cutoff [double] |
Overrides the pair-interaction spherical cutoff radius (auto-calculated from box parameters as 1/2 min. length) with user-defined value. | NONE |
crystalbuild [on|off] |
Enables the crystal builder (to build super-cells automatically). | off |
crystalbuild_x [int] |
Multiplicity of crystal in x-direction (e.g. 2 will duplicate the cell in x). |
1 |
crystalbuild_y [int] |
Same for y-direction. | 1 |
crystalbuild_z [int] |
Same for z-direction. | 1 |
crystalbuild_includemovers [on|off] |
Option to include movable molecules when duplicating system. | off |
makefrags [int] |
Enables the fragment-maker and creates the number of fragments specified. The function loops through unique atoms by their name (in the .pdb input) and makes fragments that bury each atom in a fractal-like pattern. | NONE |
atoms_per_frag [int, int, int,..] |
Sets the number of atoms that will be created within each fragment. You can do multiple #'s for different fragment sizes. | 250 |
frag_bondlength [double] |
Sets the initial/default bond-length (in Angstroms) for the fragment-maker. If a fragment fails to build within this constraint, it will grow the bond-length until the goal number of atoms is obtained. | 2.1 |
scale_charges [double] |
Multiplies all frozen-atom charge parameters by this factor before running the simulation. | NONE |
sorbate_name [string] [string] [string...] |
Allows user-selected sorbate models (you need not include the sorbate [or anything at all] in the input_atoms file IF this is used). You MUST include sorbate_fugacities if multi-sorbate (this command) is used in the uVT ensemble. |
NONE |
sorbate_fugacities [double] [double] [double...] |
Partial pressures (in atm, as explicit fugacities) of sorbates, e.g. 10 10 would yield a total pressure of 20 atm. |
NONE |
no_zero_option [on|off] |
Option to disallow zero movable molecules in the simulation system. | off |
write_lammps [on|off] |
Writes LAMMPS-style inputs from MCMD input at simulation start (for MD simulations). | off |
bias_uptake [double] [N | wt% | wt%ME | mmol/g | mg/g | cm^3/g | g/mL | g/cm^3] |
Sets a "goal-uptake", which is achieved in uVT single-sorbate-only simulations by biasing insertions and preventing removes until the goal N is reached. Can accelerate equilibration/loading significantly especially if a good reference value is known. After this, the system equilibrates normally. | NONE |
Command | Description | Default |
---|---|---|
mc_corrtime [int] |
The MC step interval at which output is generated, observable averages re-calculated, etc. | 1000 |
finalstep [int] |
Specifies the last step to perturb system and calculate energy in MC. | NONE |
rotate_option [on|off] |
Enables rigid-body molecular rotations for movable molecules in MC. | on |
volume_change [double] |
A factor that is used to change the volume in NPT MC simulations. |
2.5 -- Frenkel's value. |
vcp_factor [double] |
A factor used to calculate the probability of doing a volume change in NPT. |
1.0 -- Frenkel's value. |
displace_factor [double] |
A factor (length in Angstroms) used to calculate random translations of molecules in MC simulations. | 1.0 |
insert_factor [double] |
The probability of doing an insert/delete move in uVT MC simluations. | 0.5 |
rotate_angle_factor [double] |
A factor used to calculate a random angle of rotation for displacement in MC simluations. | 360.0 |
mc_pbc [on|off] |
Enables periodic-boundary conditions. | on |
total_energy [double] |
Potential energy in K as fixed value for NVE simulations. (Should usually be negative!). | NONE |
simulated_annealing [on|off] |
Option for simulated annealing. | off |
simulated_annealing_schedule [double] |
A factor for exponentially decreasing temperature in S.A. | 0.9999 |
simulated_annealing_target [double] |
Target end-temperature (in Kelvin) for simulated annealing. | 0.0 |
fugacity_single [h2|co2|n2|ch4] |
in uVT, specifies the molecule to calculate fugacity (from input pressure) at startup. | NONE |
step_offset [int] |
An offset value for Monte Carlo steps, e.g. to pickup restarts and count where you left off. | 0 |
auto_reject_option [on|off] |
Enables auto-reject feature which can speed up Monte Carlo, forced off for Molecular Dynamics. Only useful when using at least the LJ potential. |
on |
auto_reject_r [double] |
Parameter in Angstroms to auto-reject moves if a pair distance is less than this value. | 0.76 |
feynman_hibbs [on|off] |
Enables Feynmann-Hibbs Quantum corrections to energy calculation (useful especially for small molecules e.g. hydrogen). | off |
fh_order [2|4] |
Chooses second or fourth order correction for Feynman-Hibbs corrections. | 4 |
Command | Description | Default |
---|---|---|
integrator [rk4|vv] |
The method for integrating Newton's equations of motion. rk4 = Runge Kutte 4th order; vv = Velocity verlet. |
vv |
md_corrtime [int] |
The step interval at which output is generated, averages re-calculated, etc. | 50 |
md_pbc [on|off] |
Enables periodic-boundary conditions. | on |
md_init_vel [double] |
User defined initial velocities for movable molecules. Will randomize directions based on this magnitude in A/fs. If this is not supplied, initial velocities will be determined from temperature. | NONE |
md_dt [double] |
The actual time step used for Molecular Dynamics, in fs. | 0.1 |
md_ft [double] [string] |
The time to stop the simulation. Units can be fs, ps, ns, us, or ms. | 10000 fs |
md_mode [molecular|atomic] |
MD mode. molecular keeps molecules rigid, intact, and allows them to rotate. atomic treats all atoms as free-moving regardless of assignment in input_atoms file. flexible enables bonding parameters for movable molecules. |
molecular |
md_rotations [on|off] |
Enables molecular rotations in MD. | on |
md_translations [on|off] |
Enables molecular translations in MD. Turning this off is useful, for example, with molecular crystal simulation. | on |
cuda [on|off] |
Enables GPU-accelerated Molecular Dynamics (by calculating forces on GPU). Only compatible with CUDA GPUs. | off |
cuda_block_size [int] |
Specifies threads-per-block for CUDA parallel computation. Good values are typically multiples of the common warp size, 32. | 256 |
md_insert_frequency [int] |
Interval number of steps at which to attempt an insert/delete in uVT MD. | 20 |
calc_pressure_option [on\off] |
Enables virial pressure calculator (NVT ensemble only). |
on for NVT; off for others. |
external_force [double] [double] [double] [int] |
Applies a constant external force to all movable molecules. Expressed as a vector (x,y,z) in nanoNewtons nN followed by an integer of how often (in steps) the force should apply. 1.0 0 0 1 is a moderate force in the +x direction for molecules applied every step. |
0.0 0.0 0.0 1 |
sorbate_dofs [int,int,...] |
Manually enter the number of degrees of freedom for each prototype movable molecule. | NONE |
kspace_option [on|off] |
Enables computation of Ewald k-space (long-range) forces in MD. | on |
input_structure_ff [on|off] |
Option to use the input atomic structure for equilibrium bondlength, angle and dihedral parameters. If off, MCMD defaults to UFF/UFF4MOF parameters. | off |
thermostat [andersen|nose-hoover] |
Chooses a thermostat for NVT MD simulation. nose-hoover cannot be used for uVT MD simulation. |
nose-hoover |
nh_q [double] |
Manually set the Nose-Hoover Q parameter in K fs^2. |
none |
nh_q_scale [double] |
Scale the Nose-Hoover Q parameter by this factor. Recommended values 0.8 - 2.0 . |
1.0 |
Command | Description | Default |
---|---|---|
opt_mode [mc|sd] |
Optimization method: mc = Monte Carlo; sd = Steepest Descent. |
sd |
bondlength [double] |
Assigns maximum distance, in Angstroms, to dynamically define bonds. | 1.5 |
opt_convergence [double] |
Assigns the convergence delta-energy, in kcal/mol. | 0.00001 |
opt_step_limit [int] |
Assigns maximum number of optimization steps for convergence. | 10000 |
opt_bonds [on|off] |
Includes bonded stretching for optimization/flexible MD calculation. | on |
opt_angles [on|off] |
Includes angle bending for optimization/flexible MD calculation. | on |
opt_dihedrals [on|off] |
Includes dihedral bending (torsions) for optimization/flexible MD calculation. | on |
opt_LJ [on|off] |
Includes non-bonded Lennard-Jones interactions for optimization/flexible MD calculation. | on |
opt_ES [on|off] |
Includes non-bonded electrostatic interactions for optimization/flexible MD calculation. | on |
Command | Description | Default |
---|