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| 1 | +; VARIOUS PREPROCESSING OPTIONS |
| 2 | +; Preprocessor - specify a full path if necessary. |
| 3 | +include = |
| 4 | +define = |
| 5 | + |
| 6 | +; RUN CONTROL PARAMETERS |
| 7 | +integrator = md |
| 8 | +; Start time and timestep in ps |
| 9 | +tinit = 0 |
| 10 | +dt = 0.001 |
| 11 | +nsteps = 10000000 |
| 12 | +; For exact run continuation or redoing part of a run |
| 13 | +init_step = 0 |
| 14 | +; mode for center of mass motion removal |
| 15 | +comm-mode = Linear |
| 16 | +; number of steps for center of mass motion removal |
| 17 | +nstcomm = 10 |
| 18 | +; group(s) for center of mass motion removal |
| 19 | +comm_grps = System |
| 20 | + |
| 21 | + |
| 22 | +;periodic-molecules = yes |
| 23 | + |
| 24 | +; LANGEVIN DYNAMICS OPTIONS |
| 25 | +; Friction coefficient (amu/ps) and random seed |
| 26 | +ld-seed = 1993 |
| 27 | + |
| 28 | +; OUTPUT CONTROL OPTIONS |
| 29 | +; Output frequency for coords (x), velocities (v) and forces (f) |
| 30 | +nstxout = 0 |
| 31 | +nstvout = 0 |
| 32 | +nstfout = 0 |
| 33 | +; Output frequency for energies to log file and energy file |
| 34 | +nstlog = 1000 |
| 35 | +nstenergy = 1000 |
| 36 | +; Output frequency and precision for xtc file |
| 37 | +nstxtcout = 5000 |
| 38 | +xtc-precision = 1000 |
| 39 | +; This selects the subset of atoms for the xtc file. You can |
| 40 | +; select multiple groups. By default all atoms will be written. |
| 41 | +xtc_grps = System ;Protein |
| 42 | +; Selection of energy groups |
| 43 | +energygrps = System |
| 44 | + |
| 45 | +; NEIGHBORSEARCHING PARAMETERS |
| 46 | +; nblist update frequency |
| 47 | +cutoff-scheme = verlet |
| 48 | +nstlist = 10 |
| 49 | +; ns algorithm (simple or grid) |
| 50 | +ns_type = grid |
| 51 | +; Periodic boundary conditions: xyz (default), no (vacuum) |
| 52 | +; or full (infinite systems only) |
| 53 | +pbc = xyz |
| 54 | +; nblist cut-off |
| 55 | +rlist = 1.2 |
| 56 | + |
| 57 | +; OPTIONS FOR ELECTROSTATICS AND VDW |
| 58 | +; Method for doing electrostatics |
| 59 | +coulombtype = cut-off |
| 60 | +rcoulomb-switch = 0 |
| 61 | +rcoulomb = 1.2 |
| 62 | +; Relative dielectric constant for the medium and the reaction field |
| 63 | +epsilon_r = 1 |
| 64 | +epsilon_rf = 1 |
| 65 | +; Method for doing Van der Waals |
| 66 | +vdwtype = cut-off |
| 67 | +; cut-off lengths |
| 68 | +rvdw-switch = 0 |
| 69 | +rvdw = 1.2 |
| 70 | +; Apply long range dispersion corrections for Energy and Pressure |
| 71 | +DispCorr = No |
| 72 | +; Extension of the potential lookup tables beyond the cut-off |
| 73 | +table-extension = 1.0 |
| 74 | +; Seperate tables between energy group pairs |
| 75 | +;energygrp_table = A A |
| 76 | +; Spacing for the PME/PPPM FFT grid |
| 77 | +fourierspacing = 0.12 |
| 78 | +; FFT grid size, when a value is 0 fourierspacing will be used |
| 79 | +fourier_nx = 0 |
| 80 | +fourier_ny = 0 |
| 81 | +fourier_nz = 0 |
| 82 | +; EWALD/PME/PPPM parameters |
| 83 | +pme_order = 4 |
| 84 | +ewald_rtol = 1e-05 |
| 85 | +ewald_geometry = 3d |
| 86 | +epsilon_surface = 0 |
| 87 | +optimize_fft = no |
| 88 | + |
| 89 | +; OPTIONS FOR WEAK COUPLING ALGORITHMS |
| 90 | +; Temperature coupling |
| 91 | +tcoupl = V-rescale; No ;Nose-Hoover |
| 92 | +; Groups to couple separately |
| 93 | +tc-grps = System |
| 94 | +; Time constant (ps) and reference temperature (K) |
| 95 | +tau_t = 1.0 |
| 96 | +ref_t = 423 |
| 97 | +; Pressure coupling |
| 98 | +Pcoupl = No ;Parrinello-Rahman |
| 99 | +pcoupltype = isotropic |
| 100 | +; Time constant (ps), compressibility (1/bar) and reference P (bar) |
| 101 | +tau_p = 0.5 |
| 102 | +compressibility = 4.5e-5 |
| 103 | +ref_p = 1.0 |
| 104 | +; Random seed for Andersen thermostat |
| 105 | +andersen_seed = 815131 |
| 106 | + |
| 107 | + |
| 108 | +; GENERATE VELOCITIES FOR STARTUP RUN |
| 109 | +gen_vel = yes |
| 110 | +gen_temp = 423 |
| 111 | +gen_seed = -1 |
| 112 | + |
| 113 | +; OPTIONS FOR BONDS |
| 114 | +constraints = none |
| 115 | +; Type of constraint algorithm |
| 116 | +constraint_algorithm = LINCS |
| 117 | +; Use successive overrelaxation to reduce the number of shake iterations |
| 118 | +Shake-SOR = no |
| 119 | +; Relative tolerance of shake |
| 120 | +shake-tol = 1e-04 |
| 121 | +; Highest order in the expansion of the constraint coupling matrix |
| 122 | +lincs-order = 4 |
| 123 | +; Number of iterations in the final step of LINCS. 1 is fine for |
| 124 | +; normal simulations, but use 2 to conserve energy in NVE runs. |
| 125 | +; For energy minimization with constraints it should be 4 to 8. |
| 126 | +lincs_iter = 2 |
| 127 | +; Lincs will write a warning to the stderr if in one step a bond |
| 128 | +; rotates over more degrees than |
| 129 | +lincs-warnangle = 30 |
| 130 | +; Convert harmonic bonds to morse potentials |
| 131 | +morse = no |
| 132 | + |
| 133 | +; ENERGY GROUP EXCLUSIONS |
| 134 | +; Pairs of energy groups for which all non-bonded interactions are excluded |
| 135 | +energygrp_excl = |
| 136 | + |
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