Miscellaneous and Debugging Opcodes
The opcodes in this section are linked below:
GEOM — obtain GEOMetric information about the molecule
TIME — report cpu TIME (user+system)
NPRC — Number of PRoCessors (distributed MacroModel calculations)
DEBG — DEBuGging
Turn on program debug switch (numbered 1-1100). Use as many of these commands as necessary to turn on as many of the switches as you want.
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arg1-4 |
Debug switches |
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Values currently in use are listed below. “GV” stands for “Greater Verbosity.” Flags described with this abbreviation affect only the level of reporting; other flags affect program action. |
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1 |
GV, all commands |
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2 |
Don’t line-buffer |
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3 |
Always write full (never compressed) output files |
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5 |
GV, dynamic allocation |
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6 |
Always write old-style (mmio) files |
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7 |
Always write new-style (m2io) files |
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8 |
GV, correspondence between mainCT and sbstrCT numbering |
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9 |
GV, handling of mmio/m2io files |
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10 |
GV, RWND command |
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11 |
Get formal charge from |
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12 |
Don’t set qq product to zero, VDWB nonbondeds |
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13 |
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14 |
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15 |
GV, reading charges from ffld substructures |
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16 |
GV, VDW offset from ffld |
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17 |
Suppress elimination of constrained-atom mutual interactions |
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18 |
GV, charge delocalization |
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19 |
GV, number of matches, each ffld substructure in mol |
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20 |
GV, name of each ffld substr matched in mol, and atom #s |
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21 |
GV, more details on how each ffld substr matched mol |
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22 |
GV, write problematic structure to output structure file if MINI fails |
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23 |
GV, write MINI structure to output structure file at each MINI display interval. Incompatible with DRIV. |
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25 |
Don’t refuse to minimize extremely strained structures |
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27 |
GV, TNCG, FMNR MINI methods |
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28 |
Suppress elimination of stretching and bending interactions in which some of the atoms are fixed. |
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30 |
GV, MINI line search |
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31 |
GV, MINI gradient to log file, each iteration |
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32 |
Don’t use constant derivatives in line searching |
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33 |
Don’t separate close pairs during interaction generation |
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34 |
GV, tests for distorted sp3 atom and for chirality |
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35 |
Do write output |
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36 |
GV, do not limit the number of messages from close separation problems |
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37 |
Note that if separation of close pairs fails in a conformational search reject the structure and continue the search |
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38 |
Skip tests for distorted sp3 atoms. |
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40 |
GV, early in force-field (eqn. reading, etc.) |
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41 |
GV, BMFF IPC layer (client and server side) |
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42 |
GV, BMFF server |
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43 |
GV, BMFF-related stuff within MacroModel |
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44 |
GV, applying mmlewis and obtaining OPLS_2005 parameters |
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45 |
Do not delete dummy atoms for OPLS4. Dummy atoms are correctly handled in OPLS4. |
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46 |
Don’t use fast vdw and hbd BMFF processing |
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49 |
Don’t skip over structures that do not have all force field and solvation parameters. Stop when such a structure is encountered. |
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50 |
GV, parsing of |
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51 |
LV, parameter assignment |
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55 |
Don’t compare the connectivity of the input structure with the previous structure, but treat it as chemically different from the previous structure. |
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56 |
Don’t eliminate torsional interactions with V’s of 0 |
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57 |
Always consider input structures to be distinct CT’s, not conformations. This implies full interaction generation for each structure read in. |
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58 |
GV, when which classes of params are updated (Bonded, VDW, Geom-dependent, solvation) |
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59 |
GV, geom-dependent params & updating |
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60 |
GV, |
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61 |
GV, stretch interactions |
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62 |
GV, bend interactions |
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63 |
GV, torsional interactions |
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64 |
GV, nonbonded interactions |
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65 |
GV, bend-bend interactions |
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68 |
GV, |
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69 |
GV, |
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70 |
GV, fixed atom interactions |
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71 |
GV, parameters that change during FEP |
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72 |
GV, atoms whose surface areas change during FEP |
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73 |
Don’t eliminate str/bend involving dummy atoms or zero-order bonds in |
FEP accumulation |
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74 |
Exclude all str/bend terms from FEP accumulation |
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78 |
Calculate normal modes only for SUBS atoms in LMOD and LLMOD calculations |
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79 |
ATEQ, also consider noncyclic permutations of the |
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81 |
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82 |
GV, Comparing structures for uniqueness |
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83 |
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85 |
Use |
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86 |
Use current rather than ideal str and bend distances in computing constant part of analytical GB radius |
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87 |
GV, atom-wise solvation data to |
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88 |
GV, read |
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89 |
Don’t unite all-atom sp3 CHn groups for solvation |
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90 |
Include explicit hydrogens in GB-radius calculation |
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91 |
Use old (Hasel et al.) method for analytical surfaces |
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92 |
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93 |
Turn off surface-area 3-body function |
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94 |
GV, saddle point search. Also, write intermediate structures to output structure file. |
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95 |
Use all-atom representation in surface calcs (assuming molecule actually has H’s and/or lone pairs) |
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96 |
Ignore long range shells in numerical Born rad. calc |
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97 |
GV, solvation energy calc |
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98 |
GV, parameters for overlap array, solvation calc |
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99 |
GV, analytical and numerical GB radii and Gpol values for fixed atoms |
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100 |
Set negative areas to zero in LCPO surface calculation |
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101 |
GV, MD or MC monitor of PE avg, sd, skew and kurtosis |
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102 |
GV, timings, MD and MINI |
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103 |
Turn off adaptive mechanism for number of Monte Carlo degrees of freedom during MCSD, MCLO, IMPS |
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104 |
After MD “Abort,” continue with remainder of |
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105 |
Do not do LCPO Buried Atom Elimination (BAE) |
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106 |
GV, SHAKE |
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107 |
Do not do neighbor-list reduction (NLR) on LCPO overlap array |
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108 |
GV, write LCPO ELST |
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111 |
GV, general dynamics & MC |
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112 |
GV, write every 200th non-matching IMPS structure to output structure file |
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121 |
GV, BDCO pairlist generation |
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126 |
GV, BDCO total charge product |
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127 |
GV, BDCO pairwise charge product assignment |
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128 |
GV, more BDCO pairwise charge product assignment |
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129 |
GV, force field substructure explicit partial charge processing |
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130 |
GV, CHGF input structure file explicit partial charge to delocalized formal charge + bond charge increment decomposition |
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131 |
GV, details of lone-pair requirements for current ffld, mol |
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141 |
GV, structures accepted, etc., MC csearch |
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150 |
During dihedral driving start each incremental minimization from the initial structure as read from the filename |
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152 |
GV, interaction array changes from nonbonded update, MINI |
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169 |
GV, torsional angles stored by torsional memory |
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178 |
Use MacroModel-supplied random-number function |
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179 |
GV, print seed to log file each time random-number generator called |
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180 |
GV, movements used to generate new Monte Carlo structures |
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181 |
GV, internal coords used in tors MC and MCSD simulations |
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182 |
GV, internal coords, final limits after tors MC run |
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183 |
GV, internal coord changes at each tors MC acceptance |
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184 |
In MC, calculate total E, not just MC-variable E components |
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185 |
Allow JBW in substructures—for internal use only |
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186 |
Don’t reorient each output structure to best superimpose on input |
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187 |
GV, For IMPS, write each input structure to output, after zmat superposition of the first three atoms onto those of the first structure. Requires user specification of |
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188 |
Skip problematic ring closure rotations. This may result in chirality switches if CHIG commands are not applied to the two central atoms in the ring closure. |
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191 |
Don’t record OPLS-AA formal charges or bond orders in the output structure file. Use the ones from the input structure file. |
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200 |
GV, CGEN searches |
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202 |
Override force field setting for ConfGen. |
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210 |
GV, mass-weighted force-constants, RRHO command |
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211 |
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222 |
GV, write starting structure for each MINI to output structure file |
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230 |
GV, COPY opcode |
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235 |
GV, ALGN opcode, general |
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236 |
GV, ALGN opcode, center of mass operations |
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237 |
GV, ALGN opcode, principal axis operations |
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251 |
GV, “torsional memory” during conformation search |
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252 |
GV, conformational search of ring structures |
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333 |
GV, network-distributed processing using the |
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358 |
GV, geometrical pre-optimization of ring structures |
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360 |
Turn off use-directed csearch initialization from filename |
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370 |
Enable MOLS for molecules containing fixed atoms |
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400 |
GV, importance sampling |
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500 |
GV, source CT number tracking for Maestro project facility properties |
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510 |
Do not enforce properties dependencies (i.e., do not clear properties when the structure changes) In Embrace calculations it is turned on by default. Use arg4 of MBAE to turn it off. |
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511 |
GV, the process for recording properties |
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512 |
Do not add dependencies to MacroModel Properties that lack them. |
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513 |
Record energy components in the output structure file. This flag is on by default; use |
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514 |
Do not record energy components in output structure file. Turns |
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520 |
Basic reporting for Automatic setup (AUTO) |
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521 |
GV, reporting for Automatic setup (AUTO) and turn on |
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530 |
Record the structure for each molecule in both solvents for |
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531 |
GV, for LOGP calculations |
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550 |
GV, MBAE |
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555 |
GV, LOOP |
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570 |
Don’t turn on |
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601 |
Turn off writing to output structure file unless explicit WRIT is used |
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602 |
If old-style titles are detected in a Maestro-formatted input structure file, do not update them. |
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720 |
GV, 1st and second derivs of Wilson angle OOP terms |
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725 |
Turn off constant long-range nonbonded derivs |
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726 |
Turn off constant long-range polarization solvation terms |
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727 |
Turn off constant long-range surface-area solvation terms |
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800 |
Don’t regenerate solvation overlap array after MC accept |
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820 |
Set all atomic weights to 12 for dynamics, inc. FEP |
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825 |
Don’t correct tiny denom. in analytical solvation derivs |
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830 |
Don’t correct Gpol,i' for nonbonded pairs left off the nonbonded pairlist |
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832 |
Don’t correct Gpol,i' for F-F nonbonded pairs which are farther apart than the nonbonded cutoff |
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F = (a) fixed without flat bottom well or (b) frozen |
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835 |
GV, final Gpol,i' values for all atoms |
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836 |
GV, generalized Born CCF (Close Contact Function). Available only with single precision energies) |
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899 |
GV, FlexLM licensing general |
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900 |
GV, print RCS versions of source files used in compilation |
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901 |
GV, detailed tables of COMMON memory utilization |
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902 |
GV, table of atom info (regurgitation of |
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903 |
GV, table of atomic masses by atom number |
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920 |
Low-mode search (LMCS or LMC2), write perturbed structures in output structure file |
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930 |
Do not check for |
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931 |
Turns |
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940 |
GV, for network-distributed MacroModel jobs using the |
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950 |
GV, on IBM SP2, save file written by parallel threads |
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960 |
Turn off reporting of format problems in the |
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961 |
Cause MacroModel to stop if a format problem is found in the |
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975 |
Do not use atomic number information from the input file. Instead, obtain the atomic number information from the atom type. |
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999 |
GV, ARPK |
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1000 |
GV, give CPU timings in energetic routines. Now gives more detailed and informative output. |
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1001 |
GV, MINTA free-energy calculation. |
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1002 |
Turn off distance check on 1-3 atoms. Structures in which two atoms that are bonded to a third atom but not to each other are rejected by default if the two atoms are closer than 1 Å. |
DUMP — DUMP connection table
List the connection table to the log file (used primarily for testing purposes).
GEOM — obtain GEOMetric information about the molecule
The GEOM command allows the user to obtain geometric information about the molecule from the MacroModel command file. Bond lengths, bond angles, and dihedral angles are written as properties to the log file.
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arg1 |
Atom 1 |
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If arg1 is nonzero and arg2 is zero, then |
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arg2 |
Atom 2 |
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If arg1 and arg2 are nonzero and arg3 and arg5 are zero, |
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arg3 |
Atom 3 |
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If arg1, arg2, and arg3 are nonzero and arg4 is zero, |
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arg4 |
Atom 4 |
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If arg1, arg2, arg3, and arg4 are nonzero, |
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arg5 |
Spin-spin coupling constant |
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If arg5 > 0,
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If either of the first two conditions is not met, a warning is printed and the calculation continues without calculating the coupling constant. |
TIME — report cpu TIME (user+system)
The TIME command reports CPU time (user+system) since the previous invocation of TIME, or (on the first invocation) since program start. See also DEBG 1000 for more detailed and informative output on task timings.
JWRT — Journal WRiTe
The JRED and JWRT commands are provided in order to use MacroModel as a force-field server in connection with procedures being carried out by other processes. JWRT writes out a user-specifiable combination of coordinates, energy, gradient, and Hessian in binary form that the co-process can read. JRED reads in coordinates in a similar format that have been written out by the co-process. Thus, the co-process can provide coordinates to MacroModel, instruct it to compute the energetic terms, read back those energetic terms, manipulate the molecule, and complete the cycle. The way this facility is provided now, MacroModel has to be launched anew for each new calculation (for example, by a system() call from the client process); however, we may later enhance this facility to make it more fully interactive.
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arg1 |
Write coordinates |
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If arg1 is nonzero, write out the coordinates. |
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arg2 |
Write energy |
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If arg2 is nonzero, write out the energy. |
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arg3 |
Write gradient |
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If arg3 is nonzero, write out the gradient. |
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arg4 |
Write Hessian |
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If arg4 is nonzero, write out the Hessian. |
The filename used is filename.jwr, where filename is the prefix of the input filename. The file is opened with FORM=UNFORMATTED, but is sequential. All variables are written in double precision. Thus, if all four args are nonzero, and if there are N atoms in the part of the system being simulated (the whole system, unless SUBS is used with FXAT and all atoms are not covered by these commands), the .jwr file will contain 3N coordinates, in sequence x(1), y(1), z(1), x(2), ..., z(N), followed by one double precision value for the energy, followed by 3N gradient components, followed by (3N)2 Hessian elements, in order x(1)x(1), y(1)x(1), z(1)x(1), x(2)x(1), ..., y(N)z(N), z(N)z(N).
JRED — Journal REaD
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arg1 |
Read coordinates |
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If arg1 is nonzero, read the coordinates. |
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arg2 |
Read energy |
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If arg2 is nonzero, read the energy. |
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arg3 |
Read gradient |
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If arg3 is nonzero, read the gradient. |
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arg4 |
Read Hessian |
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If arg4 is nonzero, read the Hessian. |
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arg5 |
Print values read |
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If arg5 is nonzero, whatever is read will be printed to the |
JRED works as follows. It expects to read a file called filename.jrd, where filename is the stem of the input file name. For the purpose of debugging the JWRT command, args1-4 cause JRED to read the coordinates, the energy, the gradient, and the Hessian, respectively, if nonzero. If arg5 is nonzero, whatever is read will be printed to the .log file.
NPRC — Number of PRoCessors (distributed MacroModel calculations)
Distribute the MacroModel job over a number of different hosts. The name of the hosts to use are taken from the file schrodinger.hosts, which must be in the $SCHRODINGER directory or the user’s working directory. The NPRC command can be used with the following kinds of calculations:
- Non-serial conformational searches
- Serial conformational searches
- MULT minimizations
- Free-energy perturbation calculations (FEAV, FESA)
- Embrace (MBAE) minimization and conformational search calculations
The types of non-serial conformational searches supported are: MCMM, LMCS, LMC2, mixed LMCS/MCMM, and mixed LMC2/MCMM. The types of serial searches supported are MCMM, LMCS, and mixed LMCS/MCMM. The AUTO command is required for serial MCMM and serial mixed LMCS/MCMM jobs, and is recommended for serial LMCS jobs. The procedure is split into a number of different searches and run on the hosts as they become available. In an MCMM procedure, a different SEED value is used on each host.
For MBAE energy difference calculations the initial receptor computations are conducted by the parent process prior to distributing the calculations for the ligands amongst the child processes. Because of the complexity of MBAE computations users are encouraged to consult the description of the MBAE opcode in this manual and the examples of MBAE calculations in Command File Examples for Embrace.
See Running Remote and Distributed MacroModel Calculations for a description of internally-distributed MacroModel calculations which use NPRC and see Preparing for Remote Job Submission (DEPRECATED) for information on setting computers and accounts to permit distributed MacroModel calculations.
If a requested host becomes unavailable during a run, its status is checked periodically. If the host later becomes available, the process starts using it again. Exception: hosts unavailable at startup time are removed from the list of allowed hosts and never re-used. This is because a host that was unavailable at the start of the job cannot have been checked for energetic consistency (see arg4 below), and using it without this test having been performed is potentially dangerous.
DEBG 333 gives greater verbosity; DEBG 940 saves, rather than discards, the output files of the intermediate jobs.
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arg1 |
Number of hosts to check for availability |
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arg1 specifies how many hosts in the |
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For example, if the |
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arg2 |
Job size |
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For non-serial searches arg2 specifies the number of steps from the search that should be carried out by each job. The total number of steps is the number given by arg1 of the search command (i.e. arg1 of MCMM, LMCS, or LMC2) and the total number of jobs is roughly given by arg1 of the search command divided by arg2 of |
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For serial calculations, such as minimizations of multiple input structures and serial searches this argument specifies the number of input structures given to each job for minimization or searching. In serial searches separate searches are conducted for each structure in the input structure file. Serial searches can be conducted for MCMM, LMCS, LMC2, mixed LMCS |
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If the total number of jobs is significantly larger than some small multiple of the number of hosts specified by arg1 of |
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0 |
For non-serial searches, set the number of steps per job to the total number of steps for the search divided by the number of processors (arg1). |
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For serial searches, set the number of structures to process per job to the number of structures in the input structure file divided by the number of processors. |
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In either case, this setting is sub-optimal since no load balancing can be carried out. |
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arg3 |
Sleep time (sec) |
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The time in seconds that the “master” MacroModel process will sleep before checking on the progress of the “slave” jobs. |
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0 |
60 seconds. This is a reasonable value. |
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arg4 |
Energy-test control |
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0 |
Perform no energy tests. |
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1 |
Perform energy tests; this is highly recommended. |
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Prior to starting the distributed job, an energy calculation on the starting structure is performed on each processor. The resulting energies are compared. If any value differs from that on the current processor by more than 0.001 kJ/mol or 0.1% (whichever is smaller), the user is notified and the job is terminated. This is to make sure that the version of MacroModel and the associated solvent and force-field files are the same on all hosts. |
SPAT — SPecial Atom Treatment
This opcode is used to instruct MacroModel how to proceed when it encounters certain atom types.
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arg1-4 |
Atom types to be flagged |
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Specify which atom types are flagged by MacroModel for special treatment. See MacroModel Atom Types for a listing of MacroModel atom types. |
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arg5 |
Action to be taken on flagged atom types |
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1 |
Instructs MacroModel to stop when it encounters any of the atom types specified in args 1-4. |
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Multiple |