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📁 分子动力学模拟程序
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v2.1NVT ensemble (v2.1)  Essential reorganisation of force calculations (v2.4)NPT ensemble (v3.0)            optimization of Ewald sum calculations (v3.3)complex DNA-like molecules (v3.5)                 non-cubic (rectangular) cell (v3.6)hydrogen bonds included (10-12 potential) (v3.7)first parallel version (v3.8)    universal code for sequential and parallel executions  (v3.9) v4.0- fully parallelized code, including particle movingcorrected small bug in calculations of type-type intermolecular energies.(there were different weight from the short and long forces) v 4.1  - new format on the input file (free format with commentaries instead  of NAMELIST)- slightly changed format of .mol files - readind of initial atom or molecular center of mass coordinates   from a file included - special LJ parameters for 1-4 intramolecular interactions   - Morse potential for arbitrary bonds       - Sum(cos(fi)**n) type of torsion potential (for hydrocarbon chains)- Improper dihedral angles potential v.4.2- improved memory-saving algorithm. All two-dimensionl arrays A(NS,NS)where NS is the total number of different sites on molecules are removed without noteciable increasing of computation time.- option for separate pressure control in each direction. Components Pxx,Pyy,Pzz of the pressure tenzor are coupled to the Nose-Hoover thermostat separately (non diagonal terms of the pressure tensor are supposed to be 0). Do not use the option for isotropic systemsin which nothing prevent the system to shrink the size in one direction andincrease it in another while keeping the volume (and pressure) constant.- reaction field method for treatment of electrostatic interactions,including "generalised reaction field" method for non-zero ionic strength(I.G.Tironi, R.Sperb, P.E.Smith, W.F.van Gunsteren, J.Chem.Phys.,102,5451(1995))- cell of truncated octahedron geometry:  |x| < L/2 ; |y| < L/2 ;  |z| < L/2 ; |x|+|y|+|z| < 0.75*L- cell oh hexagonal geometry- If Ewald method for electrostatic interactions is not used, the listof neighbours for atoms on small molecules (Natoms <= 5) is defined fromthe distance between molecular centre-of-mass, that is the whole molecules occur within or out cut-off. In other cases, as before, list of neigboursfor each atom is determined from distances between the atoms. 21.10.97  Bug in pressure calculations in the case of parallel implementationof constrain dynamics (SHAKE) is removed.  v.4.2 -> 4.3------------In v.4.3 most of the subroutines were essentially regrouped into new filesSee details in file READMEA lot of comments were inserted into the code.The MD algorithm for NVT or NPT ensemble was rewritten according to "modular-invariant" version of the Nose-Hoover thermostat, see   of G.J.Martyna, D.J.Tobais and M.L.Klein,  J.Chem.Ohys., v.101(5), p.4177 (1994)  Some work has still to be done for the case of constrained dynamics (it works now, but not in the complete correspondence to the paper cited above)  04.03.98  Several small bugs were corrected:  in mpi.f procedure: addressing to NUMTASK (nonexistent) node whichsometimes happened in SINHR subroutine is removed(this might cause crash of the program; otherwise it worked )  in supl.f, TESTCONF - did not catch before all bad configurations  "molecular" pressure in the double time step algorithm now calculatedcorrectly.  Cray specific files were added  (mpi_cray.f, getcpucr.c and Makekefiles12.04.98 A new possibility to add options in the input file is introduced:  After lines defining unit vector (just before lines which defines RDFs)  one can write   add <n>  where n is number of additional options. Then follows n lines defining  additional options    Now following extra options difined:   inputf   - read restart file in ASCII format  outputf  - write restart file in ASCII format  no aver  - do not calculate averagre bond lenghts, angles and torsions.             this may save a lot of memory while simulating large	    macromolecules	    More detailed description of additional options is in file Extra_param 11.01.99  Option "Cut large forces" (see "MD.input")  is now working  22.02.99  File prcm.h is divided into two parts:    dimpar.h defines sizes of working arrays (may be customized)  prcm.h - the rest of old prcm.h file (should not be changed)26.04.99   Utility "makemol" to generate .mol files from "simple molecule file".smol and force field database is added. See Makemol.doc for details.22.06.99   projections of time correlation functions may be now calculated both   in the laboratory and in the molecular priuncipal coordinate systems  (flags 1 or 2 for corresponding tcf-s in the input file)  22.08.01  Kong combination rules for Lennard-Jones cross-interactions are introduced  (J. Kong, J.Chem.Phys., 59, 2464 (1973)). See ExtraParam file.  15.02.05  Option for reading start-up configuration has changed.  Value "0" now reads input coordinates in "XMOL" format while  value "-2" reads atom coordinates as three columnns X Y Z with  optional commentaries  v. 4.4      Possibility of separate Nose thermostat for each molecular species.  Separate temperature control over species (Nose or velocity scaling)   is now switched on by extra parameter  "T-sep" (see file Extra_param)   Out-cutoff correction for energy and pressure now correct.  It was too small (by factor between 2pi and 4pi) in older version  Thermostat/barostat algorithm with constraint dynamics - algorithm  rewritten.   XMOL trajectory file includes now information on the box sizes  in the commentory lines    Tranal:   now can read trajectories in MDynaMix binary format, XMOL format  (provided second line contains time in fs) and PDB trajectories from GROMACS    2005-12-01  Expanded ensemble version of the program is updated (mdee). It not  implements most of the features of MDynaMix except parallelization   

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