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:-) GROMACS - gmx mdrun, 2019.1 (-:
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GROMACS is written by:
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Emile Apol Rossen Apostolov Paul Bauer Herman J.C. Berendsen
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Par Bjelkmar Christian Blau Viacheslav Bolnykh Kevin Boyd
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Aldert van Buuren Rudi van Drunen Anton Feenstra Alan Gray
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Gerrit Groenhof Anca Hamuraru Vincent Hindriksen M. Eric Irrgang
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Aleksei Iupinov Christoph Junghans Joe Jordan Dimitrios Karkoulis
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Peter Kasson Jiri Kraus Carsten Kutzner Per Larsson
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Justin A. Lemkul Viveca Lindahl Magnus Lundborg Erik Marklund
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Pascal Merz Pieter Meulenhoff Teemu Murtola Szilard Pall
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Sander Pronk Roland Schulz Michael Shirts Alexey Shvetsov
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Alfons Sijbers Peter Tieleman Jon Vincent Teemu Virolainen
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Christian Wennberg Maarten Wolf
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and the project leaders:
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Mark Abraham, Berk Hess, Erik Lindahl, and David van der Spoel
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Copyright (c) 1991-2000, University of Groningen, The Netherlands.
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Copyright (c) 2001-2018, The GROMACS development team at
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Uppsala University, Stockholm University and
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the Royal Institute of Technology, Sweden.
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check out http://www.gromacs.org for more information.
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GROMACS is free software; you can redistribute it and/or modify it
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under the terms of the GNU Lesser General Public License
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as published by the Free Software Foundation; either version 2.1
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of the License, or (at your option) any later version.
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GROMACS: gmx mdrun, version 2019.1
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Executable: /apps/broadwell/centos7/GROMACS/2019.1-intel-2018b-UArecipe/bin/gmx_mpi
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Data prefix: /apps/broadwell/centos7/GROMACS/2019.1-intel-2018b-UArecipe
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Working dir: /scratch/gromacs-2019/test2019
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Process ID: 22580
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Command line:
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gmx_mpi mdrun -ntomp 1 -s 0519.tpr -o /scratch/gromacs-2019/test2019/0519.trr -x /scratch/gromacs-2019/test2019/0519.xtc -cpo /scratch/gromacs-2019/test2019/0519.cpt -c /scratch/gromacs-2019/test2019/0519.gro -e /scratch/gromacs-2019/test2019/0519.edr -dhdl /scratch/gromacs-2019/test2019/0519.xvg -g /scratch/gromacs-2019/test2019/0519.log -px /scratch/gromacs-2019/test2019/0519.x.xvg -pf /scratch/gromacs-2019/test2019/0519.f.xvg -noconfout -rcon 0.7 -pin on -dds 0.9 -dlb auto -maxh 1
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GROMACS version: 2019.1
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Precision: single
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Memory model: 64 bit
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MPI library: MPI
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OpenMP support: enabled (GMX_OPENMP_MAX_THREADS = 64)
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GPU support: disabled
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SIMD instructions: AVX2_256
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FFT library: Intel MKL
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RDTSCP usage: enabled
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TNG support: enabled
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Hwloc support: hwloc-1.11.8
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Tracing support: disabled
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C compiler: /apps/noarch/intel-psxe/2018_update3/compilers_and_libraries_2018.3.222/linux/mpi/intel64/bin/mpiicc Intel 18.0.3.20180410
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C compiler flags: -march=core-avx2 -mkl=sequential -std=gnu99 -O3 -DNDEBUG -ip -funroll-all-loops -alias-const -ansi-alias -no-prec-div -fimf-domain-exclusion=14 -qoverride-limits
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C++ compiler: /apps/noarch/intel-psxe/2018_update3/compilers_and_libraries_2018.3.222/linux/mpi/intel64/bin/mpiicpc Intel 18.0.3.20180410
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C++ compiler flags: -march=core-avx2 -mkl=sequential -std=c++11 -O3 -DNDEBUG -ip -funroll-all-loops -alias-const -ansi-alias -no-prec-div -fimf-domain-exclusion=14 -qoverride-limits
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Running on 4 nodes with total 112 cores, 112 logical cores
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Cores per node: 28
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Logical cores per node: 28
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Hardware detected on host r1c04cn1.leibniz (the node of MPI rank 0):
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CPU info:
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Vendor: Intel
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Brand: Intel(R) Xeon(R) CPU E5-2680 v4 @ 2.40GHz
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Family: 6 Model: 79 Stepping: 1
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Features: aes apic avx avx2 clfsh cmov cx8 cx16 f16c fma hle htt intel lahf mmx msr nonstop_tsc pcid pclmuldq pdcm pdpe1gb popcnt pse rdrnd rdtscp rtm sse2 sse3 sse4.1 sse4.2 ssse3 tdt x2apic
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Hardware topology: Full, with devices
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Sockets, cores, and logical processors:
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Socket 0: [ 0] [ 1] [ 2] [ 3] [ 4] [ 5] [ 6] [ 7] [ 8] [ 9] [ 10] [ 11] [ 12] [ 13]
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Socket 1: [ 14] [ 15] [ 16] [ 17] [ 18] [ 19] [ 20] [ 21] [ 22] [ 23] [ 24] [ 25] [ 26] [ 27]
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Numa nodes:
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Node 0 (68600541184 bytes mem): 0 1 2 3 4 5 6 7 8 9 10 11 12 13
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Node 1 (68719476736 bytes mem): 14 15 16 17 18 19 20 21 22 23 24 25 26 27
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Latency:
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0 1
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0 1.00 2.10
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1 2.10 1.00
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Caches:
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L1: 32768 bytes, linesize 64 bytes, assoc. 8, shared 1 ways
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L2: 262144 bytes, linesize 64 bytes, assoc. 8, shared 1 ways
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L3: 36700160 bytes, linesize 64 bytes, assoc. 20, shared 14 ways
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PCI devices:
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0000:01:00.0 Id: 8086:1521 Class: 0x0200 Numa: 0
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0000:01:00.1 Id: 8086:1521 Class: 0x0200 Numa: 0
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0000:02:00.0 Id: 15b3:1013 Class: 0x0207 Numa: 0
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0000:00:11.4 Id: 8086:8d62 Class: 0x0106 Numa: 0
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0000:07:00.0 Id: 1a03:2000 Class: 0x0300 Numa: 0
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0000:00:1f.2 Id: 8086:8d02 Class: 0x0106 Numa: 0
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++++ PLEASE READ AND CITE THE FOLLOWING REFERENCE ++++
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M. J. Abraham, T. Murtola, R. Schulz, S. Páll, J. C. Smith, B. Hess, E.
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Lindahl
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GROMACS: High performance molecular simulations through multi-level
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parallelism from laptops to supercomputers
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SoftwareX 1 (2015) pp. 19-25
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-------- -------- --- Thank You --- -------- --------
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++++ PLEASE READ AND CITE THE FOLLOWING REFERENCE ++++
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S. Páll, M. J. Abraham, C. Kutzner, B. Hess, E. Lindahl
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Tackling Exascale Software Challenges in Molecular Dynamics Simulations with
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GROMACS
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In S. Markidis & E. Laure (Eds.), Solving Software Challenges for Exascale 8759 (2015) pp. 3-27
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-------- -------- --- Thank You --- -------- --------
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++++ PLEASE READ AND CITE THE FOLLOWING REFERENCE ++++
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S. Pronk, S. Páll, R. Schulz, P. Larsson, P. Bjelkmar, R. Apostolov, M. R.
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Shirts, J. C. Smith, P. M. Kasson, D. van der Spoel, B. Hess, and E. Lindahl
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GROMACS 4.5: a high-throughput and highly parallel open source molecular
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simulation toolkit
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Bioinformatics 29 (2013) pp. 845-54
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-------- -------- --- Thank You --- -------- --------
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++++ PLEASE READ AND CITE THE FOLLOWING REFERENCE ++++
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B. Hess and C. Kutzner and D. van der Spoel and E. Lindahl
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GROMACS 4: Algorithms for highly efficient, load-balanced, and scalable
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molecular simulation
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J. Chem. Theory Comput. 4 (2008) pp. 435-447
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-------- -------- --- Thank You --- -------- --------
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++++ PLEASE READ AND CITE THE FOLLOWING REFERENCE ++++
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D. van der Spoel, E. Lindahl, B. Hess, G. Groenhof, A. E. Mark and H. J. C.
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Berendsen
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GROMACS: Fast, Flexible and Free
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J. Comp. Chem. 26 (2005) pp. 1701-1719
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-------- -------- --- Thank You --- -------- --------
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++++ PLEASE READ AND CITE THE FOLLOWING REFERENCE ++++
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E. Lindahl and B. Hess and D. van der Spoel
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GROMACS 3.0: A package for molecular simulation and trajectory analysis
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J. Mol. Mod. 7 (2001) pp. 306-317
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-------- -------- --- Thank You --- -------- --------
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++++ PLEASE READ AND CITE THE FOLLOWING REFERENCE ++++
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H. J. C. Berendsen, D. van der Spoel and R. van Drunen
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GROMACS: A message-passing parallel molecular dynamics implementation
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Comp. Phys. Comm. 91 (1995) pp. 43-56
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-------- -------- --- Thank You --- -------- --------
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++++ PLEASE CITE THE DOI FOR THIS VERSION OF GROMACS ++++
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https://doi.org/10.5281/zenodo.2564764
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-------- -------- --- Thank You --- -------- --------
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Input Parameters:
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integrator = md
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tinit = 0
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dt = 0.002
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nsteps = 500000
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init-step = 0
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simulation-part = 1
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comm-mode = Linear
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nstcomm = 100
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bd-fric = 0
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ld-seed = -1437393019
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emtol = 10
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emstep = 0.01
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niter = 20
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fcstep = 0
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nstcgsteep = 1000
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nbfgscorr = 10
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rtpi = 0.05
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nstxout = 0
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nstvout = 0
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nstfout = 0
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nstlog = 50000
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nstcalcenergy = 100
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nstenergy = 50000
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nstxout-compressed = 50000
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compressed-x-precision = 1000
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cutoff-scheme = Verlet
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nstlist = 20
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ns-type = Grid
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pbc = xyz
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periodic-molecules = false
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verlet-buffer-tolerance = 0.005
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rlist = 1.223
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coulombtype = PME
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coulomb-modifier = Potential-shift
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rcoulomb-switch = 0
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rcoulomb = 1.2
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epsilon-r = 1
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epsilon-rf = inf
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vdw-type = Cut-off
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vdw-modifier = Potential-shift
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rvdw-switch = 1
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rvdw = 1.2
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DispCorr = EnerPres
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table-extension = 1
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fourierspacing = 0.16
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fourier-nx = 96
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fourier-ny = 84
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fourier-nz = 80
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pme-order = 4
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ewald-rtol = 1e-05
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ewald-rtol-lj = 0.001
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lj-pme-comb-rule = Geometric
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ewald-geometry = 0
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epsilon-surface = 0
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tcoupl = V-rescale
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nsttcouple = 20
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nh-chain-length = 0
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print-nose-hoover-chain-variables = false
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pcoupl = Berendsen
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pcoupltype = Isotropic
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nstpcouple = 20
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tau-p = 2
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compressibility (3x3):
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compressibility[ 0]={ 4.50000e-05, 0.00000e+00, 0.00000e+00}
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compressibility[ 1]={ 0.00000e+00, 4.50000e-05, 0.00000e+00}
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compressibility[ 2]={ 0.00000e+00, 0.00000e+00, 4.50000e-05}
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ref-p (3x3):
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ref-p[ 0]={ 1.00000e+00, 0.00000e+00, 0.00000e+00}
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ref-p[ 1]={ 0.00000e+00, 1.00000e+00, 0.00000e+00}
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ref-p[ 2]={ 0.00000e+00, 0.00000e+00, 1.00000e+00}
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refcoord-scaling = COM
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posres-com (3):
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posres-com[0]= 0.00000e+00
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posres-com[1]= 0.00000e+00
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posres-com[2]= 0.00000e+00
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posres-comB (3):
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posres-comB[0]= 0.00000e+00
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posres-comB[1]= 0.00000e+00
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posres-comB[2]= 0.00000e+00
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QMMM = false
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QMconstraints = 0
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QMMMscheme = 0
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MMChargeScaleFactor = 1
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qm-opts:
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ngQM = 0
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constraint-algorithm = Lincs
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continuation = true
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Shake-SOR = false
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shake-tol = 0.0001
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lincs-order = 4
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lincs-iter = 1
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lincs-warnangle = 30
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nwall = 0
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wall-type = 9-3
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wall-r-linpot = -1
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wall-atomtype[0] = -1
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wall-atomtype[1] = -1
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wall-density[0] = 0
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wall-density[1] = 0
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wall-ewald-zfac = 3
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pull = true
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pull-cylinder-r = 1.5
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pull-constr-tol = 1e-06
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pull-print-COM = true
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pull-print-ref-value = true
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pull-print-components = true
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pull-nstxout = 50000
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pull-nstfout = 50000
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pull-pbc-ref-prev-step-com = false
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pull-xout-average = false
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pull-fout-average = false
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pull-ngroups = 3
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pull-group 0:
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atom: not available
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weight: not available
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pbcatom = -1
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pull-group 1:
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atom (1):
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atom[0]=1442
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weight: not available
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pbcatom = -1
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pull-group 2:
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atom (2):
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atom[0]=4641
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atom[1]=4643
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weight: not available
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pbcatom = 4641
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pull-ncoords = 1
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pull-coord 0:
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type = umbrella
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geometry = distance
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group[0] = 1
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group[1] = 2
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dim (3):
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dim[0]=1
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dim[1]=1
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dim[2]=1
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origin (3):
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origin[0]= 0.00000e+00
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origin[1]= 0.00000e+00
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origin[2]= 0.00000e+00
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vec (3):
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vec[0]= 0.00000e+00
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vec[1]= 0.00000e+00
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vec[2]= 0.00000e+00
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start = true
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init = 0.518654
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rate = 0
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k = 1000
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kB = 1000
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awh = false
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rotation = false
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interactiveMD = false
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disre = No
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disre-weighting = Conservative
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disre-mixed = false
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dr-fc = 1000
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dr-tau = 0
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nstdisreout = 100
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orire-fc = 0
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orire-tau = 0
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nstorireout = 100
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free-energy = no
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cos-acceleration = 0
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deform (3x3):
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deform[ 0]={ 0.00000e+00, 0.00000e+00, 0.00000e+00}
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deform[ 1]={ 0.00000e+00, 0.00000e+00, 0.00000e+00}
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deform[ 2]={ 0.00000e+00, 0.00000e+00, 0.00000e+00}
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simulated-tempering = false
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swapcoords = no
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userint1 = 0
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userint2 = 0
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userint3 = 0
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userint4 = 0
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userreal1 = 0
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userreal2 = 0
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userreal3 = 0
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userreal4 = 0
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applied-forces:
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electric-field:
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x:
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E0 = 0
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omega = 0
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t0 = 0
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sigma = 0
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y:
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E0 = 0
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omega = 0
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t0 = 0
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sigma = 0
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z:
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E0 = 0
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omega = 0
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t0 = 0
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sigma = 0
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grpopts:
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nrdf: 12909.9 439152
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ref-t: 300 300
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tau-t: 0.1 0.1
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annealing: No No
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annealing-npoints: 0 0
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acc: 0 0 0
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nfreeze: N N N
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energygrp-flags[ 0]: 0
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Changing nstlist from 20 to 80, rlist from 1.223 to 1.326
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Initializing Domain Decomposition on 112 ranks
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Dynamic load balancing: locked
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Using update groups, nr 76781, average size 2.9 atoms, max. radius 0.125 nm
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Minimum cell size due to atom displacement: 0.514 nm
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Initial maximum distances in bonded interactions:
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two-body bonded interactions: 0.443 nm, LJ-14, atoms 1990 2780
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multi-body bonded interactions: 0.443 nm, Proper Dih., atoms 1990 2780
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Minimum cell size due to bonded interactions: 0.487 nm
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User supplied maximum distance required for P-LINCS: 0.700 nm
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Guess for relative PME load: 0.13
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Will use 96 particle-particle and 16 PME only ranks
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This is a guess, check the performance at the end of the log file
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Using 16 separate PME ranks, as guessed by mdrun
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Scaling the initial minimum size with 1/0.9 (option -dds) = 1.11111
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Optimizing the DD grid for 96 cells with a minimum initial size of 0.778 nm
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The maximum allowed number of cells is: X 18 Y 17 Z 15
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Domain decomposition grid 4 x 4 x 6, separate PME ranks 16
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PME domain decomposition: 4 x 4 x 1
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Interleaving PP and PME ranks
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This rank does only particle-particle work.
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Domain decomposition rank 0, coordinates 0 0 0
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|
|
379
|
The initial number of communication pulses is: X 1 Y 1 Z 1
|
380
|
The initial domain decomposition cell size is: X 3.63 nm Y 3.31 nm Z 2.00 nm
|
381
|
|
382
|
The maximum allowed distance for atom groups involved in interactions is:
|
383
|
non-bonded interactions 1.576 nm
|
384
|
(the following are initial values, they could change due to box deformation)
|
385
|
two-body bonded interactions (-rdd) 1.576 nm
|
386
|
multi-body bonded interactions (-rdd) 1.576 nm
|
387
|
|
388
|
When dynamic load balancing gets turned on, these settings will change to:
|
389
|
The maximum number of communication pulses is: X 1 Y 1 Z 1
|
390
|
The minimum size for domain decomposition cells is 1.576 nm
|
391
|
The requested allowed shrink of DD cells (option -dds) is: 0.90
|
392
|
The allowed shrink of domain decomposition cells is: X 0.43 Y 0.48 Z 0.79
|
393
|
The maximum allowed distance for atom groups involved in interactions is:
|
394
|
non-bonded interactions 1.576 nm
|
395
|
two-body bonded interactions (-rdd) 1.576 nm
|
396
|
multi-body bonded interactions (-rdd) 1.576 nm
|
397
|
Using two step summing over 4 groups of on average 24.0 ranks
|
398
|
|
399
|
|
400
|
Using 112 MPI processes
|
401
|
Using 1 OpenMP thread per MPI process
|
402
|
|
403
|
|
404
|
Overriding thread affinity set outside gmx mdrun
|
405
|
|
406
|
Pinning threads with an auto-selected logical core stride of 1
|
407
|
System total charge: -0.000
|
408
|
Will do PME sum in reciprocal space for electrostatic interactions.
|
409
|
|
410
|
++++ PLEASE READ AND CITE THE FOLLOWING REFERENCE ++++
|
411
|
U. Essmann, L. Perera, M. L. Berkowitz, T. Darden, H. Lee and L. G. Pedersen
|
412
|
A smooth particle mesh Ewald method
|
413
|
J. Chem. Phys. 103 (1995) pp. 8577-8592
|
414
|
-------- -------- --- Thank You --- -------- --------
|
415
|
|
416
|
Using a Gaussian width (1/beta) of 0.384195 nm for Ewald
|
417
|
Potential shift: LJ r^-12: -1.122e-01 r^-6: -3.349e-01, Ewald -8.333e-06
|
418
|
Initialized non-bonded Ewald correction tables, spacing: 1.02e-03 size: 1176
|
419
|
|
420
|
Long Range LJ corr.: <C6> 3.1361e-04
|
421
|
Generated table with 1163 data points for Ewald.
|
422
|
Tabscale = 500 points/nm
|
423
|
Generated table with 1163 data points for LJ6.
|
424
|
Tabscale = 500 points/nm
|
425
|
Generated table with 1163 data points for LJ12.
|
426
|
Tabscale = 500 points/nm
|
427
|
Generated table with 1163 data points for 1-4 COUL.
|
428
|
Tabscale = 500 points/nm
|
429
|
Generated table with 1163 data points for 1-4 LJ6.
|
430
|
Tabscale = 500 points/nm
|
431
|
Generated table with 1163 data points for 1-4 LJ12.
|
432
|
Tabscale = 500 points/nm
|
433
|
|
434
|
Using SIMD 4x8 nonbonded short-range kernels
|
435
|
|
436
|
Using a dual 4x8 pair-list setup updated with dynamic pruning:
|
437
|
outer list: updated every 80 steps, buffer 0.126 nm, rlist 1.326 nm
|
438
|
inner list: updated every 13 steps, buffer 0.002 nm, rlist 1.202 nm
|
439
|
At tolerance 0.005 kJ/mol/ps per atom, equivalent classical 1x1 list would be:
|
440
|
outer list: updated every 80 steps, buffer 0.275 nm, rlist 1.475 nm
|
441
|
inner list: updated every 13 steps, buffer 0.052 nm, rlist 1.252 nm
|
442
|
|
443
|
Using full Lennard-Jones parameter combination matrix
|
444
|
|
445
|
|
446
|
Will apply potential COM pulling
|
447
|
with 1 pull coordinate and 2 groups
|
448
|
Pull group 1: 1 atoms, mass 13.019
|
449
|
Pull group 2: 2 atoms, mass 26.018
|
450
|
Will use a sub-communicator for pull communication
|
451
|
|
452
|
Initializing LINear Constraint Solver
|
453
|
|
454
|
++++ PLEASE READ AND CITE THE FOLLOWING REFERENCE ++++
|
455
|
B. Hess and H. Bekker and H. J. C. Berendsen and J. G. E. M. Fraaije
|
456
|
LINCS: A Linear Constraint Solver for molecular simulations
|
457
|
J. Comp. Chem. 18 (1997) pp. 1463-1472
|
458
|
-------- -------- --- Thank You --- -------- --------
|
459
|
|
460
|
The number of constraints is 1073
|
461
|
|
462
|
++++ PLEASE READ AND CITE THE FOLLOWING REFERENCE ++++
|
463
|
S. Miyamoto and P. A. Kollman
|
464
|
SETTLE: An Analytical Version of the SHAKE and RATTLE Algorithms for Rigid
|
465
|
Water Models
|
466
|
J. Comp. Chem. 13 (1992) pp. 952-962
|
467
|
-------- -------- --- Thank You --- -------- --------
|
468
|
|
469
|
|
470
|
Linking all bonded interactions to atoms
|
471
|
|
472
|
|
473
|
The -noconfout functionality is deprecated, and may be removed in a future version.
|
474
|
|
475
|
Intra-simulation communication will occur every 20 steps.
|
476
|
Center of mass motion removal mode is Linear
|
477
|
We have the following groups for center of mass motion removal:
|
478
|
0: rest
|
479
|
|
480
|
++++ PLEASE READ AND CITE THE FOLLOWING REFERENCE ++++
|
481
|
G. Bussi, D. Donadio and M. Parrinello
|
482
|
Canonical sampling through velocity rescaling
|
483
|
J. Chem. Phys. 126 (2007) pp. 014101
|
484
|
-------- -------- --- Thank You --- -------- --------
|
485
|
|