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726 lines
30 KiB
726 lines
30 KiB
:-) GROMACS - gmx mdrun, 2020.6-Debian-2020.6-2 (-: |
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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 Artem Zhmurov |
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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) 2001-2019, 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 2020.6-Debian-2020.6-2 |
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Executable: /usr/bin/gmx |
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Data prefix: /usr |
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Working dir: /home/student/adit/CMMDE_launching/larutan/SistemLarutan |
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Process ID: 2570744 |
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Command line: |
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gmx -quiet mdrun -deffnm nvep -ntmpi 1 -v true |
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GROMACS version: 2020.6-Debian-2020.6-2 |
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Precision: single |
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Memory model: 64 bit |
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MPI library: thread_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: SSE4.1 |
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FFT library: fftw-3.3.8-sse2-avx |
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RDTSCP usage: disabled |
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TNG support: enabled |
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Hwloc support: hwloc-2.4.1 |
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Tracing support: disabled |
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C compiler: /usr/bin/cc GNU 10.2.1 |
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C compiler flags: -msse4.1 -fexcess-precision=fast -funroll-all-loops -O3 -DNDEBUG |
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C++ compiler: /usr/bin/c++ GNU 10.2.1 |
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C++ compiler flags: -msse4.1 -fexcess-precision=fast -funroll-all-loops -fopenmp -O3 -DNDEBUG |
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Running on 1 node with total 1 cores, 2 logical cores |
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Hardware detected: |
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CPU info: |
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Vendor: Intel |
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Brand: Intel(R) Xeon(R) CPU @ 2.20GHz |
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Family: 6 Model: 79 Stepping: 0 |
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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 pdpe1gb popcnt pse rdrnd rdtscp rtm sse2 sse3 sse4.1 sse4.2 ssse3 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] |
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Numa nodes: |
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Node 0 (8343068672 bytes mem): 0 1 |
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Latency: |
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0 |
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0 1.00 |
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Caches: |
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L1: 32768 bytes, linesize 64 bytes, assoc. 8, shared 2 ways |
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L2: 262144 bytes, linesize 64 bytes, assoc. 8, shared 2 ways |
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L3: 57671680 bytes, linesize 64 bytes, assoc. 20, shared 2 ways |
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PCI devices: |
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0000:00:04.0 Id: 1af4:1000 Class: 0x0200 Numa: 0 |
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Highest SIMD level requested by all nodes in run: AVX2_256 |
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SIMD instructions selected at compile time: SSE4.1 |
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This program was compiled for different hardware than you are running on, |
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which could influence performance. |
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The current CPU can measure timings more accurately than the code in |
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gmx mdrun was configured to use. This might affect your simulation |
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speed as accurate timings are needed for load-balancing. |
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Please consider rebuilding gmx mdrun with the GMX_USE_RDTSCP=ON CMake option. |
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|
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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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The number of OpenMP threads was set by environment variable OMP_NUM_THREADS to 1 |
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Input Parameters: |
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integrator = md |
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tinit = 0 |
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dt = 0.0005 |
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nsteps = 10000 |
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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 = -140560403 |
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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 = 500 |
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nstvout = 500 |
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nstfout = 0 |
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nstlog = 500 |
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nstcalcenergy = 100 |
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nstenergy = 500 |
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nstxout-compressed = 0 |
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compressed-x-precision = 1000 |
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cutoff-scheme = Verlet |
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nstlist = 10 |
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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 = 0.961399 |
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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 = 0.961399 |
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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 = 0 |
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rvdw = 0.961399 |
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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 = 14 |
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fourier-ny = 14 |
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fourier-nz = 14 |
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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 = No |
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nsttcouple = -1 |
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nh-chain-length = 0 |
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print-nose-hoover-chain-variables = false |
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pcoupl = No |
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pcoupltype = Isotropic |
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nstpcouple = -1 |
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tau-p = 1 |
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compressibility (3x3): |
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compressibility[ 0]={ 0.00000e+00, 0.00000e+00, 0.00000e+00} |
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compressibility[ 1]={ 0.00000e+00, 0.00000e+00, 0.00000e+00} |
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compressibility[ 2]={ 0.00000e+00, 0.00000e+00, 0.00000e+00} |
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ref-p (3x3): |
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ref-p[ 0]={ 0.00000e+00, 0.00000e+00, 0.00000e+00} |
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ref-p[ 1]={ 0.00000e+00, 0.00000e+00, 0.00000e+00} |
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ref-p[ 2]={ 0.00000e+00, 0.00000e+00, 0.00000e+00} |
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refcoord-scaling = No |
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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 = false |
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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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density-guided-simulation: |
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active = false |
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group = protein |
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similarity-measure = inner-product |
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atom-spreading-weight = unity |
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force-constant = 1e+09 |
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gaussian-transform-spreading-width = 0.2 |
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gaussian-transform-spreading-range-in-multiples-of-width = 4 |
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reference-density-filename = reference.mrc |
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nst = 1 |
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normalize-densities = true |
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adaptive-force-scaling = false |
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adaptive-force-scaling-time-constant = 4 |
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grpopts: |
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nrdf: 1293 |
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ref-t: 0 |
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tau-t: 0 |
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annealing: No |
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annealing-npoints: 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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Can not increase nstlist because an NVE ensemble is used |
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Using 1 MPI thread |
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Non-default thread affinity set, disabling internal thread affinity |
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Using 1 OpenMP thread |
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System total charge: -0.000 |
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Will do PME sum in reciprocal space for electrostatic interactions. |
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|
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++++ PLEASE READ AND CITE THE FOLLOWING REFERENCE ++++ |
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U. Essmann, L. Perera, M. L. Berkowitz, T. Darden, H. Lee and L. G. Pedersen |
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A smooth particle mesh Ewald method |
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J. Chem. Phys. 103 (1995) pp. 8577-8592 |
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-------- -------- --- Thank You --- -------- -------- |
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Using a Gaussian width (1/beta) of 0.307804 nm for Ewald |
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Potential shift: LJ r^-12: -1.604e+00 r^-6: -1.266e+00, Ewald -1.040e-05 |
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Initialized non-bonded Ewald tables, spacing: 9.15e-04 size: 1052 |
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Generated table with 980 data points for 1-4 COUL. |
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Tabscale = 500 points/nm |
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Generated table with 980 data points for 1-4 LJ6. |
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Tabscale = 500 points/nm |
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Generated table with 980 data points for 1-4 LJ12. |
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Tabscale = 500 points/nm |
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Using SIMD 4x4 nonbonded short-range kernels |
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Using a 4x4 pair-list setup: |
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updated every 10 steps, buffer 0.000 nm, rlist 0.961 nm |
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Using Lorentz-Berthelot Lennard-Jones combination rule |
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Long Range LJ corr.: <C6> 3.6868e-04 |
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There are: 432 Atoms |
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Center of mass motion removal mode is Linear |
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We have the following groups for center of mass motion removal: |
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0: rest |
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Started mdrun on rank 0 Tue Jun 7 16:54:20 2022 |
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Step Time |
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0 0.00000 |
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Energies (kJ/mol) |
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Bond Angle Proper Dih. Ryckaert-Bell. LJ-14 |
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2.68571e+01 2.06130e+02 3.50263e+01 4.98516e+01 -4.70008e+00 |
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Coulomb-14 LJ (SR) Disper. corr. Coulomb (SR) Coul. recip. |
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-2.50551e+03 -3.10729e+02 -3.31483e+01 3.11356e+02 6.78661e+01 |
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Potential Kinetic En. Total Energy Temperature Pres. DC (bar) |
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-2.15700e+03 1.17316e+03 -9.83849e+02 2.18249e+02 -5.67052e+01 |
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Pressure (bar) |
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7.97352e+02 |
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Step Time |
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500 0.25000 |
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Energies (kJ/mol) |
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Bond Angle Proper Dih. Ryckaert-Bell. LJ-14 |
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5.71829e+01 1.80092e+02 3.09587e+01 5.62519e+01 -4.70784e+00 |
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Coulomb-14 LJ (SR) Disper. corr. Coulomb (SR) Coul. recip. |
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-2.50986e+03 -2.95917e+02 -3.31483e+01 2.92289e+02 7.71216e+01 |
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Potential Kinetic En. Total Energy Temperature Pres. DC (bar) |
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-2.14974e+03 1.16607e+03 -9.83664e+02 2.16932e+02 -5.67052e+01 |
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Pressure (bar) |
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2.98072e+02 |
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Step Time |
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1000 0.50000 |
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Energies (kJ/mol) |
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Bond Angle Proper Dih. Ryckaert-Bell. LJ-14 |
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6.69650e+01 2.01878e+02 3.47275e+01 5.17517e+01 -4.74050e+00 |
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Coulomb-14 LJ (SR) Disper. corr. Coulomb (SR) Coul. recip. |
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-2.51733e+03 -3.14749e+02 -3.31483e+01 2.74665e+02 7.15622e+01 |
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Potential Kinetic En. Total Energy Temperature Pres. DC (bar) |
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-2.16842e+03 1.18507e+03 -9.83349e+02 2.20466e+02 -5.67052e+01 |
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Pressure (bar) |
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4.11046e+01 |
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Step Time |
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1500 0.75000 |
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Energies (kJ/mol) |
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Bond Angle Proper Dih. Ryckaert-Bell. LJ-14 |
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5.89589e+01 2.01801e+02 2.84650e+01 4.74906e+01 -4.65939e+00 |
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Coulomb-14 LJ (SR) Disper. corr. Coulomb (SR) Coul. recip. |
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-2.50063e+03 -3.40624e+02 -3.31483e+01 2.76941e+02 8.30847e+01 |
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Potential Kinetic En. Total Energy Temperature Pres. DC (bar) |
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-2.18232e+03 1.19856e+03 -9.83759e+02 2.22976e+02 -5.67052e+01 |
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Pressure (bar) |
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5.79724e+02 |
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Step Time |
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2000 1.00000 |
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Energies (kJ/mol) |
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Bond Angle Proper Dih. Ryckaert-Bell. LJ-14 |
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8.35276e+01 1.92469e+02 3.61053e+01 5.95481e+01 -4.75944e+00 |
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Coulomb-14 LJ (SR) Disper. corr. Coulomb (SR) Coul. recip. |
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-2.53029e+03 -3.26461e+02 -3.31483e+01 2.72068e+02 7.07096e+01 |
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Potential Kinetic En. Total Energy Temperature Pres. DC (bar) |
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-2.18023e+03 1.19672e+03 -9.83508e+02 2.22634e+02 -5.67052e+01 |
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Pressure (bar) |
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4.29622e+02 |
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Step Time |
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2500 1.25000 |
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Energies (kJ/mol) |
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Bond Angle Proper Dih. Ryckaert-Bell. LJ-14 |
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7.04942e+01 1.88806e+02 4.12116e+01 6.39807e+01 -4.84451e+00 |
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Coulomb-14 LJ (SR) Disper. corr. Coulomb (SR) Coul. recip. |
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-2.53973e+03 -2.89260e+02 -3.31483e+01 2.52880e+02 6.06684e+01 |
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Potential Kinetic En. Total Energy Temperature Pres. DC (bar) |
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-2.18894e+03 1.20491e+03 -9.84036e+02 2.24156e+02 -5.67052e+01 |
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Pressure (bar) |
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7.94977e+02 |
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Step Time |
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3000 1.50000 |
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Energies (kJ/mol) |
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Bond Angle Proper Dih. Ryckaert-Bell. LJ-14 |
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6.47645e+01 1.71579e+02 2.34261e+01 5.25431e+01 -4.67042e+00 |
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Coulomb-14 LJ (SR) Disper. corr. Coulomb (SR) Coul. recip. |
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-2.50095e+03 -3.07265e+02 -3.31483e+01 2.95478e+02 7.64883e+01 |
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Potential Kinetic En. Total Energy Temperature Pres. DC (bar) |
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-2.16176e+03 1.17794e+03 -9.83812e+02 2.19140e+02 -5.67052e+01 |
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Pressure (bar) |
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5.99587e+02 |
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Step Time |
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3500 1.75000 |
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Energies (kJ/mol) |
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Bond Angle Proper Dih. Ryckaert-Bell. LJ-14 |
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9.43893e+01 1.61463e+02 2.44596e+01 6.38215e+01 -4.68754e+00 |
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Coulomb-14 LJ (SR) Disper. corr. Coulomb (SR) Coul. recip. |
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-2.50223e+03 -2.84392e+02 -3.31483e+01 2.26656e+02 6.90088e+01 |
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Potential Kinetic En. Total Energy Temperature Pres. DC (bar) |
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-2.18466e+03 1.20142e+03 -9.83235e+02 2.23508e+02 -5.67052e+01 |
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Pressure (bar) |
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3.79233e+02 |
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Step Time |
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4000 2.00000 |
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Energies (kJ/mol) |
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Bond Angle Proper Dih. Ryckaert-Bell. LJ-14 |
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9.04692e+01 1.52852e+02 2.61851e+01 4.55728e+01 -4.76396e+00 |
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Coulomb-14 LJ (SR) Disper. corr. Coulomb (SR) Coul. recip. |
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-2.52034e+03 -3.01335e+02 -3.31483e+01 2.98707e+02 7.06226e+01 |
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Potential Kinetic En. Total Energy Temperature Pres. DC (bar) |
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-2.17518e+03 1.19173e+03 -9.83449e+02 2.21705e+02 -5.67052e+01 |
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Pressure (bar) |
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9.28437e+02 |
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Step Time |
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4500 2.25000 |
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Energies (kJ/mol) |
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Bond Angle Proper Dih. Ryckaert-Bell. LJ-14 |
|
8.07335e+01 1.79767e+02 4.54518e+01 5.96417e+01 -4.80120e+00 |
|
Coulomb-14 LJ (SR) Disper. corr. Coulomb (SR) Coul. recip. |
|
-2.52796e+03 -3.17002e+02 -3.31483e+01 3.03310e+02 7.60940e+01 |
|
Potential Kinetic En. Total Energy Temperature Pres. DC (bar) |
|
-2.13792e+03 1.15426e+03 -9.83658e+02 2.14734e+02 -5.67052e+01 |
|
Pressure (bar) |
|
-3.71822e+02 |
|
|
|
Step Time |
|
5000 2.50000 |
|
|
|
Energies (kJ/mol) |
|
Bond Angle Proper Dih. Ryckaert-Bell. LJ-14 |
|
8.83895e+01 1.35048e+02 4.58026e+01 7.27292e+01 -4.87079e+00 |
|
Coulomb-14 LJ (SR) Disper. corr. Coulomb (SR) Coul. recip. |
|
-2.52845e+03 -3.30437e+02 -3.31483e+01 2.83694e+02 7.64058e+01 |
|
Potential Kinetic En. Total Energy Temperature Pres. DC (bar) |
|
-2.19483e+03 1.21136e+03 -9.83477e+02 2.25356e+02 -5.67052e+01 |
|
Pressure (bar) |
|
-4.40553e+02 |
|
|
|
Step Time |
|
5500 2.75000 |
|
|
|
Energies (kJ/mol) |
|
Bond Angle Proper Dih. Ryckaert-Bell. LJ-14 |
|
8.33474e+01 1.60111e+02 2.49346e+01 4.50281e+01 -4.84969e+00 |
|
Coulomb-14 LJ (SR) Disper. corr. Coulomb (SR) Coul. recip. |
|
-2.52294e+03 -3.44011e+02 -3.31483e+01 2.92817e+02 7.44514e+01 |
|
Potential Kinetic En. Total Energy Temperature Pres. DC (bar) |
|
-2.22426e+03 1.24060e+03 -9.83656e+02 2.30797e+02 -5.67052e+01 |
|
Pressure (bar) |
|
1.18631e+03 |
|
|
|
Step Time |
|
6000 3.00000 |
|
|
|
Energies (kJ/mol) |
|
Bond Angle Proper Dih. Ryckaert-Bell. LJ-14 |
|
6.61491e+01 1.99206e+02 2.83812e+01 4.32869e+01 -4.63137e+00 |
|
Coulomb-14 LJ (SR) Disper. corr. Coulomb (SR) Coul. recip. |
|
-2.50879e+03 -3.48650e+02 -3.31483e+01 3.06267e+02 7.48799e+01 |
|
Potential Kinetic En. Total Energy Temperature Pres. DC (bar) |
|
-2.17705e+03 1.19348e+03 -9.83563e+02 2.22031e+02 -5.67052e+01 |
|
Pressure (bar) |
|
-3.32347e+02 |
|
|
|
Step Time |
|
6500 3.25000 |
|
|
|
Energies (kJ/mol) |
|
Bond Angle Proper Dih. Ryckaert-Bell. LJ-14 |
|
8.83938e+01 1.59127e+02 4.40262e+01 6.20234e+01 -4.86572e+00 |
|
Coulomb-14 LJ (SR) Disper. corr. Coulomb (SR) Coul. recip. |
|
-2.52597e+03 -3.25515e+02 -3.31483e+01 2.94908e+02 7.41591e+01 |
|
Potential Kinetic En. Total Energy Temperature Pres. DC (bar) |
|
-2.16686e+03 1.18353e+03 -9.83332e+02 2.20180e+02 -5.67052e+01 |
|
Pressure (bar) |
|
4.52560e+02 |
|
|
|
Step Time |
|
7000 3.50000 |
|
|
|
Energies (kJ/mol) |
|
Bond Angle Proper Dih. Ryckaert-Bell. LJ-14 |
|
8.94784e+01 1.77594e+02 2.43321e+01 3.49407e+01 -4.80416e+00 |
|
Coulomb-14 LJ (SR) Disper. corr. Coulomb (SR) Coul. recip. |
|
-2.52508e+03 -3.12532e+02 -3.31483e+01 2.73032e+02 6.57994e+01 |
|
Potential Kinetic En. Total Energy Temperature Pres. DC (bar) |
|
-2.21039e+03 1.22704e+03 -9.83349e+02 2.28273e+02 -5.67052e+01 |
|
Pressure (bar) |
|
8.73185e+02 |
|
|
|
Step Time |
|
7500 3.75000 |
|
|
|
Energies (kJ/mol) |
|
Bond Angle Proper Dih. Ryckaert-Bell. LJ-14 |
|
9.28125e+01 1.62232e+02 3.35552e+01 5.94787e+01 -4.71466e+00 |
|
Coulomb-14 LJ (SR) Disper. corr. Coulomb (SR) Coul. recip. |
|
-2.51767e+03 -2.95079e+02 -3.31483e+01 2.72958e+02 7.00983e+01 |
|
Potential Kinetic En. Total Energy Temperature Pres. DC (bar) |
|
-2.15948e+03 1.17609e+03 -9.83393e+02 2.18795e+02 -5.67052e+01 |
|
Pressure (bar) |
|
-5.48705e+02 |
|
|
|
Step Time |
|
8000 4.00000 |
|
|
|
Energies (kJ/mol) |
|
Bond Angle Proper Dih. Ryckaert-Bell. LJ-14 |
|
9.96638e+01 1.62056e+02 2.80954e+01 5.80195e+01 -4.63848e+00 |
|
Coulomb-14 LJ (SR) Disper. corr. Coulomb (SR) Coul. recip. |
|
-2.49588e+03 -3.25313e+02 -3.31483e+01 2.86824e+02 7.14535e+01 |
|
Potential Kinetic En. Total Energy Temperature Pres. DC (bar) |
|
-2.15287e+03 1.16952e+03 -9.83342e+02 2.17574e+02 -5.67052e+01 |
|
Pressure (bar) |
|
2.97416e+02 |
|
|
|
Step Time |
|
8500 4.25000 |
|
|
|
Energies (kJ/mol) |
|
Bond Angle Proper Dih. Ryckaert-Bell. LJ-14 |
|
9.72742e+01 1.36549e+02 4.99397e+01 7.40676e+01 -4.85137e+00 |
|
Coulomb-14 LJ (SR) Disper. corr. Coulomb (SR) Coul. recip. |
|
-2.54643e+03 -2.83260e+02 -3.31483e+01 3.23393e+02 6.66151e+01 |
|
Potential Kinetic En. Total Energy Temperature Pres. DC (bar) |
|
-2.11986e+03 1.13679e+03 -9.83069e+02 2.11484e+02 -5.67052e+01 |
|
Pressure (bar) |
|
9.45151e+02 |
|
|
|
Step Time |
|
9000 4.50000 |
|
|
|
Energies (kJ/mol) |
|
Bond Angle Proper Dih. Ryckaert-Bell. LJ-14 |
|
8.24089e+01 1.79101e+02 3.29559e+01 4.82325e+01 -4.74104e+00 |
|
Coulomb-14 LJ (SR) Disper. corr. Coulomb (SR) Coul. recip. |
|
-2.51091e+03 -2.87232e+02 -3.31483e+01 2.83039e+02 6.98197e+01 |
|
Potential Kinetic En. Total Energy Temperature Pres. DC (bar) |
|
-2.14047e+03 1.15701e+03 -9.83462e+02 2.15245e+02 -5.67052e+01 |
|
Pressure (bar) |
|
5.52506e+02 |
|
|
|
Step Time |
|
9500 4.75000 |
|
|
|
Energies (kJ/mol) |
|
Bond Angle Proper Dih. Ryckaert-Bell. LJ-14 |
|
8.46766e+01 1.58841e+02 4.20994e+01 6.14774e+01 -4.84161e+00 |
|
Coulomb-14 LJ (SR) Disper. corr. Coulomb (SR) Coul. recip. |
|
-2.52382e+03 -2.96920e+02 -3.31483e+01 2.45470e+02 6.73681e+01 |
|
Potential Kinetic En. Total Energy Temperature Pres. DC (bar) |
|
-2.19880e+03 1.21528e+03 -9.83517e+02 2.26086e+02 -5.67052e+01 |
|
Pressure (bar) |
|
-5.11383e+02 |
|
|
|
Step Time |
|
10000 5.00000 |
|
|
|
Writing checkpoint, step 10000 at Tue Jun 7 16:54:27 2022 |
|
|
|
|
|
Energies (kJ/mol) |
|
Bond Angle Proper Dih. Ryckaert-Bell. LJ-14 |
|
8.67398e+01 1.65914e+02 5.29682e+01 6.75271e+01 -4.83456e+00 |
|
Coulomb-14 LJ (SR) Disper. corr. Coulomb (SR) Coul. recip. |
|
-2.53760e+03 -3.09650e+02 -3.31483e+01 3.06939e+02 6.95346e+01 |
|
Potential Kinetic En. Total Energy Temperature Pres. DC (bar) |
|
-2.13561e+03 1.15236e+03 -9.83256e+02 2.14380e+02 -5.67052e+01 |
|
Pressure (bar) |
|
4.15713e+02 |
|
|
|
|
|
<====== ############### ==> |
|
<==== A V E R A G E S ====> |
|
<== ############### ======> |
|
|
|
Statistics over 10001 steps using 101 frames |
|
|
|
Energies (kJ/mol) |
|
Bond Angle Proper Dih. Ryckaert-Bell. LJ-14 |
|
8.47749e+01 1.65731e+02 3.59536e+01 5.62230e+01 -4.76393e+00 |
|
Coulomb-14 LJ (SR) Disper. corr. Coulomb (SR) Coul. recip. |
|
-2.51942e+03 -3.09137e+02 -3.31483e+01 2.87991e+02 7.15408e+01 |
|
Potential Kinetic En. Total Energy Temperature Pres. DC (bar) |
|
-2.16426e+03 1.18071e+03 -9.83545e+02 2.19655e+02 -5.67052e+01 |
|
Pressure (bar) |
|
3.09581e+02 |
|
|
|
Total Virial (kJ/mol) |
|
2.92701e+02 2.08917e+01 -3.05352e+00 |
|
2.08916e+01 3.00999e+02 4.96721e-02 |
|
-3.05346e+00 4.97567e-02 3.14731e+02 |
|
|
|
Pressure (bar) |
|
3.54393e+02 -9.94881e+01 1.26737e+01 |
|
-9.94881e+01 3.11738e+02 -1.17409e+01 |
|
1.26735e+01 -1.17412e+01 2.62611e+02 |
|
|
|
|
|
M E G A - F L O P S A C C O U N T I N G |
|
|
|
NB=Group-cutoff nonbonded kernels NxN=N-by-N cluster Verlet kernels |
|
RF=Reaction-Field VdW=Van der Waals QSTab=quadratic-spline table |
|
W3=SPC/TIP3p W4=TIP4p (single or pairs) |
|
V&F=Potential and force V=Potential only F=Force only |
|
|
|
Computing: M-Number M-Flops % Flops |
|
----------------------------------------------------------------------------- |
|
Pair Search distance check 69.718542 627.467 1.5 |
|
NxN QSTab Elec. + LJ [F] 519.912272 21316.403 52.3 |
|
NxN QSTab Elec. + LJ [V&F] 5.310760 313.335 0.8 |
|
NxN QSTab Elec. [F] 283.296912 9632.095 23.7 |
|
NxN QSTab Elec. [V&F] 2.910824 119.344 0.3 |
|
1,4 nonbonded interactions 0.720072 64.806 0.2 |
|
Calc Weights 12.961296 466.607 1.1 |
|
Spread Q Bspline 276.507648 553.015 1.4 |
|
Gather F Bspline 276.507648 1659.046 4.1 |
|
3D-FFT 626.902684 5015.221 12.3 |
|
Solve PME 1.960196 125.453 0.3 |
|
Shift-X 0.432432 2.595 0.0 |
|
Bonds 3.080308 181.738 0.4 |
|
Angles 2.260226 379.718 0.9 |
|
Propers 0.270027 61.836 0.2 |
|
RB-Dihedrals 0.720072 177.858 0.4 |
|
Virial 0.048177 0.867 0.0 |
|
Stop-CM 0.043632 0.436 0.0 |
|
Calc-Ekin 0.864864 23.351 0.1 |
|
----------------------------------------------------------------------------- |
|
Total 40721.192 100.0 |
|
----------------------------------------------------------------------------- |
|
|
|
|
|
R E A L C Y C L E A N D T I M E A C C O U N T I N G |
|
|
|
On 1 MPI rank |
|
|
|
Computing: Num Num Call Wall time Giga-Cycles |
|
Ranks Threads Count (s) total sum % |
|
----------------------------------------------------------------------------- |
|
Neighbor search 1 1 1001 0.836 1.840 11.0 |
|
Force 1 1 10001 4.878 10.732 64.4 |
|
PME mesh 1 1 10001 1.647 3.623 21.7 |
|
NB X/F buffer ops. 1 1 19001 0.061 0.133 0.8 |
|
Write traj. 1 1 21 0.022 0.048 0.3 |
|
Update 1 1 10001 0.045 0.099 0.6 |
|
Rest 0.089 0.195 1.2 |
|
----------------------------------------------------------------------------- |
|
Total 7.577 16.670 100.0 |
|
----------------------------------------------------------------------------- |
|
Breakdown of PME mesh computation |
|
----------------------------------------------------------------------------- |
|
PME spread 1 1 10001 0.469 1.031 6.2 |
|
PME gather 1 1 10001 0.676 1.486 8.9 |
|
PME 3D-FFT 1 1 20002 0.296 0.651 3.9 |
|
PME solve Elec 1 1 10001 0.194 0.428 2.6 |
|
----------------------------------------------------------------------------- |
|
|
|
NOTE: 11 % of the run time was spent in pair search, |
|
you might want to increase nstlist (this has no effect on accuracy) |
|
|
|
Core t (s) Wall t (s) (%) |
|
Time: 7.577 7.577 100.0 |
|
(ns/day) (hour/ns) |
|
Performance: 57.020 0.421 |
|
Finished mdrun on rank 0 Tue Jun 7 16:54:27 2022 |
|
|
|
|