Re: [gmx-users] OPLS parameters for O2

2019-05-09 Thread David van der Spoel

Den 2019-05-10 kl. 00:42, skrev Shadi Fuladi:

Hi,

I'm trying to test molecular oxygen diffusion in electrolytes using OPLS
force field. Is there any O2 parameters tested with OPLS AA forcefield?

Thanks,
SF


There is a model described here

Hub, J. S.; de Groot, B. L. Proc. Natl. Acad. Sci. U.S.A. 2008, 105, 
1198−1203.


that we have tested in the paper below and it has has quite accurate 
solubility in water. See
Michiel van Lun, Jochen S. Hub, David van der Spoel and Inger Andersson: 
CO2 and O2 Distribution in Rubisco Suggests the Small Subunit Functions 
as a CO2 Reservoir J. Amer. Chem. Soc. 136 pp. 3165-3171 (2014)


Cheers,
--
David van der Spoel, Ph.D., Professor of Biology
Head of Department, Cell & Molecular Biology, Uppsala University.
Box 596, SE-75124 Uppsala, Sweden. Phone: +46184714205.
http://www.icm.uu.se
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Re: [gmx-users] Gromacs 2019.2 on Power9 + Volta GPUs (building and running)

2019-05-09 Thread Alex
Yup, your assessment agrees with our guess. Our HPC guru will be taking his
findings, along with your quote, to the admins.

Thank you,

Alex

On Thu, May 9, 2019 at 2:51 PM Szilárd Páll  wrote:

> On Thu, May 9, 2019 at 10:01 PM Alex  wrote:
>
> > Okay, we're positively unable to run a Gromacs (2019.1) test on Power9.
> The
> > test procedure is simple, using slurm:
> > 1. Request an interactive session: > srun -N 1 -n 20 --pty
> > --partition=debug --time=1:00:00 --gres=gpu:1 bash
> > 2. Load CUDA library: module load cuda
> > 3. Run test batch. This starts with a CPU-only static EM, which, despite
> > the mdrun variables, runs on a single thread. Any help will be highly
> > appreciated.
> >
> >  md.log below:
> >
> > GROMACS:  gmx mdrun, version 2019.1
> > Executable:   /home/reida/ppc64le/stow/gromacs/bin/gmx
> > Data prefix:  /home/reida/ppc64le/stow/gromacs
> > Working dir:  /home/smolyan/gmx_test1
> > Process ID:   115831
> > Command line:
> >   gmx mdrun -pin on -pinstride 2 -ntomp 4 -ntmpi 4 -pme cpu -nb cpu -s
> > em.tpr -o traj.trr -g md.log -c after_em.pdb
> >
> > GROMACS version:2019.1
> > Precision:  single
> > Memory model:   64 bit
> > MPI library:thread_mpi
> > OpenMP support: enabled (GMX_OPENMP_MAX_THREADS = 64)
> > GPU support:CUDA
> > SIMD instructions:  IBM_VSX
> > FFT library:fftw-3.3.8
> > RDTSCP usage:   disabled
> > TNG support:enabled
> > Hwloc support:  hwloc-1.11.8
> > Tracing support:disabled
> > C compiler: /opt/rh/devtoolset-7/root/usr/bin/cc GNU 7.3.1
> > C compiler flags:   -mcpu=power9 -mtune=power9  -mvsx -O2 -DNDEBUG
> > -funroll-all-loops -fexcess-precision=fast
> > C++ compiler:   /opt/rh/devtoolset-7/root/usr/bin/c++ GNU 7.3.1
> > C++ compiler flags: -mcpu=power9 -mtune=power9  -mvsx-std=c++11   -O2
> > -DNDEBUG -funroll-all-loops -fexcess-precision=fast
> > CUDA compiler:  /usr/local/cuda-10.0/bin/nvcc nvcc: NVIDIA (R) Cuda
> > compiler driver;Copyright (c) 2005-2018 NVIDIA Corporation;Built on
> > Sat_Aug_25_21:10:00_CDT_2018;Cuda compilation tools, release 10.0,
> > V10.0.130
> > CUDA compiler
> >
> >
> flags:-gencode;arch=compute_30,code=sm_30;-gencode;arch=compute_35,code=sm_35;-gencode;arch=compute_37,code=sm_37;-gencode;arch=compute_50,code=sm_50;-gencode;arch=compute_52,code=sm_52;-gencode;arch=compute_60,code=sm_60;-gencode;arch=compute_61,code=sm_61;-gencode;arch=compute_70,code=sm_70;-gencode;arch=compute_75,code=compute_75;-use_fast_math;;;
> >
> >
> -mcpu=power9;-mtune=power9;-mvsx;-std=c++11;-O2;-DNDEBUG;-funroll-all-loops;-fexcess-precision=fast;
> > CUDA driver:10.10
> > CUDA runtime:   10.0
> >
> >
> > Running on 1 node with total 160 cores, 160 logical cores, 1 compatible
> GPU
> > Hardware detected:
> >   CPU info:
> > Vendor: IBM
> > Brand:  POWER9, altivec supported
> > Family: 0   Model: 0   Stepping: 0
> > Features: vmx vsx
> >   Hardware topology: Only logical processor count
> >   GPU info:
> > Number of GPUs detected: 1
> > #0: NVIDIA Tesla V100-SXM2-16GB, compute cap.: 7.0, ECC: yes, stat:
> > compatible
> >
> >
> >  PLEASE READ AND CITE THE FOLLOWING REFERENCE 
> >
> > *SKIPPED*
> >
> > Input Parameters:
> >integrator = steep
> >tinit  = 0
> >dt = 0.001
> >nsteps = 5
> >init-step  = 0
> >simulation-part= 1
> >comm-mode  = Linear
> >nstcomm= 100
> >bd-fric= 0
> >ld-seed= 1941752878
> >emtol  = 100
> >emstep = 0.01
> >niter  = 20
> >fcstep = 0
> >nstcgsteep = 1000
> >nbfgscorr  = 10
> >rtpi   = 0.05
> >nstxout= 0
> >nstvout= 0
> >nstfout= 0
> >nstlog = 1000
> >nstcalcenergy  = 100
> >nstenergy  = 1000
> >nstxout-compressed = 0
> >compressed-x-precision = 1000
> >cutoff-scheme  = Verlet
> >nstlist= 1
> >ns-type= Grid
> >pbc= xyz
> >periodic-molecules = true
> >verlet-buffer-tolerance= 0.005
> >rlist  = 1.2
> >coulombtype= PME
> >coulomb-modifier   = Potential-shift
> >rcoulomb-switch= 0
> >rcoulomb   = 1.2
> >epsilon-r  = 1
> >epsilon-rf = inf
> >vdw-type   = Cut-off

[gmx-users] OPLS parameters for O2

2019-05-09 Thread Shadi Fuladi
Hi,

I'm trying to test molecular oxygen diffusion in electrolytes using OPLS
force field. Is there any O2 parameters tested with OPLS AA forcefield?

Thanks,
SF
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Re: [gmx-users] Gromacs 2019.2 on Power9 + Volta GPUs (building and running)

2019-05-09 Thread Szilárd Páll
On Thu, May 9, 2019 at 10:01 PM Alex  wrote:

> Okay, we're positively unable to run a Gromacs (2019.1) test on Power9. The
> test procedure is simple, using slurm:
> 1. Request an interactive session: > srun -N 1 -n 20 --pty
> --partition=debug --time=1:00:00 --gres=gpu:1 bash
> 2. Load CUDA library: module load cuda
> 3. Run test batch. This starts with a CPU-only static EM, which, despite
> the mdrun variables, runs on a single thread. Any help will be highly
> appreciated.
>
>  md.log below:
>
> GROMACS:  gmx mdrun, version 2019.1
> Executable:   /home/reida/ppc64le/stow/gromacs/bin/gmx
> Data prefix:  /home/reida/ppc64le/stow/gromacs
> Working dir:  /home/smolyan/gmx_test1
> Process ID:   115831
> Command line:
>   gmx mdrun -pin on -pinstride 2 -ntomp 4 -ntmpi 4 -pme cpu -nb cpu -s
> em.tpr -o traj.trr -g md.log -c after_em.pdb
>
> GROMACS version:2019.1
> Precision:  single
> Memory model:   64 bit
> MPI library:thread_mpi
> OpenMP support: enabled (GMX_OPENMP_MAX_THREADS = 64)
> GPU support:CUDA
> SIMD instructions:  IBM_VSX
> FFT library:fftw-3.3.8
> RDTSCP usage:   disabled
> TNG support:enabled
> Hwloc support:  hwloc-1.11.8
> Tracing support:disabled
> C compiler: /opt/rh/devtoolset-7/root/usr/bin/cc GNU 7.3.1
> C compiler flags:   -mcpu=power9 -mtune=power9  -mvsx -O2 -DNDEBUG
> -funroll-all-loops -fexcess-precision=fast
> C++ compiler:   /opt/rh/devtoolset-7/root/usr/bin/c++ GNU 7.3.1
> C++ compiler flags: -mcpu=power9 -mtune=power9  -mvsx-std=c++11   -O2
> -DNDEBUG -funroll-all-loops -fexcess-precision=fast
> CUDA compiler:  /usr/local/cuda-10.0/bin/nvcc nvcc: NVIDIA (R) Cuda
> compiler driver;Copyright (c) 2005-2018 NVIDIA Corporation;Built on
> Sat_Aug_25_21:10:00_CDT_2018;Cuda compilation tools, release 10.0,
> V10.0.130
> CUDA compiler
>
> flags:-gencode;arch=compute_30,code=sm_30;-gencode;arch=compute_35,code=sm_35;-gencode;arch=compute_37,code=sm_37;-gencode;arch=compute_50,code=sm_50;-gencode;arch=compute_52,code=sm_52;-gencode;arch=compute_60,code=sm_60;-gencode;arch=compute_61,code=sm_61;-gencode;arch=compute_70,code=sm_70;-gencode;arch=compute_75,code=compute_75;-use_fast_math;;;
>
> -mcpu=power9;-mtune=power9;-mvsx;-std=c++11;-O2;-DNDEBUG;-funroll-all-loops;-fexcess-precision=fast;
> CUDA driver:10.10
> CUDA runtime:   10.0
>
>
> Running on 1 node with total 160 cores, 160 logical cores, 1 compatible GPU
> Hardware detected:
>   CPU info:
> Vendor: IBM
> Brand:  POWER9, altivec supported
> Family: 0   Model: 0   Stepping: 0
> Features: vmx vsx
>   Hardware topology: Only logical processor count
>   GPU info:
> Number of GPUs detected: 1
> #0: NVIDIA Tesla V100-SXM2-16GB, compute cap.: 7.0, ECC: yes, stat:
> compatible
>
>
>  PLEASE READ AND CITE THE FOLLOWING REFERENCE 
>
> *SKIPPED*
>
> Input Parameters:
>integrator = steep
>tinit  = 0
>dt = 0.001
>nsteps = 5
>init-step  = 0
>simulation-part= 1
>comm-mode  = Linear
>nstcomm= 100
>bd-fric= 0
>ld-seed= 1941752878
>emtol  = 100
>emstep = 0.01
>niter  = 20
>fcstep = 0
>nstcgsteep = 1000
>nbfgscorr  = 10
>rtpi   = 0.05
>nstxout= 0
>nstvout= 0
>nstfout= 0
>nstlog = 1000
>nstcalcenergy  = 100
>nstenergy  = 1000
>nstxout-compressed = 0
>compressed-x-precision = 1000
>cutoff-scheme  = Verlet
>nstlist= 1
>ns-type= Grid
>pbc= xyz
>periodic-molecules = true
>verlet-buffer-tolerance= 0.005
>rlist  = 1.2
>coulombtype= PME
>coulomb-modifier   = Potential-shift
>rcoulomb-switch= 0
>rcoulomb   = 1.2
>epsilon-r  = 1
>epsilon-rf = inf
>vdw-type   = Cut-off
>vdw-modifier   = Potential-shift
>rvdw-switch= 0
>rvdw   = 1.2
>DispCorr   = No
>table-extension= 1
>fourierspacing = 0.12
>fourier-nx = 52
>fourier-ny = 52
>fourier-nz = 52
>pme-order  = 4
> 

Re: [gmx-users] Gromacs 2019.2 on Power9 + Volta GPUs (building and running)

2019-05-09 Thread Alex
Okay, we're positively unable to run a Gromacs (2019.1) test on Power9. The
test procedure is simple, using slurm:
1. Request an interactive session: > srun -N 1 -n 20 --pty
--partition=debug --time=1:00:00 --gres=gpu:1 bash
2. Load CUDA library: module load cuda
3. Run test batch. This starts with a CPU-only static EM, which, despite
the mdrun variables, runs on a single thread. Any help will be highly
appreciated.

 md.log below:

GROMACS:  gmx mdrun, version 2019.1
Executable:   /home/reida/ppc64le/stow/gromacs/bin/gmx
Data prefix:  /home/reida/ppc64le/stow/gromacs
Working dir:  /home/smolyan/gmx_test1
Process ID:   115831
Command line:
  gmx mdrun -pin on -pinstride 2 -ntomp 4 -ntmpi 4 -pme cpu -nb cpu -s
em.tpr -o traj.trr -g md.log -c after_em.pdb

GROMACS version:2019.1
Precision:  single
Memory model:   64 bit
MPI library:thread_mpi
OpenMP support: enabled (GMX_OPENMP_MAX_THREADS = 64)
GPU support:CUDA
SIMD instructions:  IBM_VSX
FFT library:fftw-3.3.8
RDTSCP usage:   disabled
TNG support:enabled
Hwloc support:  hwloc-1.11.8
Tracing support:disabled
C compiler: /opt/rh/devtoolset-7/root/usr/bin/cc GNU 7.3.1
C compiler flags:   -mcpu=power9 -mtune=power9  -mvsx -O2 -DNDEBUG
-funroll-all-loops -fexcess-precision=fast
C++ compiler:   /opt/rh/devtoolset-7/root/usr/bin/c++ GNU 7.3.1
C++ compiler flags: -mcpu=power9 -mtune=power9  -mvsx-std=c++11   -O2
-DNDEBUG -funroll-all-loops -fexcess-precision=fast
CUDA compiler:  /usr/local/cuda-10.0/bin/nvcc nvcc: NVIDIA (R) Cuda
compiler driver;Copyright (c) 2005-2018 NVIDIA Corporation;Built on
Sat_Aug_25_21:10:00_CDT_2018;Cuda compilation tools, release 10.0, V10.0.130
CUDA compiler
flags:-gencode;arch=compute_30,code=sm_30;-gencode;arch=compute_35,code=sm_35;-gencode;arch=compute_37,code=sm_37;-gencode;arch=compute_50,code=sm_50;-gencode;arch=compute_52,code=sm_52;-gencode;arch=compute_60,code=sm_60;-gencode;arch=compute_61,code=sm_61;-gencode;arch=compute_70,code=sm_70;-gencode;arch=compute_75,code=compute_75;-use_fast_math;;;
-mcpu=power9;-mtune=power9;-mvsx;-std=c++11;-O2;-DNDEBUG;-funroll-all-loops;-fexcess-precision=fast;
CUDA driver:10.10
CUDA runtime:   10.0


Running on 1 node with total 160 cores, 160 logical cores, 1 compatible GPU
Hardware detected:
  CPU info:
Vendor: IBM
Brand:  POWER9, altivec supported
Family: 0   Model: 0   Stepping: 0
Features: vmx vsx
  Hardware topology: Only logical processor count
  GPU info:
Number of GPUs detected: 1
#0: NVIDIA Tesla V100-SXM2-16GB, compute cap.: 7.0, ECC: yes, stat:
compatible


 PLEASE READ AND CITE THE FOLLOWING REFERENCE 

*SKIPPED*

Input Parameters:
   integrator = steep
   tinit  = 0
   dt = 0.001
   nsteps = 5
   init-step  = 0
   simulation-part= 1
   comm-mode  = Linear
   nstcomm= 100
   bd-fric= 0
   ld-seed= 1941752878
   emtol  = 100
   emstep = 0.01
   niter  = 20
   fcstep = 0
   nstcgsteep = 1000
   nbfgscorr  = 10
   rtpi   = 0.05
   nstxout= 0
   nstvout= 0
   nstfout= 0
   nstlog = 1000
   nstcalcenergy  = 100
   nstenergy  = 1000
   nstxout-compressed = 0
   compressed-x-precision = 1000
   cutoff-scheme  = Verlet
   nstlist= 1
   ns-type= Grid
   pbc= xyz
   periodic-molecules = true
   verlet-buffer-tolerance= 0.005
   rlist  = 1.2
   coulombtype= PME
   coulomb-modifier   = Potential-shift
   rcoulomb-switch= 0
   rcoulomb   = 1.2
   epsilon-r  = 1
   epsilon-rf = inf
   vdw-type   = Cut-off
   vdw-modifier   = Potential-shift
   rvdw-switch= 0
   rvdw   = 1.2
   DispCorr   = No
   table-extension= 1
   fourierspacing = 0.12
   fourier-nx = 52
   fourier-ny = 52
   fourier-nz = 52
   pme-order  = 4
   ewald-rtol = 1e-05
   ewald-rtol-lj  = 0.001
   lj-pme-comb-rule   = Geometric
   ewald-geometry = 0
   epsilon-surface= 0
   tcoupl = No
   nsttcouple   

[gmx-users] charge density of multiple frames in a limited region

2019-05-09 Thread p buscemi


Dear Users,
In using:
gmx density -f lipid.nvt.trr -s octanoate.nvt3.tpr -dens charge -center -symm 
-sl 100 -b 4 -e 4.5
it appears that the average charge density of all frames and the total box size 
is used in the calculation. Is there a way to
1) specify multiple ranges to output say, every , 20th frame other than running 
the command multiple times and
2) specify at least one of the x and y dimensions in which the charge density 
is calculated ?

Regards
pb

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[gmx-users] mdrun log file question

2019-05-09 Thread Hanin Omar
hello all,I am running an md simulation using gromacs 2019 with RDC restraints 
added in all steps, now in my log file i get something like this Orientation 
experiment 1:
    order parameter: -0.00156791
    eig:  1.000   -0.085  0.037  0.996
    eig: -0.636   -0.144  0.988 -0.049
    eig: -0.364    0.986  0.148  0.079

  Orientation experiment 2:
    order parameter: 0.00196219
    eig:  1.000    0.497  0.569  0.655
    eig: -0.596    0.785  0.027 -0.619
    eig: -0.404    0.370 -0.822  0.434
so my question is what does the order parameter her represents, is it a 
scalling factor for the eigen values or something elsecan someone help me with 
thisThank youHanin OMar
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Re: [gmx-users] TIP4P molecules stuck together

2019-05-09 Thread John Whittaker
Dr. Shirts,

Thank you for the swift reply.

> If you have "unprotected" electrostatic sites (i.e. with nonzero repulsive
> terms directly on top of the charge), then there will always be some
> configurations with essentially infinitely negative energy.

That makes sense. Definitely something to think about, especially in these
simulations.

>Is your cap smoothly varying?  If not, then your dynamics on hitting the
cap will be unphysical.

Indeed, our cap is implemented instantaneously and certainly introduces
non-physical dynamics when it is triggered. Our simulations consist of
non-interacting "tracer" particles that abruptly change resolution to
fully atomistic, interacting water molecules when they pass an interface
in the simulation box.

The force cap is a brute-force approach to ensure the simulation doesn't
explode when a particle crosses the boundary, gains atomistic features,
and finds itself in an unphysical configuration relative to an already
atomistically-resolved molecule (other groups have used a Monte Carlo move
to adjust the overlapping molecules... something we may consider in the
future).

We do not consider structural/dynamic properties within this interface
region where the force-cap is triggered by the immense energies due to
particle-particle overlap.

>How are the forces propagated into the energies (if grad U
>=/= F, then weird non-newtonian physics will also happen).

The forces are normalized to 2000 (iff > 2000) just before the velocities
are calculated in the first step of the stochastic dynamics integrator.

> What are the energies? Are they lower or higher than zero?

>From the single-point energy calculation of the dimer configuration, the
potential energy output is:

Energy  Average   Err.Est.   RMSD  Tot-Drift
---
Potential503436 --  0  0 
(kJ/mol)

and the output from gmx dump:

traj.trr frame 0:
   natoms=10  step= 0  time=7.144e+03  lambda= 0
   box (3x3):
  box[0]={ 3.36795e+01,  0.0e+00,  0.0e+00}
  box[1]={ 0.0e+00,  7.54019e+00,  0.0e+00}
  box[2]={ 0.0e+00,  0.0e+00,  7.54019e+00}
   x (10x3):
  x[0]={ 2.10910e+01,  3.64700e+00,  2.75200e+00}
  x[1]={ 2.11150e+01,  3.6e+00,  2.83200e+00}
  x[2]={ 2.11700e+01,  3.69400e+00,  2.72700e+00}
  x[3]={ 2.11040e+01,  3.64700e+00,  2.75900e+00}
  x[4]={ 2.10960e+01,  3.64700e+00,  2.75500e+00}
  x[5]={ 2.11700e+01,  3.72600e+00,  2.72800e+00}
  x[6]={ 2.11700e+01,  3.65300e+00,  2.66500e+00}
  x[7]={ 2.10770e+01,  3.73900e+00,  2.74900e+00}
  x[8]={ 2.11580e+01,  3.71800e+00,  2.72200e+00}
  x[9]={ 2.11650e+01,  3.72300e+00,  2.72500e+00}
   v (10x3):
  v[0]={ 0.0e+00,  0.0e+00,  0.0e+00}
  v[1]={ 0.0e+00,  0.0e+00,  0.0e+00}
  v[2]={ 0.0e+00,  0.0e+00,  0.0e+00}
  v[3]={ 0.0e+00,  0.0e+00,  0.0e+00}
  v[4]={ 0.0e+00,  0.0e+00,  0.0e+00}
  v[5]={ 0.0e+00,  0.0e+00,  0.0e+00}
  v[6]={ 0.0e+00,  0.0e+00,  0.0e+00}
  v[7]={ 0.0e+00,  0.0e+00,  0.0e+00}
  v[8]={ 0.0e+00,  0.0e+00,  0.0e+00}
  v[9]={ 0.0e+00,  0.0e+00,  0.0e+00}
   f (10x3):
  f[0]={-3.67300e+07, -3.67266e+07,  1.11572e+07}
  f[1]={-3.54829e+02, -4.32763e+01,  3.86598e+00}
  f[2]={-4.24006e+04,  9.05089e+04, -1.34170e+04}
  f[3]={ 0.0e+00,  0.0e+00,  0.0e+00}
  f[4]={ 0.0e+00,  0.0e+00,  0.0e+00}
  f[5]={ 3.67632e+07,  3.66652e+07, -1.11462e+07}
  f[6]={ 3.81472e+03, -1.38062e+04, -2.40026e+02}
  f[7]={ 5.73042e+03, -1.52270e+04,  2.66433e+03}
  f[8]={ 0.0e+00,  0.0e+00,  0.0e+00}
  f[9]={ 0.0e+00,  0.0e+00,  0.0e+00}

note: there are 5 atoms per TIP4P molecule in our case because we use a
virtual site constructed from the other atoms as the non-interacting
"tracer" particle (all 5 atoms exist at once as a hybrid molecule all the
time, interactions are just switched on for OW, HW1, HW2, and MW when they
transition to the atomistically-resolved region)

Sorry for the wall of text, I hope what I said makes sense. I appreciate
the help.

John

> On Thu, May 9, 2019 at 8:43 AM John Whittaker <
> johnwhitt...@zedat.fu-berlin.de> wrote:
>
>> Hi all,
>>
>> I have a rather strange question that I hope someone can shed some light
>> on.
>>
>> Before I begin, I want to note that I am pioneering some new
>> developments
>> of the Adaptive Resolution Simulation technique
>> (https://doi.org/10.1002/adts.201900014), so the simulations/techniques
>> I
>> am performing/implementing are fairly non-standard with respect to
>> normal
>> atomistic 

Re: [gmx-users] TIP4P molecules stuck together

2019-05-09 Thread Michael Shirts
If you have "unprotected" electrostatic sites (i.e. with nonzero repulsive
terms directly on top of the charge), then there will always be some
configurations with essentially infinitely negative energy.  For vanilla
MD, these are essentially impossible to reach kinetically at any reasonable
temperature or reasonable timestep, because the R^-12 of the neighboring
atoms creates such an enormously large barrier.  But with certain
accelerated sampling approaches, you can skip over the barrier, and access
these sites, which will either blow up the simulation, or get stuck
forever.  If you cap the forces, then weirder things will happen.  Is your
cap smoothly varying?  If not, then your dynamics on hitting the cap will
be unphysical.  How are the forces propagated into the energies (if grad U
=/= F, then weird non-newtonian physics will also happen).

> the forces on each atom are massive (on the order of 10^7).

What are the energies? Are they lower or higher than zero?

On Thu, May 9, 2019 at 8:43 AM John Whittaker <
johnwhitt...@zedat.fu-berlin.de> wrote:

> Hi all,
>
> I have a rather strange question that I hope someone can shed some light
> on.
>
> Before I begin, I want to note that I am pioneering some new developments
> of the Adaptive Resolution Simulation technique
> (https://doi.org/10.1002/adts.201900014), so the simulations/techniques I
> am performing/implementing are fairly non-standard with respect to normal
> atomistic simulations.
>
> With that in mind, I am simulating a box of TIP4P water and calculating
> structural/static properties. My simulations utilize a force-cap of 2000
> kJ/(mol nm) at each time step - i.e., when the force on an atom is larger
> than +/- 2000, the force is automatically normalized to +/- 2000 to
> prevent explosive forces due to atomic overlaps.
>
> For the most part, this works for the purposes of my simulations but I
> have observed some water molecules "sticking" together in the
> configuration shown here:
>
> https://www.dropbox.com/s/p5rkximspp25flf/tip4pDimer.jpg?dl=0
>
> with a corresponding O-H radial distribution function (unnormalized) shown
> here:
>
> https://www.dropbox.com/s/ez56db4qggv1iii/rdf_OH_long.jpg?dl=0
>
> where there is a clear (albeit, small) probability of finding a hydrogen
> atom an extremely short distance from an oxygen.
>
> The molecules travel together like this for several ps and then, for
> seemingly no reason, split apart and carry on perfectly fine for the rest
> of the simulation.
>
> I have performed a single-point energy calculation on this configuration
> in vacuum and have found, as one would expect, the forces on each atom are
> massive (on the order of 10^7). Yet, the molecules do not repel and seem
> to prefer this configuration for a short time.
>
> I have a feeling that this configuration is allowed when the forces are
> normalized to 2000 and the molecules become trapped there.
>
> I am wondering if anyone may have some experience with TIP4P water
> molecules taking on unphysical configurations for non-negligible times. I
> have not tried this same simulation using TIP3P yet, so I'm unsure if it
> has something to do with electrostatic interactions with the virtual site,
> but I will test this tomorrow.
>
> Thank you for any information/speculation/guesses as to why this is
> happening.
>
> - John
>
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[gmx-users] TIP4P molecules stuck together

2019-05-09 Thread John Whittaker
Hi all,

I have a rather strange question that I hope someone can shed some light on.

Before I begin, I want to note that I am pioneering some new developments
of the Adaptive Resolution Simulation technique
(https://doi.org/10.1002/adts.201900014), so the simulations/techniques I
am performing/implementing are fairly non-standard with respect to normal
atomistic simulations.

With that in mind, I am simulating a box of TIP4P water and calculating
structural/static properties. My simulations utilize a force-cap of 2000
kJ/(mol nm) at each time step - i.e., when the force on an atom is larger
than +/- 2000, the force is automatically normalized to +/- 2000 to
prevent explosive forces due to atomic overlaps.

For the most part, this works for the purposes of my simulations but I
have observed some water molecules "sticking" together in the
configuration shown here:

https://www.dropbox.com/s/p5rkximspp25flf/tip4pDimer.jpg?dl=0

with a corresponding O-H radial distribution function (unnormalized) shown
here:

https://www.dropbox.com/s/ez56db4qggv1iii/rdf_OH_long.jpg?dl=0

where there is a clear (albeit, small) probability of finding a hydrogen
atom an extremely short distance from an oxygen.

The molecules travel together like this for several ps and then, for
seemingly no reason, split apart and carry on perfectly fine for the rest
of the simulation.

I have performed a single-point energy calculation on this configuration
in vacuum and have found, as one would expect, the forces on each atom are
massive (on the order of 10^7). Yet, the molecules do not repel and seem
to prefer this configuration for a short time.

I have a feeling that this configuration is allowed when the forces are
normalized to 2000 and the molecules become trapped there.

I am wondering if anyone may have some experience with TIP4P water
molecules taking on unphysical configurations for non-negligible times. I
have not tried this same simulation using TIP3P yet, so I'm unsure if it
has something to do with electrostatic interactions with the virtual site,
but I will test this tomorrow.

Thank you for any information/speculation/guesses as to why this is
happening.

- John

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[gmx-users] dipole moment of water using TIP3P model

2019-05-09 Thread Sabreen Farnaz
Dear Users,
It is known that electric dipole moment of a water monomer is
experimentally 1.85 D and using the TIP3P model it's supposed to be 2.35D.
I am using the TIP3P model for a water-based simulation in Gromacs 5.1.5.
After applying sinusoidal electric fields in the Y axis, the norm of the
dipole vector per water molecule using *gmx dipoles* is closer to 1.85 D
and nowhere near 2.35D. My simulations are for 300K and 1 atm.
Can anyone guess why the discrepancy? Is it because 2.35D is for a water
monomer and my system has quite a large number of them(in the order of ten
thousands)? But literature suggests that presence of water molecules should
enhance the dipole moment. Or is 2.35D calculated under a different
temperature/pressure conditions?

If you could suggest me suitable references that might clarify this issue,
please let me know.

Thanks.
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Re: [gmx-users] ligand in water

2019-05-09 Thread Dallas Warren
This will do it (if need particular water model change with cs switch
options, and assumes ligand.gro has the correct final box size)

gmx solvate - cp ligand.gro -cs -o complex.gro

Unless you have a particular number of waters required, then use.:

gmx solvate - cp ligand.gro -cs -o complex.gro -maxsol 

To both above add -p topol.top if want it to automatically update the
topology file with number of molecules/residues. Otherwise you need to do
by hand, which is easy enough.

Or even if need a particular water coordinate file:

gmx insert-molecules -f ligand.gro -ci water.gro -nmol  -o complex.gro

On Thu, 9 May 2019, 7:02 pm RAHUL SURESH,  wrote:

> Hi Users.
>
> I want to simulate ligand in the water box. I prepared a water molecule and
> started with pdb2gmx and then planned to follow protein-ligand tutorial.
> Unfortunately ended up with an error in gro file format. Have check every
> possibility but still couldn't find any solution.
> My initial pdb is water.pdb and the corresponding gro file is water.gro. I
> clubbed the ligand gro file and water gro file as complex.gro. I have
> uploaded the file here. can anyone help me with the format issues>?
>
> --
> *Regards,*
> *Rahul *
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[gmx-users] ligand in water

2019-05-09 Thread RAHUL SURESH
Hi Users.

I want to simulate ligand in the water box. I prepared a water molecule and
started with pdb2gmx and then planned to follow protein-ligand tutorial.
Unfortunately ended up with an error in gro file format. Have check every
possibility but still couldn't find any solution.
My initial pdb is water.pdb and the corresponding gro file is water.gro. I
clubbed the ligand gro file and water gro file as complex.gro. I have
uploaded the file here. can anyone help me with the format issues>?

-- 
*Regards,*
*Rahul *
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Re: [gmx-users] gmx hbond query

2019-05-09 Thread Najamuddin Memon
Make index of water mediated hydrogens and DNA bases so that DNA bases are
in separate group and water mediated hydrogens in separate group in drop
down menu

On Thu, May 9, 2019, 11:54 AM  wrote:

> Dear all
> I want to determine the water mediated hydrogen between DNA bases and
> small molecule. What extra flag should I use in gmx hbond command? Is
> there any other option to capture the water mediated Hbonds? Please
> suggest something.
> Sunipa Sarkar
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Re: [gmx-users] Gromacs2018.5 install with gaussian09 for QM/MM

2019-05-09 Thread Groenhof, Gerrit


Hi,

I think it will still work if you use the "gau": script found here: 
http://wwwuser.gwdg.de/~ggroenh/qmmm.html#gaussian

best,

Gerrit



On 5/7/19 9:59 PM, ??? wrote:
> Dear Gromacs support,
> I want to install Gromacs 2018.5 with gaussian09 software support in Centos 
> system, I try to use ?--with-qmmm-gaussian? when I compile gromacs, but it 
> does not work. I wonder how to compile gromacs with gaussian support, please 
> help me ?
>
>
> The detail command is as follows:
>
> cmake .. -DCMAKE_INSTALL_PREFIX=/usr/local/gromacs \
>-DCMAKE_C_COMPILER=mpicc -DCMAKE_CXX_COMPILER=mpicxx \
>-DGMX_OPENMP=ON \
>-DGMX_FFT_LIBRARY=fftw3 \
>-DFFTWF_LIBRARY="/opt/fftw-3.3.8/lib/libfftw3f.a" \
>-DFFTWF_INCLUDE_DIR="/opt/fftw-3.3.8/include/"  \
>-DGMX_MPI=on \
>-DGMX_CPU_ACCELERATION=AVX_256 \
>--with-qmmm-gaussian \
>2>&1 | tee cm.log
> Gromacs 2018.5 compile and install successfully without ?--with-qmmm-gaussian 
> \?

That's extremely old syntax using the autoconf build system. What you
want is -DGMX_QMMM_PROGRAM=GAUSSIAN, but be aware that the QM/MM
interface in GROMACS is unmaintained and may not even currently work.





-Justin


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[gmx-users] gmx hbond query

2019-05-09 Thread spss4

Dear all
I want to determine the water mediated hydrogen between DNA bases and  
small molecule. What extra flag should I use in gmx hbond command? Is  
there any other option to capture the water mediated Hbonds? Please  
suggest something.

Sunipa Sarkar
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Re: [gmx-users] Implicit Solvent with User Defined Potentials

2019-05-09 Thread David van der Spoel

Den 2019-05-08 kl. 16:21, skrev Akash Banerjee:

Dear Gromacs Developer,

I want to use the implicit solvent (gbsa algorithm) along with User-defined
tabulated potentials. Apparently, the implicit solvent option is not
compatible with the vdw-type=USer option. Can I please get some advice on
this?

Thank you for your help.

Kind regards,
Akash

GB has been removed from GROMACS and if old versions do not have this 
option it seems you are out of luck.


--
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Head of Department, Cell & Molecular Biology, Uppsala University.
Box 596, SE-75124 Uppsala, Sweden. Phone: +46184714205.
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