Re: [gmx-users] Dihedral restraints in 4.6 vs 4.5.X

2013-03-18 Thread Per Larsson
Thanks  - I have filed issue #1194 and assigned it to David.
http://redmine.gromacs.org/issues/1194

Let me know if there is anything else that is needed. I could take a shot at 
myself, and will play around with it, but I don't know the details of the 
symtab in any detail, unfortunately. 

15 mar 2013 kl. 19:51 skrev David van der Spoel:
 
 Taking away the restraint allows me to start the run in 4.6.1, and also 
 reformatting the [ dihedral_restraint ] section to comply with 4.6 works.
 Is this a know issue, am I missing something obvious, or should I file an 
 issue on redmine?
 
 redmine please.
 
 
 Thanks
 /Per--
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 -- 
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 Dept. of Cell  Molec. Biol., Uppsala University.
 Box 596, 75124 Uppsala, Sweden. Phone:+46184714205.
 sp...@xray.bmc.uu.sehttp://folding.bmc.uu.se
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[gmx-users] Dihedral restraints in 4.6 vs 4.5.X

2013-03-15 Thread Per Larsson
Hi

I anyone aware of any issue starting simulations with 4.6 (or 4.6.1) from a 
4.5.X-tpr file with dihedral restraints?
I'm unsuccessful in making them start.

To investigate further, I created a small dialanine peptide in vacuum, with a 
dihedral restraint. 

Here's the details:

Making a 4.5.5 tpr with a dihedral restraint
$grompp -f md.mdp -c conf.gro -p topol.top -o md.tpr

Checking that it is there:
$gmxdump -s md.tpr |grep DIHRE
Reading file md.tpr, VERSION 4.5.5 (single precision)
functype[166]=DIHRES, label=0, power=   1 phi= 1.2000e+02, dphi= 
3.e+01, kfac= 1.e+00)



Now running this in 4.5.5 works fine, but starting it in 4.6 (or 4.6.1) gives 
me an error.

$ /Users/per/source/gromacs-4.6.1/build/src/kernel/mdrun -v -deffnm md
Reading file md.tpr, VERSION 4.5.5 (single precision)

---
Program mdrun, VERSION 4.6.1
Source code file: /Users/per/source/gromacs-4.6.1/src/gmxlib/symtab.c, line: 136

Fatal error:
symtab get_symtab_handle 1051260126 not found
For more information and tips for troubleshooting, please check the GROMACS
website at http://www.gromacs.org/Documentation/Errors
---

Taking away the restraint allows me to start the run in 4.6.1, and also 
reformatting the [ dihedral_restraint ] section to comply with 4.6 works. 
Is this a know issue, am I missing something obvious, or should I file an issue 
on redmine?

Thanks
/Per--
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Re: [gmx-users] cmaptypes format

2013-02-19 Thread Per Larsson
Hi Francesco

That number corresponds to a type for each cmap-entry. The idea (iirc, it was 
some time ago) was that it could be useful to be able to have multiple 
cmap-types (other grid values, different grid spacing etc) for the same 
cmap-dihedral (much like different torsions etc...), but based on a quick look 
in the code, the support for that is very limited. It should probably not be 
touched right now.

Cheers
/Per


19 feb 2013 kl. 15:43 skrev francesco oteri:

 Dear gromacs users,
 I am trying to figure out the meaning of the cmaptypes section in file
 section.
 As far as I understood, taking the following entry as example:
 
 C NH1 CT1 C NH1 1 24 24\
 
 C NH1 CT1 C   = phi
 H1 CT1 C NH1 = psi
 
 24*24 = dimension of the grid
 
 My question is: what does the 1 mean?
 
 Best,
 Francesco
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Re: [gmx-users] comparing gmx GB energy with Amber11

2012-11-09 Thread Per Larsson
After some investigation, it turns out that this is explained by the 
differences in input radii for the GB-calculation done by Gromacs and Amber.
The radii in the gbsa.itp-file are not the same as the ones used by Amber. 

If one changes the radii in gbsa.itp, you get a difference in 0-step energy (at 
least for the system below) of 0.2 kJ/mol, which is tolerable. I have pasted a 
copy of the gbsa.itp-file below, in case it is useful for someone. This was 
tested with amber99sb.

Cheers
/Per

[ implicit_genborn_params ]

; atype  sar  st pi   gbr   hct
;Br   0.1  1  10.125 0.85 ; H
C0.1721  1.5540.170.72 ; C
CA   0.18 1  1.0370.170.72 ; C
CB   0.1720.012  1.5540.170.72 ; C
CC   0.1721  1.5540.170.72 ; C
CN   0.1720.012  1.5540.170.72 ; C
CR   0.18 1  1.0730.170.72 ; C
CT   0.18 1  1.2760.17 0.72 ; C
CV   0.18 1  1.0730.170.72 ; C
CW   0.18 1  1.0730.170.72 ; C
C*   0.1720.012  1.5540.170.72 ; C
H0.1  1  10.13 0.85 ; H
HC   0.1  1  10.12 0.85 ; H
H1   0.1  1  10.12 0.85 ; H
HA   0.1  1  10.12 0.85 ; H
H4   0.1  1  10.12 0.85 ; H
H5   0.1  1  10.12 0.85 ; H
HO   0.1  1  10.12 0.85 ; H
HS   0.1  1  10.12 0.85 ; H
HP   0.1  1  10.12 0.85 ; H
N0.1551  1.0280.155   0.79 ; N
NA   0.1551  1.0280.155   0.79 ; N
NB   0.1551  1.2150.155   0.79 ; N
N2   0.16 1  1.2150.155   0.79 ; N
N3   0.16 1  1.2150.1550.79 ; N
O0.15 1  0.9260.15 0.85 ; O
OH   0.1521  1.0800.150.85 ; O
O2   0.17 1  0.9220.15 0.85 ; O
S0.18 1  1.1210.180.96 ; S
SH   0.18 1  1.1210.180.96 ; S

; masscenters for vsites do not have gbsa parameters

MNH3 00  00 0
MCH3 00  00 0



8 nov 2012 kl. 23:42 skrev Sandeep Somani:

 Hi Per
 
 I tried with single precision gmx as well. No change.
 
 Will send you input files soon.
 
 Best
 Sandeep
 
 On Thu, Nov 8, 2012 at 3:55 PM, Per Larsson per.lars...@sbc.su.se wrote:
 
 Hi
 
 Thanks for doing those test. They are all reassuring, I think.
 Could you maybe send me your input-files off list and I'll take a look.
 I suspect the issue is that different radii are being used, as Gromacs
 does not use the Bondi radii.
 
 Cheers
 /Per
 
 
 8 nov 2012 kl. 16:35 skrev Sandeep Somani:
 
 Hi Per
 
 Pls see inline comments:
 
 
 1. If I recall correctly, the GB-energy in gromacs is split into two
 parts, GB-polarization and non-polar solvation. Can you check whether
 this
 is the case and if the value you report is the sum of those two terms.
 
 
 Yes, gromacs prints out GB Polarization and Nonpolar Sol.
 corresponding to EGB and ESURF, respectively, from Amber.
 Right now I am just comparing EGB part (non polar also do not match but
 since it is a much smaller contribution, will worry about that later!).
 
 
 
 
 2. Try setting all cut-offs to 0 (infinite cutoffs). That will trigger a
 slightly different part of the code to do the GB-calculation (you should
 see in your log file references to all-vs-all kernels)
 
 
 Just tried -- no change.
 (btw, i didnt know 0 = no-cutoff. thnx!)
 
 
 
 3. Try running in single precision, keeping in mind 1 and 2 above to see
 if that helps. Also, try setting the GMX_NOOPTIMIZEDKERNELS variable to
 1
 (at least it used to be called that, someone else can perhaps correct
 me if
 that has changed). This will make the code run without the sse-loops.
 
 I'll try shortly.
 
 
 4. It could be that you are using different radii for the atoms in your
 system. For amber, are you using the Bondi-radii or something else?
 
 I tried both set default PBradii mbondi and set default PBradii
 mbondi2 while creating amber prmtop files in leap. The difference in EGB
 is just 2-3 kcal/mol .. not enough to bridge the gap.
 
 Best
 Sandeep
 
 
 
 
 
 
 
 Cheers
 /Per
 
 
 8 nov 2012 kl. 05:43 skrev Sandeep Somani:
 
 Hi,
 
 I am comparing single point amber ff energies from gmx4.5.5 (double
 precision) and Amber11.
 
 All bonded and non-bonded energy terms are in very good agreement
 (within
 0.1 kJ/mol) except GB:
 gmx 'GB polarization' = -200 kJ/mol
 amber 11 'EGB' = -283 kJ/mol.
 
 I am basically trying to replicate Amber's igb=5 + large cutoff in
 gmx.
 According to Amber manual igb=5 corresponds to model 2 of [2004 OBC
 paper].
 
 I translated

Re: [gmx-users] comparing gmx GB energy with Amber11

2012-11-08 Thread Per Larsson
Hi

A few things:

1. If I recall correctly, the GB-energy in gromacs is split into two parts, 
GB-polarization and non-polar solvation. Can you check whether this is the case 
and if the value you report is the sum of those two terms.

2. Try setting all cut-offs to 0 (infinite cutoffs). That will trigger a 
slightly different part of the code to do the GB-calculation (you should see in 
your log file references to all-vs-all kernels)

3. Try running in single precision, keeping in mind 1 and 2 above to see if 
that helps. Also, try setting the GMX_NOOPTIMIZEDKERNELS variable to 1 (at 
least it used to be called that, someone else can perhaps correct me if that 
has changed). This will make the code run without the sse-loops.

4. It could be that you are using different radii for the atoms in your system. 
For amber, are you using the Bondi-radii or something else?

Cheers
/Per


8 nov 2012 kl. 05:43 skrev Sandeep Somani:

 Hi,
 
 I am comparing single point amber ff energies from gmx4.5.5 (double
 precision) and Amber11.
 
 All bonded and non-bonded energy terms are in very good agreement (within
 0.1 kJ/mol) except GB:
 gmx 'GB polarization' = -200 kJ/mol
 amber 11 'EGB' = -283 kJ/mol.
 
 I am basically trying to replicate Amber's igb=5 + large cutoff in gmx.
 According to Amber manual igb=5 corresponds to model 2 of [2004 OBC
 paper].
 
 I translated this to the following mdp options:
  
 implicit_solvent= GBSA
 gb_algorithm= OBC
 All cut-offs (rcoulomb, rvdw, rlist, rgbradii) larger than the size of the
 molecule.
 {gb_epsilon_solvent, gb_saltconc, gb_obc_alpha, gb_obc_beta, gb_obc_gamma,
 gb_dielectric_offset} = corresponding Amber input.
  
 
 Is that correct?
 
 I realize that this is as much a question for Amber mailing list, but
 trying here first! Any idea?
 
 The molecule is ala-12. I'll be happy to send input files.
 
 Thanks in advance
 
 Sandeep
 
 --
 Postdoc
 Wales Group
 Cambridge
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Re: [gmx-users] comparing gmx GB energy with Amber11

2012-11-08 Thread Per Larsson
Hi

Thanks for doing those test. They are all reassuring, I think.
Could you maybe send me your input-files off list and I'll take a look. 
I suspect the issue is that different radii are being used, as Gromacs does not 
use the Bondi radii.

Cheers
/Per


8 nov 2012 kl. 16:35 skrev Sandeep Somani:

 Hi Per
 
 Pls see inline comments:
 
 
 1. If I recall correctly, the GB-energy in gromacs is split into two
 parts, GB-polarization and non-polar solvation. Can you check whether this
 is the case and if the value you report is the sum of those two terms.
 
 
 Yes, gromacs prints out GB Polarization and Nonpolar Sol.
 corresponding to EGB and ESURF, respectively, from Amber.
 Right now I am just comparing EGB part (non polar also do not match but
 since it is a much smaller contribution, will worry about that later!).
 
 
 
 
 2. Try setting all cut-offs to 0 (infinite cutoffs). That will trigger a
 slightly different part of the code to do the GB-calculation (you should
 see in your log file references to all-vs-all kernels)
 
 
 Just tried -- no change.
 (btw, i didnt know 0 = no-cutoff. thnx!)
 
 
 
 3. Try running in single precision, keeping in mind 1 and 2 above to see
 if that helps. Also, try setting the GMX_NOOPTIMIZEDKERNELS variable to 1
 (at least it used to be called that, someone else can perhaps correct me if
 that has changed). This will make the code run without the sse-loops.
 
 I'll try shortly.
 
 
 4. It could be that you are using different radii for the atoms in your
 system. For amber, are you using the Bondi-radii or something else?
 
 I tried both set default PBradii mbondi and set default PBradii
 mbondi2 while creating amber prmtop files in leap. The difference in EGB
 is just 2-3 kcal/mol .. not enough to bridge the gap.
 
 Best
 Sandeep
 
 
 
 
 
 
 
 Cheers
 /Per
 
 
 8 nov 2012 kl. 05:43 skrev Sandeep Somani:
 
 Hi,
 
 I am comparing single point amber ff energies from gmx4.5.5 (double
 precision) and Amber11.
 
 All bonded and non-bonded energy terms are in very good agreement (within
 0.1 kJ/mol) except GB:
 gmx 'GB polarization' = -200 kJ/mol
 amber 11 'EGB' = -283 kJ/mol.
 
 I am basically trying to replicate Amber's igb=5 + large cutoff in gmx.
 According to Amber manual igb=5 corresponds to model 2 of [2004 OBC
 paper].
 
 I translated this to the following mdp options:
 
 implicit_solvent= GBSA
 gb_algorithm= OBC
 All cut-offs (rcoulomb, rvdw, rlist, rgbradii) larger than the size of
 the
 molecule.
 {gb_epsilon_solvent, gb_saltconc, gb_obc_alpha, gb_obc_beta,
 gb_obc_gamma,
 gb_dielectric_offset} = corresponding Amber input.
 
 
 Is that correct?
 
 I realize that this is as much a question for Amber mailing list, but
 trying here first! Any idea?
 
 The molecule is ala-12. I'll be happy to send input files.
 
 Thanks in advance
 
 Sandeep
 
 --
 Postdoc
 Wales Group
 Cambridge
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Re: [gmx-users] MM/PBSA Gromacs

2011-11-30 Thread Per Larsson
Hi!

There is support in gromacs for gb calculations. However, I'm currently 
investigating some recent reports about  unstable simulations (unfolding 
proteins), so my advice is to use the code with caution.

Thanks
/Per


30 nov 2011 kl. 20:04 skrev R.S.K.Vijayan biovija...@gmail.com:

 Dear Gromacs users
 
 Is there any script  that does a PB or GB calculation to perform a 
 MM/PB(GB)SA free energy  calculation in Gromacs. Similar to the MMPBSA.py 
 script available in Amber.  I find a similar question raised by a user a 
 couple of years back.  Any successful implementation
 
 
 Vijayan.R  
 
 
 
 On Wed, Nov 30, 2011 at 1:26 PM, Justin A. Lemkul jalem...@vt.edu wrote:
 
 
 김현식 wrote:
 Dear Experts,
  Hi,
  Is there any tools in gromacs to get Hydrophobic cores of protein ?
  
 
 I suppose that depends on what your definition is, but in all likelihood no, 
 not directly.  A program like g_sas can give you nonpolar and polar surface 
 areas as well as volumes and surface atoms, which, through crafty use of 
 index groups, may provide you with something useful.
 
 -Justin
 
 -- 
 
 
 Justin A. Lemkul
 Ph.D. Candidate
 ICTAS Doctoral Scholar
 MILES-IGERT Trainee
 Department of Biochemistry
 Virginia Tech
 Blacksburg, VA
 jalemkul[at]vt.edu | (540) 231-9080
 http://www.bevanlab.biochem.vt.edu/Pages/Personal/justin
 
 
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Re: [gmx-users] System heating up during MD run? (Implicit solvent)

2011-10-31 Thread Per Larsson
Hi

There has been a number of reports lately about ill-behaving simulations using 
implicit solvent. I'm currently trying to investigate the cause of this, as 
such simulations used to work very nice in our hands.

In the meantime I would advice to use implicit solvent with caution.

Thanks
/Per

Skickat från min iPhone

30 okt 2011 kl. 02:10 skrev Matt Larson larsonma...@gmail.com:

 I've been having problems getting implicit solvent systems (which are
 probably fairly experiment still in gromacs) to work correctly.  I've
 been modelling a protein of about 11000 atoms with hydrogens in a 2 ns
 simulation.  By the end of the simulation, the temperature has risen
 from 300 K to 496 K - and the protein unfolds.  It was supposed to
 maintain temp at 300 K.
 
 I have an a non-zero total charge of -6.99.  With explicit
 solvent, I would normally add the appropriate matching ions, but with
 implicit solvent what should you do?   Could the non-zero total charge
 result in heating?  Or is the thermostat not working well enough
 (should I change tau-t or ref-t?)
 
 Here is my md.mdp file:
 
 
 constraints =  all-bonds ; trying..
 integrator  =  md
 dt  =  0.002; ps !
 nsteps  =  100
 nstlist =  10
 ns_type =  grid
 rlist   =  1.0
 coulombtype =  cut-off
 fourierspacing  =  0.16
 vdwtype =  cut-off
 rcoulomb=  1.0
 rvdw=  1.0  ; important for neighbor searching
 pbc =  no   ; no periodic boundary conditions
 epsilon_rf  =  0
 rgbradii=  1.0  ; must equal rlist, rcoulomb, rvdw
 comm_mode   =  angular
 optimize_fft= yes
 
 implicit_solvent= GBSA
 gb_algorithm= OBC
 gb_epsilon_solvent  = 80
 sa_surface_tension  = 2.25936
 
 nstcomm = 10
 nstxout = 1000
 nstxtcout   = 1000
 nstvout = 0
 nstfout = 0
 
 tcoupl  = andersen
 tc-grps = system
 tau-t   = 0.1
 ref-t   = 300
 
 gen_vel = yes
 gen_temp= 300
 gen_seed= -1
 
 -
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Re: [gmx-users] Energy Drift

2011-10-19 Thread Per Larsson
Hi Justin!

Do you maybe have an example of such a protein (preferably not too large :-), 
that I could run some tests on?

I'd be interested in seeing if there has been any bugs introduced in the cutoff 
code that destabilises proteins that way.

Thanks
/Per

18 okt 2011 kl. 23:41 skrev Justin A. Lemkul jalem...@vt.edu:

 
 
 Ben Reynwar wrote:
 I posted to the list a few days ago with an energy drift problem.
 Mark Abraham helpfully suggested using all-bonds rather than h-bonds
 which solved the problem.  I'm now trying to understand quite why that
 helped so much.
 The simulation is a protein of about 5000 atoms using GBSA, a time
 step of 2 fs, and a cut-off of 1.6 for VdW, coulomb and GB.
 I've run energy drift simulations using the md integrator, with no
 thermostat, and using the ld integrator with a tau_t of 100.
 Simulations were run changing various parameters.  The changes were:
 - dt reduced to 1.5
 - dt reduced to 1.0
 - cutoff increased to 2.0
 - constraint changed from h-bonds to all-bonds
 Plot of the energy drifts can be seen at
 http://www.reynwar.net/ben/gromacs/energy_drift.png.
 Noticeable features are:
 - changing the time step makes no difference (in my last post I
 claimed it did, which is why you should make plots rather than
 eyeballing log files).
 - increasing the cut-off helps a lot.
 - changing constraint to all-bonds make a dramatic difference
 - using ld there is a downwards drift in the energy when using
 all-bonds constraint.  The temperature is roughly 300 K and the set
 point is 400 K so this downwards drift seems unlikely to be due to
 coupling to the langevin thermostat.
 My questions are:
 - why does the all-bonds constraint help so much?
 - why doesn't moving to a smaller time step help with this?
 - what is the cause of the downwards drift when using ld with all-bonds?
 
 I can offer a bit of general advice here, but no specific answers.  Hopefully 
 it helps.  To get at the root cause of all of this, you should be analyzing 
 individual energy components, not just the total energy.  These will tell you 
 which terms are systematically changing.
 
 In my experience with GB simulations, using anything other than infinite 
 cutoffs (i.e. all-vs-all kernel) has resulted in unstable simulations.  I 
 don't mean that the simulations crash or anything, but the results are 
 clearly incorrect. Stably folded proteins have drastically increased RMSD and 
 lose their structure very easily.  The effect is independent of the chosen 
 force field.  I would recommend always using infinite cutoffs for GB 
 simulations.  It may improve your situation.
 
 -Justin
 
 -- 
 
 
 Justin A. Lemkul
 Ph.D. Candidate
 ICTAS Doctoral Scholar
 MILES-IGERT Trainee
 Department of Biochemistry
 Virginia Tech
 Blacksburg, VA
 jalemkul[at]vt.edu | (540) 231-9080
 http://www.bevanlab.biochem.vt.edu/Pages/Personal/justin
 
 
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Re: [gmx-users] Simulation runs on iMac but explodes on cluster

2011-07-13 Thread Per Larsson
Hi!

Could you try running with GMX_NOOPTIMIZEDKERNELS=1, to see if this could 
potentially be a bug in the sse code (I noticed nb_kernel410_x86_64_sse in your 
error message.

Thanks
/Per




13 jul 2011 kl. 09.35 skrev Luke Goodsell:

 As the subject suggests, I have a simulation that runs correctly on my iMac, 
 but fails when I try to run it on a cluster, and I am hoping someone may be 
 able to suggest which things to try first to resolve the issue.
 

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Re: [gmx-users] Questions about GB parameters

2011-07-06 Thread Per Larsson
Hi!

Yes, I did! Had to look up a conversation between me and the Tinker developers 
about precisely this.

The values are indeed not the original ones, but rather developed internally by 
Tinker people so to minimise differences between analytical surface areas and 
GB, given the HCT-algorithm and using per-atom rather than per-pair scale 
factors. The values have not been published anywhere as such but have been 
used by others and seem fairly robust, according to Tinker developers. 

In the light of all other approximations introduced with implicit solvent, the 
differences in results should be minor. 

Of course this needs to be properly documented, and it was very good that some 
light was shed on this.

/Per


6 jul 2011 kl. 04:29 skrev Justin A. Lemkul jalem...@vt.edu:

 
 
 Per Larsson wrote:
 Hi!
 I did some digging and think I can clarify at least the first question.
 Sorry for the confusion with regard to the earlier post. What is specified in
 the gbsa.itp file under the gbr column is indeed vdW-radii. These are used to
 compute Born radii, as the manual says. The dielectric offset is subtracted
 from the vdW radii, as this has been shown to improve the agreement between
 PB and GB calculations (see eg. the OBC-paper, Onufriev, Bashford and Case,
 Proteins, 55, 383-394).
 For the second question, I am a little confused myself now. The values found
 in the gbsa.itp-file are exactly those found in the Tinker package (in the
 ksolv.f-routine), which also cites the same reference. Hmm...I'll be back
 again for this one.
 
 Have you uncovered anything?  I've tried contacting the Tinker developers but 
 have received no response.  I found the routine (in Tinker's born.f) that 
 utilizes the values, but I still have no idea where they come from or why 
 they're fixed for a given atom type rather than a given pair.
 
 -Justin
 
 -- 
 
 
 Justin A. Lemkul
 Ph.D. Candidate
 ICTAS Doctoral Scholar
 MILES-IGERT Trainee
 Department of Biochemistry
 Virginia Tech
 Blacksburg, VA
 jalemkul[at]vt.edu | (540) 231-9080
 http://www.bevanlab.biochem.vt.edu/Pages/Personal/justin
 
 
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Re: [gmx-users] Questions about GB parameters

2011-06-22 Thread Per Larsson
Hi!

I did some digging and think I can clarify at least the first question.

Sorry for the confusion with regard to the earlier post. What is specified in 
the gbsa.itp file under the gbr column is indeed vdW-radii. These are used to 
compute Born radii, as the manual says. The dielectric offset is subtracted 
from the vdW radii, as this has been shown to improve the agreement between PB 
and GB calculations (see eg. the OBC-paper, Onufriev, Bashford and Case, 
Proteins, 55, 383-394).  

For the second question, I am a little confused myself now. The values found in 
the gbsa.itp-file are exactly those found in the Tinker package (in the 
ksolv.f-routine), which also cites the same reference. Hmm...I'll be back again 
for this one.

Cheers
/Per


21 jun 2011 kl. 18.42 skrev Justin A. Lemkul:

 
 Can anyone comment further on either of these issues?
 
 -Justin
 
 Mark Abraham wrote:
 On 15/06/2011 4:24 AM, Justin A. Lemkul wrote:
 
 Hi All,
 
 I wanted to dig up an old discussion that hit the list a long time ago 
 because I'm now encountering some problems understanding the GB settings 
 myself.  The discussion in question is here:
 
 http://lists.gromacs.org/pipermail/gmx-users/2010-August/053373.html
 
 I wanted to post a couple of questions based on Per's response.
 
 1. Based on that post, it seems to me that the value in the gbr column 
 should have a dielectric offset added to it during the GB calculations.  In 
 the code, though (genborn.c, around line 484 in the latest 
 release-4-5-patches), it looks like the dielectric offset is subtracted, 
 not added.  I guess the code is reversing the process, going from GB radius 
 back to vdW radius by subtracting the dielectric offset?  It seems, then, 
 that the parameters in gbsa.itp should specify GB radii, not vdW radii, 
 though the manual says the gbr column is atomic van der Waals radii, which 
 are used in computing the Born radii.  Is the opposite actually true?
 It does look to me as though something is mis-sense here. The quantity given 
 in gb_dielectric_offset is always subtracted from a value that I think is 
 found in the gbr column of [implicit_genborn_parameters].
 Mark
 2. I am still unclear on the source of the HCT scaling factors.  From the 
 reference cited in the manual, it would seem that scaling factors are 
 interaction-dependent, at least when H atoms are concerned.  I also cannot 
 find any indication of where these values came from.  None of the values of 
 Table 2 in the HCT reference match the contents of the hct column.  Again 
 I wonder if I'm missing something obvious :)
 
 Thanks for any insight!
 
 -Justin
 
 
 -- 
 
 
 Justin A. Lemkul
 Ph.D. Candidate
 ICTAS Doctoral Scholar
 MILES-IGERT Trainee
 Department of Biochemistry
 Virginia Tech
 Blacksburg, VA
 jalemkul[at]vt.edu | (540) 231-9080
 http://www.bevanlab.biochem.vt.edu/Pages/Personal/justin
 
 
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Re: [gmx-users] Questions about GB parameters

2011-06-14 Thread Per Larsson
Hi!

Hmm.. Let me see if I can shed some more light on this. It's been a while 
though since I visited the literature here, and also my laptop broke down 
today, so I need to take of that first before I can check the code!

Thanks
/Per


14 jun 2011 kl. 20:24 skrev Justin A. Lemkul jalem...@vt.edu:

 
 Hi All,
 
 I wanted to dig up an old discussion that hit the list a long time ago 
 because I'm now encountering some problems understanding the GB settings 
 myself.  The discussion in question is here:
 
 http://lists.gromacs.org/pipermail/gmx-users/2010-August/053373.html
 
 I wanted to post a couple of questions based on Per's response.
 
 1. Based on that post, it seems to me that the value in the gbr column should 
 have a dielectric offset added to it during the GB calculations.  In the 
 code, though (genborn.c, around line 484 in the latest release-4-5-patches), 
 it looks like the dielectric offset is subtracted, not added.  I guess the 
 code is reversing the process, going from GB radius back to vdW radius by 
 subtracting the dielectric offset?  It seems, then, that the parameters in 
 gbsa.itp should specify GB radii, not vdW radii, though the manual says the 
 gbr column is atomic van der Waals radii, which are used in computing the 
 Born radii.  Is the opposite actually true?
 
 2. I am still unclear on the source of the HCT scaling factors.  From the 
 reference cited in the manual, it would seem that scaling factors are 
 interaction-dependent, at least when H atoms are concerned.  I also cannot 
 find any indication of where these values came from.  None of the values of 
 Table 2 in the HCT reference match the contents of the hct column.  Again I 
 wonder if I'm missing something obvious :)
 
 Thanks for any insight!
 
 -Justin
 
 -- 
 
 
 Justin A. Lemkul
 Ph.D. Candidate
 ICTAS Doctoral Scholar
 MILES-IGERT Trainee
 Department of Biochemistry
 Virginia Tech
 Blacksburg, VA
 jalemkul[at]vt.edu | (540) 231-9080
 http://www.bevanlab.biochem.vt.edu/Pages/Personal/justin
 
 
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Re: [gmx-users] Is it possible to run implicit solvent simulations in parallel?

2011-05-04 Thread Per Larsson
Hi!

If you are running implicit solvent with no cutoffs, ie using the special 
all-vs-all kernels, then particle decomposition will be used. This exact 
combination (gb, all-vs-all, dd) is quite tricky to implement, and is not 
supported at the moment, IIRC. 
This could be documented better, sorry.

You could try changing constraints from all-bonds to h-bonds, meaning you will 
have only local constraints, which should allow you to run with particle 
decomposition. Or use a cut-off and domain decomposition. 

/Per



4 maj 2011 kl. 16.05 skrev Ozlem Ulucan:

 Dear Justin, this was only a test run and I ran the simulations on my 
 multi-core workstations (4 cores actually). MPI is no longer required for 
 such a situation. Since I did not set -nt option to 1, this can be accepted 
 as a parallel run. So the command I sent in my previous e-mail was for the 
 parallel run and for serial run I set -nt to 1.
 
 
 Dear Justin, as I said I am using a workstation of 4 processors. I have  
 approximately 2200 atoms in my system. That means for one processor I have 
 slightly more than  550 atoms. I set all the cut-offs to 0. I really need to 
 run this system in parallel. Any suggestions to make it work out? 
 
 
 Here is my run input file :
 
 ;
 ;File 'mdout.mdp' was generated
 ;By user: onbekend (0)
 ;On host: onbekend
 ;At date: Sun May  1 16:19:29 2011
 ;
 
 ; VARIOUS PREPROCESSING OPTIONS
 ; Preprocessor information: use cpp syntax.
 ; e.g.: -I/home/joe/doe -I/home/mary/roe
 include  = 
 ; e.g.: -DPOSRES -DFLEXIBLE (note these variable names are case sensitive)
 define   = 
 
 ; RUN CONTROL PARAMETERS
 integrator   = SD
 ; Start time and timestep in ps
 tinit= 0
 dt   = 0.002
 nsteps   = 50
 ; For exact run continuation or redoing part of a run
 init_step= 0
 ; Part index is updated automatically on checkpointing (keeps files separate)
 simulation_part  = 1
 ; mode for center of mass motion removal
 comm-mode= Angular
 ; number of steps for center of mass motion removal
 nstcomm  = 10
 ; group(s) for center of mass motion removal
 comm-grps= system
 
 ; LANGEVIN DYNAMICS OPTIONS
 ; Friction coefficient (amu/ps) and random seed
 bd-fric  = 0
 ld-seed  = 1993
 
 ; ENERGY MINIMIZATION OPTIONS
 ; Force tolerance and initial step-size
 emtol= 10.0
 emstep   = 0.01
 ; Max number of iterations in relax_shells
 niter= 20
 ; Step size (ps^2) for minimization of flexible constraints
 fcstep   = 0
 ; Frequency of steepest descents steps when doing CG
 nstcgsteep   = 1000
 nbfgscorr= 10
 
 ; TEST PARTICLE INSERTION OPTIONS
 rtpi = 0.05
 
 ; OUTPUT CONTROL OPTIONS
 ; Output frequency for coords (x), velocities (v) and forces (f)
 nstxout  = 1000
 nstvout  = 1000
 nstfout  = 0
 ; Output frequency for energies to log file and energy file
 nstlog   = 1000
 nstcalcenergy= -1
 nstenergy= 1000
 ; Output frequency and precision for .xtc file
 nstxtcout= 0
 xtc-precision= 500
 ; This selects the subset of atoms for the .xtc file. You can
 ; select multiple groups. By default all atoms will be written.
 xtc-grps = Protein
 ; Selection of energy groups
 energygrps   = Protein
 
 ; NEIGHBORSEARCHING PARAMETERS
 ; nblist update frequency
 nstlist  = 0
 ; ns algorithm (simple or grid)
 ns_type  = simple
 ; Periodic boundary conditions: xyz, no, xy
 pbc  = no
 periodic_molecules   = no
 ; nblist cut-off
 rlist= 0
 ; long-range cut-off for switched potentials
 rlistlong= -1
 
 ; OPTIONS FOR ELECTROSTATICS AND VDW
 ; Method for doing electrostatics
 coulombtype  = cut-off
 rcoulomb-switch  = 0
 rcoulomb = 0
 ; Relative dielectric constant for the medium and the reaction field
 epsilon_r= 1
 epsilon_rf   = 1
 ; Method for doing Van der Waals
 vdw-type = Cut-off
 ; cut-off lengths   
 rvdw-switch  = 0
 rvdw = 0
 ; Apply long range dispersion corrections for Energy and Pressure
 DispCorr = No
 ; Extension of the potential lookup tables beyond the cut-off
 table-extension  = 1
 ; Seperate tables between energy group pairs
 energygrp_table  = 
 ; Spacing for the PME/PPPM FFT grid
 fourierspacing   = 0.12
 ; FFT grid size, when a value is 0 fourierspacing will be used
 fourier_nx   = 0
 fourier_ny   = 0
 fourier_nz   = 0
 ; EWALD/PME/PPPM parameters
 pme_order  

Re: [gmx-users] implicit solvent GB force table

2011-03-31 Thread Per Larsson
Hi!

The tabulated function is applied to all interactions, both bonded and 
non-bonded. The function is initialized in make_gb_table(), and accessed in the 
non-bonded kernels the same way as other tabulated functions are accessed. See 
GBtab[nnn] in the kernels for more details.

In calc_gb_chainrule() the values of dadx (the derivative of the radii wrt. to 
the coordinates), and dvda (the derivative of the potential wrt. to the radii), 
which are calculated in the kernels, are simply multiplied together to yield 
the total force.

Cheers
/Per

31 mar 2011 kl. 21.09 skrev Chi-cheng Chiu:

 Hi,
 I have been tracking the code for implicit solvent, i.e. src/mdlib/genborn.c 
 According to the gromacs paper on implicit solvent, J Comp Chem 31:2593, 
 2010, the GB force is tabulated in the X = Rij Ci Cj dimension. 
 However, the tabulated function, which I think is stored in fr-gbtab, is 
 only used in the function gb_bonds_tab(). 
 I could not find the function of X applied in the calc_gb_chainrule() 
 function. Does the gbtab applied on dvda and dadx elsewhere? Thanks in 
 advance!
 
 regards,
 
 Chi-cheng
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Re: [gmx-users] implicit solvent model: formulation of non-polar free energy

2011-03-28 Thread Per Larsson
Hi!

I know about this difference. The only reason for it is that, when I first 
started with this I used Tinker as a reference implementation, which has the 
6-th power in the code.

The differences should be small, though. The non-polar part only amounts to a 
few percent of the total force anyway.

Cheers
/Per

28 mar 2011 kl. 21:24 skrev Chi-cheng Chiu none0...@gmail.com:

 Hi everyone,
 I am going through the source code for the GB calculation part of gromacs, 
 and found the following code in src/mdlib/genborn.c :
 in the function  real calc_gb_nonpolar()
 
 rai   = top-atomtypes.gb_radius[md-typeA[ai]];
 rbi_inv   = fr-invsqrta[ai];
 rbi_inv2  = rbi_inv * rbi_inv;
 tmp   = (rai*rbi_inv2)*(rai*rbi_inv2);
 tmp   = tmp*tmp*tmp;
 e = factor*term*(rai+probe)*(rai+probe)*tmp;
 dvda[ai]  = dvda[ai] - 6*e*rbi_inv2;
 es= es + e;
 
 so from this source code, energy seems to be (rai+probe)^2 * (rai/rbi)^6
 where rbi is the born radius, rai is the atom radius, and probe is 0.14 nm.
 I checked the reference Schaefer et al. JMB 284(3):835–848, 1998 which is 
 mentioned in the manual.
 It seems the reference used (rai+probe)^2 * (rai/rbi) 
 where (rai/rbi) term don't have power of 6 and disagree with the source code.
 Is there a reason using power 6?
 
 Chi-cheng
 
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Re: [gmx-users] IMPLICIT SOLVENT IN AMBER

2011-03-10 Thread Per Larsson
Hi!

Starting an implicit solvent simulation works just as starting a normal, 
explicit solvent simulation, except there is no solvent molecules.
You should use version 4.5.3 for this though (4.0.5 will not work). 

Then you specify in the mdp-file implicit_solvent = GBSA and use pdb2gmx, 
grompp, mdrun etc... as you otherwise would do.
The choice of the Born radii model is set by gb_algorithm = {Still,HCT,OBC} and 
the non-polar solvation is calculated using sa_algorithm=Ace-approximation.

Cheers
/Per

10 mar 2011 kl. 10.10 skrev Yulian Gavrilov:

 Dear, all
 I just begin to work in gromacs.
 I would like to run on a protein with amber99. 
 Is there someone here that successfully did a protein simulation in
 GROMACS with implicit solvent and willing to explain the procedure and
 share the parameters used (especially force field). 
 
 In mdout.mdp (gromacs 4.0.5) I found this lines. Can I add them to md.mdp? 
 How to change this parameters correctly? 
 What changes should be done on the previous steps? I mean, how to start a 
 simulation with implicit solvent model from the very beginning?
 Sorry for primitive question, but I did not found any useful information 
 about it for the begginers.
 
 ; IMPLICIT SOLVENT ALGORITHM
 implicit_solvent = No
 
 ; GENERALIZED BORN ELECTROSTATICS
 ; Algorithm for calculating Born radii
 gb_algorithm = Still
 ; Frequency of calculating the Born radii inside rlist
 nstgbradii   = 1
 ; Cutoff for Born radii calculation; the contribution from atoms
 ; between rlist and rgbradii is updated every nstlist steps
 rgbradii = 2
 ; Dielectric coefficient of the implicit solvent
 gb_epsilon_solvent   = 80
 ; Salt concentration in M for Generalized Born models
 gb_saltconc  = 0
 ; Scaling factors used in the OBC GB model. Default values are OBC(II)
 gb_obc_alpha = 1
 gb_obc_beta  = 0.8
 gb_obc_gamma = 4.85
 ; Surface tension (kJ/mol/nm^2) for the SA (nonpolar surface) part of GBSA
 ; The default value (2.092) corresponds to 0.005 kcal/mol/Angstrom^2.
 sa_surface_tension   = 2.092
 
 -- 
 Sincerely,
 Yulian Gavrilov
 
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Re: [gmx-users] IMPLICIT SOLVENT IN AMBER

2011-03-10 Thread Per Larsson
Hi!

The answer is that I do not now critical it is.
I have seen some papers that seem to hint at it not being overly critical, but, 
again, life does not come at a net charge.
You'd have to see for yourself in your system, given the observables that are 
important I suppose.
Possibly we can implement this in the future, as there indeed seems to be some 
interest in it, but that is not a task I can deal with currently.

/Per


10 mar 2011 kl. 10.52 skrev Yulian Gavrilov:

 Thanks again!
 Don't you know how to make a total charge = 0 in this case, if implicit salt 
 concentration is not implemented currently? Or it is not critically? 
 
 2011/3/10 Per Larsson per.lars...@sbc.su.se
 Hi!
 
 Yes, except that in point 2, I'm not sure about the effects of explicit ions 
 in an implicit solvent. 
 Do deal with that properly one should use an implicit salt concentration, but 
 that is not implemented currently. 
 The choice of water-model with pdb2gmx is not important. You can choose 
 'None' here.
 
 Cheers
 /Per
 
 10 mar 2011 kl. 10.39 skrev Yulian Gavrilov:
 
 Thanks!
 If I understand you correctly, I need to do this (?):
 pdb2gmx
 Adding ions (if I have no SOL, what is better to choose on this step?)
 Minimization with mdp file, that includes these lines:
 implicit_solvent = GBSA
 gb_algorithm = {Still,HCT,OBC}
 sa_algorithm=Ace-approximation
 Equilibration (nvt, npt) and MD also with these lines in mdp files.
 
 
 2011/3/10 Per Larsson per.lars...@sbc.su.se
 Hi!
 
 Starting an implicit solvent simulation works just as starting a normal, 
 explicit solvent simulation, except there is no solvent molecules.
 You should use version 4.5.3 for this though (4.0.5 will not work). 
 
 Then you specify in the mdp-file implicit_solvent = GBSA and use pdb2gmx, 
 grompp, mdrun etc... as you otherwise would do.
 The choice of the Born radii model is set by gb_algorithm = {Still,HCT,OBC} 
 and the non-polar solvation is calculated using 
 sa_algorithm=Ace-approximation.
 
 Cheers
 /Per
 
 10 mar 2011 kl. 10.10 skrev Yulian Gavrilov:
 
 Dear, all
 I just begin to work in gromacs.
 I would like to run on a protein with amber99. 
 Is there someone here that successfully did a protein simulation in
 GROMACS with implicit solvent and willing to explain the procedure and
 share the parameters used (especially force field). 
 
 In mdout.mdp (gromacs 4.0.5) I found this lines. Can I add them to md.mdp? 
 How to change this parameters correctly? 
 What changes should be done on the previous steps? I mean, how to start a 
 simulation with implicit solvent model from the very beginning?
 Sorry for primitive question, but I did not found any useful information 
 about it for the begginers.
 
 ; IMPLICIT SOLVENT ALGORITHM
 implicit_solvent = No
 
 ; GENERALIZED BORN ELECTROSTATICS
 ; Algorithm for calculating Born radii
 gb_algorithm = Still
 ; Frequency of calculating the Born radii inside rlist
 nstgbradii   = 1
 ; Cutoff for Born radii calculation; the contribution from atoms
 ; between rlist and rgbradii is updated every nstlist steps
 rgbradii = 2
 ; Dielectric coefficient of the implicit solvent
 gb_epsilon_solvent   = 80
 ; Salt concentration in M for Generalized Born models
 gb_saltconc  = 0
 ; Scaling factors used in the OBC GB model. Default values are OBC(II)
 gb_obc_alpha = 1
 gb_obc_beta  = 0.8
 gb_obc_gamma = 4.85
 ; Surface tension (kJ/mol/nm^2) for the SA (nonpolar surface) part of GBSA
 ; The default value (2.092) corresponds to 0.005 kcal/mol/Angstrom^2.
 sa_surface_tension   = 2.092
 
 -- 
 Sincerely,
 Yulian Gavrilov
 
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Re: [gmx-users] RE: g_energy inconsistent results

2011-03-10 Thread Per Larsson
Hi!

When you are computing your zero-step energies, do you then start from the 
gro-file that you got from em? If so, maybe the energies changes because 
gro-files have a fixed precision format (with three decimals), while the 
em-calculations are done using either full single or double precision.

Your second issue is almost certainly related to rounding errors. The 
all-vs-all and the cutoff-code (even with enormous cut-offs) compute 
interactions in completely order. I would not worry about a 0.005 nm difference 
in RMSD.

/Per

10 mar 2011 kl. 14.27 skrev Ehud Schreiber:

 Dear Mark Abraham (and anyone else interested),
 
 I have implemented your suggestion, changing in the status.mdp file to
 integrator = md and adding continuation = yes (this is the new name of
 the unconstrained_start parameter); however, this did not have any
 effect - the energy remained as before, different from the one obtained
 during the minimization.
 
 I have then encountered another (perhaps related) issue.
 I thought that the problem may arise from the combination of the
 generalized Born and all-vs-all settings.
 I have therefore changed in the minimization to rgbradii = rlist =
 rcoulomb = rvdw = 100 (from = 0).
 As my system is far smaller than 100 nm, I expected these parameters to
 provide also an all-vs-all setting (even if non-optimized).
 Nevertheless, the resulting structure differed from the previous
 minimized one (rmsd ~ 0.005 nm, delta energy ~ a few kJ/mol). Can this
 arise from rounding effects only or does this signify a problem? I'm not
 sure what rgbradii does, but the manual states that it must equal rlist.
 In addition, changing also status.mdp to have all radii = 100 and
 running on the new optimized output again does not yield the same energy
 as during the optimization. 
 
 Does all of this make any sense to you?
 
 Thank,
 Ehud.
 
 
 Message: 6
 Date: Tue, 08 Mar 2011 23:37:12 +1100
 From: Mark Abraham mark.abra...@anu.edu.au
 Subject: Re: [gmx-users] g_energy inconsistent results
 To: Discussion list for GROMACS users gmx-users@gromacs.org
 Message-ID: 4d7622f8.7050...@anu.edu.au
 Content-Type: text/plain; charset=iso-8859-1
 
 On 8/03/2011 9:44 PM, Ehud Schreiber wrote:
 
 Dear Gromacs users,
 
 I am working with version 4.5.3, using the opls-aa forcefield in an
 implicit solvent, all-vs-all setting:
 
 pdb2gmx -ter -ff oplsaa -water none -f file.pdb
 
 I am energy-minimizing structures in 3 stages (steep, cg and l-bfgs).
 
 The last stage is the following:
 
 grompp -f em3.mdp -p topol.top -c em2.gro -t em2.trr -o em3.tpr -po
 em3.mdout.mdp
 mdrun -nice 0 -v -pd -deffnm em3
 g_energy -s em3.tpr -f em3.edr -o em3.potential_energy.xvg
 
 where the mdp file is:
 
 ;;; em3.mdp ;;;
 integrator   = l-bfgs
 nsteps   = 5
 implicit_solvent = GBSA
 gb_algorithm = Still
 sa_algorithm = Ace-approximation
 pbc  = no
 rgbradii = 0
 ns_type  = simple
 nstlist  = 0
 rlist= 0
 coulombtype  = cut-off
 rcoulomb = 0
 vdwtype  = cut-off
 rvdw = 0
 nstcalcenergy= 1
 nstenergy= 1000
 emtol= 0
 ;;;
 
 The last line in the em3.potential_energy.xvg file should give the
 (potential) energy of the minimized structure em3.gro .
 
 I wish also to compute the potential energy of .gro files in general,
 not necessarily obtained from a simulation.
 For that, I prepared a .mdp file for a degenerate energy
 minimization, having 0 steps, designed just to give the status of the
 file:
 
 Zero-step EM does not calculate the initial energy because it is not
 useful for gradient-based energy minimization.
 I don't recall the details, but perhaps the first EM step is reported
 as step zero.
 Instead, you should use zero-step MD (with unconstrained_start = yes),
 or (for multiple single points) mdrun -rerun.
 
 You will not necessarily reproduce the g_energy energies with
 anything, because the energy is dependent on the state of the neighbour
 lists.
 If nstenergy is a multiple of nstlist, then those energies should be
 fairly reproducible.
 
 I have updated the grompp source to provide a note to the user to warn
 against zero-step EM.
 
 Mark
 
 ;;; status.mdp ;;;
 integrator   = l-bfgs
 nsteps   = 0
 implicit_solvent = GBSA
 gb_algorithm = Still
 sa_algorithm = Ace-approximation
 pbc  = no
 rgbradii = 0
 ns_type  = simple
 nstlist  = 0
 rlist= 0
 coulombtype  = cut-off
 rcoulomb = 0
 vdwtype  = cut-off
 rvdw = 0
 nstcalcenergy= 1
 nstenergy= 1
 emtol= 0
 ;;;
 
 The only changes from the former .mdp file are in nsteps and
 nstenergy.
 
 However, when I run this potential 

Re: [gmx-users] question about GBSA and opls-aa

2011-02-28 Thread Per Larsson
Hi!

The treatment of 1-2, 1-3 and 1-4 interactions with gbsa differ between the 
different born radii models, but not between force fields.

For the Still model, polarisation energies are computed once for 1-2, 1-3 and 
1-4 interactions, and never updated for these. For the HCT/OBC models, all 
interactions are included in the calculation of the born radii, and 
subsequently the polarisation energy, in every step. This is one of the reasons 
the Still model is faster, there are fewer calculations done per step.

There is thus no special scaling for these interactions in any force field when 
computing the polarisation energy. They all contribute.

For more details, please also read the original Still/HCT/OBC-papers.

Regards
/Per

28 feb 2011 kl. 16:51 skrev Baoqiang Cao bqcaom...@gmail.com:

 Hi,
 
 I'm using GBSA with opls-aa force field and have some questions that I
 couldn't find answers, I'd definitely be grateful if could get answer
 of tips. How does GBSA treat 1-2(covalent bonded), 1-3(bonded angle),
 1-4(improper torsion) interactions? Should they all contribute nothing
 to GBSA energy or except 1-4?  Thanks in advance!
 
 Baoqiang
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Re: [gmx-users] Target implementation date for gb_saltconc?

2011-02-21 Thread Per Larsson


Skickat från min iPhone

18 feb 2011 kl. 21:10 skrev Matthew Zwier mczw...@gmail.com:

 Dear GROMACS developers and users,
 
 Our research group is interested in performing GBSA simulations with
 GROMACS, but we would need to perform them with a nonzero salt
 concentration.  I was wondering if there are plans to implement the
 gb_saltconc parameter, and if so, when it might become available.
 
 Many thanks,
 Matt Zwier
 University of Pittsburgh
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Re: [gmx-users] OPLS implicit solvent problems

2011-01-21 Thread Per Larsson
Hi!

Thanks for pointing this out.
It is unfortunate that they are missing from the gbsa.itp-file. I will add 
them, but I do not have time today.
If you want to get going, you can add them yourself. 
The gb-parameters are essentially based on atom hybridization, so for each 
missing atom you find another that has the same (sp, sp2,sp3) hybridization, 
and add it to the gbsa.itp-file.

Cheers
/Per

21 jan 2011 kl. 13.51 skrev francesca.stanzi...@unina.it:

 Hello,
 
 I try to perform an implicit solvent simulation with Gromacs 4.5.3. version. 
 I have a system corresponding to 6 peptides generated by Pymol with 
 simmetrical cell, so I have a single PDB. I used OPLS-AA and i put the N-and 
 C- termini as NH2 and COOH. My topology file is correct, and is all systems 
 are included.
 
 ; Include forcefield parameters
 #include ./oplsaa.ff/forcefield.itp --- in this .itp file is included 
 gbsa.itp
 
 ; Include chain topologies
 #include topol_Protein_chain_A.itp
 #include topol_Protein_chain_B.itp
 #include topol_Protein_chain_C.itp
 #include topol_Protein_chain_D.itp
 #include topol_Protein_chain_E.itp
 #include topol_Protein_chain_F.itp
 
 ; Include water topology
 #include ./oplsaa.ff/tip3p.itp
 
 #ifdef POSRES_WATER
 ; Position restraint for each water oxygen
 [ position_restraints ]
 ;  i funct   fcxfcyfcz
11   1000   1000   1000
 #endif
  
 ; Include topology for ions
 #include ./oplsaa.ff/ions.itp
 
 [ system ]
 ; Name
 Protein
 
 [ molecules ]
 ; Compound#mols
 Protein_chain_A 1
 Protein_chain_B 1
 Protein_chain_C 1
 Protein_chain_D 1
 Protein_chain_E 1
 Protein_chain_F 1
 -
 
 When I start my simulations (md_start.mdp) in implicit solvent, i have this 
 fatal error:
 
 GB parameter(s) missing or negative for atom type 'opls_912B'
 
 GB parameter(s) missing or negative for atom type 'opls_267'
 
 GB parameter(s) missing or negative for atom type 'opls_269'
 
 GB parameter(s) missing or negative for atom type 'opls_268'
 
 GB parameter(s) missing or negative for atom type 'opls_270'
 
 Program grompp, VERSION 4.5.3
 Source code file: grompp.c, line: 1123
 
 Fatal error:
 Can't do GB electrostatics; the implicit_genborn_params section of the 
 forcefield is missing parameters for 5 atomtypes or they might be negative.
 For more information and tips for troubleshooting, please check the GROMACS
 website at http://www.gromacs.org/Documentation/Errors.
 
 
 
 Controlling these atoms they corresponding to:
 
 opls_912B= the  CA of N-terminal residue
 
 opls_267= Co in COOH
 
 opls_268= Oh in COOH
 
 opls_269= Oc in COOH neutral
 
 opls_270= H in COOH
 
 
 
 in the file gbsa.itp in opls.ff directory these atoms missing. Now, have I 
 done something wrong? If is all ok, is it possible to create these missing 
 atoms in the gbsa.itp file?
 
 thanx,
 
 francesca stanzione
 
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Re: [gmx-users] van der Walls radius and implicit solvation

2011-01-11 Thread Per Larsson
Hi!

Currently there is no support in Gromacs for implicit solvation using a 
united-atom force field.
It is definitely possible though, but you need to consult the literature for 
values for the radii. 
For united-atoms, I guess the hydrogens you mention are the polar hydrogens?

All radii in the current implementation are taken from the literature, in many 
cases though using Tinker as the primary source.

Cheers
/Per

11 jan 2011 kl. 19.19 skrev Diogo Vila Viçosa:

 Hi,
 
 I have two questions regarding the generalized born models implemented in 
 GROMACS.
 
 1) Is it possible to perform an MD run using implicit solvent with an 
 united-atom force field? If so, how are determined the van der Walls radii 
 for H atoms?
 
 2) How are determined the other van der walls radii used in GROMACS?
 
 
 Thanks in advance
 
 Diogo Vila Viçosa
 
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Re: [gmx-users] Re: gb_saltconc in implicit water simulations

2010-12-22 Thread Per Larsson
Hi!

Which results can you not recreate?

Yes - all simulations were run at zero salt concentration. 
Implicitly this means that we did not do anything special to treat the charges. 
The protein has an overall charge of -2, looking at the topology.
In hindsight, we probably should have given this issue more thought, but for 
assessing the correctness of the CHARMM implementation (the parameters) it 
seemed not so important, I'm afraid.

For the sa_algorithm option, this seems weird. If I try to set sa_algorithm = 
Still, I get an error as it is not yet implemented. The only viable options are 
etiher None or Ace-approximation. If you want to mail me your input-files 
off-list, I will have a look after Christmas.

Cheers
/Per


22 dec 2010 kl. 03.23 skrev Rogan Carr:

 Hi Per (and all),
 
 I am trying to recreate the results of the CHARMM forcefield implementation 
 to better understand how to implement implicit solvent models, but I can't 
 quite recreate your results.  If the Gromacs code doesn't use salt 
 concentrations, does that mean that your simulations were run at zero salt 
 concentration?  Also, how did you deal with the charged residues on the 
 protein?
 
 Also, sort of on the same topic, no matter what option I choose for 
 sa_algorithm with Gromacs 4.5.3, it always uses sa_algorithm=Still.
 
 Thanks for your help,
 Rogan
 
 
 On Dec 14, 2010, at 12:13 PM, Per Larsson wrote:
 
 Hi!
 
 Sorry that I missed this discussion, we recently moved the lab and there 
 where quite many things to attend to.
 
 When we did the implementation of implicit solvent into Gromacs, one of the 
 strong points was to see how fast we could make it, to speed up 
 conformational sampling as much as possible. Adding in the extra 
 Debye-Huckel term for a non-zero salt-concentration was not a priority at 
 the time. It might be a bit unfortunate that the option anyway exists in the 
 mdp-file.
 I will try and see if I can find the time to put it in, but that will not 
 happen in the next coming weeks although I agree that it would be very 
 useful to have :-)
 
 When it comes to the use of explicit ions in an implicit solvent, I hate to 
 say that I'm not much of an expert, really. Having said that, and someone 
 else is very welcome to correct me on this point, there does not seem to 
 exist a wide body of literature about this. In addition to the paper that 
 Justin pointed to, there is some work done by Michael Feig (eg. 
 http://www.ncbi.nlm.nih.gov/pubmed/16928023).
 Also I think that particularly with DNA there are problems with the theory 
 itself as it does not handle high salt-concentrations very well.
 
 Cheers
 /Per
 
 
 
 14 dec 2010 kl. 20.22 skrev devicerandom:
 
 On 14/12/10 19:04, Justin A. Lemkul wrote:
 I was going to send a very similar mail -namely, I have a coarse-grain
 system in vacuum where I'd like to simulate a charged polymer. My idea
 was that of adding a single ghost counter-ion with zero VdW
 interactions, perhaps keeping it fixed in one corner of the box, but
 I'd like to know how meaningful it is.
 
 
 In vacuum and implicit solvent are very different concepts. If you
 are indeed simulating in a vacuum, I would be willing to bet that your
 charged polymer will rapidly associate with your dummy ion simply due to
 attractive Coulombic interactions that are not screened by any
 intervening solvent.
 
 Heh, I know very well that -and that is one of the reasons I wanted to know 
 how does one cope with that.
 
 I mean, if it's a single polymer, perhaps one can naively position restrain 
 the ion in a corner of the box, away from the polymer, while the polymer 
 stays on its center of mass. But if I want multiple objects in my box, I 
 guess it's not going to work.
 
 I'd like very much to use implicit solvent as well but I have to see how 
 deep is the performance impact on my model -after all, one does coarse 
 grain to be raw but *fast* :)
 
 
 In regards to the original post, I have seen this question asked and
 ignored several times already, unfortunately. Most of the literature I
 have read (which primarily uses CHARMM) does not specify how counterions
 are handled, if at all. Maybe there is some intrinsic compensating
 factor in CHARMM that I simply don't know about. I found this:
 
 http://dx.doi.org/10.1002/jcc.20874
 
 But again, it uses CHARMM and fancy modified electrostatic models.
 
 I would really hope that someone who knows about the proper GROMACS
 methodology would comment. This has been a curiosity of mine for some
 time, as well. I have not had a pressing need to try out the implicit
 solvent features, but in the absence of being sure of the methodology, I
 am unlikely to do so.
 
 Perhaps the developers of the implicit solvent know about that? I hope so...
 
 m.
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Re: [gmx-users] Re: gb_saltconc in implicit water simulations

2010-12-14 Thread Per Larsson
Hi!

Sorry that I missed this discussion, we recently moved the lab and there where 
quite many things to attend to.

When we did the implementation of implicit solvent into Gromacs, one of the 
strong points was to see how fast we could make it, to speed up conformational 
sampling as much as possible. Adding in the extra Debye-Huckel term for a 
non-zero salt-concentration was not a priority at the time. It might be a bit 
unfortunate that the option anyway exists in the mdp-file. 
I will try and see if I can find the time to put it in, but that will not 
happen in the next coming weeks although I agree that it would be very useful 
to have :-)

When it comes to the use of explicit ions in an implicit solvent, I hate to say 
that I'm not much of an expert, really. Having said that, and someone else is 
very welcome to correct me on this point, there does not seem to exist a wide 
body of literature about this. In addition to the paper that Justin pointed to, 
there is some work done by Michael Feig (eg. 
http://www.ncbi.nlm.nih.gov/pubmed/16928023). 
Also I think that particularly with DNA there are problems with the theory 
itself as it does not handle high salt-concentrations very well.

Cheers
/Per



14 dec 2010 kl. 20.22 skrev devicerandom:

 On 14/12/10 19:04, Justin A. Lemkul wrote:
 I was going to send a very similar mail -namely, I have a coarse-grain
 system in vacuum where I'd like to simulate a charged polymer. My idea
 was that of adding a single ghost counter-ion with zero VdW
 interactions, perhaps keeping it fixed in one corner of the box, but
 I'd like to know how meaningful it is.
 
 
 In vacuum and implicit solvent are very different concepts. If you
 are indeed simulating in a vacuum, I would be willing to bet that your
 charged polymer will rapidly associate with your dummy ion simply due to
 attractive Coulombic interactions that are not screened by any
 intervening solvent.
 
 Heh, I know very well that -and that is one of the reasons I wanted to know 
 how does one cope with that.
 
 I mean, if it's a single polymer, perhaps one can naively position restrain 
 the ion in a corner of the box, away from the polymer, while the polymer 
 stays on its center of mass. But if I want multiple objects in my box, I 
 guess it's not going to work.
 
 I'd like very much to use implicit solvent as well but I have to see how deep 
 is the performance impact on my model -after all, one does coarse grain to be 
 raw but *fast* :)
 
 
 In regards to the original post, I have seen this question asked and
 ignored several times already, unfortunately. Most of the literature I
 have read (which primarily uses CHARMM) does not specify how counterions
 are handled, if at all. Maybe there is some intrinsic compensating
 factor in CHARMM that I simply don't know about. I found this:
 
 http://dx.doi.org/10.1002/jcc.20874
 
 But again, it uses CHARMM and fancy modified electrostatic models.
 
 I would really hope that someone who knows about the proper GROMACS
 methodology would comment. This has been a curiosity of mine for some
 time, as well. I have not had a pressing need to try out the implicit
 solvent features, but in the absence of being sure of the methodology, I
 am unlikely to do so.
 
 Perhaps the developers of the implicit solvent know about that? I hope so...
 
 m.
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Re: [gmx-users] Thermostat for REMD simulations in implicit solvent

2010-11-26 Thread Per Larsson
Hi!

Have never tried remd with implicit solvent, but note that the unit of tau-t in 
the mdp-file is ps, not ps-1. This means you should set tau-t = 0.0109 rather 
than 91.

Try this and see if the problem goes away!

/Per

26 nov 2010 kl. 15:55 skrev César Ávila clav...@gmail.com:

 Dear all, 
 I am trying to set up a REMD simulation for a peptide (CHARMM ff) in implicit 
 solvent (OBC GB). 
 Following Bjelkmar et al* I am using stochastics dynamics integration with an 
 inverse friction constant of 91 ps-1, 5 fs timestep, 
 virtual-sites for hydrogens, all-vs-all nonbonded (no cutoff).  The full .mdp 
 file is attached at the end of this mail. The problem I am 
 facing is that after a while, the temperatures of all replicas start dropping 
 even below the lowest target temperature. 
 Would you suggest changing some parameter or the whole thermostat to prevent 
 this from happening?
 
 @ s0 legend Temperature
 0.00  310.811523
 5.00  435.627045
10.00  417.161713
15.00  414.248901
20.00  399.390686
25.00  375.087219
30.00  338.131256
35.00  339.961151
40.00  319.424561
45.00  290.442322
50.00  289.587921
55.00  248.746246
60.00  253.192047
65.00  242.619476
70.00  256.051941
75.00  237.648468
80.00  231.938690
85.00  217.029953
90.00  211.447983
95.00  210.393890
   100.00  208.518417
   105.00  196.718445
   110.00  219.245682
   115.00  202.957993
   120.00  193.128159
   125.00  198.278198
   130.00  175.304108
   135.00  164.925613
   140.00  195.024490
   145.00  201.153046
   150.00  211.160797
   155.00  189.525085
   160.00  191.156006
   165.00  186.545242
   170.00  186.885422
   175.00  182.838486
   180.00  174.960098
   185.00  175.244049
   190.00  179.517975
   195.00  165.785416
   200.00  189.871048
   205.00  179.510178
   210.00  152.527710
   215.00  160.109955
   220.00  163.564148
 
 
 
 
 
 
 
 
 
 * Implementation of the CHARMM ff in GROMACS (2010) JCTC, 6, 459-466
 
 
 ; Run parameters
 integrator  =  sd
 dt  =  0.005; ps ! 
 nsteps  =  2
 nstcomm = 1
 comm_mode   = angular   ; non-periodic system
 
 ; Bond parameters
 constraints = all-bonds
 constraint_algorithm= lincs
 lincs-iter  = 1
 lincs-order = 6
 
 ; required cutoffs for implicit
 nstlist =  0  
 ns_type =  grid
 rlist   =  0 
 rcoulomb=  0 
 rvdw=  0 
 epsilon_rf  =  0
 rgbradii=  0
 
 ; cutoffs required for qq and vdw
 coulombtype =  cut-off
 vdwtype =  cut-off
 
 ; temperature coupling
 tcoupl  = v-rescale
 tc-grps = system
 tau-t   = 91
 ref-t   = 300
 
 ; Pressure coupling is off
 Pcoupl  = no
 
 ; Periodic boundary conditions are off for implicit
 pbc = no
 
 ; Settings for implicit solvent
 implicit_solvent= GBSA
 gb_algorithm= OBC
 gb_epsilon_solvent  = 78.3
 sa_surface_tension  = 2.25936
 
 ;Output control
 nstxout = 1000
 nstfout = 0
 nstvout = 0
 nstxtcout   = 0
 nstlog  = 1000
 nstcalcenergy   = -1
 nstenergy   = 1000
 
 ; GENERATE VELOCITIES FOR STARTUP RUN
 gen_vel = yes
 gen_temp = 300
 gen_seed = 1993
 
 
 
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Re: [gmx-users] Using Charmm FF with implicit solvent on gromacs

2010-11-19 Thread Per Larsson
Hi!

Currently it is not possible to use GBSW in Gromacs.
As you noted, there are three GB-models available (Still,HCT,OBC),
that can be run using plain cutoffs (or no cutoffs at all, using the optimized 
all-vs-all kernels).

Currently there is unfortunately no work being done to extend the range of 
implicit solvent models available.
However, we have had some promising results with the combination of CHARMM FF + 
CMAP + OBC, as discussed in the 2010 JCTC paper.

Cheers
/Per


18 nov 2010 kl. 22.49 skrev César Ávila:

 Dear all, 
 I would like to know if anyone has experience on running simulations using 
 the Charmm FF and implicit solvent model on gromacs. I have found that 
 gromacs has three implementations for GB models
 Still
 Hawkins-Cramer-Truhlar (HCT)
 Onufriev-Bashford-Case (OBC)
 The charmm FF has been extensively tested with the GBSW* implementation (in 
 Charmm program) for which the backbone phi/psi cross-term (CMAP) and the 
 atomic input radii were specifically optimized (Chan, Im and Brooks, JACS, 
 2006). 
 
 Is there a way to perform the same calculation on gromacs?
 
 * W. Im, M.S. Lee, and C.L. Brooks III  Generalized Born Model with a Simple 
 Smoothing Function. J. Comput. Chem. 24:1691-1702 (2003). 
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Re: [gmx-users] Role of epsilon_rf in implicit solvation

2010-11-19 Thread Per Larsson
Hi!

It would be nice to have reaction-field for GB as well, but currently this is 
not the case.
The polarisation energy is scaled using (1.0/epsilon_r - 
1.0/gb_epsilon_solvent) always, epsilon_rf is never used.

Cheers
/Per



19 nov 2010 kl. 12.30 skrev Christian Mücksch:

 So is this epsilon_rf also used in combination in implicit solvent models 
 regarding the dielectric constant beyond cut-off? If yes, what would be an 
 appropriate value for this constant?

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Re: [gmx-users] Re: GB-polarization

2010-11-10 Thread Per Larsson
Hi!

Sorry for the confusion here. Justin is right. In versions before 4.5.2, the 
non-polar solvation calculation was done regardless of the sa_algorithm setting.
In 4.5.2, this has to be specified explicitly using the setting 
Ace-approximation, to get the complete solvation free energy.

Also, the value of sa_surface_tension was set automatically in versions up to 
4.5.1. In 4.5.2, this is also the case as long as it is set to -1 in the 
mdp-file. Setting it to 0 means no non-polar calculation is done, and setting 
it to something else (but non-zero) will override the default values (eg. those 
that were always used in 4.5.1)

Again, sorry for the confusion. 

I will update the manual to make this more clear.

/Per


Skickat från min iPhone

9 nov 2010 kl. 23:53 skrev Justin A. Lemkul jalem...@vt.edu:

 
 
 Christian Mücksch wrote:
 But in order to get the complete solvation free energy these calculations 
 for the van der Waals and cavity terms have to be done.
 So does that mean that the solvation free energy calculated by default 
 without specifying sa_algorithm=Ace-approximation is missing these terms?
 I thought that the ACE-type approximation is done by default (due to the 
 manual) when using GBSA.
 
 I think it all depends on the version you're using.  Ace-approximation became 
 default in version 4.5.2 (I think).  In previous versions, no was the 
 default, at least such was the case in my testing of 4.5.1.
 
 -Justin
 
 Kind regards,
 Christian
 Christian Mücksch wrote:
   Thanks for the clarification but I can't find anything in the .log or
   .edr-files that would correspond to the non-polar solvation energy.
   
 I think you have to set sa_algorithm=Ace-approximation for this 
 calculation to
 be done, and thus written.
 -Justin
   Christian Mücksch
   Department of Physics
   TU Kaiserslautern
   Erwin Schrödinger Straße
   67663 Kaiserslautern
   Germany
 Phone: +49 (0)631 205 4287
   Fax:   +49 (0)631 205 4965
   Email:mueck...@rhrk.uni-kl.de
  
   Hi! Yes, the GB-polarization energy corresponds to the solvent-solute
   electrostatics polarization energy. The non-polar part of the
   solvation energy (the solvent-solvent cavity term and the
   solute-solvent vdw-term) are named Non. polar solvation (or something
   like that) in the log-file. /Per 4 nov 2010 kl. 11.10 skrev Christian
   Mücksch:
   Dear all,
  I've got a general question regarding implicit solvent
   simulations.
   Using g_energy there's an option to print out the 
  GB-polarization.
   Is that the solvent-solute electrostatics polarization free energy?
  How can one interpret a rise or decrease in the 
  GB-polarization?
  Kind regards,
 --  Justin A. Lemkul Ph.D. Candidate 
 ICTAS Doctoral Scholar MILES-IGERT Trainee Department of Biochemistry 
 Virginia Tech Blacksburg, VA jalemkul[at]vt.edu | (540) 231-9080 
 http://www.bevanlab.biochem.vt.edu/Pages/Personal/justin 
 
 
 -- 
 
 
 Justin A. Lemkul
 Ph.D. Candidate
 ICTAS Doctoral Scholar
 MILES-IGERT Trainee
 Department of Biochemistry
 Virginia Tech
 Blacksburg, VA
 jalemkul[at]vt.edu | (540) 231-9080
 http://www.bevanlab.biochem.vt.edu/Pages/Personal/justin
 
 
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Re: [gmx-users] GB-polarization

2010-11-04 Thread Per Larsson
Hi!

Yes, the GB-polarization energy corresponds to the solvent-solute 
electrostatics polarization energy.
The non-polar part of the solvation energy (the solvent-solvent cavity term and 
the solute-solvent vdw-term) are named Non. polar solvation (or something like 
that) in the log-file.

/Per
 
4 nov 2010 kl. 11.10 skrev Christian Mücksch:

 Dear all,
 
 I've got a general question regarding implicit solvent simulations.
 Using g_energy there's an option to print out the GB-polarization. Is that 
 the solvent-solute electrostatics polarization free energy?
 
 How can one interpret a rise or decrease in the GB-polarization?
 
 Kind regards,
 
 -- 
 Christian Mücksch
 Department of Physics
 TU Kaiserslautern
 Erwin Schrödinger Straße
 67663 Kaiserslautern
 Germany
 
 Phone: +49 (0)631 205 4287
 Email: mueck...@rhrk.uni-kl.de
 
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Re: [gmx-users] about sa_surface_tension

2010-10-18 Thread Per Larsson
Hi!

This is unfortunately a bit confusing, but prior to the release of 4.5.2 
gromacs did not use the value of
the sa_surface_tension that was specified in the mdp-file. It was always set to 
2.092, and then hardcode to take a certain
value (other than 2.092) depending on the GB-model. 

2.25936 is the value used together with OBC/HCT models, it is slightly lower 
with the Still model. 
In 4.5.2 the default will be -1, which, if left unchanged, will be changed to 
proper values (and a note written about this).
The effect on the result will be very small, since the 
sa_surface_tension-parameter is only used for the non-polar part
of solvation, which in turn is a very minor part of the total force. 

Also in 4.5.2, setting sa_surface_tension=0 means that no non-polar solvation 
is being calculated. 

Sorry for the confusion
/Per

18 okt 2010 kl. 14.07 skrev Christian Mücksch:

 Dear all,
 
 when using implicit solvent models, the sa_surface_tension parameter is set 
 to 2.092 kJ/mol/nm2 by default.
 
 However in Gromacs benchmarks with dihydrofolate reductase this parameter is 
 set to 2.25936.
 
 Can someone please explain this parameter and in how far this would change 
 the simulation outcome.
 
 Kind regards,
 
 -- 
 Christian Mücksch
 Department of Physics
 TU Kaiserslautern
 Erwin Schrödinger Straße
 67663 Kaiserslautern
 Germany
 
 Phone: +49 (0)631 205 4287
 Email: mueck...@rhrk.uni-kl.de
 
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Re: [gmx-users] best parameters for energy determination with GBSA

2010-10-07 Thread Per Larsson
Hi Ehud!

Your settings are correct.
However, you can also use domain decomposition with GB,
and I at least usually bypass the editconf stage, and do 
pdb2gmx-grompp-mdrun, when you do not want any pbc.

/Per



7 okt 2010 kl. 12.29 skrev Ehud Schreiber:

 Dear GROMACS users,
  
 I try to compute energies of a small peptide-domain complex and of its 
 constituents using implicit solvent, so that I can get the binding Delta E. I 
 need the accuracy to be high enough so that I can reliably measure the Delta 
 Delta E between the wildtype peptide and a mutation of it.
  
 I would like to get advice as to the best setting and parameters to use; are 
 the ones given below the correct and best ones (most in an mdp file, some run 
 control parameters of GROMACS commands)? Are other defaults in need to be 
 changed?
  
 As the GBSA method necessitates using the inexact cut-off interactions, and 
 my system is rather small, I consider using no cut-off at all, i.e. an 
 all-vs.-all approach. For that I understand the parameters should be
 nstlist=0
 ns_type=simple
 -pd ; in mdrun
 coulombtype=cut-off
 rcoulomb=0
 vdwtype=cut-off
 rvdw=0
 rlist=0
  
 Then, there are the implicit solvent parameters themselves:
 implicit_solvent=GBSA
 gb_algorithm= Still
 sa_algorithm=Ace-approximation
 rgbradii=0
  
 Finally, regarding the simulation box, I see no need for periodic boundary 
 conditions, and I pick some big margin around the system (as there are no 
 water molecules, no need to spare):
 pbc=no
 -d 5.0 ; in editconf
  
 What do you say?
  
 Thanks,
 Ehud.
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Re: [gmx-users] potential energy in implicit solvent simulations

2010-09-17 Thread Per Larsson
Hi

It seems that the non-polar energy term has gone missing, and does not get 
included in the print-out. 

While adding it back again properly  I found some other issues that I need to 
check before committing. The total potential energy should be correct. 

/Per

16 sep 2010 kl. 17:47 skrev Ehud Schreiber schr...@compugen.co.il:

 Can you explain this situation?
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Re: [gmx-users] About implicit water simulations

2010-09-09 Thread Per Larsson
Hi!

This is not something that is planned for the immediate future, as useful as it 
might be. 

However, for small to medium sized systems one can get good performance by 
using the all-vs-all kernels. Then the problem of poor energy conservation 
disappears. 

Cheers
/Per

Skickat från min iPhone

9 sep 2010 kl. 15:54 skrev Christian Mücksch mueck...@rhrk.uni-kl.de:

 Dear users,
 
 I got a question concerning simulations with implicit solvent. So far it is 
 only possible to use this model when applying a cut-off for the long range 
 electrostatic and vdW interactions which leads to bad energy conservation etc.
 
 Will there be an update allowing to use reaction-field for instance or 
 user-defined potentials with implicit solvent models?
 
 Best regards,
 Christian Mücksch
 
 -- 
 Christian Mücksch  Phone: +49 (0)631 205 4287
 Department of Physics  Fax:   +49 (0)631 205 4965
 TU Kaiserslautern  Email: mueck...@rhrk.uni-kl.de
 Erwin Schrödinger Straße
 67663 Kaiserslautern
 Germany
 
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Re: [gmx-users] Generalized Born segfaults with v4.5.1

2010-09-07 Thread Per Larsson
Hi!

I am currently working on another issue with the GB-double precision loops. 
I'll include this as well. 
But your pdb-file only contains 1 residue with the name UNK (by openBabel).
Could you please send me another pdb-file that reproduces this error off-list, 
and I'll get to it.

Cheers
/Per


7 sep 2010 kl. 09.59 skrev Silvio a Beccara:

 Dear friends,
 
 when trying to run a double precision vanilla MD, version 4.5.1, with a small 
 hairpin molecule (248 atoms) in implicit solvent (generalized Born 
 approximation) this is what I get:
 
 -
 Getting Loaded...
 Reading file hairpin-md-gb-1.tpr, VERSION 4.5.1 (double precision)
 Loaded with Money
 
 starting mdrun 'Protein'
 5 steps, 50.0 ps.
 Segmentation fault
 -
 
 In some trials, I also get a message about the distance in an 1-4 interaction 
 being beyond the table size, but this is not the case.
 
 Strangely enough, the MD runs fine with a development version (4.0.99, 
 downloaded from the GIT repository).
 
 I am attaching my mdp and pdb files.
 
 
 Regards
 
 
 Silvio a Beccara
 
 
 Dip. di Fisica - Universita` di Trento
 14 Via Sommarive
 38123 Povo - TN
 tel: 0461-881631
 md-gb.mdpratch-frame63.pdb-- 
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Re: [gmx-users] grompp_d and mdrun_d issues with GBSA and normal mode analysis

2010-09-07 Thread Per Larsson
This has been fixed with Berk's commit c06ee471...
The error was not related to GB, but rather a combination of domain 
decomp.+nm+cut-offs.

Cheers
/Per


6 sep 2010 kl. 11.38 skrev Ehud Schreiber:

 Dear GROMACS users,
  
 I am encountering a couple of issues when trying to perform normal mode 
 analysis in an implicit solvent (GBSA) setting.
 I am using version 4.5.1 with double precision; unfortunately I do not have 
 the single precision version installed for comparison.
  
 The starting point is a small protein which was energy minimized in two 
 stages, also in double precision and with GBSA, producing “em2” files. The 
 mdp file used for the normal mode analysis is the following:
  
 - nm.mdp -
 integrator   = nm
 nsteps   = 1
 implicit_solvent = GBSA
 gb_algorithm = Still ; the default
 rgbradii = 1.0 ; must be equal to rlist
 rlist= 1.0
 coulombtype  = cut-off
 rcoulomb = 1.0
 vdwtype  = cut-off
 rvdw = 1.0
 ---  
  
 The command used is
  
 grompp_d -f nm.mdp -p topol.top -c em2.gro -t em2.trr -o nm.tpr
  
 which ran fine except for the following note:
  
 NOTE 1 [file nm.mdp]:
   You are using a plain Coulomb cut-off, which might produce artifacts.
   You might want to consider using PME electrostatics.
  
 Then, I tried to run
  
 mdrun_d -v -nice 0 -deffnm nm
  
 However, the command seems to be stuck, and the following serious warning is 
 produced:
  
 Warning: 1-4 interaction between 64 and 71 at distance 3.114 which is larger 
 than the 1-4 table size 2.000 nm
 These are ignored for the rest of the simulation
 This usually means your system is exploding,
 if not, you should increase table-extension in your mdp file
 or with user tables increase the table size
 Maximum force: 3.48709e+06
 Maximum force probably not small enough to ensure that you are in an
 energy well. Be aware that negative eigenvalues may occur when the
 resulting matrix is diagonalized.
  
 The em2.gro is definitely not having such a large distance between atoms 64 
 and 71:
  
 6GLN CB   64   1.879   1.895   2.423
 .
 .
 6GLNOE1   71   2.047   1.715   2.642
  
 which are only about 0.346 nm apart. Also, the energy minimization, which 
 used the same options, mutatis mutandis,
  
 -- em2.mdp --
 integrator   = cg
 nsteps   = 1000
 nstcgsteep   = 40
 implicit_solvent = GBSA
 gb_algorithm = Still ; the default
 rgbradii = 1.0 ; must be equal to rlist
 nstlist  = 10
 rlist= 1.0
 coulombtype  = cut-off
 rcoulomb = 1.0
 vdwtype  = cut-off
 rvdw = 1.0
 nstenergy= 10
 -
  
 converged to machine precision having a much smaller maximum force:
  
 Stepsize too small, or no change in energy.
 Converged to machine precision,
 but not to the requested precision Fmax  10
  
 Polak-Ribiere Conjugate Gradients converged to machine precision in 0 steps,
 but did not reach the requested Fmax  10.
 Potential Energy  = -2.71868395521758e+04
 Maximum force =  4.63436548427712e+02 on atom 584
 Norm of force =  1.25296847735530e+02
  
 The other problem arises when I try to follow the grompp_d note above and 
 change in nm.mdp to
  
 coulombtype  = pme
  
 I then have a fatal error:
  
 ERROR 1 [file nm.mdp]:
   With GBSA, coulombtype must be equal to Cut-off
  
 Am I doing something wrong or are there still some problems in the new GBSA 
 option of version 4.5.1?
  
 Thanks,
 Ehud Schreiber.
   
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Re: [gmx-users] grompp_d and mdrun_d issues with GBSA and normal mode analysis

2010-09-06 Thread Per Larsson
Hi!

This should work. I checked the code but did not find anything obvious.
Could you please file a bugzilla and I'll have a look as soon as possible.

Thanks!
/Per

6 sep 2010 kl. 11.38 skrev Ehud Schreiber:

 Dear GROMACS users,
  
 I am encountering a couple of issues when trying to perform normal mode 
 analysis in an implicit solvent (GBSA) setting.
 I am using version 4.5.1 with double precision; unfortunately I do not have 
 the single precision version installed for comparison.
  
 The starting point is a small protein which was energy minimized in two 
 stages, also in double precision and with GBSA, producing “em2” files. The 
 mdp file used for the normal mode analysis is the following:
  
 - nm.mdp -
 integrator   = nm
 nsteps   = 1
 implicit_solvent = GBSA
 gb_algorithm = Still ; the default
 rgbradii = 1.0 ; must be equal to rlist
 rlist= 1.0
 coulombtype  = cut-off
 rcoulomb = 1.0
 vdwtype  = cut-off
 rvdw = 1.0
 ---  
  
 The command used is
  
 grompp_d -f nm.mdp -p topol.top -c em2.gro -t em2.trr -o nm.tpr
  
 which ran fine except for the following note:
  
 NOTE 1 [file nm.mdp]:
   You are using a plain Coulomb cut-off, which might produce artifacts.
   You might want to consider using PME electrostatics.
  
 Then, I tried to run
  
 mdrun_d -v -nice 0 -deffnm nm
  
 However, the command seems to be stuck, and the following serious warning is 
 produced:
  
 Warning: 1-4 interaction between 64 and 71 at distance 3.114 which is larger 
 than the 1-4 table size 2.000 nm
 These are ignored for the rest of the simulation
 This usually means your system is exploding,
 if not, you should increase table-extension in your mdp file
 or with user tables increase the table size
 Maximum force: 3.48709e+06
 Maximum force probably not small enough to ensure that you are in an
 energy well. Be aware that negative eigenvalues may occur when the
 resulting matrix is diagonalized.
  
 The em2.gro is definitely not having such a large distance between atoms 64 
 and 71:
  
 6GLN CB   64   1.879   1.895   2.423
 .
 .
 6GLNOE1   71   2.047   1.715   2.642
  
 which are only about 0.346 nm apart. Also, the energy minimization, which 
 used the same options, mutatis mutandis,
  
 -- em2.mdp --
 integrator   = cg
 nsteps   = 1000
 nstcgsteep   = 40
 implicit_solvent = GBSA
 gb_algorithm = Still ; the default
 rgbradii = 1.0 ; must be equal to rlist
 nstlist  = 10
 rlist= 1.0
 coulombtype  = cut-off
 rcoulomb = 1.0
 vdwtype  = cut-off
 rvdw = 1.0
 nstenergy= 10
 -
  
 converged to machine precision having a much smaller maximum force:
  
 Stepsize too small, or no change in energy.
 Converged to machine precision,
 but not to the requested precision Fmax  10
  
 Polak-Ribiere Conjugate Gradients converged to machine precision in 0 steps,
 but did not reach the requested Fmax  10.
 Potential Energy  = -2.71868395521758e+04
 Maximum force =  4.63436548427712e+02 on atom 584
 Norm of force =  1.25296847735530e+02
  
 The other problem arises when I try to follow the grompp_d note above and 
 change in nm.mdp to
  
 coulombtype  = pme
  
 I then have a fatal error:
  
 ERROR 1 [file nm.mdp]:
   With GBSA, coulombtype must be equal to Cut-off
  
 Am I doing something wrong or are there still some problems in the new GBSA 
 option of version 4.5.1?
  
 Thanks,
 Ehud Schreiber.
   
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Re: [gmx-users] ffamber03 H0 atomtype in 4.5.1

2010-09-06 Thread Per Larsson
Hi!

This seems to be an unfortunate mistake. It should not be commented out.
Thank you for reporting this, I will fix it for the next release.

Cheers
/Per

6 sep 2010 kl. 17.08 skrev William Joseph Allen:

 Hello Gromacs users,
 
 I have recently set up some simulations of a peptide using the amber03 force 
 field in 4.5.1 and implicit solvent. When I run it through grompp, it gives 
 me the following:
 
 ---
 Program grompp-4.5.1, VERSION 4.5.1
 Source code file: grompp.c, line: 870
 
 Fatal error:
 Can't do GB electrostatics; the forcefield is missing 1 values for
 atomtype radii, or they might be negative
 .
 For more information and tips for troubleshooting, please check the GROMACS
 website at http://www.gromacs.org/Documentation/Errors
 ---
 
 The missing value it is referring to was also mentioned in the grompp output:
 
 ***
 GB parameter(s) missing or negative for atom type 'H0'
 ***
 
 The 'H0' (read h-zero) atomtype only appears in glycine residues. It is 
 equivalent in all ways to the 'H1' (read h-one) atomtype. But for some 
 reason, in the gbsa.itp file, the 'H0' atomtype is commented out. When it is 
 un-commented, grompp proceeds as normal. My question is why is this specific 
 atomtype commented out in the amber03 gbsa.itp file?
 
 Thanks in advance,
 
 Joe
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Re: [gmx-users] GB Parameters

2010-08-24 Thread Per Larsson
Hi!

You are correct, expect that the values in column 4 (the Vdw-radii for atom 
types) that are being used to calculate the Born radii currently are force 
field and radii-algorithm agnostic (as is indeed the case in Tinker as well).
Obviously, if someone wants to use other Vdw-radii, such as eg. the Bondi, 
these values will need to be changed.

Good luck!
/Per

24 aug 2010 kl. 13.05 skrev Elizabeth Ploetz:

 Greetings!  
 
 Thank you both for such timely and helpful responses.  Below I have listed 
 how I (and anyone interested in using their own force field) should modify 
 the gbsa.itp file, according to my new understanding.  Please let me know if 
 I am wrong.
 
 Columns 1-3:  Leave them alone, they are not used in 4.5beta3
 Column 4: Use the force field's LJ sigma/2 (except for hydrogen: use 
 0.115 regardless of the hydrogen's sigma value)
 Column 5: Leave it as is, because the HCT scaling factors are not force 
 field specific
 
 Prof. van der Spoel, unfortunately our force field does not support nucleic 
 acids either.  Per, I will let you know if I find any errors, however I am 
 new to implicit solvent methods, so I have a lot of learning to do first!  
 
 Best, 
 
 E. A. Ploetz
 
 - Original Message -
 From: gmx-users-requ...@gromacs.org
 To: gmx-users@gromacs.org
 Sent: Tuesday, August 24, 2010 2:51:14 AM
 Subject: gmx-users Digest, Vol 76, Issue 120
 
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 than Re: Contents of gmx-users digest...
 
 
 Today's Topics:
 
   1. Re: GB Parameters (Per Larsson)
   2. Re: Charmm to Gromacs: Polyols force field [Justin] (Bruce D. Ray)
   3. Re: Re: Re: [gmx-users] Charmm to Gromacs: Polyols force
  field [Mark, Justin] (Eudes Fileti)
   4. Re: Does anyone know how to get the file
  charmm_gromacs.tar.gz? (Mark Abraham)
   5. gmx 4.5 and openmm on Mac, still not compiling (Alan)
 
 
 --
 
 Message: 1
 Date: Mon, 23 Aug 2010 20:41:51 +0200
 From: Per Larsson per.lars...@sbc.su.se
 Subject: Re: [gmx-users] GB Parameters
 To: Discussion list for GROMACS users gmx-users@gromacs.org
 Message-ID: 21e19e54-404f-42d2-8ddc-0684c6bb9...@sbc.su.se
 Content-Type: text/plain; charset=us-ascii
 
 Also, again, as David said, if you find any errors in the parameters or in 
 the code, please let me know!
 
 Cheers
 /Per
 
 
 23 aug 2010 kl. 20:09 skrev Per Larsson per.lars...@sbc.su.se:
 
 Hi!
 
 Values in columns 1-3 are not currently used in version beta3. They pertain 
 to more elaborate surface area algorithms, the one from Still et al in 
 particular.
 
 Column 4 is the Vdw-radii for atom types that are used for computing the 
 Born radii. The dielectric offset is specified in the mdp-file, and gets 
 added to the input radii for the different radii methods.
 
 Column 5 is the scale factor for the HCT/OBC models. The values are taken 
 from the original HCT reference, as well as the corresponding implementation 
 in Tinker. 
 
 /Per
 
 23 aug 2010 kl. 19:27 skrev Elizabeth Ploetz plo...@ksu.edu:
 
 Dear Gromacs Users, 
 
 I am interested in implementing implicit solvent using the OBC GBSA method. 
  In the Gromacs 4.5beta3 top directory, several force fields (oplsaa and 
 multiple versions of amber) contain the gbsa.itp file, and one (charmm27), 
 contains a gb.itp file.  They all have the same column titles (sar, st, pi, 
 gbr, and hct).  I have read the six articles listed at 
 http://www.gromacs.org/Documentation/Terminology/Implicit_Solvent, however 
 I still have the following two questions regarding the contents of this 
 file:
 
 (1.)  What values are tabulated in these columns and what are the 
 corresponding references for each of them?
 (2.)  Which columns are used (versus ignored) by Gromacs in the 
 implementation of each of the methods (Still/HCT/OBC)?
 
 Here are my guesses for Question 1:
 (a.)  sar: solvent accessible surface area?
 (b.)  st: surface tension?
 (c.)  pi: ?
 (d.)  gbr: generalized born radius?  These values correspond to sigma/2 
 from Jorgensen and Tirado-Rives' 1988 JACS paper (v. 110, p. 1657).  
 However the generalized born radius is equal to Rvdw plus a dielectric 
 offset distance, according to Still et al's 1997 J. Phys. Chem. A paper (v. 
 101, p. 3005).  This would mean the dielectric offset distance is set to 
 zero (?).  
 (e.)  hct: HCT parameter
 
 With an eventual goal of implementing implicit solvent using my lab's force 
 field, insight into the meaning of the columns and/or references for their 
 origin would be greatly

Re: [gmx-users] GB Parameters

2010-08-23 Thread Per Larsson
Hi!

Values in columns 1-3 are not currently used in version beta3. They pertain to 
more elaborate surface area algorithms, the one from Still et al in particular.

Column 4 is the Vdw-radii for atom types that are used for computing the Born 
radii. The dielectric offset is specified in the mdp-file, and gets added to 
the input radii for the different radii methods.

Column 5 is the scale factor for the HCT/OBC models. The values are taken from 
the original HCT reference, as well as the corresponding implementation in 
Tinker. 

/Per

23 aug 2010 kl. 19:27 skrev Elizabeth Ploetz plo...@ksu.edu:

 Dear Gromacs Users, 
 
 I am interested in implementing implicit solvent using the OBC GBSA method.  
 In the Gromacs 4.5beta3 top directory, several force fields (oplsaa and 
 multiple versions of amber) contain the gbsa.itp file, and one (charmm27), 
 contains a gb.itp file.  They all have the same column titles (sar, st, pi, 
 gbr, and hct).  I have read the six articles listed at 
 http://www.gromacs.org/Documentation/Terminology/Implicit_Solvent, however I 
 still have the following two questions regarding the contents of this file:
 
 (1.)  What values are tabulated in these columns and what are the 
 corresponding references for each of them?
 (2.)  Which columns are used (versus ignored) by Gromacs in the 
 implementation of each of the methods (Still/HCT/OBC)?
 
 Here are my guesses for Question 1:
 (a.)  sar: solvent accessible surface area?
 (b.)  st: surface tension?
 (c.)  pi: ?
 (d.)  gbr: generalized born radius?  These values correspond to sigma/2 from 
 Jorgensen and Tirado-Rives' 1988 JACS paper (v. 110, p. 1657).  However the 
 generalized born radius is equal to Rvdw plus a dielectric offset distance, 
 according to Still et al's 1997 J. Phys. Chem. A paper (v. 101, p. 3005).  
 This would mean the dielectric offset distance is set to zero (?).  
 (e.)  hct: HCT parameter
 
 With an eventual goal of implementing implicit solvent using my lab's force 
 field, insight into the meaning of the columns and/or references for their 
 origin would be greatly appreciated. 
 
 Thanks in advance! 
 
 Sincerely yours,
 
 E. A. Ploetz
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Re: [gmx-users] GB Parameters

2010-08-23 Thread Per Larsson
Also, again, as David said, if you find any errors in the parameters or in the 
code, please let me know!

Cheers
/Per


23 aug 2010 kl. 20:09 skrev Per Larsson per.lars...@sbc.su.se:

 Hi!
 
 Values in columns 1-3 are not currently used in version beta3. They pertain 
 to more elaborate surface area algorithms, the one from Still et al in 
 particular.
 
 Column 4 is the Vdw-radii for atom types that are used for computing the Born 
 radii. The dielectric offset is specified in the mdp-file, and gets added to 
 the input radii for the different radii methods.
 
 Column 5 is the scale factor for the HCT/OBC models. The values are taken 
 from the original HCT reference, as well as the corresponding implementation 
 in Tinker. 
 
 /Per
 
 23 aug 2010 kl. 19:27 skrev Elizabeth Ploetz plo...@ksu.edu:
 
 Dear Gromacs Users, 
 
 I am interested in implementing implicit solvent using the OBC GBSA method.  
 In the Gromacs 4.5beta3 top directory, several force fields (oplsaa and 
 multiple versions of amber) contain the gbsa.itp file, and one (charmm27), 
 contains a gb.itp file.  They all have the same column titles (sar, st, pi, 
 gbr, and hct).  I have read the six articles listed at 
 http://www.gromacs.org/Documentation/Terminology/Implicit_Solvent, however I 
 still have the following two questions regarding the contents of this file:
 
 (1.)  What values are tabulated in these columns and what are the 
 corresponding references for each of them?
 (2.)  Which columns are used (versus ignored) by Gromacs in the 
 implementation of each of the methods (Still/HCT/OBC)?
 
 Here are my guesses for Question 1:
 (a.)  sar: solvent accessible surface area?
 (b.)  st: surface tension?
 (c.)  pi: ?
 (d.)  gbr: generalized born radius?  These values correspond to sigma/2 from 
 Jorgensen and Tirado-Rives' 1988 JACS paper (v. 110, p. 1657).  However the 
 generalized born radius is equal to Rvdw plus a dielectric offset distance, 
 according to Still et al's 1997 J. Phys. Chem. A paper (v. 101, p. 3005).  
 This would mean the dielectric offset distance is set to zero (?).  
 (e.)  hct: HCT parameter
 
 With an eventual goal of implementing implicit solvent using my lab's force 
 field, insight into the meaning of the columns and/or references for their 
 origin would be greatly appreciated. 
 
 Thanks in advance! 
 
 Sincerely yours,
 
 E. A. Ploetz
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Re: [gmx-users] cutoff for implicit solvent in gromacs4.5

2010-08-09 Thread Per Larsson
Hi,

for implicit solvent, people generally use longer cut-offs, as you noted.

There can be many reasons for your seg. fault, however.
Did you do energy minimization before starting md? 
Please also test the same system with using a cut-off to see if that works.

/Per



8 aug 2010 kl. 22.36 skrev BIN ZHANG:

 But the problem is with this set up, I will always get a Segmentation fault 
 with gromacs VERSION 4.5-beta2.
 
 Is this supposed to be a bug or for this version, I can only use a large 
 cutoff?

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Re: [gmx-users] new beta release - gromacs-4.5-beta2

2010-08-05 Thread Per Larsson
Hi!

Is this with GBSA implicit solvent, and in that case what Born radii model?
Could you mail me the tpr off-list, and I'll have a look at it.

Cheers
/Per




5 aug 2010 kl. 20.26 skrev Elio Cino:

 
 Since the charmm force field has some instances with large charge groups  
 (grompp warns you for it) it is advisable to use a longer cut-off (or no  
 cut-off at all, by setting them all to 0). I've run 200 ns simulations  with 
 1.5 nm and nstlist = 5 and a timestep of 2 fs and constraints =  all-bonds.
 I could not have them set to infinite because I am using PBC. I used 1.5 and 
 the system ran fine with 2fs timestep. On another note, I installed 4.5 beta2 
 on another computer today and using the exact same system and settings I get 
 tons of lincs errors (bond rotate over 30 deg) and cannot even do position 
 restrain dynamics without segmentation fault. I even tried using the exact 
 same tpr files as my successful runs.  The one that works was my laptop (OSX 
 10.6 core2 duo) and the one that fails is centos5 dual quad core xenon. If I 
 run a normal solvated simulation, the linux machine runs fine.
 
 Elio Cino
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Re: [gmx-users] Re: gromacs with CMAP

2010-06-29 Thread Per Larsson
Hi,

I do not fully understand what you are trying to do, but currently CMAP is only
available for the standard amino acid residues present in the rtp-file for the
Charmm-forcefield, and the values for the grid are specified in the 
cmap.itp-file.

Do you use something else?

/Per


29 jun 2010 kl. 14.45 skrev Da-Wei Li:

 HI, David,
 
 thanks for your advise. I remove the bond angle force and get same
 result. It is really strange. If I set +5 on all the 24*24 grid, I
 just get a inverted distribution and if I set 0 on all grid, I will
 get a uniformed distribution. It is like that 27 regions are force to
 have zero cmap potential. I cannot attach figure due to size limit the
 list. I have sent the figure to you directly.
 
 best,
 
 dawei
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Re: [gmx-users] Charmm without CMAP

2010-06-22 Thread Per Larsson
Hi!

You can choose cmap/no cmap when you run pdb2gmx. 

/Per

Skickat från min iPhone

22 jun 2010 kl. 19:24 skrev Sai Pooja saipo...@gmail.com:

 Hi,
 
 I am using gromacs from the git repository which I downloaded 2 days back. 
 Charmm has been implemented in this version. Is it possible to use the Charmm 
 ff without CMAP with it?
 
 Regards
 Pooja
 
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Re: [gmx-users] protein structure prediction

2009-02-23 Thread Per Larsson


23 feb 2009 kl. 12.55 skrev Mark Abraham:


José Carlos Calvo Tudela wrote:
can I use the GROMACS software to get the energy of a protein  
conformation?


Yes, but your question is not well-formed. Only energy differences  
can have meaning.


Up to now I am using TINKER library (analyze program). Is there any  
similar software in GROMACS?


I don't know.


If I'm not mistaken, the energy you get from analyse.x  program in  
Tinker is the potential energy for a protein in is current  
conformation, given a particular force-field.


In that case, you might be able to get the same from Gromacs if you do  
a simulation with 0 steps, ie without any integration, and then look  
at the potential energy terms in the log file (or do many steps, and  
look at the energy before the first step)


Cheers
/Per




Mark
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Re: [gmx-users] Error in pdb2gmx.....Atom CE2 not found in residue PHE270 while adding hydrogens

2008-08-12 Thread Per Larsson
If atoms are missing in the sidechains of your protein, you can try a  
program like scwrl3 to rebuild all or some of the sidechains. This  
will give you complete sidechains in sort of reasonable positions.


Cheers
/Per




12 aug 2008 kl. 15.04 skrev vivek sharma:


Hi David,
Thanx a lot again. can you please tell me the criteria or the  
standards to do such correction or can you suggest some link or  
tutorial for the same?

whether swiss pdb can help in such cases?

With Thanx,
Vivek



2008/8/12 David van der Spoel [EMAIL PROTECTED]
vivek sharma wrote:
Hi There,

I am new to molecular dynamics and GROMACS.
While trying MD for 1XU9.pdb (pdbid) in the very 1st step on using  
the command


 pdb2gmx -f 1XU9.pdb -o 1XU9.gro -p 1XU9.top -i 1XU9.itp -vsite  
hydrogen -water spce


I got the following in the last of error.
..
..
..
...
N-terminus: NH3+
C-terminus: COO-
WARNING: atom CE2 not found in residue 270 while adding atom

---
Program pdb2gmx, VERSION 3.3.3
Source code file: genhydro.c, line: 304

Fatal error:
Atom CE2 not found in residue PHE270 while adding hydrogens
---
 I tried the same with different force field and water models, but  
getting the same error again and again.

any suggestion will be highly appreciated.

You have an incorrect pdb file. An atom is missing. You have to fix  
it yourself.



With thanx,
Vivek



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Re: [gmx-users] (no subject)

2008-07-17 Thread Per Larsson

Check the information on the gromacs wiki about this:

 
http://wiki.gromacs.org/index.php/Errors#T-Coupling_group_XXX_has_fewer_than_10.25_of_the_atoms

Cheers
/Per


17 jul 2008 kl. 14.38 skrev [EMAIL PROTECTED]:


Hi all
I have installed gromacs 3.3.3 in one of my 32 machine fedora core 2.
so check i tried to to do speptide tutorial in
/usr/local/gromacs/share/gromacs/tutor/speptide

But when i m running grompp for position restraint with the command
grompp -f pr -o pr -c after_em -r after_em -p speptide

i get the following warning

WARNING 1 [file aminoacids.dat, line 1]:
 T-Coupling group Protein has fewer than 10% of the atoms (191 out of
 2741)
 Maybe you want to try Protein and Non-Protein instead?

I tried to change SOL with non protein but getting the same warning.  
is it

ok to go further with this warning

When i did grompp for full MD with the command

grompp -v -f full -o full -c after_pr -p speptide

again i m getting the same warning

WARNING 1 [file aminoacids.dat, line 1]:
 T-Coupling group Protein has fewer than 10% of the atoms (191 out of
 2741)
 Maybe you want to try Protein and Non-Protein instead?


I tried to change SOL with non protein but getting the same warning.

I don't know what to do now and how can i overcome this, if anyone  
could

help me.

Thanks

ALKA



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Re: [gmx-users] regarding rmsd !!

2008-06-17 Thread Per Larsson

Check your input/output!
In this case it seems you are missing/forgetting the -s flag to  
specify the name of the tpr-file.


/Per




17 jun 2008 kl. 17.07 skrev Anamika Awasthi:




Dear All,
My protein is simulating for 20 ns and 16 ns has already  
over, but I want to analyze RMSD and RMSF for this 16 ns simulation,  
without stopping the running simulation.it was crashed before, so I  
used tpbconv -f  previous.trr -e previous.edr -s previous.tpr -o  
new.tpr -until 2

 then gave the command --
 mdrun -s new.tpr -o new.trr -c new.gro -g new.log -e new.edr

now job is running

now for analysis I am giving this command
g_rms new.tpr -f new.trr -o new_rmsd.xvg -xvgr

it is giving this output
:-)  g_rms  (-:

Option Filename  Type Description

  -s  topol.tpr  InputStructure+mass(db): tpr tpb tpa  
gro g96 pdb xml

  -f   new.trr  Input   Generic trajectory: xtc trr t  pdb
 -f2   traj.xtc  Input, Opt.  Generic trajectory: xtc trr trj  
gro g96 pdb

  -n  index.ndx  Input, Opt.  Index file
  -o   new_rmsd.xvg  Output   xvgr/xmgr file
-mirrmsdmir.xvg  Output, Opt. xvgr/xmgr file
  -a  avgrp.xvg  Output, Opt. xvgr/xmgr file
-dist rmsd-dist.xvg  Output, Opt. xvgr/xmgr file
  -m   rmsd.xpm  Output, Opt. X PixMap compatible matrix file
-bin   rmsd.dat  Output, Opt. Generic data file
 -bm   bond.xpm  Output, Opt. X PixMap compatible matrix file

  Option   Type  Value  Description
--
  -[no]h   bool no  Print help info and quit
  -[no]X   bool no  Use dialog box GUI to edit command line  
options

   -niceint 19  Set the nicelevel
  -b   time  0  First frame (ps) to read from trajectory
  -e   time  0  Last frame (ps) to read from trajectory
 -dt   time  0  Only use frame when t MOD dt = first  
time (ps)

 -tu   enum ps  Time unit: ps, fs, ns, us, ms, s, m or h
  -[no]w   bool no  View output xvg, xpm, eps and pdb files
   -[no]xvgr   boolyes  Add specific codes (legends etc.) in the  
output

xvg files for the xmgrace program
   -what   enum   rmsd  Structural difference measure: rmsd, rho  
or rhosc

-[no]pbc   boolyes  PBC check
-fit   enum rot+trans  Fit to reference structure: rot+trans,
translation or none
   -prevint  0  Compare with previous frame
  -[no]split   bool no  Split graph where time is zero
   -skipint  1  Only write every nr-th frame to matrix
  -skip2int  1  Only write every nr-th frame to matrix
-max   real -1  Maximum level in comparison matrix
-min   real -1  Minimum level in comparison matrix
   -bmax   real -1  Maximum level in bond angle matrix
   -bmin   real -1  Minimum level in bond angle matrix
-nlevelsint 80  Number of levels in the matrices
 -ngint  1  Number of groups to compute RMS between

---
Program g_rms, VERSION 3.3
Source code file: statutil.c, line: 787

Invalid command line argument:
new.tpr
---

 WHY THIS IS SHOWING THIS ERROR?


Thanks in advance

 Anamika

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Re: [gmx-users] Implicit Solvent Simulations

2008-05-22 Thread Per Larsson

Hello Una (and everyone else)

I'm happy to announce that, while not yet available in cvs, it will  
very soon be possible to do implicit solvation with Gromacs.
I'm have a working implementation almost finished, and are currently  
running some tests to assure that the code is stable.


With any luck we should be able to commit this to cvs in the next  
month or so :-)


Cheers
/Per Larsson, PhD student in the Lindahl group


22 maj 2008 kl. 16.13 skrev Una Bjarnadottir:


To the Gromacs user community,

As of April 2007 it was not possible to do implicit solvent MDs with  
Gromacs
(http://www.gromacs.org/pipermail/gmx-users/2007-April/026849.html).  
Has

this changed since then?

Kind regards, Una


--
Una Bjarnadottir   School of Biomolecular and Biomedical  
Science

Conway Institute   UCD
Dublin 4, Ireland  Phone: +353 1 716 6874, Fax: +353 1 716  
6898

Email: [EMAIL PROTECTED]
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Re: [gmx-users] Help for GNUPlot

2008-05-06 Thread Per Larsson

Hello!

Please note that xmgrace and gunplot are two different programs and as  
such work in different ways, for example in terms of what types of  
input and output they expect. The xvg-files that Gromacs produces are  
indended for xmgrace, and will not work out-of-the-box with gnuplot.


There are tons of tutorials on the internet on how to use gnuplot, and  
I suggest that you start by following a few of those, learning how to  
first make some simple toy-plots


Cheers
/Per




6 maj 2008 kl. 15.07 skrev s lal badshah:


Dear Mark,
Hi ! Currently I tried to install xmgrace but the toolbar menue is  
not shown on window screen so I am using gnuplot for analysis as I  
have little know how about unix/linux.Please set to me the following.

[EMAIL PROTECTED]:~ cd project
[EMAIL PROTECTED]:~/project ls
#bfac.pdb.1#   conf.pdb  genion.log  md323.tpr pr.edr  
topol_A.itp
#rmsf.xvg.1#   dist.xvg  gyrate.xvg  md323.trr pr.gro  
topol_B.itp
#topol.top.1#  distance.xvg  index.ndx   md323.xtc pr.log  
traj.trr
#traj.trr.1#   em.mdpions.pdbmd323lie.xvg  pr.mdp  
water.pdb

2a5f.pdb   em.pdbmd323.edr   mdout.mdp pr.tpr
bfac.pdb   em.tprmd323.gro   pe.xvgpr.trr
bonds.xvg  ener.edr  md323.log   posre_A.itp   rmsf.xvg
box.pdbenergy.xvgmd323.mdp   posre_B.itp   topol.top
[EMAIL PROTECTED]:~/project gnuplot

G N U P L O T
Version 4.2 patchlevel 0
last modified March 2007
System: Linux 2.6.22.5-31-default

Copyright (C) 1986 - 1993, 1998, 2004, 2007
Thomas Williams, Colin Kelley and many others

Type `help` to access the on-line reference manual.
The gnuplot FAQ is available from
http://www.gnuplot.info/faq/

Send comments and help requests to  [EMAIL PROTECTED] 

Send bug reports and suggestions to [EMAIL PROTECTED] 




Terminal type set to 'x11'
gnuplot plot rmsf.xvg u 1:2 w
 ^
 expecting 'lines', 'points', 'linespoints', 'dots',  
'impulses',

'yerrorbars', 'xerrorbars', 'xyerrorbars', 'steps', 'fsteps',
'histeps', 'filledcurves', 'boxes', 'boxerrorbars',  
'boxxyerrorbars',
'vectors', 'financebars', 'candlesticks', 'errorlines',  
'xerrorlines',

'yerrorlines', 'xyerrorlines', 'pm3d', 'labels', 'histograms',
 'image', 'rgbimage'

gnuplot boxes
 ^
 invalid command

gnuplot plot lines rmsf.xvg u 1:2 w
 undefined variable: lines

gnuplot plot gyrate.xvg
 undefined variable: gyrate

gnuplot plot gyrate.xvg
  ^
 Bad data on line 9

gnuplot
Regards,
Lal badshah
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Re: [gmx-users] results of energy minimization

2008-03-12 Thread Per Larsson

Hello!

Check out
http://wiki.gromacs.org/index.php/Errors#Stepsize_too_small.2C_or_no_change_in_energy._Converged_to_machine_precision.2C_but_not_to_the_requested_precision

Cheers
/Per


12 mar 2008 kl. 11.58 skrev s lal badshah:


Dear gromacs experts,
I have run the energy minimization of a protein.With the tail  
command it shows the following results:

[EMAIL PROTECTED]:~/protein tail -15 md.log
 NS-Pairs 94.365846 1981.68276620.0
 Reset In Box  0.5693855.124465 0.1
 Shift-X   0.5693103.415860 0.0
 CG-CoM0.1907855.532765 0.1
 Bonds 0.394530   16.964790 0.2
 Angles0.253320   41.291160 0.4
 Propers   0.0098552.256795 0.0
 RB-Dihedrals  0.086835   21.448245 0.2
---
 Total  9893.632954   100.0
---

   NODE (s)   Real (s)  (%)
   Time: 15.000 15.000100.0
Finished mdrun on node 0 Wed Mar 12 12:50:59 2008
I have check the em.log file, which shows the following data:

Steepest Descents converged to machine precision in 15 steps,
but did not reach the requested Fmax  1000.
Potential Energy  = -1.9742134e+21
Maximum force =  4.1648520e+06 on atom 1934
Norm of force =  5.6557945e+06
Is the energy minimization finished or not? when I use the top  
command the values fluctuates.As there any specific value or  
notation below the command name from which I know that energy  
minimization is running or finished.As in amber software the word  
sander is written below the command when check with top .Here X is  
written.

Regards,
Lal badshah.
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Re: [gmx-users] Step size too small

2007-08-17 Thread Per Larsson

Hello!

Check out
http://wiki.gromacs.org/index.php/Errors#Stepsize_too_small. 
2C_or_no_change_in_energy._Converged_to_machine_precision. 
2C_but_not_to_the_requested_precision


Cheers
/Per

17 aug 2007 kl. 18.28 skrev Sheyore Omovie:


Dear gmx-users,

I have 2 molecules in a box, as usual pdb2gmx saw them as one. i  
edited the .top file to remove the bonds created between the two  
molecules, I also added a distance restraint btw the molecules.  
(The 2 structures have been separately minimized). However, I get  
the ff message for EM run:

Stepsize too small, or no change in energy.
Converged to machine precision,
but not to the requested precision Fmax  1000

Double precision normally gives you higher accuracy.

Steepest Descents converged to machine precision in 15 steps,
but did not reach the requested Fmax  1000.
Potential Energy  =  1.0246325e+20
Maximum force =inf on atom 1
Norm of force =inf
I would appreciate any advice on how to fix this.
Rgds
John

See what you’re getting into…before you go there See it!
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Re: [gmx-users] stepsize too small

2007-08-13 Thread Per Larsson

Hello!

There are many discussions on the maillist about this...

In short, if all you want to do is normal md, it should be ok to just  
proceed with that. Just check that your potential energy is negative  
and everything should fine.


Otherwise, recompiling Gromacs to use double precision might get you  
a bit lower in energy, or change integrator to see if you get any lower.


Cheers
/Per


13 aug 2007 kl. 20.08 skrev burkhard rammner:



Hi,

This is the first time I`m using gromacs.
That`s why I`m having a beginners`question.
I tried to do an energy minimization, but after 45 steps this  
message appears

and I know that the following lines have led to questions before:

Stepsize too small (9.09769e-007 nm)Converged to machine precision,
but not to the requested precision (1000)

I`m using single precision windows compiled gromacs. I know, I have
to change whatever parameter, but so far I didn`t succeed.

This is the mdp file:

integrator= steep   emtol  =  
1000   emstep   = 0.01
nsteps= 200   nstenergy   =  
10   nstxtcout= 10
xtc_grps= Protein   energygrps =  
Protein   nstlist = 5   ns_type  
= simple   rlist   = 1.0
coulombtype= cut-off   rcoulomb  =  
1.0   rvdw= 1.0
constraints= none   pbc  = no

So, what`s wrong here?
What do I have to change?

Many thanks for help!

Burkhard
















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Re: [gmx-users] problem with writing energies

2007-08-02 Thread Per Larsson

Hello!

Are you out of disk-space?

Cheers
/Per

2 aug 2007 kl. 08.49 skrev aneesh chandran:


Hello Users

I am using gromacs 3.3 with g43a1 force field.

I am running a MD without  any position restraints.
After around 770 ps system stoped running with  an error could not  
write energies.

what could be the problem?
waiting for an early reply

Thanks in advance

with regards
Aneesh

following is the part of log file
Energies (kJ/mol)
G96Bond   G96AngleProper Dih.  Improper  
Dih.  LJ-14
2.12163e+033.41254e+031.42482e+031.04269e+03 
4.50126e+02
 Coulomb-14LJ (SR)   Coulomb (SR)   Coul. recip.   
Potential
2.43870e+041.06622e+05   -7.33872e+05   -9.53957e+04
-6.89807e+05

Kinetic En.   Total EnergyTemperature Pressure (bar)
1.26392e+05   -5.63415e+053.00768e+021.69426e+02

   Step   Time Lambda
 386000  772.60.0

   Rel. Constraint Deviation:  Maxbetween atoms RMS
   Before LINCS 0.048496   2033   2034   0.013339
After LINCS 0.26269271   0.03
Energies (kJ/mol)
G96Bond   G96AngleProper Dih.  Improper  
Dih.  LJ-14
2.21432e+033.34757e+031.50922e+039.45264e+02 
4.92081e+02
 Coulomb-14LJ (SR)   Coulomb (SR)   Coul. recip.   
Potential
2.46610e+041.04777e+05   -7.32472e+05   -9.54459e+04
-6.89972e+05

Kinetic En.   Total EnergyTemperature Pressure (bar)
1.26415e+05   -5.63557e+053.00823e+02   -3.26087e+01

   Step   Time Lambda
 386100  772.200010.0

   Rel. Constraint Deviation:  Maxbetween atoms RMS
   Before LINCS 0.060718968969   0.014659
After LINCS 0.15602605   0.02

---
Program mdrun, VERSION 3.3
Source code file: enxio.c, line: 343

Fatal error:
could not write energies
---
following is my input file

 integrator= md
   dt= 0.002
   nsteps= 125000
   nstxout   = 100
nstvout   = 100
   nstlog= 100
nstenergy = 100
nstxtcout = 0
energygrps= protein sol MG2+
   nstlist   = 10
ns_type   = grid
   rlist = 1.0
coulombtype   = PME
   rcoulomb  = 1.0
vdwtype   = cut-off
   rvdw  = 1.0
pbc   = xyz
tcoupl= berendsen
   tc-grps   = protein sol MG2+
   tau_t = 0.1 0.1 MG2+
   ref_t = 300 300 300
   Pcoupl= berendsen
   Pcoupltype= isotropic
   tau_p = 1.0
   compressibility   = 4.5e-5
   ref_p = 1.0
gen_vel   = yes
   gen_temp  = 300
   gen_seed  = 173529
   constraints   = hbonds







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Re: [gmx-users] error in pdb2gmx step

2006-03-31 Thread Per Larsson
Check you pdb file and see if the chain identifier A occurs at different 
places in the file. Pdb2gmx expects a chain to be continous, and if it 
isn't, it gets confused. If you have several chains, rename them 
accordingly.


Cheers
/Per


Annie Albin wrote:


Dear all,

 I faced a problem in the  pdb2gmx step as i got this following error 
message,

Fatal error:
Chain identifier 'A' was used in two non-sequential blocks (residue 
908, atom 7013)


As I'm pretty new to this field. I'm finding it difficult to 
troubleshoot. Any suggestions would be of great help.

Thank you,
Annie Albin.



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--

Per Larsson
PhD Student
Stockholm Bioinformatics Center
+46 (0) 8 55378577
+46 (0) 733 461467
[EMAIL PROTECTED]
www.sbc.su.se

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