[gmx-users] select groups in g_rms

2011-12-20 Thread yp sun
Dear Sir, 
 
When I run g_rms -s md.tpr -f md.trr -o rmsd.xvg, the program requires me 
selecting a group twice as following: 
 
g_rms -s md.tpr -f md.trr -o rmsd.xvg后, 程序两次要求选结构组,如下: 
Reading file md.tpr, VERSION 3.3.1 (single precision)
Reading file md.tpr, VERSION 3.3.1 (single precision)
Select group for least squares fit
Opening library file /home/gromacs-3.3.1/share/gromacs/top/aminoacids.dat
Group     0 (      System) has 519889 elements
Group     1 (     Protein) has 24649 elements
Group     2 (   Protein-H) has 12688 elements
Group     3 (     C-alpha) has  1540 elements
Group     4 (    Backbone) has  4620 elements
Group     5 (   MainChain) has  6172 elements
Group     6 (MainChain+Cb) has  7620 elements
Group     7 ( MainChain+H) has  7668 elements
Group     8 (   SideChain) has 16981 elements
Group     9 ( SideChain-H) has  6516 elements
Group    10 ( Prot-Masses) has 24649 elements
Group    11 ( Non-Protein) has 495240 elements
Group    12 (         SOL) has 495240 elements
Group    13 (       Other) has 495240 elements
Select a group: 1
Selected 1: 'Protein'
Select group for RMSD calculation
Opening library file /home/gromacs-3.3.1/share/gromacs/top/aminoacids.dat
Group     0 (      System) has 519889 elements
Group     1 (     Protein) has 24649 elements
Group     2 (   Protein-H) has 12688 elements
Group     3 (     C-alpha) has  1540 elements
Group     4 (    Backbone) has  4620 elements
Group     5 (   MainChain) has  6172 elements
Group     6 (MainChain+Cb) has  7620 elements
Group     7 ( MainChain+H) has  7668 elements
Group     8 (   SideChain) has 16981 elements
Group     9 ( SideChain-H) has  6516 elements
Group    10 ( Prot-Masses) has 24649 elements
Group    11 ( Non-Protein) has 495240 elements
Group    12 (         SOL) has 495240 elements
Group    13 (       Other) has 495240 elements
Select a group: 3
Selected 3: 'C-alpha'
trn version: GMX_trn_file (single precision)
Last frame        100 time  100.000

I don't understand how to make the first selction Select group for least 
squares fit, and the secend select Select group for RMSD calculation, and I 
don't understand the meaning of these selection. I hope you can help me. Thanks.
 
Best regards!

Yeping Sun
CAS Key Laboratory of Pathogenic Microbiology  Immunology
INSTITUTE OF MICROBIOLOGY CHINESE ACADEMY OF SCIENCES 
NO.1 Beichen West Road,Chaoyang District,Beijing 100101,china-- 
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Re: [gmx-users] select groups in g_rms

2011-12-20 Thread Gianluca Santoni

You could start by reading the gromacs manual,
Section 8.9
On 12/20/11 9:30 AM, yp sun wrote:

Dear Sir,
When I run g_rms -s md.tpr -f md.trr -o rmsd.xvg, the program requires 
me selecting a group twice as following:

g_rms -s md.tpr -f md.trr -o rmsd.xvg?, ??? ? ??,??:
Reading file md.tpr, VERSION 3.3.1 (single precision)
Reading file md.tpr, VERSION 3.3.1 (single precision)
Select group for least squares fit
Opening library file /home/gromacs-3.3.1/share/gromacs/top/aminoacids.dat
Group 0 (  System) has 519889 elements
Group 1 ( Protein) has 24649 elements
Group 2 (   Protein-H) has 12688 elements
Group 3 ( C-alpha) has  1540 elements
Group 4 (Backbone) has  4620 elements
Group 5 (   MainChain) has  6172 elements
Group 6 (MainChain+Cb) has  7620 elements
Group 7 ( MainChain+H) has  7668 elements
Group 8 (   SideChain) has 16981 elements
Group 9 ( SideChain-H) has  6516 elements
Group10 ( Prot-Masses) has 24649 elements
Group11 ( Non-Protein) has 495240 elements
Group12 ( SOL) has 495240 elements
Group13 (   Other) has 495240 elements
Select a group: 1
Selected 1: 'Protein'
Select group for RMSD calculation
Opening library file /home/gromacs-3.3.1/share/gromacs/top/aminoacids.dat
Group 0 (  System) has 519889 elements
Group 1 ( Protein) has 24649 elements
Group 2 (   Protein-H) has 12688 elements
Group 3 ( C-alpha) has  1540 elements
Group 4 (Backbone) has  4620 elements
Group 5 (   MainChain) has  6172 elements
Group 6 (MainChain+Cb) has  7620 elements
Group 7 ( MainChain+H) has  7668 elements
Group 8 (   SideChain) has 16981 elements
Group 9 ( SideChain-H) has  6516 elements
Group10 ( Prot-Masses) has 24649 elements
Group11 ( Non-Protein) has 495240 elements
Group12 ( SOL) has 495240 elements
Group13 (   Other) has 495240 elements
Select a group: 3
Selected 3: 'C-alpha'
trn version: GMX_trn_file (single precision)
Last frame100 time  100.000
I don't understand how to make the first selction Select group for 
least squares fit, and the secend select Select group for RMSD 
calculation, and I don't understand the meaning of these selection. I 
hope you can help me. Thanks.

Best regards!

Yeping Sun
CAS Key Laboratory of Pathogenic Microbiology  Immunology
INSTITUTE OF MICROBIOLOGY CHINESE ACADEMY OF SCIENCES
NO.1 Beichen West Road,Chaoyang District,Beijing 100101,china






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Structural Protein Dynamics Research Team
Institut de Biologie Structurale
41 rue Jules Horowitz   
38027 Grenoble Cedex 1  
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See http://www.gnu.org/philosophy/no-word-attachments.html

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[gmx-users] EM curve question

2011-12-20 Thread parto haghighi
Dear GMX-users
I am working on lipid-drug system.I have done these stages:
1.creating topology for drug and lipid
2.solvation
3.Ion addition
4.Energy minimization
5.NVT
My question is,why does the energy and temperature curves converge to
zero(I have used 320 K for my temperature in mdp file)?

Thanks a lot in advance.
 P.Haghighi
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[gmx-users] regarding rtp file

2011-12-20 Thread priya thiyagarajan
hello sir,
i go through the manual and your link..
 i need to add BFC residue type in rtp file and residuetype.dat..
thing is i need to  include charges angles bonds dihedrals impropers for
residue in my rtp file ,,
i dono  how to define its value..
mine is 14 carbon fattyacid..(BFC)
give some idea to define my residue,,
 thanking you,
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[gmx-users] Normal Mode Analysis starting from an optimized geometry and known partial charges

2011-12-20 Thread Thomas Evangelidis
Dear GROMACS users,


I have done Normal Mode Analysis and have calculated partial charges and
the optimized geometry of a few compounds using high-level QM calculations.
Now I want to see (if possible) how well GROMACS can reproduce the normal
modes if I start from the same optimized geometry and use the same partial
charges. The command lines I use are the following:

ligand=10058_F4.nw.new_GMX

## do Normal Mode Analysis
grompp_d4.5.5 -f nm.mdp -c ${ligand}.gro -p ${ligand}.top -o nm.tpr
mdrun_d4.5.5 -v -deffnm nm

## calculate the eigenvectors/values of the Hessian matrix and write the
eigenvectors to a trajectory file
g_nmeig_d4.5.5 -f nm.mtx -s nm.tpr -of -ol -v -m -last 81

## plot the vector components and the RMS fluctuation per atom of
eigenvectors for all eigenvectors
echo 0 | g_anaeig_d4.5.5 -v eigenvec.trr -s nm.tpr -eig eigenval.xvg -comp
-rmsf -last -1

## create a trajectory from the eigenvector 76 (the first 6 are the
rotation and translation) to visualize the vibrations in VMD
g_nmtraj_d4.5.5 -s nm.tpr -v eigenvec.trr -eignr 76 -nframes 10
-amplitude 1 -o

Most of the resulting normal modes do not coincide with the respective ones
calculated through QM. Does the order of the above command lines make sense?


An obvious problem is that the starting compound geometry is not in full
precision as highlighted in the documentation:

http://www.gromacs.org/Documentation/How-tos/Normal_Mode_Analysis

Is it possible to create a full precision .trr coordinate file from a .gro
or any other structure file with modified 8-decimal point coordinates?


I am looking forward for an answer,
Thomas
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[gmx-users] Possible typo in nb_kernel_x86_64_sse.c (4.5.5)

2011-12-20 Thread Daniel Adriano Silva M
Hi Devs,

Is this intended or just a typo:

#nb_kernel_x86_64_sse/nb_kernel_x86_64_sse.c#
.:
211:fprintf(log,Testing x86_64 SSE2 support...);
.:
##

instead of:

.:
211:fprintf(log,Testing x86_64 SSE1 support...);
.:


The same thing appears in other _sse.c files.


Thanks,
Daniel
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Re: [gmx-users] regarding rtp file

2011-12-20 Thread Mark Abraham


On 20/12/11, priya thiyagarajan  priya.thiyagaraja...@gmail.com wrote:
 hello sir,
 i go through the manual and your link..
  i need to add BFC residue type in rtp file and residuetype.dat..
 thing is i need to  include charges angles bonds dihedrals impropers for 
 residue in my rtp file ,,
 
 i dono  how to define its value..
 mine is 14 carbon fattyacid..(BFC)
 give some idea to define my residue,,
 
Actually with such species it is usually more a matter of choosing which atom 
types should be used for which atom, which usually determines the above 
parameters, which will then be looked up automatically, just as for the other 
.rtp entries. Parameters probably already exist in your force field for a fatty 
acid, and if they don't, that's probably a good reason to choose another force 
field.


Mark
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Re: [gmx-users] Normal Mode Analysis starting from an optimized geometry and known partial charges

2011-12-20 Thread Mark Abraham


On 20/12/11, Thomas Evangelidis  teva...@gmail.com wrote:
 Dear GROMACS users,
 
 
 I have done Normal Mode Analysis and have calculated partial charges and the 
 optimized geometry of a few compounds using high-level QM calculations. Now I 
 want to see (if possible) how well GROMACS can reproduce the normal modes if 
 I start from the same optimized geometry and use the same partial charges.
 


In general for NMA to make sense you need to be at a stationary point w.r.t. 
the atomic degrees of freedom of the model being used. That won't be quite true 
at a QM geometry, so there's a sense of apples-vs-oranges comparison.
 

  The command lines I use are the following:
 
 
 ligand=10058_F4.nw.new_GMX
 
 ## do Normal Mode Analysis
 grompp_d4.5.5 -f nm.mdp -c ${ligand}.gro -p ${ligand}.top -o nm.tpr
 mdrun_d4.5.5 -v -deffnm nm
 
 ## calculate the eigenvectors/values of the Hessian matrix and write the 
 eigenvectors to a trajectory file
 
 g_nmeig_d4.5.5 -f nm.mtx -s nm.tpr -of -ol -v -m -last 81
 
 ## plot the vector components and the RMS fluctuation per atom of 
 eigenvectors for all eigenvectors
 echo 0 | g_anaeig_d4.5.5 -v eigenvec.trr -s nm.tpr -eig eigenval.xvg -comp 
 -rmsf -last -1
 
 
 ## create a trajectory from the eigenvector 76 (the first 6 are the rotation 
 and translation) to visualize the vibrations in VMD
 g_nmtraj_d4.5.5 -s nm.tpr -v eigenvec.trr -eignr 76 -nframes 10 -amplitude 
 1 -o
 
 
 Most of the resulting normal modes do not coincide with the respective ones 
 calculated through QM. Does the order of the above command lines make sense?
 
 
 An obvious problem is that the starting compound geometry is not in full 
 precision
 


The starting geometry is in full precision if it's the same as that used for 
the QM calculation. That is quite possible to achieve with .pdb or .gro input.
 

  as highlighted in the documentation:
 
 
 http://www.gromacs.org/Documentation/How-tos/Normal_Mode_Analysis
 
 Is it possible to create a full precision .trr coordinate file from a .gro or 
 any other structure file with modified 8-decimal point coordinates?
 


I think you are misunderstanding the use of the word precision here. In 
general, the same configuration will be represented differently in .trr and 
.gro formats, with the former being a closer approximation. Accordingly, one 
will get a different result for NMA on the endpoint of GROMACS EM as observed 
in the .trr file and as observed in the .gro file. The former will be closer to 
the stationary point, and so lead to more acceptable estimates of the normal 
modes. However, here you want to do NMA on the same coordinates with two 
programs, so it is up to you to represent the coordinates in a way that the two 
programs can compute on the same approximation to the coordinates of the 
stationary point. There's no need to convert to .trr (or the QM binary format), 
because all that does is treat 2.613 as 2.613.


Mark
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Re: [gmx-users] EM curve question

2011-12-20 Thread Mark Abraham


On 20/12/11, parto haghighi  parto.haghi...@gmail.com wrote:
 Dear GMX-users
 I am working on lipid-drug system.I have done these stages:
 1.creating topology for drug and lipid
 2.solvation
 3.Ion addition
 4.Energy minimization
 5.NVT
 My question is,why does the energy and temperature curves converge to
 zero(I have used 320 K for my temperature in mdp file)?
 


You've done something wrong, but on the available information we can't tell if 
you aren't modelling what you think you're modelling, or aren't observing what 
you think you're observing, or both.


Mark
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[gmx-users] Re: LINCS error

2011-12-20 Thread aiswarya pawar
i went through the mailing list, but i dont understand when i run the same
protein on my computer it runs correctly without any LINCS warning. On the
cluster with 64 processors the job runs but crashes in between and shows
the LINCS warning.


Please anyone tell me what could be the reason. Is anything wrong with my
protein.


On Sun, Dec 18, 2011 at 7:35 PM, aiswarya pawar aiswarya.pa...@gmail.comwrote:

 Hi users,

 I did energy minimization of a protein complex using the following
 minimization mdp file.

 ; Lines starting with ';' ARE COMMENTS
 ; Everything following ';' is also comment

 title = Energy Minimization ; Title of run

 ; The following line tell the program the standard locations where to find
 certain files
 cpp = /lib/cpp ; Preprocessor


 ; Define can be used to control processes
 define  = -DFLEXIBLE

 ; Parameters describing what to do, when to stop and what to save
 integrator = steep ; Algorithm (steep = steepest descent minimization)
 emtol = 1000.0   ; Stop minimization when the maximum force  1.0 kJ/mol
 emstep  = 0.01
 nsteps = 5000 ; Maximum number of (minimization) steps to perform
 nstenergy = 10 ; Write energies to disk every nstenergy steps
 energygrps = Protein ; Which energy group(s) to write to disk

 ; Parameters describing how to find the neighbors of each atom and how to
 calculate the interactions
 nstlist = 10 ; Frequency to update the neighbor list and long range forces
 ns_type = grid   ; Method to determine neighbor list (simple, grid)
 rlist = 1.0 ; Cut-off for making neighbor list (short range forces)
 coulombtype = PME   ; Treatment of long range electrostatic interactions
 rcoulomb = 1.0 ; long range electrostatic cut-off
 rvdw = 1.4 ; long range Van der Waals cut-off
 constraints = none ; Bond types to replace by constraints
 pbc= xyz ; Periodic Boundary Conditions (yes/no)


 and the pr.mdp =

 ; VARIOUS PREPROCESSING OPTIONS
 title= Position Restrained Molecular Dynamics
 define   = -DPOSRES

 constraints  = all-bonds
 integrator   = md
 dt   = 0.001 ; ps !
 nsteps   = 25000 ; total 50 ps.
 nstcomm  = 10
 nstxout  = 500 ; collect data every 1 ps
 nstxtcout= 500
 nstvout  = 0
 nstfout  = 0
 nstlist  = 10
 ns_type  = grid
 rlist= 1.0
 coulombtype  = PME
 rcoulomb = 1.0
 vdwtype  = cut-off
 rvdw = 1.4
 pme_order= 4
 ewald_rtol   = 1e-5
 optimize_fft = yes
 DispCorr = no
 ; Berendsen temperature coupling is on
 Tcoupl   = v-rescale
 tau_t= 0.1 0.1
 tc-grps = protein non-protein
 ref_t= 300 300
 ; Pressure coupling is on
 Pcoupl   = parrinello-rahman
 Pcoupltype   = isotropic
 tau_p= 1.0
 compressibility  = 4.5e-5
 ref_p= 1.0
 ; Generate velocites is on at 300 K.
 gen_vel  = yes
 gen_temp = 300.0
 gen_seed = -1

 and md.mdp file =

 ; VARIOUS PREPROCESSING OPTIONS
 title= Position Restrained Molecular Dynamics


 ; RUN CONTROL PARAMETERS
 constraints = all-bonds
 integrator = md
 dt = 0.002 ; 2fs !
 nsteps = 250 ; total 5000 ps.
 nstcomm = 10
 nstxout = 500 ; collect data every 1 ps
 nstxtcout = 0
 nstvout = 0
 nstfout = 0
 nstlist = 10
 ns_type = grid
 rlist = 1.0
 coulombtype = PME
 rcoulomb = 1.0
 vdwtype = cut-off
 rvdw = 1.4
 pme_order = 4
 ewald_rtol = 1e-5
 optimize_fft = yes
 DispCorr = no
 ; Berendsen temperature coupling is on
 Tcoupl = v-rescale
 tau_t = 0.1 0.1
 tc-grps = protein non-protein
 ref_t = 300 300
 ; Pressure coupling is on
 Pcoupl = parrinello-rahman
 Pcoupltype = isotropic
 tau_p = 1.0
 compressibility = 4.5e-5
 ref_p = 1.0
 ; Generate velocites is on at 300 K.
 gen_vel = yes
 gen_temp = 300.0
 gen_seed = -1


 The minimization step went well. but while doing the final mdrun am
 getting LINCS error. i read through the numerous mailing list on grimaces
 but still couldn't understand how would i fix this. am getting this error
 for all the 10 protein complex i did minimization for. Please help.


 Thanks,
 Aiswarya


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Re: [gmx-users] Re: LINCS error

2011-12-20 Thread Mark Abraham


On 20/12/11, aiswarya pawar  aiswarya.pa...@gmail.com wrote:
 i went through the mailing list, but i dont understand when i run the same 
 protein on my computer it runs correctly without any LINCS warning. On the 
 cluster with 64 processors the job runs but crashes in between and shows the 
 LINCS warning. 
 


That happens. Your different computers are running different versions of the 
calculation. Numerical artefacts do happen, especially if you use algorithms 
that are known to be unstable when not in equilibrium, like I said three days 
ago. Why have you repeated your question instead of trying my suggestion?



 Please anyone tell me what could be the reason. Is anything wrong with my 
 protein.
 


Something is very likely wrong with your system preparation. The links people 
have been giving you detail the advice on how to diagnose the problem or how to 
be more gentle. There's little else for me to say.


Mark 

 
 
 
 On Sun, Dec 18, 2011 at 7:35 PM, aiswarya pawar aiswarya.pa...@gmail.com 
 wrote:
 
 
  Hi users,
  
  I did energy minimization of a protein complex using the following 
  minimization mdp file.
  
  
  
  ; Lines starting with ';' ARE COMMENTS
  ; Everything following ';' is also comment
  
  
  
  title   = Energy Minimization   ; Title of run
  
  
  ; The following line tell the program the standard locations where to find 
  certain files
  
  
  cpp = /lib/cpp  ; Preprocessor
  
  
  
  
  ; Define can be used to control processes
  
  define          = -DFLEXIBLE
  
  
  ; Parameters describing what to do, when to stop and what to save
  integrator  = steep ; Algorithm (steep = steepest descent 
  minimization)
  
  
  emtol   = 1000.0    ; Stop minimization when the maximum 
  force  1.0 kJ/mol
  emstep      = 0.01
  
  nsteps  = 5000  ; Maximum number of (minimization) 
  steps to perform
  nstenergy   = 10; Write energies to disk every nstenergy steps
  
  
  energygrps  = Protein   ; Which energy group(s) to write to disk
  
  
  ; Parameters describing how to find the neighbors of each atom and how to 
  calculate the interactions
  
  
  nstlist = 10; Frequency to update the neighbor list 
  and long range forces
  ns_type = grid  ; Method to determine neighbor list 
  (simple, grid)
  
  
  rlist   = 1.0   ; Cut-off for making neighbor list 
  (short range forces)
  coulombtype = PME   ; Treatment of long range electrostatic 
  interactions
  
  
  rcoulomb= 1.0   ; long range electrostatic cut-off
  rvdw= 1.4   ; long range Van der Waals cut-off
  
  
  constraints = none  ; Bond types to replace by constraints
  pbc     = xyz   ; Periodic Boundary Conditions (yes/no)
  
  
  
  
  
  
  
  and the pr.mdp =
  
  
  ; VARIOUS PREPROCESSING OPTIONS
  title                    = Position Restrained Molecular Dynamics
  define                   = -DPOSRES
  
  
  
  
  constraints              = all-bonds
  integrator               = md
  dt                       = 0.001 ; ps !
  nsteps                   = 25000 ; total 50 ps.
  nstcomm                  = 10
  
  
  nstxout                  = 500 ; collect data every 1 ps
  nstxtcout                = 500
  nstvout                  = 0
  nstfout                  = 0
  nstlist                  = 10
  
  
  ns_type                  = grid
  rlist                    = 1.0
  coulombtype              = PME
  rcoulomb                 = 1.0
  vdwtype                  = cut-off
  rvdw                     = 1.4
  
  
  pme_order                = 4
  ewald_rtol               = 1e-5
  optimize_fft             = yes
  DispCorr                 = no
  ; Berendsen temperature coupling is on
  Tcoupl                   = v-rescale
  
  
  tau_t                    = 0.1 0.1
  tc-grps = protein non-protein
  ref_t                    = 300 300
  ; Pressure coupling is on
  Pcoupl                   = parrinello-rahman
  
  
  Pcoupltype               = isotropic
  tau_p                    = 1.0
  compressibility          = 4.5e-5
  ref_p                    = 1.0
  ; Generate velocites is on at 300 K.
  
  
  gen_vel                  = yes
  gen_temp                 = 300.0
  gen_seed                 = -1
  
  
  
  
  and md.mdp file =
  
  
  ; VARIOUS PREPROCESSING OPTIONS
  
  
  title                    = Position Restrained Molecular Dynamics
  
  
  
  
  ; RUN CONTROL PARAMETERS
  constraints = all-bonds
  integrator = md
  dt = 0.002 ; 2fs !
  
  
  nsteps = 250 ; total 5000 ps.
  nstcomm = 10
  nstxout = 500 ; collect data every 1 ps
  nstxtcout = 0
  nstvout = 0
  nstfout = 0
  nstlist = 10
  ns_type = grid
  
  
  rlist = 1.0
  coulombtype = PME
  rcoulomb = 1.0
  vdwtype = cut-off
  rvdw = 1.4
  pme_order = 4
  ewald_rtol = 1e-5
  optimize_fft = yes
  DispCorr = no
  
  
  ; Berendsen temperature coupling 

Re: [gmx-users] Normal Mode Analysis starting from an optimized geometry and known partial charges

2011-12-20 Thread Thomas Evangelidis
Mark, thanks for the prompt response!

I have done Normal Mode Analysis and have calculated partial charges and
 the optimized geometry of a few compounds using high-level QM calculations.
 Now I want to see (if possible) how well GROMACS can reproduce the normal
 modes if I start from the same optimized geometry and use the same partial
 charges.


 In general for NMA to make sense you need to be at a stationary point
 w.r.t. the atomic degrees of freedom of the model being used. That won't be
 quite true at a QM geometry, so there's a sense of apples-vs-oranges
 comparison.


If I get it right you mean that NMA in GROMACS must start from an energy
minimum (stationary point) w.r.t the ff used (GAFF in my case), which means
that an energy minimization is neccessary ever if I use an QM optimum
geometry and the respective partial charges. Namely there is no way to
reproduce the normal modes I obtained from QM calculations, correct?


 An obvious problem is that the starting compound geometry is not in full
 precision

 The starting geometry is in full precision if it's the same as that used
 for the QM calculation. That is quite possible to achieve with .pdb or .gro
 input.


The same as the starting geometry or as the optimized geometry?


 as highlighted in the documentation:

 http://www.gromacs.org/Documentation/How-tos/Normal_Mode_Analysis

 Is it possible to create a full precision .trr coordinate file from a .gro
 or any other structure file with modified 8-decimal point coordinates?


 I think you are misunderstanding the use of the word precision here. In
 general, the same configuration will be represented differently in .trr and
 .gro formats, with the former being a closer approximation. Accordingly,
 one will get a different result for NMA on the endpoint of GROMACS EM as
 observed in the .trr file and as observed in the .gro file. The former will
 be closer to the stationary point, and so lead to more acceptable estimates
 of the normal modes. However, here you want to do NMA on the same
 coordinates with two programs, so it is up to you to represent the
 coordinates in a way that the two programs can compute on the same
 approximation to the coordinates of the stationary point. There's no need
 to convert to .trr (or the QM binary format), because all that does is
 treat 2.613 as 2.613.


So a command line like this will do the job, right?

grompp_d4.5.5 -f nm.mdp -c ${ligand}_8_decimal_points.gro -p ${ligand}.top
-o nm.tpr



Thomas





==

Thomas Evangelidis

PhD student

Biomedical Research Foundation, Academy of Athens

4 Soranou Ephessiou , 115 27 Athens, Greece

email: tev...@bioacademy.gr

  teva...@gmail.com


website: https://sites.google.com/site/thomasevangelidishomepage/
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[gmx-users] A simulation of pure chloroform with AMBER compatible parameters never gives the right density

2011-12-20 Thread anaome

Dear Users,

I am trying to reproduce the results obtained by Fox  Kollman on  
chloroform presented in the following papers but can never achieve the  
proper density of 1.459 they obtain with their own rigid CHCL3 model.  
The best I obtain with the parameters presented below is 1.390. I  
tried with both version 4.5.3 and 4.0.7.

Can anyone help me on that ?
Thank you

Aymeric Naômé

The Journal of Physical Chemistry, 1996, 100, 25, 10779-10783
The Journal of Physical Chemistry B, 1998, 102, 41, 8070-8079

The parameters are:
qC=-0.345 eps=0.1094 kcal/mol R*=1.908 Ang.
qCl=0.012 eps=0.2550 R*=2.000
qH=0.309  eps=0.0157 R*=1.187
C-Cl=1.758 Ang.
C-H=1.100
H-C-Cl=107.7°
Cl-C-Cl=112.2°

And my corresponding topology file is the following:
sigma=2*(R*/10)/(2^(1/6))
epsilon=eps*4.184


[ defaults ]
; nbfunccomb-rule   gen-pairs   fudgeLJ fudgeQQ
1   2   no  0.5 0.8333

[ atomtypes ]
; name  at.num  mass charge ptype  sigma  epsilon
CT   6  12.010.  A   3.39967e-01  4.57730e-01
H3   1   1.008   0.  A   2.11499e-01  6.56888e-02
Cl  17  35.453   0.  A   3.56359e-01  1.10669e+00


[ moleculetype ]
; Namenrexcl
CHCL3 3

[ atoms ]
;   nr   type  resnr residue  atom   cgnr charge   mass   
typeBchargeB  massB
 1 CT  1  CHCL3  C  1 -0.345 12.011
; qtot -0.386
 2 H3  1  CHCL3  H  1  0.309  1.008
; qtot -0.120
 3 Cl  1  CHCL3Cl1  1  0.012 35.453
; qtot -0.080
 4 Cl  1  CHCL3Cl2  1  0.012 35.453
; qtot -0.040
 5 Cl  1  CHCL3Cl3  1  0.012 35.453
; qtot  0

[ constraints ]
1 3 10.1758
1 4 10.1758
1 5 10.1758
1 2 10.1100
;2 3 20.2340
2 4 20.2340
2 5 20.2340
3 4 20.2901
4 5 20.2901
5 3 20.2901

[ system ]
; Name
CHCl3_256

[ molecules ]
; Compound#mols
CHCL3 256


The simulation parameters in the first paper:
MD program: AMBER 4.1
200-300 molecules
dt=2fs (rigid model)
cut-off=12 Ang.
long range correction according to AllenTildesley
Berendsen thermostat with coupling constant 0.4 ps-1
temperature=300 K
inverse compressibility 1.086 10-4 bar-1
Berendsen barostat with coupling constant 0.2 ps-1
pressure=1 atm
SHAKE constraint solver

Below is my mdp file with the corresponding parameters:

title   =  CHCl3_box
cpp =  /lib/cpp -traditional
define  =
constraints =
integrator  =  md
dt  =  0.002; fs !
nsteps  =  40   ; total 1 ps.
nstcomm =  1
nstxout =  500
nstvout =  1000
nstfout =  0
nstlog  =  500
nstenergy   =  500
nstlist =  10
ns_type =  grid
rlist   =  1.2
coulombtype =  cut-off
rcoulomb=  1.2
rvdw=  1.2
DispCorr=  EnerPres
fourierspacing  =  0.12
fourier_nx  =  0
fourier_ny  =  0
fourier_nz  =  0
pme_order   =  6
ewald_rtol  =  1e-5
optimize_fft=  yes
energygrps  =  CHCL3
; Berendsen temperature coupling is on in three groups
Tcoupl  =  berendsen
tau_t   = 5
tc_grps = CHCL3
ref_t   = 300
; Pressure coupling is on
Pcoupl  =  Berendsen
pcoupltype  =  isotropic
tau_p   =  2.5
compressibility =  10.86e-5
ref_p   =  1.0
; Generate velocites is on at 300 K.
gen_vel =  yes
gen_temp=  300.0
gen_seed=  173529
; Energy group exclusion
energygrp_excl  =
freezegrps  =
freezedim   =
; Non-equilibrium Thermodynamics
acc_grps=
accelarate  =
; center of mass
comm_mode   = linear
comm_grps   =
; Type of constraint algorithm
constraint-algorithm = Shake


--
Aymeric Naômé
Ph. D. Student
UCPTS Division
University of Namur
61 Rue de Bruxelles
5000 Namur
BELGIUM


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Re: [gmx-users] A simulation of pure chloroform with AMBER compatible parameters never gives the right density

2011-12-20 Thread David van der Spoel

On 2011-12-20 15:03, ana...@fundp.ac.be wrote:

Dear Users,

I am trying to reproduce the results obtained by Fox  Kollman on
chloroform presented in the following papers but can never achieve the
proper density of 1.459 they obtain with their own rigid CHCL3 model.
The best I obtain with the parameters presented below is 1.390. I tried
with both version 4.5.3 and 4.0.7.
Can anyone help me on that ?
Thank you


Haven't tried that one, but we have OPLS/AA and GAFF, see:
http://virtualchemistry.org/molecules/67-66-3/index.php
for those the density is too low as well.



Aymeric Naômé

The Journal of Physical Chemistry, 1996, 100, 25, 10779-10783
The Journal of Physical Chemistry B, 1998, 102, 41, 8070-8079

The parameters are:
qC=-0.345 eps=0.1094 kcal/mol R*=1.908 Ang.
qCl=0.012 eps=0.2550 R*=2.000
qH=0.309 eps=0.0157 R*=1.187
C-Cl=1.758 Ang.
C-H=1.100
H-C-Cl=107.7°
Cl-C-Cl=112.2°

And my corresponding topology file is the following:
sigma=2*(R*/10)/(2^(1/6))
epsilon=eps*4.184


[ defaults ]
; nbfunc comb-rule gen-pairs fudgeLJ fudgeQQ
1 2 no 0.5 0.8333

[ atomtypes ]
; name at.num mass charge ptype sigma epsilon
CT 6 12.01 0. A 3.39967e-01 4.57730e-01
H3 1 1.008 0. A 2.11499e-01 6.56888e-02
Cl 17 35.453 0. A 3.56359e-01 1.10669e+00


[ moleculetype ]
; Name nrexcl
CHCL3 3

[ atoms ]
; nr type resnr residue atom cgnr charge mass typeB chargeB massB
1 CT 1 CHCL3 C 1 -0.345 12.011 ; qtot -0.386
2 H3 1 CHCL3 H 1 0.309 1.008 ; qtot -0.120
3 Cl 1 CHCL3 Cl1 1 0.012 35.453 ; qtot -0.080
4 Cl 1 CHCL3 Cl2 1 0.012 35.453 ; qtot -0.040
5 Cl 1 CHCL3 Cl3 1 0.012 35.453 ; qtot 0
[ constraints ]
1 3 1 0.1758
1 4 1 0.1758
1 5 1 0.1758
1 2 1 0.1100
; 2 3 2 0.2340
2 4 2 0.2340
2 5 2 0.2340
3 4 2 0.2901
4 5 2 0.2901
5 3 2 0.2901

[ system ]
; Name
CHCl3_256

[ molecules ]
; Compound #mols
CHCL3 256


The simulation parameters in the first paper:
MD program: AMBER 4.1
200-300 molecules
dt=2fs (rigid model)
cut-off=12 Ang.
long range correction according to AllenTildesley
Berendsen thermostat with coupling constant 0.4 ps-1
temperature=300 K
inverse compressibility 1.086 10-4 bar-1
Berendsen barostat with coupling constant 0.2 ps-1
pressure=1 atm
SHAKE constraint solver

Below is my mdp file with the corresponding parameters:

title = CHCl3_box
cpp = /lib/cpp -traditional
define =
constraints =
integrator = md
dt = 0.002 ; fs !
nsteps = 40 ; total 1 ps.
nstcomm = 1
nstxout = 500
nstvout = 1000
nstfout = 0
nstlog = 500
nstenergy = 500
nstlist = 10
ns_type = grid
rlist = 1.2
coulombtype = cut-off
rcoulomb = 1.2
rvdw = 1.2
DispCorr = EnerPres
fourierspacing = 0.12
fourier_nx = 0
fourier_ny = 0
fourier_nz = 0
pme_order = 6
ewald_rtol = 1e-5
optimize_fft = yes
energygrps = CHCL3
; Berendsen temperature coupling is on in three groups
Tcoupl = berendsen
tau_t = 5
tc_grps = CHCL3
ref_t = 300
; Pressure coupling is on
Pcoupl = Berendsen
pcoupltype = isotropic
tau_p = 2.5
compressibility = 10.86e-5
ref_p = 1.0
; Generate velocites is on at 300 K.
gen_vel = yes
gen_temp = 300.0
gen_seed = 173529
; Energy group exclusion
energygrp_excl =
freezegrps =
freezedim =
; Non-equilibrium Thermodynamics
acc_grps =
accelarate =
; center of mass
comm_mode = linear
comm_grps =
; Type of constraint algorithm
constraint-algorithm = Shake





--
David van der Spoel, Ph.D., Professor of Biology
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] [Fwd: h-bonds constraints]

2011-12-20 Thread Gavin Melaugh

---BeginMessage---
Hi

I want to run an NPT simulation with all h-bonds constrained. How does
grompp identify the Hydrogen atoms given that forcefield labels like HA,
HC, HE are used. Is it the mass?

Many Thanks

Gavin

---End Message---
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[gmx-users] About conformation choice for Umbrella sampling

2011-12-20 Thread vidhya sankar
Dear justin ,  i regret inconvenience in the previous mail  

Instead of taking PDB based on g_dist over all frames Can  i  choose various 
.gro files for doing umbrella sampling based on the pullf.xvg . file 

In that file plot of force Vs time is available. i am selecting the PDBs from  
near  maxima of force time profile curve to time of major structural change  .
in my case Example ( 120ps to 380ps) 

can i use those PDBs for Umbrella sampling othewise  should i not  consider 
time for umbrella sampling?

I am expecting your valuable reply

Thanks in Advance 
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[gmx-users] umbrella sampling with replica exchange

2011-12-20 Thread Sanku M
Hi,
  I have a technical question regarding feasibility of  combining replica 
exchange with umbrella sampling or any other pulling simulations in gromacs.
Since the umbrella sampling or any other pulling simulations are 
non-equilibrium simulation due to presence of external bias, I wonder whether 
the detailed balance in  replica exchange simulation  will be maintained .
I ask this because replica exchange  uses Monte Carlo metropolis algorithm to 
swap configurations and so I wanted to know what is the energy-difference ( New 
energy - old energy) in metropolis algorithm gromacs will use : Is it the 
energy difference after taking into account the biasing potential or is is only 
the internal potential energy-difference ( i.e not including biasing potential 
) ?

Any response from the users or developer will be highly appreciated.

Thanks

Sanku-- 
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Re: [gmx-users] [Fwd: h-bonds constraints]

2011-12-20 Thread Justin A. Lemkul



Gavin Melaugh wrote:




Subject:
h-bonds constraints
From:
Gavin Melaugh gmelaug...@qub.ac.uk
Date:
Mon, 19 Dec 2011 10:20:40 +
To:
Discussion list for GROMACS users gmx-users@gromacs.org

To:
Discussion list for GROMACS users gmx-users@gromacs.org


Hi

I want to run an NPT simulation with all h-bonds constrained. How does
grompp identify the Hydrogen atoms given that forcefield labels like HA,
HC, HE are used. Is it the mass?



The atom name designates whether or not it's a hydrogen.  See the 
count_hydrogens routine in topshake.c.


-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] About conformation choice for Umbrella sampling

2011-12-20 Thread Justin A. Lemkul



vidhya sankar wrote:
Dear justin ,  i regret inconvenience in the previous mail 


I have no experience with PLUMED; I could not comment.  I have been extremely 
busy lately.


Instead of taking PDB based on g_dist over all frames Can  i  choose 
various .gro files for doing umbrella sampling based on the pullf.xvg . 
file
In that file plot of force Vs time is available. i am selecting the PDBs 
from  near  maxima of force time profile curve to time of major 
structural change  .

in my case Example ( 120ps to 380ps)
can i use those PDBs for Umbrella sampling othewise  should i not  
consider time for umbrella sampling?


I'm sorry, I have no clear idea what you're even trying to accomplish.

-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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[gmx-users] a doubt about pbc nojump or mol or whole

2011-12-20 Thread Anna Marabotti
Dear gmx-users,
I've just finished several simulations of 4 single point mutants of my
dimeric protein in rhombic dodecahedron box (-d 1.5 nm) centered on the
protein, filled with water, neutralized with sodium, simulated with Gromacs
4.5.3 for 30 ns after NVT and NPT dynamics. I made simulations in the same
way and with the same settings, obtaining 4 trajectories.
When I obtained trajectories, I used trjconv to reset the visualization of
my systems:
 
trjconv -f traj.xtc -s traj.tpr -pbc mol -ur compact -o traj_mol.xtc
(selecting 0=System when prompted)
 
then I used g_mindist to calculate minimum distance between periodic images.
The resulting graphs showed me that for all simulations the distance is
never lower than 2.0 nm, but for only one system there are some spikes in
the final part of the simulation (between 25 and 30 ns) lowering the min
distance below 1 nm (only in correspondence of these spikes). 
 
I also calculated the rmsd using as reference the .gro file obtained in this
way (as suggested sometimes ago by somebody of you, perhaps Justin or
Tsjerk):
editconf -f traj.tpr -o traj_0ns.gro
trjconv -f traj_0ns.gro -s traj.tpr -pbc mol -ur compact -o traj_mol.gro
(selecting 0=System when prompted)
then:
g_rms -f traj_mol.xtc -s traj_mol.gro -o traj_mol_rms.xvg (selecting
4=Backbone when prompted)
 
I see a quite stable rmsd around 0.2 nm for all systems, with spikes up to 4
nm in the same system that showed problems with g_mindist, in positions
corresponding to the spikes in the g_mindist.xvg graph.
 
Looking at this trajectory with VMD, I saw that in correspondence with the
spikes, the two monomers of the protein dissociate and appear in different
parts of the simulation box (i.e. my periodic image is formed by one
monomer, and another monomer is seen in correspondence with another periodic
image). All the other systems move into the periodic box, without
dissociating into monomers.
 
In order to manage this issue, I applied nojump to the trajectory of this
anomalous system:
trjconv -f traj_mol.xtc -s traj.tpr -pbc nojump -o traj_molnoj.xtc
 
When I repeated the analyses with g_mindist and g_rms, I see graphs
perfectly superimposed to the former graphs, except for spikes that have
been disappeared.
 
What I would like to know is:
- Did I make the correct procedure to treat these systems?
- Can I compare the results obtained on this -mol + -noj trajectory with the
other trajectories -mol only?
- In your opinion, is the dissociation of the two monomers only a problem
of visualization (given that this protein behaves apparently normally
after applying pbc nojump), or I have to suppose that this system is
anomalous only for this fact?
 
Any help would be very appreciated.
Many thanks in advance and best regards
Anna
__
Anna Marabotti, Ph.D.
Web site: http://bioinformatica.isa.cnr.it/anna/anna.htm
 
When a man with a gun meets a man with a pen, the man with the gun is a
dead man
(Roberto Benigni, about Roberto Saviano)
 
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Re: [gmx-users] a doubt about pbc nojump or mol or whole

2011-12-20 Thread Tsjerk Wassenaar
Hi Anna,

Jumps like that are a consequence of PBC. Nothing wrong. Removing jumps
like you did is the proper treatment.

Cheers,

Tsjerk

On Dec 20, 2011 9:27 PM, Anna Marabotti anna.marabo...@isa.cnr.it wrote:

**
Dear gmx-users,
I've just finished several simulations of 4 single point mutants of my
dimeric protein in rhombic dodecahedron box (-d 1.5 nm) centered on the
protein, filled with water, neutralized with sodium, simulated with Gromacs
4.5.3 for 30 ns after NVT and NPT dynamics. I made simulations in the same
way and with the same settings, obtaining 4 trajectories.
When I obtained trajectories, I used trjconv to reset the visualization of
my systems:

trjconv -f traj.xtc -s traj.tpr -pbc mol -ur compact -o traj_mol.xtc
(selecting 0=System when prompted)

then I used g_mindist to calculate minimum distance between periodic
images. The resulting graphs showed me that for all simulations the
distance is never lower than 2.0 nm, but for only one system there are some
spikes in the final part of the simulation (between 25 and 30 ns) lowering
the min distance below 1 nm (only in correspondence of these spikes).

I also calculated the rmsd using as reference the .gro file obtained in
this way (as suggested sometimes ago by somebody of you, perhaps Justin or
Tsjerk):
editconf -f traj.tpr -o traj_0ns.gro
trjconv -f traj_0ns.gro -s traj.tpr -pbc mol -ur compact -o traj_mol.gro
(selecting 0=System when prompted)
then:
g_rms -f traj_mol.xtc -s traj_mol.gro -o traj_mol_rms.xvg (selecting
4=Backbone when prompted)

I see a quite stable rmsd around 0.2 nm for all systems, with spikes up to
4 nm in the same system that showed problems with g_mindist, in
positions corresponding to the spikes in the g_mindist.xvg graph.

Looking at this trajectory with VMD, I saw that in correspondence with the
spikes, the two monomers of the protein dissociate and appear in
different parts of the simulation box (i.e. my periodic image is formed by
one monomer, and another monomer is seen in correspondence with another
periodic image). All the other systems move into the periodic box, without
dissociating into monomers.

In order to manage this issue, I applied nojump to the trajectory of this
anomalous system:
trjconv -f traj_mol.xtc -s traj.tpr -pbc nojump -o traj_molnoj.xtc

When I repeated the analyses with g_mindist and g_rms, I see graphs
perfectly superimposed to the former graphs, except for spikes that have
been disappeared.

What I would like to know is:
- Did I make the correct procedure to treat these systems?
- Can I compare the results obtained on this -mol + -noj trajectory with
the other trajectories -mol only?
- In your opinion, is the dissociation of the two monomers only a problem
of visualization (given that this protein behaves apparently normally
after applying pbc nojump), or I have to suppose that this system is
anomalous only for this fact?

Any help would be very appreciated.
Many thanks in advance and best regards
Anna
 __
Anna Marabotti, Ph.D.
Web site: http://bioinformatica.isa.cnr.it/anna/anna.htm

When a man with a gun meets a man with a pen, the man with the gun is a
dead man
(Roberto Benigni, about Roberto Saviano)


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Re: [gmx-users] Voronoi tessellation

2011-12-20 Thread Ramya Parthasarathi
Thanks a  lot , will try that


Ramya Parthasarathi
ramya.sar...@aol.com




-Original Message-
From: Justin A. Lemkul jalem...@vt.edu
To: Discussion list for GROMACS users gmx-users@gromacs.org
Sent: Fri, Dec 16, 2011 11:16 am
Subject: Re: [gmx-users] Voronoi tessellation




Ramya Parthasarathi wrote:
 Hi
 
 I am working with phospholipid bilayers and I would like to plot the 2D 
 Voronoi Tessellation , can any one tell me how to start about it.
 

Not with any Gromacs tool.  But these might be useful:

http://onlinelibrary.wiley.com/doi/10.1002/jcc.21973/abstract
http://www.bevanlab.biochem.vt.edu/GridMAT-MD/

-Justin

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MILES-IGERT Trainee
Department of Biochemistry
Virginia Tech
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http://www.bevanlab.biochem.vt.edu/Pages/Personal/justin


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RE: [gmx-users] pressure profiles

2011-12-20 Thread Dallas Warren
It will be saved in the .edr file.  Use g_energy to extract the data you are 
interested in.

Catch ya,

Dr. Dallas Warren
Medicinal Chemistry and Drug Action
Monash Institute of Pharmaceutical Sciences, Monash University
381 Royal Parade, Parkville VIC 3010
dallas.war...@monash.edu
+61 3 9903 9304
-
When the only tool you own is a hammer, every problem begins to resemble a nail.

From: gmx-users-boun...@gromacs.org [mailto:gmx-users-boun...@gromacs.org] On 
Behalf Of Ramya Parthasarathi
Sent: Wednesday, 21 December 2011 9:06 AM
To: gmx-users@gromacs.org
Subject: [gmx-users] pressure profiles

Hi,

I am simulating DOPC lipid molecules in water, i would like to plot the 
pressure profiles, for the systems i have . Can someone tell me , is there any 
option in GROMACS which can give the pressure profile?
Ramya Parthasarathi
ramya.sar...@aol.com
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Re: [gmx-users] Normal Mode Analysis starting from an optimized geometry and known partial charges

2011-12-20 Thread Mark Abraham

On 12/21/2011 12:57 AM, Thomas Evangelidis wrote:

Mark, thanks for the prompt response!


I have done Normal Mode Analysis and have calculated partial
charges and the optimized geometry of a few compounds using
high-level QM calculations. Now I want to see (if possible) how
well GROMACS can reproduce the normal modes if I start from the
same optimized geometry and use the same partial charges.


In general for NMA to make sense you need to be at a stationary
point w.r.t. the atomic degrees of freedom of the model being
used. That won't be quite true at a QM geometry, so there's a
sense of apples-vs-oranges comparison.

If I get it right you mean that NMA in GROMACS must start from an 
energy minimum (stationary point) w.r.t the ff used (GAFF in my case), 
which means that an energy minimization is neccessary ever if I use an 
QM optimum geometry and the respective partial charges. Namely there 
is no way to reproduce the normal modes I obtained from QM 
calculations, correct?


You can choose to compare the two models on the same configuration, or 
at the local minimum w.r.t. each model that is nearest some 
configuration. Each approach has a minor flaw. How you need to manage 
precision varies with the choice you make.





An obvious problem is that the starting compound geometry is not
in full precision

The starting geometry is in full precision if it's the same as
that used for the QM calculation. That is quite possible to
achieve with .pdb or .gro input.

The same as the starting geometry or as the optimized geometry?


Your choice - your original workflow did no EM in GROMACS, so the use of 
.trr format was immaterial.



as highlighted in the documentation:

http://www.gromacs.org/Documentation/How-tos/Normal_Mode_Analysis

Is it possible to create a full precision .trr coordinate file
from a .gro or any other structure file with modified 8-decimal
point coordinates?


I think you are misunderstanding the use of the word precision
here. In general, the same configuration will be represented
differently in .trr and .gro formats, with the former being a
closer approximation. Accordingly, one will get a different result
for NMA on the endpoint of GROMACS EM as observed in the .trr file
and as observed in the .gro file. The former will be closer to the
stationary point, and so lead to more acceptable estimates of the
normal modes. However, here you want to do NMA on the same
coordinates with two programs, so it is up to you to represent the
coordinates in a way that the two programs can compute on the same
approximation to the coordinates of the stationary point. There's
no need to convert to .trr (or the QM binary format), because all
that does is treat 2.613 as 2.613.


So a command line like this will do the job, right?

grompp_d4.5.5 -f nm.mdp -c ${ligand}_8_decimal_points.gro -p 
${ligand}.top -o nm.tpr


That copies the configuration in -c in the full precision available from 
the format of -c into the .tpr.


Mark

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[gmx-users] CTAB force field

2011-12-20 Thread cuong nguyen
Dear all,

I prepare to do simulation about the solution of CTAB. Does anyone know the
force field (top and gro files) of CTAB which were published before?

Thank you very much.

Best regards,



Nguyen Van Cuong
PhD student - Curtin University of Technology
Mobile: (+61) 452213981
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Re: [gmx-users] Possible typo in nb_kernel_x86_64_sse.c (4.5.5)

2011-12-20 Thread Roland Schulz
Hi,

this is on purpose. Since 4.5 GROMACS requires SSE2. It is used for e.g.
the GB kernels. Because CPUs with SSE1 support but no SSE2 are so old we
don't try to support them anymore even for those kernels not requiring SSE2.

Roland

On Tue, Dec 20, 2011 at 6:05 AM, Daniel Adriano Silva M
dadri...@gmail.comwrote:

  Hi Devs,

  Is this intended or just a typo:

  #nb_kernel_x86_64_sse/nb_kernel_x86_64_sse.c#
 .:
 211:fprintf(log,Testing x86_64 SSE2 support...);
 .:
 ##

  instead of:

  .:
 211:fprintf(log,Testing x86_64 SSE1 support...);
 .:


  The same thing appears in other _sse.c files.


  Thanks,
 Daniel




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Re: [gmx-users] maxh not causing termination

2011-12-20 Thread Mark Abraham

On 12/19/2011 1:51 PM, Ben Reynwar wrote:

I'm having a problem with gromacs not terminating as expected when
using the maxh option.
It is an REMD simulation with 32 replicas.
I'm specifying -maxh 24 and as expected see the following in the stderr output.

Step 773882: Run time exceeded 23.760 hours, will terminate the run

Step 773876: Run time exceeded 23.760 hours, will terminate the run

Step 773880: Run time exceeded 23.760 hours, will terminate the run

etc

However I can see that the output files continued to be written for
another hour until at 25 hours the simulation was terminated by the
queueing system.
No checkpoint files were produced.  The output files show that the
simulation continued until about step 797000.

I've done similar things previously without running into this problem.
  Anyone have any ideas for what stupid mistake I could be making?


Perhaps none. What GROMACS version is this? Does the latest version have 
the same behaviour?


Mark

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Re: [gmx-users] Possible typo in nb_kernel_x86_64_sse.c (4.5.5)

2011-12-20 Thread Daniel Adriano Silva M
Got it. Thanks.

Daniel
On Dec 21, 2011 9:46 AM, Roland Schulz rol...@utk.edu wrote:

 Hi,

 this is on purpose. Since 4.5 GROMACS requires SSE2. It is used for e.g.
 the GB kernels. Because CPUs with SSE1 support but no SSE2 are so old we
 don't try to support them anymore even for those kernels not requiring SSE2.

 Roland

 On Tue, Dec 20, 2011 at 6:05 AM, Daniel Adriano Silva M 
 dadri...@gmail.com wrote:

  Hi Devs,

  Is this intended or just a typo:

  #nb_kernel_x86_64_sse/nb_kernel_x86_64_sse.c#
 .:
 211:fprintf(log,Testing x86_64 SSE2 support...);
 .:
 ##

  instead of:

  .:
 211:fprintf(log,Testing x86_64 SSE1 support...);
 .:


  The same thing appears in other _sse.c files.


  Thanks,
 Daniel




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[gmx-users] regarding rtp file

2011-12-20 Thread priya thiyagarajan
hello sir,
 Thanks for your reply..
As you suggest i tried with all available forcefield for my lipopeptide but
i am getting the same error,,


*Processing chain 2 'A' (16 atoms, 1 residues)
Warning: Starting residue BFC1 in chain not identified as Protein/RNA/DNA.
Problem with chain definition, or missing terminal residues.
This chain does not appear to contain a recognized chain molecule.
If this is incorrect, you can edit residuetypes.dat to modify the behavior.
8 out of 8 lines of specbond.dat converted successfully

---
Program pdb2gmx, VERSION 4.5.5
Source code file: resall.c, line: 581

Fatal error:
Residue 'BFC' not found in residue topology database
For more information and tips for troubleshooting, please check the GROMACS
website at http://www.gromacs.org/Documentation/Errors
---*


since mine is connected cyclic lipopeptide even i cant try using  prodrg
server too.
i dono how to generate my topology  file.
pls help me with your answer.
   Thanking you,
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Re: [gmx-users] regarding rtp file

2011-12-20 Thread Justin A. Lemkul



priya thiyagarajan wrote:

hello sir,
 Thanks for your reply..
As you suggest i tried with all available forcefield for my lipopeptide 
but i am getting the same error,,




I have posted this link several times before:

http://www.gromacs.org/Documentation/How-tos/Adding_a_Residue_to_a_Force_Field

All the necessary steps are spelled out there.  There is no force field that 
will contain the residue you seek; you have to add it yourself.




*Processing chain 2 'A' (16 atoms, 1 residues)
Warning: Starting residue BFC1 in chain not identified as Protein/RNA/DNA.
Problem with chain definition, or missing terminal residues.
This chain does not appear to contain a recognized chain molecule.
If this is incorrect, you can edit residuetypes.dat to modify the behavior.


The error message tells you exactly what is wrong (in this case, not completing 
step #5 in the link above).



8 out of 8 lines of specbond.dat converted successfully

---
Program pdb2gmx, VERSION 4.5.5
Source code file: resall.c, line: 581

Fatal error:
Residue 'BFC' not found in residue topology database
For more information and tips for troubleshooting, please check the GROMACS
website at http://www.gromacs.org/Documentation/Errors
---*



http://www.gromacs.org/Documentation/Errors#Residue_'XXX'_not_found_in_residue_topology_database

Also, a result of not completing step #1 in the adding a residue link above.



since mine is connected cyclic lipopeptide even i cant try using  prodrg 
server too.

i dono how to generate my topology  file.
pls help me with your answer.


I've tried and at this point am repeating myself.  Also note that there are 
numerous posts in the list archive about dealing with cyclic peptides (which are 
not trivial).  I would suggest you search for them.  You should also simplify 
your system until you understand the workflow.  Deal with a custom residue in a 
normal linear peptide, then introduce the cyclic peptide and the issues it may 
present.


-Justin

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Ph.D. Candidate
ICTAS Doctoral Scholar
MILES-IGERT Trainee
Department of Biochemistry
Virginia Tech
Blacksburg, VA
jalemkul[at]vt.edu | (540) 231-9080
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Re: [gmx-users] g_hbond

2011-12-20 Thread sulatha M. S
As suggested by David I extended the simulations (total of 25ns) for a
single chain polyacid in 5500 water molecules and tried to calculate the
H-bond ACF. I get the same negative lifetime for Hbonds between COOH groups
and water. Is it that the g_hbond ACF giving weird results for this case.
For chains with COO- and COOH groups (50% each), I got positive life times
of Hbond. Ayy ideas on how to solve this will be of great help. I am using
4.0.7 version. The command line I gave was
g_hbond -f traj.xtc -s traj.tpr -n index.ndx -ac and chose the polyacid and
the water as  the two groups.


ACF 22057/22057
Normalization for c(t) = 0.0217714 for gh(t) = 4.35398e-06
Hydrogen bond thermodynamics at T = 298.15 K
Fitting parameters chi^2 =  0.0146697
Q =  0
--

Type  Rate (1/ps) Time (ps)  DG (kJ/mol)  Chi^2
Forward-0.271 -3.687-666.000   0.0146697
Backward   -2.291 -0.437-666.000
One-way 0.101  9.882  10.207
Integral0.034 29.376  12.907
Relaxation  0.063 15.803  11.370


Thankyou for any help,

Dr. M. S. Sulatha
Dept. of Chemical Engineering
IIT-Madras
India


On Tue, Dec 13, 2011 at 10:12 AM, sulatha M. S mssula...@gmail.com wrote:



 I did not get a warning here. I also have simulations (20ns) of
 copolyacids where again it gave me negative life time. These runs are
 well equilibrated with respect to energy and Rg of the polymers. The
 system is a 20 repeat unit chain in approx. 5500 water molecules. I have
 done simulations in which 10 units are COO- and the remaining 10 as COOH
 along the chain. With a 10ns trajectory, the average life time of
 H-bonds is positive.Only in the case of unionized acid I am getting a
 negative life time.

  Did you look at the ACF graph? It could be constant at 1 or 0.


 Yes, the ACF decays to 0 and remains constant in all cases





Thankyou for any help,

Dr. M. S. Sulatha
Dept. of Chemical Engineering
IIT-Madras
India




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What is the value for free energy of H-bonding.






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[gmx-users] Re:Getting energy values in kcal/mol

2011-12-20 Thread Sairam Tatikonda
Hi,
I am running MD simulation  for my system using Gromacs , as the output
energies values generated are in the units of kJ/mol , Is there any option
or method while running the simulation which i can use  so that i get
output energies in the units of kcal/mol rather than in kJ/mol.I have gone
through the gromacs manual and mailing list but could not find the solution.
Any help will be highly appreciated.




Rajitha
Ph.D student
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Re: [gmx-users] Re:Getting energy values in kcal/mol

2011-12-20 Thread Mark Abraham

On 12/21/2011 5:44 PM, Sairam Tatikonda wrote:

Hi,
I am running MD simulation  for my system using Gromacs , as the 
output energies values generated are in the units of kJ/mol , Is there 
any option or method while running the simulation which i can use  so 
that i get output energies in the units of kcal/mol rather than in 
kJ/mol.I have gone through the gromacs manual and mailing list but 
could not find the solution.

Any help will be highly appreciated.


No. You will need to convert these yourself if you need it.

Mark

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[gmx-users] regarding itp

2011-12-20 Thread priya thiyagarajan
hello sir,
thanks for your reply..
sorry for disturbing you again and again..
i understood that i need to add my residue BFC in my rtp file and
residuetype.dat file.
i like to clarify one thing.
i added BFC as lipid in my residuetypes.dat file.
then i need to include my residue BFC  in .rtp file.
To add in that rtp file i need itp file for my fattyacid. so that can use
those atomtypes dihedrals  in my rtp.
am i correct..
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Re: [gmx-users] regarding itp

2011-12-20 Thread Mark Abraham

On 12/21/2011 5:53 PM, priya thiyagarajan wrote:

hello sir,
thanks for your reply..
sorry for disturbing you again and again..
i understood that i need to add my residue BFC in my rtp file and 
residuetype.dat file.

i like to clarify one thing.
i added BFC as lipid in my residuetypes.dat file.
then i need to include my residue BFC  in .rtp file.
To add in that rtp file i need itp file for my fattyacid. so that can 
use those atomtypes dihedrals  in my rtp.

am i correct..


pdb2gmx uses the .rtp entries to construct a [moleculetype], as you 
already know from your reading of chapter 5 (particularly section 5.6) 
of the manual... right? A molecule .itp file already contains a 
[moleculetype]. Both of those need to either declare their function 
parameters on the line that uses them, or rely on grompp to later look 
them up from the atom types in the force field .itp files. So you need 
either to map the atoms in your BFC to the pre-defined atomtypes so that 
the existing parameters can be looked up, or you need to develop the 
parameters yourself (which would be a bad idea at what appears to be 
your current level of experience).


Mark

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[gmx-users] restraint force and free enrgy code.

2011-12-20 Thread sunhanzi
Dear Everyone:
  
  I need to calculate the free energy change of restraining the ligand in the 
binding site. I wonder if or not the restraint force can be directly controlled 
by the free energy code, which means by different lambda values. I checked the 
manual of gromacs 4.5.4 but can not found any clue for that. But I do think 
someone mentioned that it can be done in some version of gromacs. Does anyone 
can tell me if it is true?
  
  Thanks a lot!



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Best regards,

Hanzi Sun@HuangLab NIBS





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