Re: [gmx-users] position restraint

2013-08-22 Thread Gaurav Goel
One quick observation-- you mention the filename as posre_ion.itp, but are
using  ion_posre.itp at #include. -g


On Thu, Aug 22, 2013 at 4:24 PM, Shima Arasteh
shima_arasteh2...@yahoo.comwrote:

 Hi,

 I want to put position restraint on an ion ,

 First made an .itp file of the ion: posre_ion.itp

 Then added these line to top file:
 #include ./charmm36-modified.ff/ions.itp
 #ifdef POSRES_ION
 #include ion_posre.itp
 #endif

 And added the line to mdp file

 define = -DPOSRES_ION

 But the grompp failed because it gives me the fatal error that the include
 line is not in the correct position.



 Would you please let me know if the inclusion of posre_ion.itp is not as I
 did? What's the problem?

 Thanks in advance for your suggesions.

 Sincerely,
 Shima
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Re: [gmx-users] TRACE OF RMSD COMPARISON MATRIX

2013-07-02 Thread Gaurav Goel
Following link might be helpful:
http://orbeckst.github.io/GromacsWrapper/gromacs/core/fileformats/xpm.html

-g
-- 
Gaurav Goel
Assistant Professor
Department of Chemical Engineering
Indian Institute of Technology, Delhi
Hauz Khas, New Delhi 110016
India

On 02-Jul-2013, at 10:45 AM, Richa Singh richa.s.rathor...@gmail.com wrote:

 Hello users,
 
 I'm using g_rms to compare my actual trajectory obtained from
 simulation with the filtered trajectory (along given set of
 eigenvectors), this gives me an RMSD comparison matrix in xpm format
 where the values of the plot are not clear. Is there any way which can
 help me to get the values along the diagonal of the matrix?
 the command that i followed is:
 g_rms -s ref.tpr -f actual.xtc -f2 filtered.xtc -m rmsd.xpm
 
 I want to calculate the trace of the matrix basically.
 
 
 Regards..
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Re: [gmx-users] MD simulation with varying pH

2012-07-05 Thread Gaurav Goel
Dear Peterson,

There's no magic wand for this. You'll need to find out pKa values of
titrable amino acids in your protein (in literature, MEAD software,
etc.). Then, you can protonate (pHpKa) / deprotonate (pHpKa)  those
group according to the pH.

-G


On Thu, Jul 5, 2012 at 12:33 PM, J Peterson think_bey...@aol.com wrote:
 Dear GROMACS Users,

 I'm planning to work on a protein that activates itself under lower pH
 conditions. And I don't have any clues how to do it in GROMACS. My first
 question is about the possibilities to do this in GROMACS, has anyone done
 this before? It can even be a constant simulations at a particular
 lower/higher pH or gradually lowering/increasing pH.

 Any suggestion on this would give me a lead.

 Thanks

 Peterson J

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 View this message in context: 
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Re: [gmx-users] Is GPU GTX 560 compatible with GROMACS?

2012-04-16 Thread Gaurav Goel
Dear Shouliang,

Thanks. Maybe the developers can help undertand why GTX560 is not
included on the GPU compatibility list for GROMACS?

-G

2012/4/16 shouliang dong shouliangd...@gmail.com:
 It is compatible with GROMACS.

 在 2012年4月14日 上午11:32,Gaurav Goel gauravgoel...@gmail.com写道:

 Dear All,

 Can you please guide me on how to find out if GeForce GTX 560 GPU card
 by NVIDIA will be compatible with GROMACS? On the website GTX 560 Ti
 is mentioned, but GTX 560 is not.

 Thanks,
 G

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Department of Chemical Engineering
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[gmx-users] Is GPU GTX 560 compatible with GROMACS?

2012-04-13 Thread Gaurav Goel
Dear All,

Can you please guide me on how to find out if GeForce GTX 560 GPU card
by NVIDIA will be compatible with GROMACS? On the website GTX 560 Ti
is mentioned, but GTX 560 is not.

Thanks,
G

-- 
Gaurav Goel, PhD
Assistant Professor
Department of Chemical Engineering
Indian Institute of Technology, Delhi
Hauz Khas, New Delhi 110016
India
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[gmx-users] Nonequilibrium MD- implementing a temperature gradient simulation

2011-02-03 Thread Gaurav Goel
My aim is to establish a temperature gradient in the MD simulation box. I'm
simulating a magnesium silicate system with interatomic potentials (Mg-Mg,
Mg-Si, etc.) and no bond or angle potentials.

My algorithm:

1. Divide the MD box in 12 slabs along the x-axis.
2. Pick slab 3 as my source and slab 9 as sink.
3. Find the atom with highest kinetic energy in slab 3 and the atom with
lowest KE in slab 9 (I amke sure both atoms have same type and hence same
mass)
4. Exchange their velocity vectors.

I achieve this by making following changes to the update.c routine:

**In static void do_update_md(

*I comment out the position update line.

 v[n][d]= vb;
  /*xprime[n][d]   = x[n][d]+vb*dt;*/

*then I exchange velocities as mentioned above

*and now I update the positions based on these new velocities:

xprime[n][d]   = x[n][d]+v[n][d]*dt;

---
I print out the kinetic energy of atoms before and after exchanging and see
no problem there. Total KE of these two atoms is the same before and after.
But, over the length of my simulation I see average temperature of the
system keeps on increasing in the NVE ensemble-- in 1ns temperature of the
system increased from 3000K - 3500K.
Note that the average temperature does not increase in the equilibrium NVE
with same '.mdp' parameters (no velocity exchange).

Any thoughts?

Thanks,
Gaurav
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Re: [gmx-users] Speeding up simulation

2010-08-18 Thread Gaurav Goel
Large cut-offs can bring artificial artifacts.

e.g. *Chemical Physics
Letters*http://www.sciencedirect.com/science/journal/00092614
 Volume 406, Issues
1-3http://www.sciencedirect.com/science?_ob=PublicationURL_tockey=%23TOC%235231%232005%23995939998%23591997%23FLA%23_cdi=5231_pubType=Jview=c_auth=y_acct=C62818_version=1_urlVersion=0_userid=6325866md5=51f91ba17c3ce282da206786a17d50d5,
23 April 2005, Pages 49-53

-Gaurav

On Wed, Aug 18, 2010 at 12:04 PM, sapna sarupria
sapna.sarup...@gmail.comwrote:

 That might actually be the best approach speed wise. But it depends on what
 level of accuracy you wish for your calculations. What is your system like?
 May be you can have a large cut off but you will have to see what the trade
 off between speed and accuracy is.


 On Wed, Aug 18, 2010 at 10:26 AM, ms deviceran...@gmail.com wrote:

 On 17/08/10 22:36, Justin A. Lemkul wrote:

  There is no way to limit PME to certain ranges. It is a method for
 solving infinite sums. Usually PME is a poor choice for in vacuo
 simulations and the like, since there's nothing to be done for most of
 the simulation box.


 This interests me -I've used simple cut-off for in vacuo tests, but I
 still hadn't made my mind on what electrostatic model I should truly use. Do
 you have any suggestion?

 thanks,
 M.


  You may want to see how others (in the literature)
 deal with droplet-type simulations.

 -Justin


 Thanks for your help.

 Sapna

 On Tue, Aug 17, 2010 at 5:29 PM, Justin A. Lemkul jalem...@vt.edu
 mailto:jalem...@vt.edu wrote:



 sapna sarupria wrote:

 Hi all,

 I am running (NVT) simulations of a drop of water (~5 nm in
 radius) in a big box (~25 nm) in a box and find that the
 simulations are rather slow. I am getting about 0.8 ns per day
 when a simulation of bulk system of equivalent number of waters
 will be much faster. The number of waters is ~12000. I was
 wondering if anyone can suggest methods with which I can speed
 up the simulations. I am using domain decomposition and
 optimize_fft is set to yes. PME is used for the electrostatics.


 I would suspect that the lag comes from a lot of unused PME
 calculations. During your run, PME grid points will be assigned to
 vacuum space, for which nothing needs to be done. You can check
 imbalances and performance loss in the log file.

 -Justin


 Thank you

 Sincerely
 Sapna


 -- 

 Justin A. Lemkul
 Ph.D. Candidate
 ICTAS Doctoral Scholar
 MILES-IGERT Trainee
 Department of Biochemistry
 Virginia Tech
 Blacksburg, VA
 jalemkul[at]vt.edu http://vt.edu | (540) 231-9080
 http://www.bevanlab.biochem.vt.edu/Pages/Personal/justin

 
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 Princeton University
 New Jersey 08540
 U.S.A.

 Life isn't about finding yourself. Life is about creating yourself. --
 George Bernard Shaw.
 Dare to Dream



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 --
 Sapna Sarupria
 Post-doctoral Researcher
 Princeton University
 New Jersey 08540
 U.S.A.

 Life isn't about finding yourself. Life is about creating yourself. --
 George Bernard Shaw.
 Dare to Dream

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Re: [gmx-users] Speeding up simulation

2010-08-17 Thread Gaurav Goel
Sapna,

Is there a particular reason you're using a box so much larger than the
droplet diameter? If your only concern is that periodic images should not
see each-other maybe you can use a box length=droplet diameter+2*largest
cut-off in the system.

Also using a more spherical box shape such as  rhombic dodecahedron or the
truncated octahedron will help you in reducing the volume of unfilled space.

-Gaurav

On Tue, Aug 17, 2010 at 5:40 PM, sapna sarupria sapna.sarup...@gmail.comwrote:

 Hi Justin

 Thanks for your input. I guess I will do some more literature search and
 try to optimize the simulations as much as I can.

 Thanks,
 Sapna


 On Tue, Aug 17, 2010 at 5:36 PM, Justin A. Lemkul jalem...@vt.edu wrote:



 sapna sarupria wrote:

 Hi Justin
 Thanks for your response. I suspect that it is the same thing. Is there a
 way to make gromacs use PME only within a certain region of the simulation
 box? Also, how does one know how to fix the load imbalances (in this
 context)?


 There is no way to limit PME to certain ranges.  It is a method for
 solving infinite sums.  Usually PME is a poor choice for in vacuo
 simulations and the like, since there's nothing to be done for most of the
 simulation box.  You may want to see how others (in the literature) deal
 with droplet-type simulations.

 -Justin


 Thanks for your help.

 Sapna

 On Tue, Aug 17, 2010 at 5:29 PM, Justin A. Lemkul jalem...@vt.edumailto:
 jalem...@vt.edu wrote:



sapna sarupria wrote:

Hi all,

I am running (NVT) simulations of a drop of water (~5 nm in
radius) in a big box (~25 nm) in a box and find that the
simulations are rather slow. I am getting about 0.8 ns per day
when a simulation of bulk system of equivalent number of waters
will be much faster. The number of waters is ~12000. I was
wondering if anyone can suggest methods with which I can speed
up the simulations. I am using domain decomposition and
optimize_fft is set to yes. PME is used for the electrostatics.


I would suspect that the lag comes from a lot of unused PME
calculations. During your run, PME grid points will be assigned to
vacuum space, for which nothing needs to be done.  You can check
imbalances and performance loss in the log file.

-Justin


Thank you

Sincerely
Sapna


-- 

Justin A. Lemkul
Ph.D. Candidate
ICTAS Doctoral Scholar
MILES-IGERT Trainee
Department of Biochemistry
Virginia Tech
Blacksburg, VA
jalemkul[at]vt.edu http://vt.edu | (540) 231-9080

http://www.bevanlab.biochem.vt.edu/Pages/Personal/justin


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 --
 Sapna Sarupria
 Post-doctoral Researcher
 Princeton University
 New Jersey 08540
 U.S.A.

 Life isn't about finding yourself. Life is about creating yourself. --
 George Bernard Shaw.
 Dare to Dream


 --
 

 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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 --
 Sapna Sarupria
 Post-doctoral Researcher
 Princeton University
 New Jersey 08540
 U.S.A.

 Life isn't about finding yourself. Life is about creating yourself. --
 George Bernard Shaw.
 Dare to Dream

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Re: [gmx-users] RE: log files

2010-08-12 Thread Gaurav Goel
On Wed, Aug 11, 2010 at 1:10 PM, Nimesh Jain 
nimeshjain2...@u.northwestern.edu wrote:

 Well, no. I got a 20GB log file when nstlog was 1000. When I changed it to
 1, the log file was about 1 MB after a few minutes of simulation which
 means that it will be in GBs in a few days.

 Did you re-compile using grompp after changing nstlog? Otherwise in md.tpr
(output of grompp), nstlog=1000.

-Gaurav


 On Wed, Aug 11, 2010 at 10:49 AM, Gaurav Goel gauravgoel...@gmail.comwrote:

 You've set the frequency of writing to log file as
 'nstlog   = 10'.
 Given that 'nsteps   = 1', you're writing to the
 log file only 1000 times. Do you get a 20GB md.log file with these settings?

 -Gaurav

 On Wed, Aug 11, 2010 at 10:52 AM, Nimesh Jain 
 nimeshjain2...@u.northwestern.edu wrote:

 Hi,

 I am having some problem in my simulations related to log files. The file
 sizes are enormous, its like after 3 days of simulation I had a 20 GB md.log
 file. One of my grompps looks like this:
 [tau_t is very low because I am using bd and it doesn't work otherwise].
 [I am doing a replica exchange with 10,000 as exchange frequency]


 include  =
 define   =
 integrator   = bd
 tinit= 0
 dt   = 0.001
 nsteps   = 1 ;10
 simulation_part  = 1
 init_step= 0
 comm-mode= Angular
 nstcomm  = 1
 comm-grps=


 emtol= 0.01
 emstep   = 1.5

 nstxout  = 1
 nstvout  = 1
 nstfout  = 1

 nstlog   = 10
 nstenergy= 1000

 nstxtcout= 1000
 xtc-precision= 1000

 xtc-grps =
 energygrps   =

 ns_type  = grid
 pbc  = xyz
 periodic_molecules   = no

 rlist= 8.95

 coulombtype  = user
 rcoulomb-switch  = 0
 rcoulomb = 8.95

 epsilon-r= 1

 vdw-type = user  ;cutoff
 rvdw-switch  = 0
 rvdw = 8.95
 DispCorr = No
 table-extension  = 1
 ; Seperate tables between energy group pairs
 energygrps   = A T G C P260 SA SB

 energygrp_table  = A A  A T  A G  A C  A P260  A SA  A SB  T T  T
 G  T C  T P260  T S
 A  T SB  G G  G C  G P260  G SA  G SB  C C  C P260  C SA  C SB  P260
 P260  P260 SA  P260 SB
 SA SA  SA SB  SB SB

 ; Spacing for the PME/PPPM FFT grid
 fourierspacing   = 0.10

 Tcoupl   = Nose-Hoover
 tc-grps  = System
 tau_t= 0.0001
 ref_t= 260.00

 Pcoupl   = No

 andersen_seed= 815131

 gen_vel  = yes
 gen_temp = 260.
 gen_seed = 1993

 ; ENERGY GROUP EXCLUSIONS
 ; Pairs of energy groups for which all non-bonded interactions are
 excluded
 energygrp_excl   =



 Please let me know if anyone knows whats the problem.

 Thanks,
 Nimesh

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 --
 Nimesh Jain
 Graduate Student
 Biomedical Engineering
 Northwestern University

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Re: [gmx-users] RE: log files

2010-08-11 Thread Gaurav Goel
You've set the frequency of writing to log file as 'nstlog
= 10'.
Given that 'nsteps   = 1', you're writing to the log
file only 1000 times. Do you get a 20GB md.log file with these settings?

-Gaurav

On Wed, Aug 11, 2010 at 10:52 AM, Nimesh Jain 
nimeshjain2...@u.northwestern.edu wrote:

 Hi,

 I am having some problem in my simulations related to log files. The file
 sizes are enormous, its like after 3 days of simulation I had a 20 GB md.log
 file. One of my grompps looks like this:
 [tau_t is very low because I am using bd and it doesn't work otherwise]. [I
 am doing a replica exchange with 10,000 as exchange frequency]


 include  =
 define   =
 integrator   = bd
 tinit= 0
 dt   = 0.001
 nsteps   = 1 ;10
 simulation_part  = 1
 init_step= 0
 comm-mode= Angular
 nstcomm  = 1
 comm-grps=


 emtol= 0.01
 emstep   = 1.5

 nstxout  = 1
 nstvout  = 1
 nstfout  = 1

 nstlog   = 10
 nstenergy= 1000

 nstxtcout= 1000
 xtc-precision= 1000

 xtc-grps =
 energygrps   =

 ns_type  = grid
 pbc  = xyz
 periodic_molecules   = no

 rlist= 8.95

 coulombtype  = user
 rcoulomb-switch  = 0
 rcoulomb = 8.95

 epsilon-r= 1

 vdw-type = user  ;cutoff
 rvdw-switch  = 0
 rvdw = 8.95
 DispCorr = No
 table-extension  = 1
 ; Seperate tables between energy group pairs
 energygrps   = A T G C P260 SA SB

 energygrp_table  = A A  A T  A G  A C  A P260  A SA  A SB  T T  T
 G  T C  T P260  T S
 A  T SB  G G  G C  G P260  G SA  G SB  C C  C P260  C SA  C SB  P260 P260
 P260 SA  P260 SB
 SA SA  SA SB  SB SB

 ; Spacing for the PME/PPPM FFT grid
 fourierspacing   = 0.10

 Tcoupl   = Nose-Hoover
 tc-grps  = System
 tau_t= 0.0001
 ref_t= 260.00

 Pcoupl   = No

 andersen_seed= 815131

 gen_vel  = yes
 gen_temp = 260.
 gen_seed = 1993

 ; ENERGY GROUP EXCLUSIONS
 ; Pairs of energy groups for which all non-bonded interactions are excluded
 energygrp_excl   =



 Please let me know if anyone knows whats the problem.

 Thanks,
 Nimesh

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Re: [gmx-users] Reduced Units

2010-08-10 Thread Gaurav Goel
On Mon, Aug 9, 2010 at 9:58 AM, poj...@icp.uni-stuttgart.de wrote:

 Hi,

 I want to use the pme algorithm in GROMACS. Thge size of my box is
 8.2x8.2x8.2 in reduced units. I am considering a collection of 1000
 of CO2 molecules. If I am using reduced units, the values of the
 parameters rcoulomb=0.9 I think should be converted to reduced
 units rcoulomb=2.45 (my \sigma=0.366nm). But my question is how
 can one convert the value of fourierspacing=0.12 to reduced units?


'fourierspacing' is also in units of length and it's value is used to
determine 'fourier_nx' etc., if the latter are set to zero. In that case,
fourier_nx=(box length along x)/fourierspacing. So for same level of PME
accuracy scale down 'fourierspacing' by sigma=0.366 also.






 (This script is in SI standard units)
 ; OPTIONS FOR ELECTROSTATICS AND VDW
 ; Method for doing electrostatics
 coulombtype  = pme
 rcoulomb-switch  = 0
 rcoulomb = 0.9
 ; Dielectric constant (DC) for cut-off or DC of reaction field
 epsilon-r= 1
 ; Method for doing Van der Waals
 vdw-type = Cut-off
 ; cut-off lengths
 rvdw-switch  = 0
 rvdw = 0.9
 ; Apply long range dispersion corrections for Energy and Pressure
 DispCorr = EnerPres
 ; Extension of the potential lookup tables beyond the cut-off
 table-extension  = 1
 ; 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= 4
 ewald_rtol   = 1e-05
 ewald_geometry   = 3d
 epsilon_surface  = 0
 optimize_fft = no


 Thanks.

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[gmx-users] does generating velocity keep centre of mass motion zero?

2010-07-30 Thread Gaurav Goel
I'm doing NVE simulations so I've set comm_mode=None. Now my questions is
regarding the generation of initial velocity with this-
gen_vel =  yes
gen_temp=  4000 ; initial temperature
gen_seed=  10234

The reason I do not want to use velocities from the end of my
pre-equilibrated simulation (a NPT simulations followed by NVT simulation to
get desired P,T) is to generate different trajectories by changing gen_seed.

Does the generation of velocities above keep the centre of mass motion zero?
It is important for me since comm_mode=None.

Thanks,
Gaurav
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Re: [gmx-users] extracting coordinates

2010-07-20 Thread Gaurav Goel
What do you want to do with the coordinates?

Look-up 'trjconv'

-Gaurav

On Tue, Jul 20, 2010 at 11:32 AM, Vishal Agarwal vishal.iit...@gmail.comwrote:

 Dear All,
 I am new to using GROMACS. I have done some NVT simulation on glucose
 molecule. Can one anyone tell me how to extract the coordinates of atoms for
 each frame from the output trajectory file.

 Thanks,
 Vishal

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Re: [gmx-users] g_msd

2010-07-12 Thread Gaurav Goel
On Mon, Jul 12, 2010 at 5:22 PM, Ricardo Cuya Guizado
rcu...@hotmail.com wrote:
 Dear gromacs users
 I make a MD of 20 ns of a solute in water
 With the g_msd program the msd vs the time was obtained
 In the plot, I observed a linear behaviour of the MSD from 0 to 15 ns and a
 plateau with no linear tendence at the last 5 ns arpoximately.
 In order to know if the observed plateau was due to the data or is due to
 the way as the algorithm process the data, I divided the MD in two
 trajectories and obtained the msd for each one.
 From 0-10ns, the plot observed shows a linear tendence en the begining and a
 plateau with no linear tendence from 9 to 10 ns.
 From 10-20 ns the plot observed was linear from 10 to 18 ns and not linear
 at the last, the same plateau was observed.
 Comparing the plots there are not equivalent,.
 Why g_msd produces a non linear plot at the last of the calculation and the
 plateau is ever produces.
 Somebody will explain the way as the g_msd algorithm work? and why the plot
 are no equivalent or why there must be equivalent?

I will explain how the g_msd algorithm works and hopefully that will
answer all your questions above. What you see in the output file is
average-MSD versus time. This average is done over all the particles
in the group you selected and over multiple time origins (this last
option can be selected with the -trestart parameter). Also, time in
column 1 is time difference from the start of your trajectory to
current time.

E.g., let's say you collected a trajectory over 5 time units and
choose -trestart=1 time unit and -dt=1 time unit.

dt=1 means you'll have 6 configurations for your analysis (including
the configuration at t=0).

trestart=1 means you'll have 5 distinct trajectories for your analysis:
Trajectory 1: 0-5
T2: 1-5
T3: 2-5
T4: 3-5
T5: 4-5

Now you can notice that all 5 trajectories contribute to the average
MSD after 1 time unit (T1-T5), 4 trajectories contribute to the
average MSD after 2 time units (T1-T4),  3 trajectories to the average
MSD after 3 time units (T1-T3), , and only one trajectory to the
MSD after 5 time units (T1). Of course, this assumes that trestart is
large enough that all all these trajectories are uncorrelated.

So, it's clear that longer the time interval at which you want to
evaluate the MSD lesser the number of trajectories used to evaluate
it...and hence, higher error in MSD values at longer times. That might
explain deviation from linear behaviour at long times.

However, you must be careful in interpreting the MSD data and I
recommend reading some literature on the subject. A plateau in MSD
versus time data might also signify what is called cage motion, in
which a particle or atom is trapped by the surrounding particles and
is not able to move out of that hole on the simulation time scale. If
you want you can send me your MSD versus time data along with some
information on your system (such as potentials, density, temperature
etc.) and I can let you know my comments.

Few words of caution:
Make sure that the center of mass of your particle (or atom or
molecule) is diffusing several particle diameters. Also, make sure
that you're calculating the self-diffusion coefficient  by fitting a
straight line to the linear region of MSD versus time data. You can
either modify the -beginfit and -endfit options... or calculate the
slope of the MSD versus time data using some other software (e.g.,
gnuplot, excel, etc.). If you're doing the latter you'll need to take
a look at the code in gmx_msd.c to know how the diffusion coefficent
is calculated from the slope of MSD versus time data (tog et correct
units, use proper scaling factors, etc.).

I hope that helped.

-Gaurav




 Regards
 Ricardo Cuya



 
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Re: [gmx-users] Problem with Lennard Jones cross terms

2010-07-01 Thread Gaurav Goel
By specifying both c6 and c12 to be zero, you've set both the attractive and
repulsive components of SI-OA, Si-CH2, Si-CH3 dispersion interactions to
zero. If you don't have any electrostatic repulsions in your system polymer
might be attracted to Silica substrate for entropic reasons...e.g.,
centers of  mass of Si and CH2 can overlap without any energy penalty.

One solution will be to fix c6, c12 for  SI-OA, Si-CH2, Si-CH3 to their
original values under *[ nonbond_params ] *and then do whatever you want to
do with the Si-Si interactions in [atomtypes].

-Gaurav

2010/7/1 xrysostomos sfhsdfghsdfhsdgh cbat...@yahoo.gr

 I am trying to simulate the following system: 5-layer FCC substrate
 consisting of Si particles which interact only with Lennard-Jones potential
 and vertical to the substrate I put polymer chains of (CH2-OA), starting
 from a distance of 0,4nm.

 What I want is to be able to manage completely independently the LJ
 interactions between the substrate and the polymers and not according to the
 combination rules, i.e. to have very very strong LJ interaction only between
 the Si particles but these to interact normally with the polymer chains.

 I use the Gromos-96 force-field. The initial values for the c6 and c12
 parameters are the following:

 *[ atomtypes ]*

 name  at.num   mass  charge  ptypec6
 c12

 OA  8  0.000  0.000 A 0.0022619536
 1.505529e-06

 CH26  0.000  0.000 A 0.0074684164
 3.3965584e-05

 SI140.000  0.000 A 0.01473796
 2.2193521e-05



 *[ nonbond_params ]*

 i   j  func  c6   c12

 SI   OA  1  0.000  0.

 SI  CH2 1  0.000  0.

 SI  CH3 1  0.000  0.



 What I did is to run 2 different simulations in NVT ensemble. In the *
 first*, I multiplied by 10 the c6, c12 values of Si in the [atomtypes ]  and
 in the *second* I multiplied (the initial values again) by 100. In both
 cases I didn’t change the values on the [nonbond_params ].

 I would expect that in both cases there should be no adsorption of the
 polymers in the substrate, since I  change the interaction between the
 substrate and the polymers in the [nonbond_params ] equal to zero.

 What I observed is that after 5 steps with 2 fs time step the polymers
 in the second case adsorbed to the surface.

 Can anybody help me or explain me why is this happening?



 Thanks in advance



 Chrysostomos


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Re: [gmx-users] Problem with Lennard Jones cross terms

2010-07-01 Thread Gaurav Goel
2010/7/1 xrysostomos sfhsdfghsdfhsdgh cbat...@yahoo.gr

 Dear Gaurav

 Thanks a lot for your quick reply

 I have done also what you suggested but the result is the same. I mean that
 I observe stronger adsorption of the polymers to the surface, when I
 increased the values of c6 and c12 for Si  in the [atomtypes], but
 continue having original values in the *[ nonbond_params ].*
 But in general, am I not able with gromacs to switch-off the LJ
 interactions between the polymers and the substrate?
 Is it possible to have this problems because I use NVT ensemble?


You can switch-off all non-bonded interactions between a pair of energy
groups by defining Energy group exclusions. Sec. 7.3.19 of the gromacs
manual 4.0.

-Gaurav


 Thanks again, Chrysostomos
 --- Στις *Πέμ., 01/07/10, ο/η Gaurav Goel gauravgoel...@gmail.com*έγραψε:


 Από: Gaurav Goel gauravgoel...@gmail.com
 Θέμα: Re: [gmx-users] Problem with Lennard Jones cross terms
 Προς: Discussion list for GROMACS users gmx-users@gromacs.org
 Ημερομηνία: Πέμπτη, 1 Ιούλιος 2010, 16:10


 By specifying both c6 and c12 to be zero, you've set both the attractive
 and repulsive components of SI-OA, Si-CH2, Si-CH3 dispersion interactions to
 zero. If you don't have any electrostatic repulsions in your system polymer
 might be attracted to Silica substrate for entropic reasons...e.g.,
 centers of  mass of Si and CH2 can overlap without any energy penalty.

 One solution will be to fix c6, c12 for  SI-OA, Si-CH2, Si-CH3 to their
 original values under *[ nonbond_params ] *and then do whatever you want
 to do with the Si-Si interactions in [atomtypes].

 -Gaurav

 2010/7/1 xrysostomos sfhsdfghsdfhsdgh 
 cbat...@yahoo.grhttp://mc/compose?to=cbat...@yahoo.gr
 

  I am trying to simulate the following system: 5-layer FCC substrate
 consisting of Si particles which interact only with Lennard-Jones potential
 and vertical to the substrate I put polymer chains of (CH2-OA), starting
 from a distance of 0,4nm.

 What I want is to be able to manage completely independently the LJ
 interactions between the substrate and the polymers and not according to the
 combination rules, i.e. to have very very strong LJ interaction only between
 the Si particles but these to interact normally with the polymer chains.

 I use the Gromos-96 force-field. The initial values for the c6 and c12
 parameters are the following:

 *[ atomtypes ]*

 name  at.num   mass  charge  ptypec6
c12

 OA  8  0.000  0.000 A 0.0022619536
 1.505529e-06

 CH26  0.000  0.000 A 0.0074684164
 3.3965584e-05

 SI140.000  0.000 A 0.01473796
2.2193521e-05



 *[ nonbond_params ]*

 i   j  func  c6   c12

 SI   OA  1  0.000  0.

 SI  CH2 1  0.000  0.

 SI  CH3 1  0.000  0.



 What I did is to run 2 different simulations in NVT ensemble. In the *
 first*, I multiplied by 10 the c6, c12 values of Si in the [atomtypes ]  and
 in the *second* I multiplied (the initial values again) by 100. In both
 cases I didn’t change the values on the [nonbond_params ].

 I would expect that in both cases there should be no adsorption of the
 polymers in the substrate, since I  change the interaction between the
 substrate and the polymers in the [nonbond_params ] equal to zero.

 What I observed is that after 5 steps with 2 fs time step the polymers
 in the second case adsorbed to the surface.

 Can anybody help me or explain me why is this happening?



 Thanks in advance



 Chrysostomos


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[gmx-users] Should I use separate PME nodes

2010-06-25 Thread Gaurav Goel
I ran my simulation in parallel on 4 nodes (with zero separate PME
nodes). Below is the information printed in md.log.

I see that PME-Mesh calculations took 60% of CPU time. Any
recommendations on using 1 or more separate PME nodes to speed up?


 Computing: M-Number M-Flops  % Flops
---
 Coul(T) + VdW(T) 1761401.496982   119775301.79520.2
 Outer nonbonded loop  106414.135764 1064141.358 0.2
 Calc Weights   32400.006480 1166400.233 0.2
 Spread Q Bspline 2332800.466560 4665600.933 0.8
 Gather F Bspline 2332800.46656027993605.599 4.7
 3D-FFT  47185929.437184   377487435.49763.6
 Solve PME 675840.13516843253768.651 7.3
 NS-Pairs  823453.92765617292532.481 2.9
 Reset In Box2160.0021606480.006 0.0
 CG-CoM  2160.0043206480.013 0.0
 Virial 11700.002340  210600.042 0.0
 Ext.ens. Update10800.002160  583200.117 0.1
 Stop-CM10800.002160  108000.022 0.0
 Calc-Ekin  10800.004320  291600.117 0.0
---
 Total 593905146.863   100.0
---

  R E A L   C Y C L E   A N D   T I M E   A C C O U N T I N G

 Computing: Nodes Number G-CyclesSeconds %
---
 Domain decomp. 4101 3859.416 1488.1 0.6
 Comm. coord.   4501 1874.635  722.8 0.3
 Neighbor search410178640.72230322.211.2
 Force  4501   180659.90269658.525.8
 Wait + Comm. F 4501 2578.994  994.4 0.4
 PME mesh   4501   422268.834   162817.760.4
 Write traj.4  10001   17.5266.8 0.0
 Update 4501 2981.794 1149.7 0.4
 Comm. energies 4501 2633.176 1015.3 0.4
 Rest   43580.341 1380.5 0.5
---
 Total  4  699095.342   269556.0   100.0
---

Thanks,
Gaurav
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Re: [gmx-users] vdwtype=shift

2010-06-24 Thread Gaurav Goel
section 7.3.11 of gromacs manual (v4.0)/

-Gaurav

On Thu, Jun 24, 2010 at 4:40 AM, Erik Marklund er...@xray.bmc.uu.se wrote:
 you zou skrev:

 Dear users,

 I have a question about vdwtype. My question is if I use vdwtype=shift in
 nvt.mdp file:

 ; Neighborsearching
 ns_type = grid ; search neighboring grid cels
 nstlist = 5 ; 10 fs
 rlist = 1.0 ; short-range neighborlist cutoff (in nm)
 rcoulomb = 1.0   ; short-range electrostatic cutoff (in nm)
 ; Method for doing Van der Waals
 vdwtype         = shift
 ; cut-off lengths       rvdw-switch              = 0
 rvdw                     = 0.9,

 I have this error:
 Fatal error:
 With dispersion correction rvdw-switch can not be zero for vdw-type =
 Shift

 That I don't know how can I solve this problem.

 Thank you
 
 Hotmail: Powerful Free email with security by Microsoft. Get it now.
 https://signup.live.com/signup.aspx?id=60969

 Errr... Setting rvdw-switch to a non-zero value might be worth trying.

 --
 ---
 Erik Marklund, PhD student
 Dept. of Cell and Molecular Biology, Uppsala University.
 Husargatan 3, Box 596,    75124 Uppsala, Sweden
 phone:    +46 18 471 4537        fax: +46 18 511 755
 er...@xray.bmc.uu.se    http://folding.bmc.uu.se/

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[gmx-users] problem install gromacs in parallel

2010-06-23 Thread Gaurav Goel
I'm trying to install a local copy of GROMACS on Ohio Super Computer.
I was able to build single and double precision versions (did make
distclean after each), however, got errors while installing parallel
version.

I will appreciate you taking time to help with this installation. Thanks.

This is what I did:

export CPPFLAGS=$FFTW_CFLAGS
export LDFLAGS=$FFTW_LIBS

contents of FFTW_CFLAGS=-I/usr/local/fftw3-3.1.2/include
fftw3.f  fftw3.h

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Re: [gmx-users] how small rcoulomb can be

2010-06-18 Thread Gaurav Goel
Thanks for your reply Mark.

On Wed, Jun 16, 2010 at 6:11 PM, Mark Abraham mark.abra...@anu.edu.au wrote:


 - Original Message -
 From: Gaurav Goel gauravgoel...@gmail.com
 Date: Thursday, June 17, 2010 5:21
 Subject: [gmx-users] how small rcoulomb can be
 To: Discussion list for GROMACS users gmx-users@gromacs.org

 For my NPT/NVT simulations I'm using a BKS potential for dispersion
 interactions (VdWtype=USER)  which has a cut-off of 0.55
 nm. I also
 set rcoulomb=rlist=0.55 nm.

 My first question is regarding the choice of rcoulomb=0.55nm. Any
 thoughts on whether this rcoulomb is large enough to ascertain that
 real space electrostatics interactions are fairly small (in comparison
 to total coulombic interactions)?

 That's around half the size of typical rcoulomb values used for PME, so
 you'll need to adjust ewald_rtol and fourier_spacing to a considerable
 degree in order that the electrostatics your PME model is comparably
 accurate. If this model has been used with PME in the past, then you will
 have some guidance in its literature (though GROMACS does not make it easy
 to choose beta directly). This will mean the reciprocal-space processors are
 doing lots more work than normal, and you'll want to set -npme to be half of
 -np, or maybe zero. Even so, your parallel scaling will be noticeably worse
 than normal PME.

Thanks for your reply Mark. Any thoughts on instead increasing
rcoulomb and rlist. Will that be more efficient and/or accurate rather
than trying to adjust ewald_rtol and fourier_spacing with a very short
rcoulomb? In literature I found that the optimal value people have
used for beta is, beta*L=10.

In my simulations, for rcoulomb=0.55, beta*L=15.52
 rcoulomb=0.9, beta*L=   9.49
How can I obtain the magnitude of maximum wave vector (i.e., 'm' in
Eq. 4.159 of manual 4.0)?

I have a separate question in regards to (conserved) energy drift in a
NVT simulation.

I first equilibrated my system for 1 ns in NPT ensemble. Then, I
turned-off the pressure coupling, further equilibrated my system for 1
ns In NVT ensemble [N=2160, V=20.43 nm^3, T=4000K; rcoulomb=rlist=0.9,
rvdw=0.55, nstlist=5]. Then in a production run of 3.5ns I get
following energy drifts:
Statistics over 3549897 steps [ 1000. thru 4549.8960 ps ], 1 data sets
All averages are exact over 3549897 steps

Energy  Average   RMSD Fluct.  Drift  Tot-Drift
---
Conserved En.-3.65264e+06  1893673.102718.4782
   65595.7

i.e. drift=0.16 kT/ns.

If nstlist=10, drift= 0.5kT/ns

Should I worry about these drifts?

-Gaurav


 Mark

 My second question is in regards to doing long (~15-100 ns) NVE
 simulations. It appears using coulombtype=PME-Switch will be the best
 option to accurately conserve energy. Any thoughts on how to choose
 rcoulomb_switch and rcoulomb?

 Thanks,
 Gaurav
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Re: [gmx-users] how small rcoulomb can be

2010-06-18 Thread Gaurav Goel
I will re-ask my question as it didn't come out right in previous
mail. Read below.

On Wed, Jun 16, 2010 at 6:11 PM, Mark Abraham mark.abra...@anu.edu.au wrote:


 - Original Message -
 From: Gaurav Goel gauravgoel...@gmail.com
 Date: Thursday, June 17, 2010 5:21
 Subject: [gmx-users] how small rcoulomb can be
 To: Discussion list for GROMACS users gmx-users@gromacs.org

 For my NPT/NVT simulations I'm using a BKS potential for dispersion
 interactions (VdWtype=USER)  which has a cut-off of 0.55
 nm. I also
 set rcoulomb=rlist=0.55 nm.

 My first question is regarding the choice of rcoulomb=0.55nm. Any
 thoughts on whether this rcoulomb is large enough to ascertain that
 real space electrostatics interactions are fairly small (in comparison
 to total coulombic interactions)?

 That's around half the size of typical rcoulomb values used for PME, so
 you'll need to adjust ewald_rtol and fourier_spacing to a considerable
 degree in order that the electrostatics your PME model is comparably
 accurate. If this model has been used with PME in the past, then you will
 have some guidance in its literature (though GROMACS does not make it easy
 to choose beta directly). This will mean the reciprocal-space processors are
 doing lots more work than normal, and you'll want to set -npme to be half of
 -np, or maybe zero. Even so, your parallel scaling will be noticeably worse
 than normal PME.

Thanks for your reply Mark. Any thoughts on instead increasing
rcoulomb and rlist. Will that be more efficient and/or accurate rather
than trying to adjust ewald_rtol and fourier_spacing with a very short
rcoulomb? In literature I found that the optimal value people have
used for beta is, beta*L=10.

In my simulations, for rcoulomb=0.55, beta*L=15.52
rcoulomb=0.9, beta*L=   9.49
How can I obtain the magnitude of maximum wave vector (i.e., 'm' in
Eq. 4.159 of manual 4.0)?

I have a separate question in regards to (conserved) energy drift in a
NVT simulation.

I first equilibrated my system for 1 ns in NPT ensemble. Then, I
turned-off the pressure coupling, further equilibrated my system for 1
ns In NVT ensemble [N=2160, V=20.43 nm^3, T=4000K; rcoulomb=rlist=0.9,
rvdw=0.55, nstlist=5]. Then in a production run of 3.5ns I get
following energy drifts:
Statistics over 3549897 steps [ 1000. thru 4549.8960 ps ], 1 data sets
All averages are exact over 3549897 steps

Energy  Average   RMSD Fluct.  Drift  Tot-Drift
---
Conserved En.-3.65264e+06  1893673.102718.4782
  65595.7

i.e. drift=0.16 kT/ns.

If nstlist=10, drift= 0.5kT/ns

Should I worry about these drifts?

-Gaurav

 Mark

 My second question is in regards to doing long (~15-100 ns) NVE
 simulations. It appears using coulombtype=PME-Switch will be the best
 option to accurately conserve energy. Any thoughts on how to choose
 rcoulomb_switch and rcoulomb?

 Thanks,
 Gaurav
 --
 gmx-users mailing list    gmx-users@gromacs.org
 http://lists.gromacs.org/mailman/listinfo/gmx-users
 Please search the archive at http://www.gromacs.org/search
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 Please don't post (un)subscribe requests to the list. Use the
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[gmx-users] how small rcoulomb can be

2010-06-16 Thread Gaurav Goel
For my NPT/NVT simulations I'm using a BKS potential for dispersion
interactions (VdWtype=USER)  which has a cut-off of 0.55 nm. I also
set rcoulomb=rlist=0.55 nm.

My first question is regarding the choice of rcoulomb=0.55nm. Any
thoughts on whether this rcoulomb is large enough to ascertain that
real space electrostatics interactions are fairly small (in comparison
to total coulombic interactions)?

My second question is in regards to doing long (~15-100 ns) NVE
simulations. It appears using coulombtype=PME-Switch will be the best
option to accurately conserve energy. Any thoughts on how to choose
rcoulomb_switch and rcoulomb?

Thanks,
Gaurav
-- 
gmx-users mailing listgmx-users@gromacs.org
http://lists.gromacs.org/mailman/listinfo/gmx-users
Please search the archive at http://www.gromacs.org/search before posting!
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Re: [gmx-users] enegry minimisation

2010-05-20 Thread Gaurav Goel
Can you try using g_rms to compare the difference between the
structures before and after EM.

-Gaurav

On Thu, May 20, 2010 at 7:53 AM, Justin A. Lemkul jalem...@vt.edu wrote:


 sonali dhindwal wrote:

 Hello Gaurav,
 Thanks for your reply,
 I did position restrained enegry minimisation, and used following .mdp
 file for the same

 title            =  protein
 cpp              =  /usr/bin/cpp ; the c pre-processor
 define           =  -DPOSRE
 constraints      =  none
 integrator       =  steep
 dt               =  0.002    ; ps !
 nsteps           =  1000
 nstlist          =  10
 ns_type          =  grid
 rlist            =  0.9
 coulombtype      =  PME
 rcoulomb         =  0.9
 rvdw             =  0.9
 fourierspacing   =  0.12
 fourier_nx       =  0
 fourier_ny       =  0
 fourier_nz       =  0
 pme_order        =  4
 ewald_rtol       =  1e-5
 optimize_fft     =  yes
 ;
 ;      Energy minimizing stuff
 ;
 emtol            =  1000.0
 emstep           =  0.01
 pbc            =  xyz

 I included define =  -DPOSRE, for restraining the atom postion,
 I used posre.itp  which was genertaed by pdb2gmx.

 Have I done it correctly, because after this also many of the beeta sheets
 have become short, forming loops.

 Well, you haven't properly defined position restraints.  The default
 (produced by pdb2gmx) requires define = -DPOSRES not -DPOSRE.  If you
 have for some reason modified the topology, then maybe your approach is
 correct, but otherwise your position restraints are not being applied.

 I also find it very curious that such substantial changes are taking place
 during a simple energy minimization.  Are you sure the effects you are
 seeing are not simply due to the visualization software you are using
 guessing the incorrect secondary structure type?  I have had that experience
 numerous times, especially in the case of beta-strands.  DSSP tells me that,
 geometrically, I have beta-strands, but the visualization software renders
 coil structures.

 In any case, large structural deviations during EM suggest something
 fundamentally wrong with the model.  Usually the changes in EM are small,
 since it is performed at 0 K.  Only huge forces would cause any sort of
 structural change.

 I also want to ask what is the meaning of fx fy and fz :


 Force constants (kJ mol^-1 nm^-2) in the x, y, and z directions.

 ; atom  type      fx      fy      fz
     1     1  1000  1000  1000
     5     1  1000  1000  1000
     6     1  1000  1000  1000
     7     1  1000  1000  1000
     8     1  1000  1000  1000
     9     1  1000  1000  1000
    11     1  1000  1000  1000
    12     1  1000  1000  1000
    15     1  1000  1000  1000
    18     1  1000  1000  1000
    19     1  1000  1000  1000
    20     1  1000  1000  1000
    21     1  1000  1000  1000
    22     1  1000  1000  1000
    23     1  1000  1000  1000

 which is there in posre.itp file, and if these should have value of 1000
 1000 1000 each ?


 These default values are typically quite sufficient to restrain the
 structure.

 -Justin

 Thanks in advance.
 --
 Sonali Dhindwal


 --- On *Wed, 19/5/10, Gaurav Goel /gauravgoel...@gmail.com/* wrote:


    From: Gaurav Goel gauravgoel...@gmail.com
    Subject: Re: [gmx-users] enegry minimisation
    To: sonali dhindwal sonali11dhind...@yahoo.co.in
    Date: Wednesday, 19 May, 2010, 8:39 PM

    For position restraints you need to do the following:

    1. define a name.itp file which looks like:

    ; In this topology include file, you will find position restraint
    ; entries for all the heavy atoms in your original pdb file.
    ; This means that all the protons which were added by pdb2gmx are
    ; not restrained.

    [ position_restraints ]
    ; atom type fx fy fz
    1 1 1000 1000 1000
    5 1 1000 1000 1000
    6 1 1000 1000 1000
    ...
    ...
    _
    1,5,6 etc. are the atom indices you want to restrain. section 4.3.1
    in manual.

    2. Add define = -Dname to your mdp file

    3. Add following lines to your topology file
    ; Include Position restraint file
    #ifdef name
    #include name.itp
    #endif

    4. compile and run.

    I'm sure you will find mroe information on position-restrain
    simulation on gmx-users archive.

    -Gaurav

    On Wed, May 19, 2010 at 10:26 AM, sonali dhindwal
    sonali11dhind...@yahoo.co.in
    /mc/compose?to=sonali11dhind...@yahoo.co.in wrote:

        Hello Gaurav,
        Can you please help me in suggesting where should I look for
        providing parameters to constrain the protein backbone and then
        do EM and then how to run a short MD simulation by constraining
        the protein backbone.
        Sorry to bother you, but as I am new to Gromacs, your help will
        be highly appreciable.
        Thanks in advance

        --
        Sonali Dhindwal


        --- On *Wed, 19/5/10, Gaurav Goel /gauravgoel...@gmail.com
        /mc/compose?to=gauravgoel...@gmail.com/* wrote:


            From: Gaurav Goel gauravgoel

Re: [gmx-users] enegry minimisation

2010-05-19 Thread Gaurav Goel
After adding water you can do energy minimization (EM) in two steps:

1. Constrain the protein backbone and do EM.
2. Now do EM on the full system.
3. Run a short MD simulation by constraining the protein backbone.
The above three steps will help hydrate the protein molecule with minimal
distortion of protein structure.

4. Now run a MD on full system.

for details looks here:
http://www.google.com/url?sa=tsource=webct=rescd=2ved=0CBcQFjABurl=http%3A%2F%2Feugen.leitl.org%2Fchem%2Fkerrigje%2Fpdf_files%2Ffwspidr_tutor.pdfei=jOPzS8a3Lab2MdX1_aAOusg=AFQjCNGB_3mXSQRHuqehBSHXsRyXP1Gymgsig2=bY3NqXHmruR7eSLVyAuCHQ

-Gaurav

On Wed, May 19, 2010 at 8:18 AM, sonali dhindwal 
sonali11dhind...@yahoo.co.in wrote:

 Sorry, but I couldnt get your question,
 I have used this .mdp file for energy minimisation after addition of water
 and using

 GROMOS96 43a1 force field :


 title= drg_trp
 cpp  = /lib/cpp ; location of cpp on SGI
 define   = -DFLEX_SPC ; Use Ferguson’s Flexible water model [4]
 constraints  = none
 integrator   = steep
 dt   = 0.002; ps !
 nsteps   = 2000
 nstlist  = 10
 ns_type  = grid
 rlist= 0.9
 coulombtype  = PME ; Use particle-mesh ewald
 rcoulomb = 0.9
 rvdw = 1.0
 fourierspacing   = 0.12
 fourier_nx =  0
 fourier_ny =  0
 fourier_nz =  0
 pme_order  =  4
 ewald_rtol =  1e-5
 optimize_fft  = yes
 ;
 ;   Energy minimizing stuff
 ;
 emtol   = 1000.0
 emstep  = 0.01

 I hope it will help you to guide me further
 Thanks
 --
 Sonali Dhindwal


 --- On *Wed, 19/5/10, Erik Marklund er...@xray.bmc.uu.se* wrote:


 From: Erik Marklund er...@xray.bmc.uu.se
 Subject: Re: [gmx-users] enegry minimisation
 To: Discussion list for GROMACS users gmx-users@gromacs.org
 Date: Wednesday, 19 May, 2010, 5:31 PM


 sonali dhindwal skrev:
  Hello All
  This question may sound trivial to many, but as i am new to this field,
 please help.
  I want to ask a question regarding my previous query of distortion of
 protein strucutre after molecular dynamcs simulation.
  I have noticed that after enegry minimisation using steepest decent
 algorithm, using emtol of 1000 kJ mol^-1 nm^-1 , large amount of distortion
 occurs.
  So is it necessary to do enegry minimisation step before MD, because this
 is my modeled protein, and i have  already done energy minimisation using
 different program and after that I have done refinement also.
  Thanks and regards
  ^
 
 
  --
  Sonali Dhindwal
 
 
 So how has your system setup changed since your previous EM? Addition of
 water? Cutoffs? PME?

 -- ---
 Erik Marklund, PhD student
 Dept. of Cell and Molecular Biology, Uppsala University.
 Husargatan 3, Box 596,75124 Uppsala, Sweden
 phone:+46 18 471 4537fax: +46 18 511 755
 er...@xray.bmc.uu.se http://mc/compose?to=er...@xray.bmc.uu.se
 http://folding.bmc.uu.se/

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Re: [gmx-users] enegry minimisation

2010-05-19 Thread Gaurav Goel
On Wed, May 19, 2010 at 9:18 AM, Justin A. Lemkul jalem...@vt.edu wrote:


 Gaurav Goel wrote:

 After adding water you can do energy minimization (EM) in two steps:

 1. Constrain the protein backbone and do EM.
 2. Now do EM on the full system.
 3. Run a short MD simulation by constraining the protein backbone.
 The above three steps will help hydrate the protein molecule with minimal
 distortion of protein structure.


 Such finesse may certainly be beneficial.  Just for clarity, though, what
 you are referring to is the application of (position) restraints, not
 constraints.

 http://www.gromacs.org/Documentation/Terminology/Constraints_and_Restraints

Justin, thanks for clarifying. I was referring to position restraints.
-Gaurav
 -Justin

 4. Now run a MD on full system.

 for details looks here:

 http://www.google.com/url?sa=tsource=webct=rescd=2ved=0CBcQFjABurl=http%3A%2F%2Feugen.leitl.org%2Fchem%2Fkerrigje%2Fpdf_files%2Ffwspidr_tutor.pdfei=jOPzS8a3Lab2MdX1_aAOusg=AFQjCNGB_3mXSQRHuqehBSHXsRyXP1Gymgsig2=bY3NqXHmruR7eSLVyAuCHQ
 http://www.google.com/url?sa=tsource=webct=rescd=2ved=0CBcQFjABurl=http%3A%2F%2Feugen.leitl.org%2Fchem%2Fkerrigje%2Fpdf_files%2Ffwspidr_tutor.pdfei=jOPzS8a3Lab2MdX1_aAOusg=AFQjCNGB_3mXSQRHuqehBSHXsRyXP1Gymgsig2=bY3NqXHmruR7eSLVyAuCHQ

 -Gaurav

 On Wed, May 19, 2010 at 8:18 AM, sonali dhindwal
 sonali11dhind...@yahoo.co.in mailto:sonali11dhind...@yahoo.co.in wrote:

    Sorry, but I couldnt get your question,
    I have used this .mdp file for energy minimisation after addition of
    water and using

    GROMOS96 43a1 force field :


    title            = drg_trp
    cpp              = /lib/cpp ; location of cpp on SGI
    define           = -DFLEX_SPC ; Use Ferguson’s Flexible water model [4]
    constraints      = none
    integrator       = steep
    dt               = 0.002    ; ps !
    nsteps           = 2000
    nstlist          = 10
    ns_type          = grid
    rlist            = 0.9
    coulombtype      = PME ; Use particle-mesh ewald
    rcoulomb         = 0.9
    rvdw             = 1.0
    fourierspacing   = 0.12
    fourier_nx     =  0
    fourier_ny     =  0
    fourier_nz     =  0
    pme_order      =  4
    ewald_rtol     =  1e-5
    optimize_fft      = yes
    ;
    ;       Energy minimizing stuff
    ;
    emtol               = 1000.0
    emstep              = 0.01

    I hope it will help you to guide me further
    Thanks
    --
    Sonali Dhindwal


    --- On *Wed, 19/5/10, Erik Marklund /er...@xray.bmc.uu.se
    mailto:er...@xray.bmc.uu.se/* wrote:


        From: Erik Marklund er...@xray.bmc.uu.se
        mailto:er...@xray.bmc.uu.se
        Subject: Re: [gmx-users] enegry minimisation
        To: Discussion list for GROMACS users gmx-users@gromacs.org
        mailto:gmx-users@gromacs.org
        Date: Wednesday, 19 May, 2010, 5:31 PM


        sonali dhindwal skrev:
          Hello All
          This question may sound trivial to many, but as i am new to
        this field, please help.
          I want to ask a question regarding my previous query of
        distortion of protein strucutre after molecular dynamcs simulation.
          I have noticed that after enegry minimisation using steepest
        decent algorithm, using emtol of 1000 kJ mol^-1 nm^-1 , large
        amount of distortion occurs.
          So is it necessary to do enegry minimisation step before MD,
        because this is my modeled protein, and i have  already done
        energy minimisation using different program and after that I
        have done refinement also.
          Thanks and regards
          ^
         
         
          --
          Sonali Dhindwal
         
         
        So how has your system setup changed since your previous EM?
        Addition of water? Cutoffs? PME?

        -- ---
        Erik Marklund, PhD student
        Dept. of Cell and Molecular Biology, Uppsala University.
        Husargatan 3, Box 596,    75124 Uppsala, Sweden
        phone:    +46 18 471 4537        fax: +46 18 511 755
        er...@xray.bmc.uu.se
        http://mc/compose?to=er...@xray.bmc.uu.se
 http://folding.bmc.uu.se/

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[gmx-users] reading velocity in the g_msd routine

2010-05-18 Thread Gaurav Goel
Hello gmx-users users :)

I am modifying the 'g_msd' utility to be able to calculate viscosities
using the corresponding Einstein relationship according to equation
3.14 in Helfand E., Physical Review, 119, 1, 1960. The equation is
similar to the mean-square displacement equation for self-diffusion
coefficient with the position vector 'r_i ' replaced by 'r_ix p_iy'
where p_iy is the particle momenta in y-direction.

So basically I need to be able to read both position and velocities
from the trajectory. Presently, gmx_msd.c uses 'read_first_x' and
'read_next_x' to read the coordinates. Can you please comment on how I
can modify this code to read the corresponding velocities?

Any help is greatly appreciated.

thanks,
Gaurav
-- 
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