Re: [gmx-users] Constant-Force Pulling of Ubiquitin

2013-10-29 Thread XAvier Periole

You want to switch to sd instead of md. 

 On Oct 29, 2013, at 17:43, Vivian ww...@bu.edu wrote:
 
 Hi GMX Users, 
 
 I am using Gromacs (Version 4.5.5) to do constant-force pulling of ubiquitin
 and it's a implicit model. My mdp file for pulling is shown as following. 
 
 integrator  =  md 
 dt  =  0.001; ps ! 
 nsteps  =  50 ; total 500 ps. 
 
 nstxout =  100 
 nstvout =  100 
 nstfout =  100 
 nstlist =  10 
 nstlog  =  100 
 nstcalcenergy=100 
 
 rlist   =  5 
 rvdw  =  5 
 rcoulomb = 5 
 coulombtype = cut-off 
 vdwtype = cut-off 
 table-extension =  5 
 bd_fric =  0 
 ld_seed =  -1 
 pbc =  no 
 ns_type =  simple 
 constraints = all-bonds 
 lincs_order = 4 
 lincs_iter  = 1 
 lincs-warnangle = 30 
 
 Tcoupl  = v-rescale 
 tau_t   = 1.0 
 tc-grps =  Protein 
 ref_t   =  300 
 
 Pcoupl  =  no 
 
 gen_vel =  yes 
 gen_temp=  300 
 gen_seed=  173529 
 
 comm_mode = Angular 
 nstcomm  =100 
 
 
 ; IMPLICIT SOLVENT ALGORITHM 
 implicit_solvent = gbsa 
 
 ; GENERALIZED BORN ELECTROSTATICS 
 ; Algorithm for calculating Born radii 
 gb_algorithm = Still 
 ; Frequency of calculating the Born radii inside rlist 
 nstgbradii   = 1 
 ; Cutoff for Born radii calculation; the contribution from atoms 
 ; between rlist and rgbradii is updated every nstlist steps 
 rgbradii = 5 
 ; Dielectric coefficient of the implicit solvent 
 gb_epsilon_solvent   = 80 
 ; Salt concentration in M for Generalized Born models 
 gb_saltconc  = 0 
 ; Scaling factors used in the OBC GB model. Default values are OBC(II) 
 gb_obc_alpha = 1 
 gb_obc_beta  = 0.8 
 gb_obc_gamma = 4.85 
 gb_dielectric_offset = 0.009 
 sa_algorithm = Ace-approximation 
 ; Surface tension (kJ/mol/nm^2) for the SA (nonpolar surface) part of GBSA 
 ; The value -1 will set default value for Still/HCT/OBC GB-models. 
 sa_surface_tension   = 2.05016 
 
 ; Pull code 
 pull= constant_force 
 ;Center of mass pulling using a linear potential and therefore a constant
 force. 
 pull_geometry   = direction 
 pull_start  = yes   ; define initial COM distance  0 
 pull_ngroups= 1 
 pull_group1 = Chain_B 
 pull_group0 = Chain_A 
 pull_k1 = -500  ; kJ mol^-1 nm^-2 
 pull_vec1 = 0.0 0.0 1.0 
 
 However, after pulling simulation, it turns out the potential of this system
 becomes lower rather than higher (from -1 to -2). It's very wired
 since potential should become larger after pulling. 
 Here is the notification after g_energy: 
 
 Energy  Average   Err.Est.   RMSD  Tot-Drift 
 ---
  
 Potential  -20734.52301268.47   -1385.71 
 (kJ/mol) 
 
 You may want to use the -driftcorr flag in order to correct for spurious
 drift in the graphs. Note that this is not 
 a substitute for proper equilibration and sampling! You should select the
 temperature in order to obtain fluctuation properties. 
 
 I wonder whether there is any problem with my mdp file. 
 Thank you so much!! 
 
 Best, 
 Vivian
 
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Re: [gmx-users] Is the website of Martini Force Field down for maintenance?

2013-10-17 Thread XAvier Periole

Try cgmartini.nl


On Oct 16, 2013, at 10:29 PM, 朱文鹏 jasonzhu...@gmail.com wrote:

 Dear GMX users,
 
 I am going to do some coarse-grained simulations in which the lipid
 bilayeris covered by
 polysarccharide. I remember the website of Martini Force Field (http://md
 .chem.rug.nl/cgmartini/) provides a database for sugar including .itp and .
 gro files of long chains of different polysarccharide.
 
 But I can not open the website now. Is it down for maintenance or changed
 to another address? Do you have these .itp and .gro files of
 polysarccharidefor Martini Force Field?
 
 Thank you very much for your help.
 
 Best,
 Jason
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Re: [gmx-users] default -rdd with distance restraints seems too large

2013-10-17 Thread XAvier Periole

Yes it is a pity! 

But particle decomposition helps :)) well helped! 

 
 It's a shame that long distance restraints limit the parallalization so much, 
 but it is understandable. Thanks for helping me with this.
 
 Chris.
 
 -- original message --
 
 Initializing Domain Decomposition on 8 nodes
 Dynamic load balancing: auto
 Will sort the charge groups at every domain (re)decomposition
 Initial maximum inter charge-group distances:
two-body bonded interactions: 2.636 nm, Dis. Rest., atoms 1701 4425
  multi-body bonded interactions: 0.479 nm, CMAP Dih., atoms 1062 1081
 Minimum cell size due to bonded interactions: 2.899 nm
 Maximum distance for 7 constraints, at 120 deg. angles, all-trans: 1.172 nm
 Estimated maximum distance required for P-LINCS: 1.172 nm
 Using 0 separate PME nodes, as there are too few total
 nodes for efficient splitting
 Scaling the initial minimum size with 1/0.8 (option -dds) = 1.25
 Optimizing the DD grid for 8 cells with a minimum initial size of 3.624 nm
 The maximum allowed number of cells is: X 1 Y 1 Z 2
 
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Re: [gmx-users] default -rdd with distance restraints seems too large

2013-10-17 Thread XAvier Periole

Hi Chris,

I mentioned that PS would have helped! I am sorry about the confusion. I should 
have been more clear. I guess you have not followed the particle decomposition 
threads lately :)) 

The PD option has been associated some serious issues lately … notably I 
noticed it does not work well in combination of REMD. Some info is not 
communicated correctly and thus a few variables are wrong. I forgot which ones 
… 

Most recently Floris (a PhD student with us in Groningen) has noticed that 
turning PD on would lead to severe buckling of a membrane to the point that the 
system would crash. The is happening quite fast. 

If you can use an older version of GMX (4.0.7) this would be fine but starting 
4.5.5 things are ugly :))

I hope this helps.

On Oct 17, 2013, at 5:57 PM, Christopher Neale chris.ne...@mail.utoronto.ca 
wrote:

 Thanks for the hint XAvier.
 
 Unfortunately, I get crashes with particle decomposition (see below). If I 
 use either DD or PD, I can run on up to 2 threads 
 without adjusting -rdd or -dds. I can only use 2 thread with DD if I set 
 -rdd 2.8. If I try to use more than 2 threads with PD, 
 I get lincs problems and immediate crashes. If I export GMX_MAXCONSTRWARN=-1 
 with the same setup , then I get a segfault immediately. 
 Note, however, that if I use constraints=none and set my timestep to 0.5 fs, 
 I can indeed use PD with 8 threads (without exporting GMX_MAXCONSTRWARN). 
 Also note that I am using the SD integrator, but I just tested and PD also 
 gives me an error with the md integrator.
 (( I don't think that the crashes have anything to do with improper setup. 
 These runs are fine in serial or in parallel as described 
 above and only ever explode/crash with PD and 2 threads, for which they do 
 so immediately )).
 
 Here is the error that I get when I 
 
 Step 0, time 0 (ps)  LINCS WARNING
 relative constraint deviation after LINCS: 
 rms 218.843810, max 8135.581543 (between atoms 15623 and 15624)
 bonds that rotated more than 30 degrees: 
 atom 1 atom 2  angle  previous, current, constraint length
  13908  13916   90.80.2130   0.8066  0.1538 
  13916  13917   90.30.2402   0.7979  0. 
  13916  13918   90.20.2403   0.8452  0.
  13916  13919   89.31.3408   0.9956  0.1430
 ...
 ...
  22587  22589   31.70.4648   0.1144  0.
  22587  22590   90.20.4168   0.1273  0.
 
 Wrote pdb files with previous and current coordinates
 starting mdrun 'Gallium Rubidium Oxygen Manganese Argon Carbon Silicon in 
 water'
 500 steps,  1.0 ps.
 
 WARNING: Listed nonbonded interaction between particles 13908 and 13920
 at distance 3f which is larger than the table limit 3f nm.
 
 This is likely either a 1,4 interaction, or a listed interaction inside
 a smaller molecule you are decoupling during a free energy calculation.
 Since interactions at distances beyond the table cannot be computed,
 they are skipped until they are inside the table limit again. You will
 only see this message once, even if it occurs for several interactions.
 
 IMPORTANT: This should not happen in a stable simulation, so there is
 probably something wrong with your system. Only change the table-extension
 distance in the mdp file if you are really sure that is the reason.
 
 
 
 step 0: Water molecule starting at atom 39302 can not be settled.
 Check for bad contacts and/or reduce the timestep if appropriate.
 
 step 0: Water molecule starting at atom 53072 can not be settled.
 Check for bad contacts and/or reduce the timestep if appropriate.
 
 Step 0, time 0 (ps)  LINCS WARNING
 relative constraint deviation after LINCS:
 rms 2569455308.447471, max 215672291328.00 (between atoms 14054 and 14055)
 bonds that rotated more than 30 degrees:
 atom 1 atom 2  angle  previous, current, constraint length
  13442  13444   90.00.   0.1147  0.
  13503  13506   40.80.1538   0.2002  0.1538
  13506  13507   45.20.   0.1541  0.
 ...
 ...
  19020  19023   89.80.1534 66420.9531  0.1530
 ;;dispcorr = EnerPres  ;; not using for CHARMM simulations
 
 
 ###
 
 mdp options:
 
 constraints = all-bonds
 lincs-iter =  1
 lincs-order =  6
 constraint_algorithm =  lincs
 integrator = sd
 dt = 0.002
 tinit = 0
 nsteps = 500
 nstcomm = 1
 nstxout = 500
 nstvout = 500
 nstfout = 500
 nstxtcout = 500
 nstenergy = 500
 nstlist = 10
 nstlog=0 ; reduce log file size
 ns_type = grid
 vdwtype = switch
 rlist = 1.2
 rlistlong = 1.3
 rvdw = 1.2
 rvdw-switch = 0.8
 rcoulomb = 1.2
 coulombtype = PME
 ewald-rtol = 1e-5
 optimize_fft = yes
 fourierspacing = 0.12
 fourier_nx = 0
 fourier_ny = 0
 fourier_nz = 0
 pme_order = 4
 tc_grps =  System   
 tau_t   =  1.0   
 ld_seed =  -1   
 ref_t = 310
 gen_temp = 310
 gen_vel = yes
 unconstrained_start = no
 gen_seed = -1
 Pcoupl = berendsen
 pcoupltype = 

Re: [gmx-users] recalculating .trr from .xtc

2013-10-15 Thread XAvier Periole

Interactions will be off, especially the bonded terms. 

 On Oct 15, 2013, at 7:21, Mark Abraham mark.j.abra...@gmail.com wrote:
 
 Also, the precision was selected when the xtc file was written, ie in the
 mdp file.
 
 Mark
 On Oct 15, 2013 3:24 AM, Justin Lemkul jalem...@vt.edu wrote:
 
 
 
 On 10/14/13 7:56 PM, Leandro Bortot wrote:
 
 Dear GROMACS users,
 
  Does anyone know how significant is the difference between the
 original .trr file from a simulation and a recalculated .trr from a
 whole system .xtc (mdrun -rerun traj.xtc -o traj.trr)?
  I mean... do you know how big would be the error induced by this
 recalculation procedure?
 
  I'm not interested in calculating autocorrelation functions. Most of
 my analysis are related to the atom positions over time and free energy
 calculations.
 Position-related quantities should be impacted very little.  Given that
 you can't acquire precision though, I see no point in even generating a
 .trr file - the .xtc has the same information while occupying less disk
 space.
 
 -Justin
 
 --
 ==**
 
 Justin A. Lemkul, Ph.D.
 Postdoctoral Fellow
 
 Department of Pharmaceutical Sciences
 School of Pharmacy
 Health Sciences Facility II, Room 601
 University of Maryland, Baltimore
 20 Penn St.
 Baltimore, MD 21201
 
 jalemkul@outerbanks.umaryland.**edu jalem...@outerbanks.umaryland.edu |
 (410) 706-7441
 
 ==**
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Re: [gmx-users] energy drift - comparison of double and single precision

2013-10-12 Thread XAvier Periole

Could you try to reduce the nstcalcenergy flag from 100 to 10 and then one?

 Similar flags apply to temperature and pressure and I believe might seriously 
affect energy conservation. 

XAvier. 

 On Oct 12, 2013, at 0:50, Mark Abraham mark.j.abra...@gmail.com wrote:
 
 Didn't see any problem in the .mdp. -4500 kJ/mol in 10ns over (guessing)
 30K atoms is 0.015 kJ/mol/ns/atom. k_B T is at least 100 times larger than
 that. I bet the rest of the lysozyme model physics is not accurate to less
 than 1% ;-) There are some comparative numbers at
 http://dx.doi.org/10.1016/j.cpc.2013.06.003 - the two systems are rather
 different but they share the use of SETTLE.
 
 Note that using md-vv guarantees the 2007 paper is inapplicable, because
 GROMACS did not have a velocity Verlet integrator back then. Sharing the
 .log files might be informative.
 
 Mark
 
 
 On Fri, Oct 11, 2013 at 11:38 PM, Guillaume Chevrot 
 guillaume.chev...@gmail.com wrote:
 
 Hi,
 
 sorry for my last post! I re-write my e-mail (with some additional
 information) and I provide the links to my files ;-)
 
 I compared the total energy of 2 simulations:
 lysozyme in water / NVE ensemble / single precision / Gromacs 4.6.3
 lysozyme in water / NVE ensemble / double precision / Gromacs 4.6.3
 
 ... and what I found was quite ... disturbing (see the plots of the total
 energy: http://dx.doi.org/10.6084/m9.figshare.820153). I observe a
 constant
 drift in energy in the case of the single precision simulation.
 
 Did I do something wrong*? Any remarks are welcomed! Here is the link to
 the ‘mdout.mdp’ file (http://dx.doi.org/10.6084/m9.figshare.820154) so you
 can check what mdp options I used.
 
 My second question is: if I did not do something wrong, what are the
 consequences on the simulation? Can I trust the results of single precision
 simulations?
 
 Regards,
 
 Guillaume
 
 *PS: I am not the only one encountering this behavior. In the literature,
 this problem has already been mentioned:
 http://jcp.aip.org/resource/1/jcpsa6/v126/i4/p046101_s1
 
 
 
 
 2013/10/11 Mark Abraham mark.j.abra...@gmail.com
 
 On Oct 11, 2013 7:59 PM, Guillaume Chevrot 
 guillaume.chev...@gmail.com
 wrote:
 
 Hi all,
 
 I recently compared the total energy of 2 simulations:
 lysozyme in water / NVE ensemble / single precision
 lysozyme in water / NVE ensemble / double precision
 
 ... and what I found was quite ... disturbing (see the attached figure
 -
 plots of the total energy). I observe a constant drift in energy in the
 case of the single precision simulation.
 
 Did I do something wrong*? Any remarks are welcomed! I join the
 ‘mdout.mdp’
 file so you can check what mdp options I used.
 
 Maybe. Unfortunately we cannot configure the mailing list to allow people
 to send attachments to thousands of people, so you will need to do
 something like provide links to files on a sharing service.
 
 
 My second question is: if I did not do something wrong, what are the
 consequences on the simulation? Can I trust the results of single
 precision
 simulations?
 
 Yes, as you have no doubt read in the papers published by the GROMACS
 team.
 
 Regards,
 
 Guillaume
 
 *PS: I am not the only one encountering this behavior. In the
 literature,
 this problem has already been mentioned:
 http://jcp.aip.org/resource/1/jcpsa6/v126/i4/p046101_s1
 
 ... which is six years old, examining the properties of code seven years
 old. Life has moved on! :-) Even if you have found a problem, it is a big
 assumption that this is (still) the cause.
 
 Mark
 
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Re: [gmx-users] Performance of Gromacs-4.6.1 on BlueGene/Q

2013-06-04 Thread XAvier Periole

BG CPUs are generally much slower (clock whose) but scale better.

You should try to run on 64 CPUs on the Blue gene too for faire comparison. 
The number of CPUs per nodes is also an important factor: the more CPUs per 
nodes the more communications needs to be done. I observed a significant slow 
down while going from 16 to 32 CPUs nodes (recent intel) but using the same 
number of CPUs.

On Jun 4, 2013, at 4:02 PM, Jianguo Li ljg...@yahoo.com.sg wrote:

 Dear All,
 
 
 Has anyone has Gromacs benchmark on Bluegene/Q? 
 I recently installed gromacs-461 on BG/Q using the following command:
 cmake .. -DCMAKE_TOOLCHAIN_FILE=BlueGeneQ-static-XL-C \
   -DGMX_BUILD_OWN_FFTW=ON \
  -DBUILD_SHARED_LIBS=OFF \
  -DGMX_XML=OFF \
  -DCMAKE_INSTALL_PREFIX=/scratch/home/biilijg/package/gromacs-461
 make
 make install
 
 After that, I did a benchmark simulation using a box of pure water containing 
 140k atoms. 
 The command I used for the above test is:
 srun --ntasks-per-node=32 --overcommit 
 /scratch/home/biilijg/package/gromacs-461/bin/mdrun -s box_md1.tpr -c 
 box_md1.gro -x box_md1.xtc -g md1.log  job_md1
 
 And I got the following performance:
 Num. cores   hour/ns
 128   9.860
 256  4.984
 512  2.706
 10241.544
 20480.978
 40920.677
 
 The scaling seems ok, but the performance is far from what I expected. In 
 terms CPU-to-CPU performance, the Bluegene is 8 times slower than other 
 clusters. For comparison, I also did the same simulation using 64 processors 
 in a SGI cluster, and I got 2.8 hour/ns, which is roughly equivalent to using 
 512 cores in BlueGene/Q. 
 
 I am wondering if the above benchmark results are reasonable or not? Or Am I 
 doing something wrong in compiling?
 Any comments/suggestions are appreciated, thank you very much!
 
 Have a nice day!
 Jianguo 
 
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Re: [gmx-users] Re: REMD analysis

2013-05-17 Thread XAvier Periole

Well use a regular plotting software and look at it or do some more elaborated 
operation in or out the software to estimate the overlap :))

On May 17, 2013, at 1:14 PM, bharat gupta bharat.85.m...@gmail.com wrote:

 Dear Sir,
 
 I ran the REMD simulation with temp. distribution discussed in my last
 thread. Each replica was run for 50 ns
 
 Replica exchange statistics
 Repl  24999 attempts, 12500 odd, 12499 even
 Repl  average probabilities:
 Repl 0123456789   10   11   12
 Repl  .22  .19  .18  .16  .19  .21  .23  .25  .26  .29  .28  .28
 Repl  number of exchanges:
 Repl 0123456789   10   11   12
 Repl 2661 2369 2296 2008 2360 2668 2866 3119 3234 3549 3469 3475
 Repl  average number of exchanges:
 Repl 0123456789   10   11   12
 Repl  .21  .19  .18  .16  .19  .21  .23  .25  .26  .28  .28  .28
 
 Now, how to find the potential energy overlap for each replica??.. I have
 obtained the pot. energy for each replica separately..
 
 -- 
 Bharat
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Re: [gmx-users] Re: REMD analysis

2013-05-17 Thread XAvier Periole

What do you not like in your distributions? What are your looking for in these 
distributions? 

I am not sure what you are expecting from the list here … your distributions 
are fine, but, as Mark noted, it does not mean your simulation and sampling 
will be optimal … 

On May 17, 2013, at 3:51 PM, bharat gupta bharat.85.m...@gmail.com wrote:

 Dear Sir,
 
 I tried plotting the PE overlap using the following way :-
 
 1. extract PE of each replica using g_energy
 2. get the PE distribution using g_analyze -f potential_0.xvg -dist pot0.xvg
 3. used xmgrace to plot all the PE distribution graphs together.
 
 The same thing I did for temperature distribution for each replica.
 
 Here's the file for both PE overlap (
 https://www.dropbox.com/s/895f1bi0hkuy884/pe_dist.png)
 temp distribution (https://www.dropbox.com/s/ed66uop16blgqwa/temp_dist.png)
 Is this the correct way ??
 
 
 But the plot doesnot look like this (
 https://www.dropbox.com/s/fsuabkl7zrydnib/sample%20PE%20overlap.jpg). Do i
 have to normalize the data and then plot in order to get a smooth plot like
 this one??
 
 
 Bharat
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Re: [Spam:*****] [gmx-users] REMD analysis

2013-05-16 Thread XAvier Periole

An acceptance ratio of 0.2/0.3 is normally best. The problem with high 
acceptance ratio is that it means that a large portion of the exchanges are 
just back and forth exchanges between consecutive exchange and are thus 
disturbing the system more that actually helping sampling. 

I do not know particularly the paper you mention but if you like what they do, 
it is your choice at the end. 

Why don;t you just increase the spacing between the replicas? You will need 
less replicas and potentially you could run two simulations instead of one and 
evaluate the convergence ...

On May 16, 2013, at 1:50 AM, bharat gupta bharat.85.m...@gmail.com wrote:

 The plots that I showed in my last mail were for all replicas. I tried
 plotting the first 500 ps of replica_index and replica_time files. I think
 the plots look fine, and there could be problem with the plotting tool .
 Here the link for both files ,
 https://www.dropbox.com/s/2g16mlxfsme4rx2/replica_temp.bmp
 https://www.dropbox.com/s/8jfs0b9whu6j7lo/replica_index.bmp
 
 Now regarding the high acceptance ratio which is 0.5 , I came across a
 paper (http://www.pnas.org/content/100/13/7587.full.pdf), here they have
 mentioned that their average acceptance ratio ranged between 30 to 80%. I
 have a question here, how did they calculate the range for the average
 acceptance ratio or is it average ratio for each replica . Actually, this
 is the reference I am following. I am also interested in peptide folding
 simulation, similar to this article.
 
 I want to know, whether the average acceptance ratio that I have got for my
 trial simulation is correct , together with the replica_temp and
 replica_remd plots. Can I proceed for large production runs to complete my
 experiment ??
 
 
 
 
 On Tue, May 14, 2013 at 6:34 PM, XAvier Periole x.peri...@rug.nl wrote:
 
 
 The interval between the exchange trial affect the efficiency of REMD but
 not the the exchange ratio (at least in principle).
 
 In you case I am not sure what the plot are showing! Are these showing all
 the replicas? what are the units?
 
 On May 14, 2013, at 5:07 AM, bharat gupta bharat.85.m...@gmail.com
 wrote:
 
 Dear Sir,
 
 Here's the result for the REMD trial with large temperature gaps.
 
 Temp. distribution : 280.0 294.9 310.7 327.3 344.7 363.1 382.5 402.9
 424.4
 447.1 471.0 496.1 522.6 550.5 579.9 610.8
 
 Out of md16.log :
 
 Replica exchange statistics
 Repl  249 attempts, 125 odd, 124 even
 Repl  average probabilities:
 Repl 0123456789   10   11   12
 13   14   15
 Repl  .40  .34  .38  .43  .43  .36  .45  .40  .37  .48  .47  .45  .47
 .44  .46
 
 Repl  number of exchanges:
 Repl 0123456789   10   11   12
 13   14   15
 Repl   50   42   46   52   57   40   58   49   42   53   61   63   56
 57   58
 
 Repl  average number of exchanges:
 Repl 0123456789   10   11   12
 13   14   15
 Repl  .40  .34  .37  .42  .46  .32  .46  .40  .34  .43  .49  .51  .45
 .46  .46
 Average acceptance ratio : 0.46
 
 But, the repli_index.xvg and replica_temp.xvg files still shows that the
 replicas does not exchange equally well .
 
 https://www.dropbox.com/s/zkbwpuj7l2o282b/replica_index.png
 https://www.dropbox.com/s/0c8gp584v1hvlbx/replica_temp.png
 
 what could be wrong in this case?? Is it the mdp file settings or
 implicit
 solvent setting. Does the time to replica to exhange also affects their
 swapping ??
 
 
 
 On Tue, May 14, 2013 at 12:24 AM, XAvier Periole x.peri...@rug.nl
 wrote:
 
 
 You need to increase the temperature gaps indeed if you want acceptance
 ratio ~0.2/0.3. But again this won't work with the water …
 
 It is not clear what happens in your index file but probably a problem
 from grace to plot so many points … you can try to increase the Max
 drawing path length in the preference menu of grace.
 
 On May 13, 2013, at 4:22 PM, bharat gupta bharat.85.m...@gmail.com
 wrote:
 
 Dear Sir,
 
 I repeated the simulation again for 25 replicas with the following
 temp.
 distribution .
 
 280
 289.1
 298.5
 308.2
 318.2
 328.6
 339.3
 350.3
 361.7
 373.5
 385.6
 398.1
 411.1
 424.4
 438.3
 452.5
 467.2
 482.4
 498.1
 514.3
 531.0
 548.3
 566.1
 584.5
 603.5
 623.2
 
 The output of md.log file is :-
 
 Replica exchange statistics
 Repl  24999 attempts, 12500 odd, 12499 even
 Repl  average probabilities:
 Repl 0123456789   10   11   12
 13   14   15   16   17   18   19   20   21   22   23   24   25
 Repl  .63  .63  .62  .62  .61  .61  .60  .60  .59  .59  .58  .59
 .59
 .60  .60  .61  .62  .62  .63  .64  .64  .65  .65  .66  .66
 
 Repl  number of exchanges:
 Repl 0123456789   10   11   12
 13   14   15   16   17   18   19   20   21   22   23   24   25
 Repl 7822 7752 7816 7760 7639 7628 7511 7442 7375 7332 7312 7424
 7408
 7410 7522 7559 7684 7697 7878 7927 7917 8073 8151 8208 8266

Re: [Spam:*****] [gmx-users] REMD analysis

2013-05-16 Thread XAvier Periole

You have to convince yourself, not me :)) But I can give you my opinion … 

On May 16, 2013, at 10:33 AM, bharat gupta bharat.85.m...@gmail.com wrote:

 Okay Sir, I will try two-three combinations this time and will report back
 to you ...
 
 
 On Thu, May 16, 2013 at 5:25 PM, XAvier Periole x.peri...@rug.nl wrote:
 
 
 An acceptance ratio of 0.2/0.3 is normally best. The problem with high
 acceptance ratio is that it means that a large portion of the exchanges are
 just back and forth exchanges between consecutive exchange and are thus
 disturbing the system more that actually helping sampling.
 
 I do not know particularly the paper you mention but if you like what they
 do, it is your choice at the end.
 
 Why don;t you just increase the spacing between the replicas? You will
 need less replicas and potentially you could run two simulations instead of
 one and evaluate the convergence ...
 
 On May 16, 2013, at 1:50 AM, bharat gupta bharat.85.m...@gmail.com
 wrote:
 
 The plots that I showed in my last mail were for all replicas. I tried
 plotting the first 500 ps of replica_index and replica_time files. I
 think
 the plots look fine, and there could be problem with the plotting tool .
 Here the link for both files ,
 https://www.dropbox.com/s/2g16mlxfsme4rx2/replica_temp.bmp
 https://www.dropbox.com/s/8jfs0b9whu6j7lo/replica_index.bmp
 
 Now regarding the high acceptance ratio which is 0.5 , I came across a
 paper (http://www.pnas.org/content/100/13/7587.full.pdf), here they have
 mentioned that their average acceptance ratio ranged between 30 to 80%. I
 have a question here, how did they calculate the range for the average
 acceptance ratio or is it average ratio for each replica . Actually, this
 is the reference I am following. I am also interested in peptide folding
 simulation, similar to this article.
 
 I want to know, whether the average acceptance ratio that I have got for
 my
 trial simulation is correct , together with the replica_temp and
 replica_remd plots. Can I proceed for large production runs to complete
 my
 experiment ??
 
 
 
 
 On Tue, May 14, 2013 at 6:34 PM, XAvier Periole x.peri...@rug.nl
 wrote:
 
 
 The interval between the exchange trial affect the efficiency of REMD
 but
 not the the exchange ratio (at least in principle).
 
 In you case I am not sure what the plot are showing! Are these showing
 all
 the replicas? what are the units?
 
 On May 14, 2013, at 5:07 AM, bharat gupta bharat.85.m...@gmail.com
 wrote:
 
 Dear Sir,
 
 Here's the result for the REMD trial with large temperature gaps.
 
 Temp. distribution : 280.0 294.9 310.7 327.3 344.7 363.1 382.5 402.9
 424.4
 447.1 471.0 496.1 522.6 550.5 579.9 610.8
 
 Out of md16.log :
 
 Replica exchange statistics
 Repl  249 attempts, 125 odd, 124 even
 Repl  average probabilities:
 Repl 0123456789   10   11   12
 13   14   15
 Repl  .40  .34  .38  .43  .43  .36  .45  .40  .37  .48  .47  .45
 .47
 .44  .46
 
 Repl  number of exchanges:
 Repl 0123456789   10   11   12
 13   14   15
 Repl   50   42   46   52   57   40   58   49   42   53   61   63
 56
 57   58
 
 Repl  average number of exchanges:
 Repl 0123456789   10   11   12
 13   14   15
 Repl  .40  .34  .37  .42  .46  .32  .46  .40  .34  .43  .49  .51
 .45
 .46  .46
 Average acceptance ratio : 0.46
 
 But, the repli_index.xvg and replica_temp.xvg files still shows that
 the
 replicas does not exchange equally well .
 
 https://www.dropbox.com/s/zkbwpuj7l2o282b/replica_index.png
 https://www.dropbox.com/s/0c8gp584v1hvlbx/replica_temp.png
 
 what could be wrong in this case?? Is it the mdp file settings or
 implicit
 solvent setting. Does the time to replica to exhange also affects their
 swapping ??
 
 
 
 On Tue, May 14, 2013 at 12:24 AM, XAvier Periole x.peri...@rug.nl
 wrote:
 
 
 You need to increase the temperature gaps indeed if you want
 acceptance
 ratio ~0.2/0.3. But again this won't work with the water …
 
 It is not clear what happens in your index file but probably a problem
 from grace to plot so many points … you can try to increase the Max
 drawing path length in the preference menu of grace.
 
 On May 13, 2013, at 4:22 PM, bharat gupta bharat.85.m...@gmail.com
 wrote:
 
 Dear Sir,
 
 I repeated the simulation again for 25 replicas with the following
 temp.
 distribution .
 
 280
 289.1
 298.5
 308.2
 318.2
 328.6
 339.3
 350.3
 361.7
 373.5
 385.6
 398.1
 411.1
 424.4
 438.3
 452.5
 467.2
 482.4
 498.1
 514.3
 531.0
 548.3
 566.1
 584.5
 603.5
 623.2
 
 The output of md.log file is :-
 
 Replica exchange statistics
 Repl  24999 attempts, 12500 odd, 12499 even
 Repl  average probabilities:
 Repl 0123456789   10   11
 12
 13   14   15   16   17   18   19   20   21   22   23   24   25
 Repl  .63  .63  .62  .62  .61  .61  .60  .60  .59  .59  .58  .59
 .59
 .60  .60  .61  .62  .62  .63

Re: [gmx-users] REMD analysis

2013-05-16 Thread XAvier Periole

Indeed the Repeat-3 seems good. But I would guess you did not run too long, 
right! That would explain the distribution of values!

On May 16, 2013, at 2:04 PM, bharat gupta bharat.85.m...@gmail.com wrote:

 Dear Sir,
 
 Here's the result of three different runs :
 
 Temperature distribution for three trials
 
 Repeat-1  280 298 317 337 359 382 406 432 460 489 520 554 589 627
 Repeat-2  280 299 319 340 363 388 414 441 471 503 536 572 611
 Repeat-3  280 300 322 345 370 397 426 457 490 526 564 605 649
 
 md.log files output from three different trials:
 
 Repeat-1  .37  .28  .26  .30  .25  .29  .32  .35  .32  .35  .36  .32  .31
 Repeat-2  .30  .33  .30  .25  .19  .27  .30  .31  .27  .40  .34  .31
 Repeat-3  .18  .22  .26  .34  .26  .28  .25  .27  .27  .25  .27  .22
 
 I think as the required acceptance value all the three trials are fine, but
 trail 3 would be much better to continue the further runs and anlysis ??
 
 So, is it fine to continue with the third simulation ?? But still the
 problem is that I am not getting the exact graphs with xmgrace??
 
 
 On Thu, May 16, 2013 at 5:36 PM, XAvier Periole x.peri...@rug.nl wrote:
 
 
 You have to convince yourself, not me :)) But I can give you my opinion …
 
 On May 16, 2013, at 10:33 AM, bharat gupta bharat.85.m...@gmail.com
 wrote:
 
 Okay Sir, I will try two-three combinations this time and will report
 back
 to you ...
 
 
 On Thu, May 16, 2013 at 5:25 PM, XAvier Periole x.peri...@rug.nl
 wrote:
 
 
 An acceptance ratio of 0.2/0.3 is normally best. The problem with high
 acceptance ratio is that it means that a large portion of the exchanges
 are
 just back and forth exchanges between consecutive exchange and are thus
 disturbing the system more that actually helping sampling.
 
 I do not know particularly the paper you mention but if you like what
 they
 do, it is your choice at the end.
 
 Why don;t you just increase the spacing between the replicas? You will
 need less replicas and potentially you could run two simulations
 instead of
 one and evaluate the convergence ...
 
 On May 16, 2013, at 1:50 AM, bharat gupta bharat.85.m...@gmail.com
 wrote:
 
 The plots that I showed in my last mail were for all replicas. I tried
 plotting the first 500 ps of replica_index and replica_time files. I
 think
 the plots look fine, and there could be problem with the plotting tool
 .
 Here the link for both files ,
 https://www.dropbox.com/s/2g16mlxfsme4rx2/replica_temp.bmp
 https://www.dropbox.com/s/8jfs0b9whu6j7lo/replica_index.bmp
 
 Now regarding the high acceptance ratio which is 0.5 , I came across a
 paper (http://www.pnas.org/content/100/13/7587.full.pdf), here they
 have
 mentioned that their average acceptance ratio ranged between 30 to
 80%. I
 have a question here, how did they calculate the range for the average
 acceptance ratio or is it average ratio for each replica . Actually,
 this
 is the reference I am following. I am also interested in peptide
 folding
 simulation, similar to this article.
 
 I want to know, whether the average acceptance ratio that I have got
 for
 my
 trial simulation is correct , together with the replica_temp and
 replica_remd plots. Can I proceed for large production runs to complete
 my
 experiment ??
 
 
 
 
 On Tue, May 14, 2013 at 6:34 PM, XAvier Periole x.peri...@rug.nl
 wrote:
 
 
 The interval between the exchange trial affect the efficiency of REMD
 but
 not the the exchange ratio (at least in principle).
 
 In you case I am not sure what the plot are showing! Are these showing
 all
 the replicas? what are the units?
 
 On May 14, 2013, at 5:07 AM, bharat gupta bharat.85.m...@gmail.com
 wrote:
 
 Dear Sir,
 
 Here's the result for the REMD trial with large temperature gaps.
 
 Temp. distribution : 280.0 294.9 310.7 327.3 344.7 363.1 382.5 402.9
 424.4
 447.1 471.0 496.1 522.6 550.5 579.9 610.8
 
 Out of md16.log :
 
 Replica exchange statistics
 Repl  249 attempts, 125 odd, 124 even
 Repl  average probabilities:
 Repl 0123456789   10   11
 12
 13   14   15
 Repl  .40  .34  .38  .43  .43  .36  .45  .40  .37  .48  .47  .45
 .47
 .44  .46
 
 Repl  number of exchanges:
 Repl 0123456789   10   11
 12
 13   14   15
 Repl   50   42   46   52   57   40   58   49   42   53   61   63
 56
 57   58
 
 Repl  average number of exchanges:
 Repl 0123456789   10   11
 12
 13   14   15
 Repl  .40  .34  .37  .42  .46  .32  .46  .40  .34  .43  .49  .51
 .45
 .46  .46
 Average acceptance ratio : 0.46
 
 But, the repli_index.xvg and replica_temp.xvg files still shows that
 the
 replicas does not exchange equally well .
 
 https://www.dropbox.com/s/zkbwpuj7l2o282b/replica_index.png
 https://www.dropbox.com/s/0c8gp584v1hvlbx/replica_temp.png
 
 what could be wrong in this case?? Is it the mdp file settings or
 implicit
 solvent setting. Does the time to replica to exhange also affects
 their
 swapping

Re: [gmx-users] point in source code to access atom position

2013-05-16 Thread XAvier Periole

Do you need it in the code? g_traj would help you do that on the trajectory.

On May 17, 2013, at 3:17 AM, Sikandar Mashayak symasha...@gmail.com wrote:

 Hi
 
 I want to store Z coordinates of atoms at the beginning of each time step
 when I am doing 'mdrun -rerun'. I am not able to find the line and file in
 the source code where I can implement this. Can anyone please help me with
 that?
 
 Thanks
 Sikandar
 -- 
 gmx-users mailing listgmx-users@gromacs.org
 http://lists.gromacs.org/mailman/listinfo/gmx-users
 * Please search the archive at 
 http://www.gromacs.org/Support/Mailing_Lists/Search before posting!
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Re: [gmx-users] Large number of solvent molecules

2013-05-14 Thread XAvier Periole

Well, a linear 80aa peptide will need that much water anyways! 

The question is more how relevant and realistic is such a structure and how 
long the peptide is going to keep it? You could resolvate it after some time, 
reducing the box, you could also start by a vacuo simulation to help colapse 
your peptide. 

But the chance to actually observe folding of such a peptide from a single MD 
simulation is about zero. Even using enhance sampling the chance is about zero 
unless you get some large access to supercomputers. See DE Shaw papers on 
folding. 

On May 14, 2013, at 9:44, Erik Marklund er...@xray.bmc.uu.se wrote:

 Hi,
 
 Have a look at the following article. It describes a non-standard box type 
 that seems ideal for your application. I don't know what is the latest 
 gromacs version where it is implemented, however.
 
 Author = {Wassenaar, TA and Mark, AE},
 Title = {{The effect of box shape on the dynamic properties of proteins 
 simulated
   under periodic boundary conditions}},
 Journal = {{JOURNAL OF COMPUTATIONAL CHEMISTRY}},
 Year = {{2006}},
 Volume = {{27}},
 Number = {{3}},
 Pages = {{316-325}},
 
 
 On 14 May 2013, at 07:44, Nikunj Maheshwari nixcrazyfor...@gmail.com wrote:
 
 Thank you Dr. Dallas. Yes I think the issue is that the starting
 conformation is linear, as I want to study its folding properties. I tried
 the same with helical starting conformation, and got around 11 water
 molecules, which is still ok.
 I am trying to find a way to simulate a 89 aa peptide in linear starting
 conformation such that the simulation is practically feasible.
 
 On Tue, May 14, 2013 at 10:45 AM, Dallas Warren 
 dallas.war...@monash.eduwrote:
 
 From the box volume printed in the script output it appears you have a
 box that is approximately a 28nm cube.  And that size box requires a
 significant number of water molecules to fill up, so that number you have
 in there (~770,000) seems about correct.
 
 If you want to have less water molecules, then you will need to make the
 simulation cell smaller.  Whether that is possible or not depends on what
 you are looking to observe, how big the molecule you are solvating is etc.
 
 Catch ya,
 
 Dr. Dallas Warren
 Drug Discovery Biology
 Monash Institute of Pharmaceutical Sciences, Monash University
 381 Royal Parade, Parkville VIC 3052
 dallas.war...@monash.edu
 +61 3 9903 9304
 -
 When the only tool you own is a hammer, every problem begins to resemble a
 nail.
 
 
 -Original Message-
 From: gmx-users-boun...@gromacs.org [mailto:gmx-users-
 boun...@gromacs.org] On Behalf Of Nikunj Maheshwari
 Sent: Tuesday, 14 May 2013 3:04 PM
 To: Discussion list for GROMACS users
 Subject: [gmx-users] Large number of solvent molecules
 
 Dear all,
 
 I am trying to see the folding of a 89 aa peptide. So I am setting up
 the
 system from linear conformation.
 I gave the following commands to build the box and add the solvent
 molecules.
 
 editconf -f output.gro -c -d 1.0 -bt dodecahedron -o outbox.gro
 
 genbox -cp outbox.gro -cs spc216.gro -p topol.top -o outh2o.gro
 
 Reading solute configuration
 Go Rough, Oppose Many Angry Chinese Serial killers
 Containing 1440 atoms in 89 residues
 Initialising van der waals distances...
 
 WARNING: Masses and atomic (Van der Waals) radii will be guessed
based on residue and atom names, since they could not be
definitively assigned from the information in your input
files. These guessed numbers might deviate from the mass
and radius of the atom type. Please check the output
files if necessary.
 
 Reading solvent configuration
 216H2O,WATJP01,SPC216,SPC-
 MODEL,300K,BOX(M)=1.86206NM,WFVG,MAR. 1984
 solvent configuration contains 648 atoms in 216 residues
 
 Initialising van der waals distances...
 Will generate new solvent configuration of 18x18x13 boxes
 Generating configuration
 Sorting configuration
 Found 1 molecule type:
   SOL (   3 atoms): 909792 residues
 Calculating Overlap...
 box_margin = 0.315
 Removed 324522 atoms that were outside the box
 Neighborsearching with a cut-off of 0.48
 Table routines are used for coulomb: FALSE
 Table routines are used for vdw: FALSE
 Cut-off's:   NS: 0.48   Coulomb: 0.48   LJ: 0.48
 System total charge: 0.000
 Grid: 73 x 73 x 51 cells
 Successfully made neighbourlist
 nri = 3007232, nrj = 82473964
 Checking Protein-Solvent overlap: tested 36005 pairs, removed 1653
 atoms.
 Checking Solvent-Solvent overlap: tested 7152003 pairs, removed 73182
 atoms.
 Added 776673 molecules
 Generated solvent containing 2330019 atoms in 776673 residues
 Writing generated configuration to outh2o.gro
 
 Back Off! I just backed up outh2o.gro to ./#outh2o.gro.1#
 Go Rough, Oppose Many Angry Chinese Serial killers
 
 Output configuration contains 2331459 atoms in 776762 residues
 Volume : 23276.3 (nm^3)
 Density: 1001.32 (g/l)
 Number of SOL molecules:  776673
 
 Processing topology
 

Re: [Spam:*****] [gmx-users] REMD analysis

2013-05-14 Thread XAvier Periole

The interval between the exchange trial affect the efficiency of REMD but not 
the the exchange ratio (at least in principle).

In you case I am not sure what the plot are showing! Are these showing all the 
replicas? what are the units? 

On May 14, 2013, at 5:07 AM, bharat gupta bharat.85.m...@gmail.com wrote:

 Dear Sir,
 
 Here's the result for the REMD trial with large temperature gaps.
 
 Temp. distribution : 280.0 294.9 310.7 327.3 344.7 363.1 382.5 402.9 424.4
 447.1 471.0 496.1 522.6 550.5 579.9 610.8
 
 Out of md16.log :
 
 Replica exchange statistics
 Repl  249 attempts, 125 odd, 124 even
 Repl  average probabilities:
 Repl 0123456789   10   11   12
 13   14   15
 Repl  .40  .34  .38  .43  .43  .36  .45  .40  .37  .48  .47  .45  .47
 .44  .46
 
 Repl  number of exchanges:
 Repl 0123456789   10   11   12
 13   14   15
 Repl   50   42   46   52   57   40   58   49   42   53   61   63   56
 57   58
 
 Repl  average number of exchanges:
 Repl 0123456789   10   11   12
 13   14   15
 Repl  .40  .34  .37  .42  .46  .32  .46  .40  .34  .43  .49  .51  .45
 .46  .46
 Average acceptance ratio : 0.46
 
 But, the repli_index.xvg and replica_temp.xvg files still shows that the
 replicas does not exchange equally well .
 
 https://www.dropbox.com/s/zkbwpuj7l2o282b/replica_index.png
 https://www.dropbox.com/s/0c8gp584v1hvlbx/replica_temp.png
 
 what could be wrong in this case?? Is it the mdp file settings or implicit
 solvent setting. Does the time to replica to exhange also affects their
 swapping ??
 
 
 
 On Tue, May 14, 2013 at 12:24 AM, XAvier Periole x.peri...@rug.nl wrote:
 
 
 You need to increase the temperature gaps indeed if you want acceptance
 ratio ~0.2/0.3. But again this won't work with the water …
 
 It is not clear what happens in your index file but probably a problem
 from grace to plot so many points … you can try to increase the Max
 drawing path length in the preference menu of grace.
 
 On May 13, 2013, at 4:22 PM, bharat gupta bharat.85.m...@gmail.com
 wrote:
 
 Dear Sir,
 
 I repeated the simulation again for 25 replicas with the following temp.
 distribution .
 
 280
 289.1
 298.5
 308.2
 318.2
 328.6
 339.3
 350.3
 361.7
 373.5
 385.6
 398.1
 411.1
 424.4
 438.3
 452.5
 467.2
 482.4
 498.1
 514.3
 531.0
 548.3
 566.1
 584.5
 603.5
 623.2
 
 The output of md.log file is :-
 
 Replica exchange statistics
 Repl  24999 attempts, 12500 odd, 12499 even
 Repl  average probabilities:
 Repl 0123456789   10   11   12
 13   14   15   16   17   18   19   20   21   22   23   24   25
 Repl  .63  .63  .62  .62  .61  .61  .60  .60  .59  .59  .58  .59  .59
 .60  .60  .61  .62  .62  .63  .64  .64  .65  .65  .66  .66
 
 Repl  number of exchanges:
 Repl 0123456789   10   11   12
 13   14   15   16   17   18   19   20   21   22   23   24   25
 Repl 7822 7752 7816 7760 7639 7628 7511 7442 7375 7332 7312 7424 7408
 7410 7522 7559 7684 7697 7878 7927 7917 8073 8151 8208 8266
 
 Repl  average number of exchanges:
 Repl 0123456789   10   11   12
 13   14   15   16   17   18   19   20   21   22   23   24   25
 Repl  .63  .62  .63  .62  .61  .61  .60  .60  .59  .59  .58  .59  .59
 .59  .60  .60  .61  .62  .63  .63  .63  .65  .65  .66  .66
 
 The average acceptance ration is around 0.6 which is still high.
 
 The link for replica_temp,replica_index :
 https://www.dropbox.com/s/c7soajnwc3uww8j/replica_temp.png
 https://www.dropbox.com/s/wvx82m4c6cnsfit/replica_index.png
 
 The temp files look better but the index file looks weird ...
 
 Do i need to experiment with the gap difference in order to get the
 required ration of 0.2-0.3 ?? There is some problem with the .mdp file
 settings??
 
 --
 Bharat
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Re: [gmx-users] Issue running gromacs in Cluster

2013-05-13 Thread XAvier Periole

You may have created large files and thus got out of quota on the disc. 

Check your quota and consider reducing the frequency of saving coordinates. 

On May 13, 2013, at 9:46, Sainitin Donakonda saigr...@gmail.com wrote:

 Hello,
 
 I am trying to run 20 ns protein ligand simulation on cluster using
 following MD.MDP file
 
 ; 7.3.3 Run Control
 integrator  = md; leap-frog integrator
 dt  = 0.002 ; 2 fs
 nsteps  = 500; maximum number of steps
 to integrate
 
 
 
 ; 7.3.8 Output Control
 nstxout = 200 ; suppress .trr output
 nstvout = 200; suppress .trr output
 nstenergy   = 1000  ; save energies every 2 ps
 nstlog  = 1000  ; update log file every 2 ps
 nstxtcout   = 1000  ; write .xtc trajectory every 2 ps
 energygrps  = Protein LIG
 
 ; 7.3.9 Neighbor Searching
 nstlist = 5 ; [steps] freq to update neighbor
 list
 ns_type = grid  ; method of updating neighbor list
 pbc = xyz   ; periodic boundary conditions in
 all directions
 rlist   = 1.2   ; [nm] cut-off distance for the
 short-range neighbor list
 
 ; 7.3.10 Electrostatics
 coulombtype = PME   ; Particle-Mesh Ewald electrostatics
 rcoulomb= 1.2   ; [nm] distance for Coulomb cut-off
 
 ; 7.3.11 VdW
 vdwtype = switch   ; twin-range cut-off with rlist
 where rvdw = rlist
 rvdw= 1.2   ; [nm] distance for LJ cut-off
 rvdw_switch = 0.8   ; Start switching th LJ potential
 DispCorr= EnerPres ; apply long range dispersion
 corrections for energy
 
 ; 7.3.13 Ewald
 fourierspacing  = 0.12  ; [nm] grid spacing for FFT grid
 when using PME
 pme_order   = 4 ; interpolation order for PME, 4 =
 cubic
 ewald_rtol  = 1e-5  ; relative strength of
 Ewald-shifted potential at rcoulomb
 
 ; 7.3.14 Temperature Coupling
 tcoupl  = V-rescale ; temperature
 coupling with Berendsen-thermostat
 tc_grps = Protein_LIG Water_and_ions; groups to couple
 seperately to temperature bath
 tau_t   = 0.10.1; [ps] time
 constant for coupling
 ref_t   = 300300; [K] reference
 temperature for coupling
 
 ; Pressure coupling
 pcoupl  = Parrinello-Rahman ; pressure coupling is on for
 NPT
 pcoupltype  = isotropic ; uniform scaling of box vectors
 tau_p   = 2.0   ; time constant, in ps
 ref_p   = 1.0   ; reference pressure, in bar
 compressibility = 4.5e-5; isothermal compressibility of
 water, bar^-1
 refcoord_scaling= com
 
 ; 7.3.17 Velocity Generation
 gen_vel = no; velocity generation turned off
 
 ; 7.3.18 Bonds
 constraints = all-bonds ; convert all bonds to constraints
 constraint_algorithm= LINCS ; LINear Constraint Solver
 continuation= yes   ; apply constraints to the start
 configuration
 lincs_order = 4 ; highest order in the expansion of
 the contraint coupling matrix
 lincs_iter  = 1 ; number of iterations to correct
 for rotational lengthening
 lincs_warnangle = 30; [degrees] maximum angle that a
 bond can rotate before LINCS will complain
 
 
 *and im using following commands dividing 20 ns to 10 ns each via extending
 simulation*
 
 
 *#This is the first simulation MD.mdp file contains 20 ns setup*
 grompp -f MD.mdp -c npt.gro -t npt.cpt -p topol.top -n index.ndx -o
 MD_first10.tpr
 
 mpirun -n 16 mdrun -s MD_first10.tpr -deffnm MD_first10 -np 16
 
 *#This extends 10 ns simulation*
 tpbconv -s MD_first10.tpr -extend 1 -o md_extended.tpr
 
 mpirun -n 16 mdrun -s md_extended.tpr -deffnm MD_first10 -cpi
 MD_first10.cpt -append -np 16
 
 
 But it is crashed giving following error
 
 *XTC error - maybe you are out of quota?*
 *
 *
 *dont know why it happened it is because as im saving .trr file every
 200ps? is it creating large files? or should i give different name in
 extending simulation?*
 *
 *
 *Please help*
 *
 *
 *Thanks,*
 *Nitin*
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Re: [gmx-users] issue in replica exchange

2013-05-13 Thread XAvier Periole

Ok, the redmine is filled up and anybody who has time to help finding the issue 
is welcome :) I can't do much more!

As an alternative a colleague suggested that I could potentially get around the 
problem by using a compilation combining Open-MP or thread-MPI for each replica 
running on one node (shared memory=no need of decomposition) and MPI across 
nodes. 
Would it work? 

But I might have a problem, the CG uses shifted potentials and they seem not to 
be implemented with OpenMP and thread-MPI is not compatible with MPI … 

Any other solution one could imagine?

XAvier.

On May 9, 2013, at 1:01 PM, XAvier Periole x.peri...@rug.nl wrote:

 
 I finally could reproduce the problem in gmx461 and have fled up a red mine 
 report. 
 
 I hope we can fix this easily but I am not sure how things go go from now! 
 Someone will get the bug assigned and fix it when ever possible or something 
 else?
 
 Thank you all for the help,
 XAvier.
 
 On May 2, 2013, at 10:15 PM, XAvier Periole x.peri...@rug.nl wrote:
 
 
 I'll look at the 4.6.1 version next week, I could install it but I got a 
 conflict between the environmental variable defining openMP variable but I 
 turned it off during compilation … 
 
 You could try to run on particle decomposition to see if you get a problem … 
 it should one quite quick.
 
 On May 2, 2013, at 2:36 PM, Michael Shirts mrshi...@gmail.com wrote:
 
 Both.  So if 4.6.1 doesn't work, I want to know so we can patch it
 before 4.6.2 comes out.  If it does work, then there is probably stuff
 that can be backported.
 
 On Thu, May 2, 2013 at 8:32 AM, XAvier Periole x.peri...@rug.nl wrote:
 
 You mean working with or working on the code?
 
 I'll try gmx-4.6.1
 
 On May 2, 2013, at 2:26 PM, Michael Shirts mrshi...@gmail.com wrote:
 
 Quick check here -- is 4.6 behaving correctly?  I actually spent some
 time working on REMD in 4.6, and it seems to be behaving  correctly in
 my hands with temperature and pressure control.
 
 Thanks for any additional info on this!
 
 On Thu, May 2, 2013 at 8:18 AM, Mark Abraham mark.j.abra...@gmail.com 
 wrote:
 On Thu, May 2, 2013 at 12:58 PM, XAvier Periole x.peri...@rug.nl wrote:
 
 
 I saw that redmine report, which could be related but it seems to happen
 only for runs done outside the domain and particle decompositions.
 
 I'll fill up a red mine.
 
 Anything I could do to help speeding the fix?
 
 
 What'd be really nice is some thought on how one can demonstrate that the
 implementation of the exchange matches what would be expected from the
 theory. For T-exchange under NVT, it is sufficient to rescale velocities
 and quantities derived from them by the correct factor. That includes
 various things like T-coupling history and integrator half-step 
 quantities
 (and does REMD with leap-frog make sense anyway?). For NPT, there's
 probably also some P-coupling quantities to scale, and the box to 
 exchange.
 Anything I've missed? Hopefully virial contributions don't matter either
 way?
 
 Perhaps a decent first step is to hack the code to do a self exchange, 
 by
 clearing the entire state and rebuilding with what would/should be 
 received
 from an exchange with a hypothethetical replica in an identical
 pre-exchange state. Only if the code can do that (i.e. mdrun -reprod
 produces a trajectory indistinguishable from a run that does not attempt
 this self exchange) is it worth considering proper state exchanges, and 
 the
 process of making the code do the former should illustrate what is 
 required
 for the latter.
 
 Mark
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Re: [Spam:*****] [gmx-users] REMD analysis

2013-05-13 Thread XAvier Periole

You need to increase the temperature gaps indeed if you want acceptance ratio 
~0.2/0.3. But again this won't work with the water … 

It is not clear what happens in your index file but probably a problem from 
grace to plot so many points … you can try to increase the Max drawing path 
length in the preference menu of grace.

On May 13, 2013, at 4:22 PM, bharat gupta bharat.85.m...@gmail.com wrote:

 Dear Sir,
 
 I repeated the simulation again for 25 replicas with the following temp.
 distribution .
 
 280
 289.1
 298.5
 308.2
 318.2
 328.6
 339.3
 350.3
 361.7
 373.5
 385.6
 398.1
 411.1
 424.4
 438.3
 452.5
 467.2
 482.4
 498.1
 514.3
 531.0
 548.3
 566.1
 584.5
 603.5
 623.2
 
 The output of md.log file is :-
 
 Replica exchange statistics
 Repl  24999 attempts, 12500 odd, 12499 even
 Repl  average probabilities:
 Repl 0123456789   10   11   12
 13   14   15   16   17   18   19   20   21   22   23   24   25
 Repl  .63  .63  .62  .62  .61  .61  .60  .60  .59  .59  .58  .59  .59
 .60  .60  .61  .62  .62  .63  .64  .64  .65  .65  .66  .66
 
 Repl  number of exchanges:
 Repl 0123456789   10   11   12
 13   14   15   16   17   18   19   20   21   22   23   24   25
 Repl 7822 7752 7816 7760 7639 7628 7511 7442 7375 7332 7312 7424 7408
 7410 7522 7559 7684 7697 7878 7927 7917 8073 8151 8208 8266
 
 Repl  average number of exchanges:
 Repl 0123456789   10   11   12
 13   14   15   16   17   18   19   20   21   22   23   24   25
 Repl  .63  .62  .63  .62  .61  .61  .60  .60  .59  .59  .58  .59  .59
 .59  .60  .60  .61  .62  .63  .63  .63  .65  .65  .66  .66
 
 The average acceptance ration is around 0.6 which is still high.
 
 The link for replica_temp,replica_index :
 https://www.dropbox.com/s/c7soajnwc3uww8j/replica_temp.png
 https://www.dropbox.com/s/wvx82m4c6cnsfit/replica_index.png
 
 The temp files look better but the index file looks weird ...
 
 Do i need to experiment with the gap difference in order to get the
 required ration of 0.2-0.3 ?? There is some problem with the .mdp file
 settings??
 
 -- 
 Bharat
 -- 
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 http://lists.gromacs.org/mailman/listinfo/gmx-users
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Re: [gmx-users] REMD average acceptance ratio

2013-05-11 Thread XAvier Periole

Well, actually things do not look so good. But is it possible that grace is 
actually no able to plot things correctly? You have line going throughout the 
plot from complete-left to complete-right! 

I am do not know what the t-rems calculator does but apparently it is not 
optimal in your case. Did you try to use the simple rule Tn=T0 x exp(n c), 
where T0 is close to your starting temperature and c is a constant that you can 
tune and will define the spacing between the temperatures. From your current 
data you can guess the spacing and thus the c value you need. Note that the 
exchange ratio is quickly converging in the simulation so you can make a few 
trials … 

On May 11, 2013, at 1:40 PM, bharat gupta bharat.85.m...@gmail.com wrote:

 Dear Sir,
 
 Thank you for your reply. I choose the temperature distribution using
 t-remd calculator. Here's the link for index and temp files .
 https://www.dropbox.com/s/uvwsdqjix49lg93/remd_index.png
 https://www.dropbox.com/s/78vcnaxzpgeekti/remd_temp.png?m.
 
 
 
 
 
 
 
 On Sat, May 11, 2013 at 12:04 AM, XAvier Periole x.peri...@rug.nl wrote:
 
 
 The replicas seem indeed to have exchange. Using a colour for the #
 replicas would help.
 
 I could not access to the first link.
 
 Note also that the increase of exchange ratio with the temperature suggest
 the distribution of the temperature is not optimal and may be with regular
 intervals? You want to use a exponential distribution.
 
 On May 10, 2013, at 4:53 PM, bharat gupta bharat.85.m...@gmail.com
 wrote:
 
 Dear gmx members,
 
 I have posted the same question previously , but I didn't get any reply.
 So, if anyone can help me out ...
 
 I performed a REMD simulation on a peptide 384 atoms (24 residues). In
 total 11 replicas were simulated for a period of 50ns each. The exchange
 was allwoed at every 1000 steps. The output of md.log file is :
 
 Replica exchange statistics
 Repl  24999 attempts, 12500 odd, 12499 even
 Repl  average probabilities:
 Repl 0123456789   10
 Repl  .16  .16  .16  .17  .18  .21  .24  .26  .28  .30
 Repl  number of exchanges:
 Repl 0123456789   10
 Repl 2038 2007 2065 2117 2182 2587 3022 3213 3554 3703
 Repl  average number of exchanges:
 Repl 0123456789   10
 Repl  .16  .16  .17  .17  .17  .21  .24  .26  .28  .30
 
 The acceptance ratio for each replica and average acceptance ratio is as
 calculated below :-
 
   accp. ratio
 2038 0.16304
 2007 0.16056
 2065 0.1652
 2117 0.16936
 2182 0.17456
 2587 0.20696
 3022 0.24176
 3213 0.25704
 3554 0.28432
 3703 0.29624
 0.211904 (avg accp ratio) (Is this value correct ??)
 
 The Pdes used while generating temp. range was also 0.2. Does that mean
 that  replicas have exchanged for the given temp.range ??.  Here's the
 link
 for both remd_temp and remd_index files (
 https://www.dropbox.com/s/uvwsdqjix49lg93/remd_index.png
 https://www.dropbox.com/s/uvwsdqjix49lg93/remd_index.png;cid=1368069857486-810
 )
 , (
 https://www.dropbox.com/s/78vcnaxzpgeekti/remd_temp.png?m
 https://www.dropbox.com/s/78vcnaxzpgeekti/remd_temp.png?mcid=1368069857486-810
 
 )
 
 --
 Bharat
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 -- 
 Bharat
 Ph.D. Candidate
 Biomolecular Engineering Laboratory
 Pusan National University
 South Korea
 Mobile no. - 010-5818-3680
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Re: [gmx-users] REMD average acceptance ratio

2013-05-11 Thread XAvier Periole

You are simulating in vacuo! Otherwise the temperature gaps are way too large … 

If you want to analyse the sampling at 300 K, I would suggest you start you 
first temperature lower, around 280/285 may be. At least to have your second 
temperature at 300 K. 

the value of c has absolutely not importance … the temperature distribution has 
… make some test to see how the acceptance ratio evolves … 

On May 11, 2013, at 5:05 PM, bharat gupta bharat.85.m...@gmail.com wrote:

 Dear Sir,
 
 Here's the temperature range that I got form t-remd :
 1 300
 2 323.7
 3 348.75
 4 375.23
 5 403.22
 6 432.83
 7 464.14
 8 497.24
 9 532.26
 10 569.32
 11 608.51
 
 
 according the above equation c should be somewhere around 2.37.
 
 
 On Sat, May 11, 2013 at 11:10 PM, XAvier Periole x.peri...@rug.nl wrote:
 
 
 Well, actually things do not look so good. But is it possible that grace
 is actually no able to plot things correctly? You have line going
 throughout the plot from complete-left to complete-right!
 
 I am do not know what the t-rems calculator does but apparently it is not
 optimal in your case. Did you try to use the simple rule Tn=T0 x exp(n c),
 where T0 is close to your starting temperature and c is a constant that you
 can tune and will define the spacing between the temperatures. From your
 current data you can guess the spacing and thus the c value you need. Note
 that the exchange ratio is quickly converging in the simulation so you can
 make a few trials …
 
 On May 11, 2013, at 1:40 PM, bharat gupta bharat.85.m...@gmail.com
 wrote:
 
 Dear Sir,
 
 Thank you for your reply. I choose the temperature distribution using
 t-remd calculator. Here's the link for index and temp files .
 https://www.dropbox.com/s/uvwsdqjix49lg93/remd_index.png
 https://www.dropbox.com/s/78vcnaxzpgeekti/remd_temp.png?m.
 
 
 
 
 
 
 
 On Sat, May 11, 2013 at 12:04 AM, XAvier Periole x.peri...@rug.nl
 wrote:
 
 
 The replicas seem indeed to have exchange. Using a colour for the #
 replicas would help.
 
 I could not access to the first link.
 
 Note also that the increase of exchange ratio with the temperature
 suggest
 the distribution of the temperature is not optimal and may be with
 regular
 intervals? You want to use a exponential distribution.
 
 On May 10, 2013, at 4:53 PM, bharat gupta bharat.85.m...@gmail.com
 wrote:
 
 Dear gmx members,
 
 I have posted the same question previously , but I didn't get any
 reply.
 So, if anyone can help me out ...
 
 I performed a REMD simulation on a peptide 384 atoms (24 residues). In
 total 11 replicas were simulated for a period of 50ns each. The
 exchange
 was allwoed at every 1000 steps. The output of md.log file is :
 
 Replica exchange statistics
 Repl  24999 attempts, 12500 odd, 12499 even
 Repl  average probabilities:
 Repl 0123456789   10
 Repl  .16  .16  .16  .17  .18  .21  .24  .26  .28  .30
 Repl  number of exchanges:
 Repl 0123456789   10
 Repl 2038 2007 2065 2117 2182 2587 3022 3213 3554 3703
 Repl  average number of exchanges:
 Repl 0123456789   10
 Repl  .16  .16  .17  .17  .17  .21  .24  .26  .28  .30
 
 The acceptance ratio for each replica and average acceptance ratio is
 as
 calculated below :-
 
  accp. ratio
 2038 0.16304
 2007 0.16056
 2065 0.1652
 2117 0.16936
 2182 0.17456
 2587 0.20696
 3022 0.24176
 3213 0.25704
 3554 0.28432
 3703 0.29624
 0.211904 (avg accp ratio) (Is this value correct ??)
 
 The Pdes used while generating temp. range was also 0.2. Does that mean
 that  replicas have exchanged for the given temp.range ??.  Here's the
 link
 for both remd_temp and remd_index files (
 https://www.dropbox.com/s/uvwsdqjix49lg93/remd_index.png
 
 https://www.dropbox.com/s/uvwsdqjix49lg93/remd_index.png;cid=1368069857486-810
 )
 , (
 https://www.dropbox.com/s/78vcnaxzpgeekti/remd_temp.png?m
 
 https://www.dropbox.com/s/78vcnaxzpgeekti/remd_temp.png?mcid=1368069857486-810
 
 )
 
 --
 Bharat
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 Pusan National University
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 Mobile no. - 010-5818-3680
 --
 gmx

Re: [gmx-users] REMD average acceptance ratio

2013-05-11 Thread XAvier Periole

The values of exchange ratio look much better: they are similar over the range 
of temperatures. 

To reduce the ratio you have to increase the spacing between temperatures, 
which means increase the value of c in the formula I gave earlier. 

When you but the water in, the degrees of freedom (and thus the potential 
energy) will increase and the temperature distribution won't work at all! To 
cover the same temperature range you'll need much more temperatures. 

On May 11, 2013, at 19:59, bharat gupta bharat.85.m...@gmail.com wrote:

 Dear Sir,
 
 I tried again with the following temp. ditribution, this time with 30
 replicas (280 K -624K) and 500 ps simulation time for each one.
 
 0 280
 1 287.8
 2 295.9
 3 304.2
 4 312.7
 5 321.5
 6 330.5
 7 339.8
 8 349.3
 9 359.1
 10 369.1
 11 379.5
 12 390.1
 13 401.0
 14 412.3
 15 423.8
 16 435.7
 17 447.9
 18 460.4
 19 473.3
 20 486.6
 21 500.2
 22 514.3
 23 528.7
 24 543.5
 25 558.7
 26 574.4
 27 590.4
 28 607.0
 29 624.0
 
 
 The output of   md29.log file is :-
 
 Replica exchange statistics
 Repl  249 attempts, 125 odd, 124 even
 Repl  average probabilities:
 Repl 0123456789   10   11   12   13
  14   15   16   17   18   19   20   21   22   23   24   25   26   27   28
  29
 Repl  .68  .63  .62  .68  .71  .66  .69  .68  .71  .67  .64  .71  .69
 .71  .66  .69  .73  .73  .72  .73  .69  .71  .71  .74  .73  .70  .72  .74
 .71
 Repl  number of exchanges:
 Repl 0123456789   10   11   12   13
  14   15   16   17   18   19   20   21   22   23   24   25   26   27   28
  29
 Repl   81   77   79   90   93   78   91   80   88   78   81   92   96
 94   81   83   90   92   83   97   89   87   91   94   88   84   85   89
 86
 Repl  average number of exchanges:
 Repl 0123456789   10   11   12   13
  14   15   16   17   18   19   20   21   22   23   24   25   26   27   28
  29
 Repl  .65  .62  .63  .73  .74  .63  .73  .65  .70  .63  .65  .74  .77
 .76  .65  .67  .72  .74  .66  .78  .71  .70  .73  .76  .70  .68  .68  .72
 .69
 
 
 The average acceptance ration comes around 0.69 , which is very high. Now,
 in order to get the avg. acceptance ration between 0.2 to 0.3 and also all
 the replicas should exchange , what has to be done.
 
 Here's the link for remd_index and remd_temp files
 https://www.dropbox.com/s/sgpblcdg9zh7f52/remd_temp.png
 https://www.dropbox.com/s/6hvqlqmu64mb2jy/remd_index.png
 
 I want to that if I include water for the simulation, the same temp.
 distribution would work or not ??
 
 
 
 
 On Sun, May 12, 2013 at 12:10 AM, XAvier Periole x.peri...@rug.nl wrote:
 
 
 You are simulating in vacuo! Otherwise the temperature gaps are way too
 large …
 
 If you want to analyse the sampling at 300 K, I would suggest you start
 you first temperature lower, around 280/285 may be. At least to have your
 second temperature at 300 K.
 
 the value of c has absolutely not importance … the temperature
 distribution has … make some test to see how the acceptance ratio evolves …
 
 On May 11, 2013, at 5:05 PM, bharat gupta bharat.85.m...@gmail.com
 wrote:
 
 Dear Sir,
 
 Here's the temperature range that I got form t-remd :
 1 300
 2 323.7
 3 348.75
 4 375.23
 5 403.22
 6 432.83
 7 464.14
 8 497.24
 9 532.26
 10 569.32
 11 608.51
 
 
 according the above equation c should be somewhere around 2.37.
 
 
 On Sat, May 11, 2013 at 11:10 PM, XAvier Periole x.peri...@rug.nl
 wrote:
 
 
 Well, actually things do not look so good. But is it possible that grace
 is actually no able to plot things correctly? You have line going
 throughout the plot from complete-left to complete-right!
 
 I am do not know what the t-rems calculator does but apparently it is
 not
 optimal in your case. Did you try to use the simple rule Tn=T0 x exp(n
 c),
 where T0 is close to your starting temperature and c is a constant that
 you
 can tune and will define the spacing between the temperatures. From your
 current data you can guess the spacing and thus the c value you need.
 Note
 that the exchange ratio is quickly converging in the simulation so you
 can
 make a few trials …
 
 On May 11, 2013, at 1:40 PM, bharat gupta bharat.85.m...@gmail.com
 wrote:
 
 Dear Sir,
 
 Thank you for your reply. I choose the temperature distribution using
 t-remd calculator. Here's the link for index and temp files .
 https://www.dropbox.com/s/uvwsdqjix49lg93/remd_index.png
 https://www.dropbox.com/s/78vcnaxzpgeekti/remd_temp.png?m.
 
 
 
 
 
 
 
 On Sat, May 11, 2013 at 12:04 AM, XAvier Periole x.peri...@rug.nl
 wrote:
 
 
 The replicas seem indeed to have exchange. Using a colour for the #
 replicas would help.
 
 I could not access to the first link.
 
 Note also that the increase of exchange ratio with the temperature
 suggest
 the distribution of the temperature is not optimal and may be with
 regular
 intervals? You want to use a exponential distribution.
 
 On May 10, 2013, at 4:53 PM

Re: [gmx-users] Re: REMD average acceptance ratio

2013-05-10 Thread XAvier Periole

The replicas seem indeed to have exchange. Using a colour for the # replicas 
would help.

I could not access to the first link. 

Note also that the increase of exchange ratio with the temperature suggest the 
distribution of the temperature is not optimal and may be with regular 
intervals? You want to use a exponential distribution.

On May 10, 2013, at 4:53 PM, bharat gupta bharat.85.m...@gmail.com wrote:

 Dear gmx members,
 
 I have posted the same question previously , but I didn't get any reply.
 So, if anyone can help me out ...
 
 I performed a REMD simulation on a peptide 384 atoms (24 residues). In
 total 11 replicas were simulated for a period of 50ns each. The exchange
 was allwoed at every 1000 steps. The output of md.log file is :
 
 Replica exchange statistics
 Repl  24999 attempts, 12500 odd, 12499 even
 Repl  average probabilities:
 Repl 0123456789   10
 Repl  .16  .16  .16  .17  .18  .21  .24  .26  .28  .30
 Repl  number of exchanges:
 Repl 0123456789   10
 Repl 2038 2007 2065 2117 2182 2587 3022 3213 3554 3703
 Repl  average number of exchanges:
 Repl 0123456789   10
 Repl  .16  .16  .17  .17  .17  .21  .24  .26  .28  .30
 
 The acceptance ratio for each replica and average acceptance ratio is as
 calculated below :-
 
accp. ratio
 2038 0.16304
 2007 0.16056
 2065 0.1652
 2117 0.16936
 2182 0.17456
 2587 0.20696
 3022 0.24176
 3213 0.25704
 3554 0.28432
 3703 0.29624
 0.211904 (avg accp ratio) (Is this value correct ??)
 
 The Pdes used while generating temp. range was also 0.2. Does that mean
 that  replicas have exchanged for the given temp.range ??.  Here's the link
 for both remd_temp and remd_index files (
 https://www.dropbox.com/s/uvwsdqjix49lg93/remd_index.pnghttps://www.dropbox.com/s/uvwsdqjix49lg93/remd_index.png;cid=1368069857486-810)
 , (
 https://www.dropbox.com/s/78vcnaxzpgeekti/remd_temp.png?mhttps://www.dropbox.com/s/78vcnaxzpgeekti/remd_temp.png?mcid=1368069857486-810
 )
 
 -- 
 Bharat
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Re: [gmx-users] issue in replica exchange

2013-05-09 Thread XAvier Periole

I finally could reproduce the problem in gmx461 and have fled up a red mine 
report. 

I hope we can fix this easily but I am not sure how things go go from now! 
Someone will get the bug assigned and fix it when ever possible or something 
else?

Thank you all for the help,
XAvier.

On May 2, 2013, at 10:15 PM, XAvier Periole x.peri...@rug.nl wrote:

 
 I'll look at the 4.6.1 version next week, I could install it but I got a 
 conflict between the environmental variable defining openMP variable but I 
 turned it off during compilation … 
 
 You could try to run on particle decomposition to see if you get a problem … 
 it should one quite quick.
 
 On May 2, 2013, at 2:36 PM, Michael Shirts mrshi...@gmail.com wrote:
 
 Both.  So if 4.6.1 doesn't work, I want to know so we can patch it
 before 4.6.2 comes out.  If it does work, then there is probably stuff
 that can be backported.
 
 On Thu, May 2, 2013 at 8:32 AM, XAvier Periole x.peri...@rug.nl wrote:
 
 You mean working with or working on the code?
 
 I'll try gmx-4.6.1
 
 On May 2, 2013, at 2:26 PM, Michael Shirts mrshi...@gmail.com wrote:
 
 Quick check here -- is 4.6 behaving correctly?  I actually spent some
 time working on REMD in 4.6, and it seems to be behaving  correctly in
 my hands with temperature and pressure control.
 
 Thanks for any additional info on this!
 
 On Thu, May 2, 2013 at 8:18 AM, Mark Abraham mark.j.abra...@gmail.com 
 wrote:
 On Thu, May 2, 2013 at 12:58 PM, XAvier Periole x.peri...@rug.nl wrote:
 
 
 I saw that redmine report, which could be related but it seems to happen
 only for runs done outside the domain and particle decompositions.
 
 I'll fill up a red mine.
 
 Anything I could do to help speeding the fix?
 
 
 What'd be really nice is some thought on how one can demonstrate that the
 implementation of the exchange matches what would be expected from the
 theory. For T-exchange under NVT, it is sufficient to rescale velocities
 and quantities derived from them by the correct factor. That includes
 various things like T-coupling history and integrator half-step quantities
 (and does REMD with leap-frog make sense anyway?). For NPT, there's
 probably also some P-coupling quantities to scale, and the box to 
 exchange.
 Anything I've missed? Hopefully virial contributions don't matter either
 way?
 
 Perhaps a decent first step is to hack the code to do a self exchange, 
 by
 clearing the entire state and rebuilding with what would/should be 
 received
 from an exchange with a hypothethetical replica in an identical
 pre-exchange state. Only if the code can do that (i.e. mdrun -reprod
 produces a trajectory indistinguishable from a run that does not attempt
 this self exchange) is it worth considering proper state exchanges, and 
 the
 process of making the code do the former should illustrate what is 
 required
 for the latter.
 
 Mark
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Re: [gmx-users] keeping water (entirely) out of the bilayer core

2013-05-05 Thread XAvier Periole

You could define a repulsive potential that would apply to water molecules. I 
am not sure how it is called but it is available and described in the manual. 

On May 4, 2013, at 2:46, Christopher Neale chris.ne...@mail.utoronto.ca wrote:

 Dear users:
 
 I am interested in running simulations of lipid bilayers in which I keep all 
 water molecules out of the bilayer core
 (not just statistically, but absolutely). However, I have been unable to 
 figure out how to do it. 
 I'll list what I have tried in the hope that others have some ideas or even 
 perhaps know how to do this 
 with standard gromacs.
 
 Everything that I have tried revolves around using the pull code, setting the 
 entire lipid bilayer as the reference 
 group, and having thousands of pulled groups -- one for each water molecule. 
 Also, I modified the gromacs
 source code in mdlib/pull.c (version 4.6.1) so that the force is only applied 
 when the displacement is smaller than 
 the desired distance and not when the displacement is larger than the 
 specified distance (to keep water out but
 then to otherwise let it go anywhere without bias):
 
 static void do_pull_pot(int ePull,
t_pull *pull, t_pbc *pbc, double t, real lambda,
real *V, tensor vir, real *dVdl)
 {
intg, j, m;
dvec   dev;
double ndr, invdr;
real   k, dkdl;
t_pullgrp *pgrp;
 
/* loop over the groups that are being pulled */
*V= 0;
*dVdl = 0;
for (g = 1; g  1+pull-ngrp; g++)
{
pgrp = pull-grp[g];
get_pullgrp_distance(pull, pbc, g, t, pgrp-dr, dev);
 
 /*  ## HERE IS THE CODE CHANGE 
if(dev[0]0.0){
dev[0]=0.0;
}
 /* End code snippit */
 
 
 The most relevant lines from the .mdp file were:
 
 pull = umbrella
 pull_geometry= distance
 pull_dim = N N Y
 pull_start   = no
 pull_ngroups = 9000
 pull_group0  = POPC
 
 pull_group1  = r_1__OW
 pull_init1   = 1.9
 pull_k1  = 500
 
 pull_group2  = r_2__OW
 pull_init2   = 1.9
 pull_k2  = 500
 
 ... etc...
 
 
 The problem with this was that it crashed immediately with an error that my 
 pulling distance was 
 greater than 1/2 of the box vector.:
 
 Fatal error:
 Distance of pull group 165 (5.353939 nm) is larger than 0.49 times the box 
 size (5.395960)
 
 Pretty obvious in retrospect. If I could get this error to go away, then 
 everything should be fine because I have modified the code so that forces are 
 zero at large displacements. However, I am worried that if I simply modify 
 grompp to bypass this error then I might get some type of strange and 
 possibly silent error in mdrun. Any thoughts on this are really appreciated.
 
 For my second try, I used pull_geometry = direction-periodic (see more 
 details below), but that also didn't work 
 because if I set pull_vec1 = 0 0 1, then everything gets pulled to the upper 
 part of the box (and LINCS errors 
 ensue), rather than simply pulling away from the bilayer.
 
 Pcoupl= berendsen
 pcoupltype   = semiisotropic
 compressibility= 4.5e-5 0
 pull = umbrella
 pull_geometry= direction-periodic
 pull_start   = no
 pull_ngroups = 9000
 pull_group0  = POPC
 
 pull_group1  = r_1__OW
 pull_init1   = 1.9
 pull_k1  = 500
 pull_vec1= 0 0 1
 
 pull_group2  = r_2__OW
 pull_init2   = 1.9
 pull_k2  = 500
 pull_vec2= 0 0 1
 
 ... etc...
 
 
 If anybody has an idea about how I could get this to work with standard 
 gromacs or with a modified version, I would be very grateful to hear your 
 thoughts. 
 
 Thank you,
 Chris.
 
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Re: [gmx-users] local pressure

2013-05-02 Thread XAvier Periole

What are you looking for? Have a look at the papers they might be inspiring :))

On May 1, 2013, at 10:33 PM, Sikandar Mashayak symasha...@gmail.com wrote:

 Ok, I did rerun with local pressure mdrun, and got pressure.dat* files in
 binary format. how do I proceed from here? Any utility to analyze or
 post-process this?
 
 
 On Wed, May 1, 2013 at 11:11 AM, Sikandar Mashayak 
 symasha...@gmail.comwrote:
 
 Thanks Xavier,
 
 I will give it a try.
 
 
 On Wed, May 1, 2013 at 10:56 AM, XAvier Periole x.peri...@rug.nl wrote:
 
 
 
 Well I am not the expert. O.H.S. Ollila, M. Louhivuori and E. Lindahl are
 :)).
 
 The paper related to the use would be:
 Ollila et al, PRL 102, 078101 (2009)
 Ollila et al, Biophysical Journal (100)1651–59
 
 On May 1, 2013, at 5:48 PM, Sikandar Mashayak symasha...@gmail.com
 wrote:
 
 Thanks Xavier
 
 
 Can you please elaborate on how to use and post-process the local
 pressure
 version of gromacs? Do you have any examples or reference article?
 
 May be you can create a HowTo wiki as Justin suggested, it would be of
 great help.
 
 Thanks
 Sikandar
 
 
 On Wed, May 1, 2013 at 5:03 AM, Justin Lemkul jalem...@vt.edu wrote:
 
 
 
 On 5/1/13 5:12 AM, XAvier Periole wrote:
 
 
 The use of the original code is quite straightforward, the post
 processing is a bit more confusing but quite accessible.
 
 
 That would be a great topic for a wiki How-To.
 
 
 We have been using this code (the one available on the site) and
 related
 version in the lab and we definitely would find it very sad to not
 keep
 this feature available in GROMACS.
 
 
 I never said it would go away, but given the fact that there have been
 no
 updates to the git branch in over 3 years, it's simply unlikely that
 anyone
 has cared to move it forward.  If someone wants to update the code to
 be
 compatible with 4.6, that would be a welcome contribution.  Lack of any
 request for improvements and inclusion in an official release has
 likely
 led to the decline in interest from the development team.  If you want
 something included, you should file a feature request on
 redmine.gromacs.org - it's the only official way we keep track of
 fixes
 and features.  If it's not there, it likely won't get addressed until
 one
 of the developers has a compelling need to work on it.
 
 -Justin
 
 
 On May 1, 2013, at 2:34 AM, Justin Lemkul jalem...@vt.edu wrote:
 
 
 
 On 4/30/13 8:01 PM, Sikandar Mashayak wrote:
 
 Hi
 
 I found the branch of gromacs code called localpressure-4.0 at
 http://redmine.gromacs.org/**projects/gromacs/repository/**
 show?rev=localpressure-4-0
 http://redmine.gromacs.org/projects/gromacs/repository/show?rev=localpressure-4-0
 
 .
 I am wondering whether this code can compute the spatial variation
 of
 pressure in given system. And if it does, how stable is this
 branch? Are
 there any known issues with it? And any particular reason this is
 not
 included in main gromacs releases?
 
 
 Lack of documentation has made it very difficult to use, it is
 extremely
 slow, and no one ever asks about it except once every few years.
 All of
 those factors make it unlikely to ever incorporate into an actual
 release.
 Given that the development process has gone on for years in the
 absence of
 any real interest in the localpressure branch, it's probably more
 trouble
 than it's worth to get it up and running effectively.
 
 -Justin
 
 --
 ==**==
 
 Justin A. Lemkul, Ph.D.
 Research Scientist
 Department of Biochemistry
 Virginia Tech
 Blacksburg, VA
 jalemkul[at]vt.edu | (540) 231-9080
 http://www.bevanlab.biochem.**vt.edu/Pages/Personal/justin
 http://www.bevanlab.biochem.vt.edu/Pages/Personal/justin
 
 ==**==
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 http://www.gromacs.org/Support/Mailing_Lists
 
 
 
 --
 ==**==
 
 Justin A. Lemkul, Ph.D.
 Research Scientist
 Department of Biochemistry
 Virginia Tech
 Blacksburg, VA
 jalemkul[at]vt.edu | (540) 231-9080
 http://www.bevanlab.biochem.**vt.edu/Pages/Personal/justin
 http://www.bevanlab.biochem.vt.edu/Pages/Personal/justin
 
 ==**==
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Re: [gmx-users] issue in replica exchange

2013-05-02 Thread XAvier Periole

Did you look at some data like temperature/pressure/box size/Epot as a function 
of time and especially around some exchanges? 

Your system is atomistic I presume.

On May 2, 2013, at 12:38 PM, Simone Conti simone...@gmail.com wrote:

 I'm running remd in NPT ensemble for a small peptide and all is ok if the
 maximum temperature is below 510/520 kelvin. I use Nosé-Hoover termostat
 and Parrinello-Rahman barostat. Ref T from 285 to 500K and ref P equals to
 1bar. Gromacs version 4.5.5. Exchange trials every 5 ps.
 If I try to add replica at a higher temperature the system crash, but I
 think it is a problem of equilibration.
 
 
 2013/5/1 XAvier Periole x.peri...@rug.nl
 
 
 Ok here is my current status on that REMD issue.
 
 For info: I use
 Temperature: v-rescale, tau_t = 2.0 ps
 Pressure: berendsen, tau_p = 5.0 ps,
 time step: dt=0.002 - 0.020 fs,
 COM removal on for bilayer/water separately
 
 The symptoms: explosion of the system after 2-5 steps following the swap,
 first sign is a huge jump in LJ interactions and pressure. This jump seems
 to be absorbed by the box size and temperature when possible … see example
 I provided earlier. A large VCM (velocity centre of mass?) is often
 associated with the crash. But also pressure scaling more than 1% ...
 
 1- the problem mentioned above remains in gmx-4.5.7 and it might actually
 got worse. I was able to run a 500 ns simulation with gmx405 using similar
 setup as for gmx457. The following point happened in gmx457.
 2- it persists with a time step of 2 fs. Actually all tests performed in
 the following used dt=2fs.
 3- if I perform an exchange that explodes within mdrun myself (externally
 to the remd gromacs by getting the gro file with the mdp adjusting the
 temperature) it goes all fine.
 4- the issue gets much worst when the consecutive replicas differ
 (different protein conformations and the box size etc) … explosion at first
 exchange.
 5- the use of parrinelo-raman does not help
 6- cancelling the centre of mass removal does not remove the problem.
 7- switching to NVT ensemble does not help but makes it worst (crash in 2
 steps). All exchanges accepted at first attempt crash with the message
 Large VCM(group SOL): -0.0XXX , -0.XXX, -0.16XXX, Temp-cm:6.55XXX
 8- using a unique conformation (the same) for all replicas in the NVT REMD
 simulation after equilibration in the same NVT ensemble (for 1 ns) removes
 the problem.
 9- taking the equilibrated NVT conformations, equilibrate them in an NPT
 ensemble (1 ns) and let go the exchanges afterwards restores the problem …
 one exchange is not properly done at the second trial, while the first ones
 were fine. Well if errors were made that was with reasonable
 10- note also that the coarse grain I use is extremely forgiving, meaning
 you can perform really nasty transformations and run it further after
 simple minimisation … so even abrupt changes in temperatures should be fine
 and relax quickly.
 11- when looking at the conformations themselves nothing appears to have
 jumped over or nothing funky.
 
 At this point I am not sure what to think and what to do next. There is
 definitely something not going right during the exchanges.
 
 Anyone has been able to run a REMD simulation in an NPT ensemble without
 crashes? I would imagine someone has and something particular to my system
 is making it going wrong but I am really wondering what it could be. My
 feeling is that something relative to the box size or pressure is not going
 across but it might be something completely different, when the consecutive
 systems differ reasonably.
 
 However that would suggest that the manner the exchanges are made is
 severely wrong in some cases.
 
 Any help to resolve the problem would be greatly appreciated.
 
 XAvier.
 
 On Apr 26, 2013, at 9:21 AM, Mark Abraham mark.j.abra...@gmail.com
 wrote:
 
 On Thu, Apr 25, 2013 at 11:05 PM, XAvier Periole x.peri...@rug.nl
 wrote:
 
 
 Thanks for the answer. I'll check gmx4.5.7 and report back.
 
 I am not sure what you mean by GROMACS swaps the coordinates not the
 ensemble data. The coupling to P and T and not exchanged with it?
 
 
 The code in src/kernel/repl_ex.c:
 
 static void exchange_state(const gmx_multisim_t *ms, int b, t_state
 *state)
 {
   /* When t_state changes, this code should be updated. */
   int ngtc, nnhpres;
   ngtc= state-ngtc * state-nhchainlength;
   nnhpres = state-nnhpres* state-nhchainlength;
   exchange_rvecs(ms, b, state-box, DIM);
   exchange_rvecs(ms, b, state-box_rel, DIM);
   exchange_rvecs(ms, b, state-boxv, DIM);
   exchange_reals(ms, b, (state-veta), 1);
   exchange_reals(ms, b, (state-vol0), 1);
   exchange_rvecs(ms, b, state-svir_prev, DIM);
   exchange_rvecs(ms, b, state-fvir_prev, DIM);
   exchange_rvecs(ms, b, state-pres_prev, DIM);
   exchange_doubles(ms, b, state-nosehoover_xi, ngtc);
   exchange_doubles(ms, b, state-nosehoover_vxi, ngtc);
   exchange_doubles(ms, b, state-nhpres_xi, nnhpres);
   exchange_doubles(ms, b

Re: [gmx-users] issue in replica exchange

2013-05-02 Thread XAvier Periole

I saw that redmine report, which could be related but it seems to happen only 
for runs done outside the domain and particle decompositions.

I'll fill up a red mine. 

Anything I could do to help speeding the fix? 

On May 2, 2013, at 11:53 AM, Mark Abraham mark.j.abra...@gmail.com wrote:

 On Wed, May 1, 2013 at 10:24 PM, XAvier Periole x.peri...@rug.nl wrote:
 
 
 Ok here is my current status on that REMD issue.
 
 For info: I use
 Temperature: v-rescale, tau_t = 2.0 ps
 Pressure: berendsen, tau_p = 5.0 ps,
 time step: dt=0.002 - 0.020 fs,
 COM removal on for bilayer/water separately
 
 The symptoms: explosion of the system after 2-5 steps following the swap,
 first sign is a huge jump in LJ interactions and pressure. This jump seems
 to be absorbed by the box size and temperature when possible … see example
 I provided earlier. A large VCM (velocity centre of mass?) is often
 associated with the crash. But also pressure scaling more than 1% ...
 
 1- the problem mentioned above remains in gmx-4.5.7 and it might actually
 got worse. I was able to run a 500 ns simulation with gmx405 using similar
 setup as for gmx457. The following point happened in gmx457.
 2- it persists with a time step of 2 fs. Actually all tests performed in
 the following used dt=2fs.
 3- if I perform an exchange that explodes within mdrun myself (externally
 to the remd gromacs by getting the gro file with the mdp adjusting the
 temperature) it goes all fine.
 4- the issue gets much worst when the consecutive replicas differ
 (different protein conformations and the box size etc) … explosion at first
 exchange.
 5- the use of parrinelo-raman does not help
 6- cancelling the centre of mass removal does not remove the problem.
 7- switching to NVT ensemble does not help but makes it worst (crash in 2
 steps). All exchanges accepted at first attempt crash with the message
 Large VCM(group SOL): -0.0XXX , -0.XXX, -0.16XXX, Temp-cm:6.55XXX
 8- using a unique conformation (the same) for all replicas in the NVT REMD
 simulation after equilibration in the same NVT ensemble (for 1 ns) removes
 the problem.
 9- taking the equilibrated NVT conformations, equilibrate them in an NPT
 ensemble (1 ns) and let go the exchanges afterwards restores the problem …
 one exchange is not properly done at the second trial, while the first ones
 were fine. Well if errors were made that was with reasonable
 10- note also that the coarse grain I use is extremely forgiving, meaning
 you can perform really nasty transformations and run it further after
 simple minimisation … so even abrupt changes in temperatures should be fine
 and relax quickly.
 11- when looking at the conformations themselves nothing appears to have
 jumped over or nothing funky.
 
 At this point I am not sure what to think and what to do next. There is
 definitely something not going right during the exchanges.
 
 
 OK, thanks for the effort. That all agrees with my suspicion that the full
 state is not being exchanged.
 
 Anyone has been able to run a REMD simulation in an NPT ensemble without
 crashes? I would imagine someone has and something particular to my system
 is making it going wrong but I am really wondering what it could be. My
 feeling is that something relative to the box size or pressure is not going
 across but it might be something completely different, when the consecutive
 systems differ reasonably.
 
 
 I've never tried, but an experiment with a water box might be instructive.
 
 However that would suggest that the manner the exchanges are made is
 severely wrong in some cases.
 
 Any help to resolve the problem would be greatly appreciated.
 
 
 There is an outstanding REMD issue on redmine that could be related (
 http://redmine.gromacs.org/issues/1191). I'd suggest you open a new issue
 there, upload a minimal set of .tprs that can reproduce the problem and
 anything you can think of that might help investigate. For something I'm
 doing, I'd like to be sure the full T-coupling state is being exchanged,
 and we may as well kill all the bugs at once.
 
 Mark
 
 
 XAvier.
 
 On Apr 26, 2013, at 9:21 AM, Mark Abraham mark.j.abra...@gmail.com
 wrote:
 
 On Thu, Apr 25, 2013 at 11:05 PM, XAvier Periole x.peri...@rug.nl
 wrote:
 
 
 Thanks for the answer. I'll check gmx4.5.7 and report back.
 
 I am not sure what you mean by GROMACS swaps the coordinates not the
 ensemble data. The coupling to P and T and not exchanged with it?
 
 
 The code in src/kernel/repl_ex.c:
 
 static void exchange_state(const gmx_multisim_t *ms, int b, t_state
 *state)
 {
   /* When t_state changes, this code should be updated. */
   int ngtc, nnhpres;
   ngtc= state-ngtc * state-nhchainlength;
   nnhpres = state-nnhpres* state-nhchainlength;
   exchange_rvecs(ms, b, state-box, DIM);
   exchange_rvecs(ms, b, state-box_rel, DIM);
   exchange_rvecs(ms, b, state-boxv, DIM);
   exchange_reals(ms, b, (state-veta), 1);
   exchange_reals(ms, b, (state-vol0), 1);
   exchange_rvecs(ms, b, state

Re: [gmx-users] issue in replica exchange

2013-05-02 Thread XAvier Periole

Could you send me a set of tar files that I could look at things the same way I 
do with my system? I would guess that 6 tar files where you same energies and 
print log file every step but xtc and trr files not that often would be really 
cool. 

You can send them directly to my email (x.peri...@rug.nl) unless they are too 
big. If you do not like the idea it is also ok.

On May 2, 2013, at 1:38 PM, Simone Conti simone...@gmail.com wrote:

 Yes, my system is described at atomic level.
 No, I can't see any strange value around exchanges. I analyzed only a
 very little number of trajectories, but temperature, volume, potential
 energy, pressure seem all to be around normal fluctuations.
 
 
 2013/5/2 XAvier Periole x.peri...@rug.nl
 
 
 Did you look at some data like temperature/pressure/box size/Epot as a
 function of time and especially around some exchanges?
 
 Your system is atomistic I presume.
 
 On May 2, 2013, at 12:38 PM, Simone Conti simone...@gmail.com wrote:
 
 I'm running remd in NPT ensemble for a small peptide and all is ok if the
 maximum temperature is below 510/520 kelvin. I use Nosé-Hoover termostat
 and Parrinello-Rahman barostat. Ref T from 285 to 500K and ref P equals
 to
 1bar. Gromacs version 4.5.5. Exchange trials every 5 ps.
 If I try to add replica at a higher temperature the system crash, but I
 think it is a problem of equilibration.
 
 
 2013/5/1 XAvier Periole x.peri...@rug.nl
 
 
 Ok here is my current status on that REMD issue.
 
 For info: I use
 Temperature: v-rescale, tau_t = 2.0 ps
 Pressure: berendsen, tau_p = 5.0 ps,
 time step: dt=0.002 - 0.020 fs,
 COM removal on for bilayer/water separately
 
 The symptoms: explosion of the system after 2-5 steps following the
 swap,
 first sign is a huge jump in LJ interactions and pressure. This jump
 seems
 to be absorbed by the box size and temperature when possible … see
 example
 I provided earlier. A large VCM (velocity centre of mass?) is often
 associated with the crash. But also pressure scaling more than 1% ...
 
 1- the problem mentioned above remains in gmx-4.5.7 and it might
 actually
 got worse. I was able to run a 500 ns simulation with gmx405 using
 similar
 setup as for gmx457. The following point happened in gmx457.
 2- it persists with a time step of 2 fs. Actually all tests performed in
 the following used dt=2fs.
 3- if I perform an exchange that explodes within mdrun myself
 (externally
 to the remd gromacs by getting the gro file with the mdp adjusting the
 temperature) it goes all fine.
 4- the issue gets much worst when the consecutive replicas differ
 (different protein conformations and the box size etc) … explosion at
 first
 exchange.
 5- the use of parrinelo-raman does not help
 6- cancelling the centre of mass removal does not remove the problem.
 7- switching to NVT ensemble does not help but makes it worst (crash in
 2
 steps). All exchanges accepted at first attempt crash with the message
 Large VCM(group SOL): -0.0XXX , -0.XXX, -0.16XXX, Temp-cm:6.55XXX
 8- using a unique conformation (the same) for all replicas in the NVT
 REMD
 simulation after equilibration in the same NVT ensemble (for 1 ns)
 removes
 the problem.
 9- taking the equilibrated NVT conformations, equilibrate them in an NPT
 ensemble (1 ns) and let go the exchanges afterwards restores the
 problem …
 one exchange is not properly done at the second trial, while the first
 ones
 were fine. Well if errors were made that was with reasonable
 10- note also that the coarse grain I use is extremely forgiving,
 meaning
 you can perform really nasty transformations and run it further after
 simple minimisation … so even abrupt changes in temperatures should be
 fine
 and relax quickly.
 11- when looking at the conformations themselves nothing appears to have
 jumped over or nothing funky.
 
 At this point I am not sure what to think and what to do next. There is
 definitely something not going right during the exchanges.
 
 Anyone has been able to run a REMD simulation in an NPT ensemble without
 crashes? I would imagine someone has and something particular to my
 system
 is making it going wrong but I am really wondering what it could be. My
 feeling is that something relative to the box size or pressure is not
 going
 across but it might be something completely different, when the
 consecutive
 systems differ reasonably.
 
 However that would suggest that the manner the exchanges are made is
 severely wrong in some cases.
 
 Any help to resolve the problem would be greatly appreciated.
 
 XAvier.
 
 On Apr 26, 2013, at 9:21 AM, Mark Abraham mark.j.abra...@gmail.com
 wrote:
 
 On Thu, Apr 25, 2013 at 11:05 PM, XAvier Periole x.peri...@rug.nl
 wrote:
 
 
 Thanks for the answer. I'll check gmx4.5.7 and report back.
 
 I am not sure what you mean by GROMACS swaps the coordinates not the
 ensemble data. The coupling to P and T and not exchanged with it?
 
 
 The code in src/kernel/repl_ex.c:
 
 static void exchange_state(const

Re: [gmx-users] issue in replica exchange

2013-05-02 Thread XAvier Periole

I mean tpr files not tar! Autocorrection is sometimes funny :))

On May 2, 2013, at 2:11 PM, XAvier Periole x.peri...@rug.nl wrote:

 
 Could you send me a set of tar files that I could look at things the same way 
 I do with my system? I would guess that 6 tar files where you same energies 
 and print log file every step but xtc and trr files not that often would be 
 really cool. 
 
 You can send them directly to my email (x.peri...@rug.nl) unless they are too 
 big. If you do not like the idea it is also ok.
 
 On May 2, 2013, at 1:38 PM, Simone Conti simone...@gmail.com wrote:
 
 Yes, my system is described at atomic level.
 No, I can't see any strange value around exchanges. I analyzed only a
 very little number of trajectories, but temperature, volume, potential
 energy, pressure seem all to be around normal fluctuations.
 
 
 2013/5/2 XAvier Periole x.peri...@rug.nl
 
 
 Did you look at some data like temperature/pressure/box size/Epot as a
 function of time and especially around some exchanges?
 
 Your system is atomistic I presume.
 
 On May 2, 2013, at 12:38 PM, Simone Conti simone...@gmail.com wrote:
 
 I'm running remd in NPT ensemble for a small peptide and all is ok if the
 maximum temperature is below 510/520 kelvin. I use Nosé-Hoover termostat
 and Parrinello-Rahman barostat. Ref T from 285 to 500K and ref P equals
 to
 1bar. Gromacs version 4.5.5. Exchange trials every 5 ps.
 If I try to add replica at a higher temperature the system crash, but I
 think it is a problem of equilibration.
 
 
 2013/5/1 XAvier Periole x.peri...@rug.nl
 
 
 Ok here is my current status on that REMD issue.
 
 For info: I use
 Temperature: v-rescale, tau_t = 2.0 ps
 Pressure: berendsen, tau_p = 5.0 ps,
 time step: dt=0.002 - 0.020 fs,
 COM removal on for bilayer/water separately
 
 The symptoms: explosion of the system after 2-5 steps following the
 swap,
 first sign is a huge jump in LJ interactions and pressure. This jump
 seems
 to be absorbed by the box size and temperature when possible … see
 example
 I provided earlier. A large VCM (velocity centre of mass?) is often
 associated with the crash. But also pressure scaling more than 1% ...
 
 1- the problem mentioned above remains in gmx-4.5.7 and it might
 actually
 got worse. I was able to run a 500 ns simulation with gmx405 using
 similar
 setup as for gmx457. The following point happened in gmx457.
 2- it persists with a time step of 2 fs. Actually all tests performed in
 the following used dt=2fs.
 3- if I perform an exchange that explodes within mdrun myself
 (externally
 to the remd gromacs by getting the gro file with the mdp adjusting the
 temperature) it goes all fine.
 4- the issue gets much worst when the consecutive replicas differ
 (different protein conformations and the box size etc) … explosion at
 first
 exchange.
 5- the use of parrinelo-raman does not help
 6- cancelling the centre of mass removal does not remove the problem.
 7- switching to NVT ensemble does not help but makes it worst (crash in
 2
 steps). All exchanges accepted at first attempt crash with the message
 Large VCM(group SOL): -0.0XXX , -0.XXX, -0.16XXX, Temp-cm:6.55XXX
 8- using a unique conformation (the same) for all replicas in the NVT
 REMD
 simulation after equilibration in the same NVT ensemble (for 1 ns)
 removes
 the problem.
 9- taking the equilibrated NVT conformations, equilibrate them in an NPT
 ensemble (1 ns) and let go the exchanges afterwards restores the
 problem …
 one exchange is not properly done at the second trial, while the first
 ones
 were fine. Well if errors were made that was with reasonable
 10- note also that the coarse grain I use is extremely forgiving,
 meaning
 you can perform really nasty transformations and run it further after
 simple minimisation … so even abrupt changes in temperatures should be
 fine
 and relax quickly.
 11- when looking at the conformations themselves nothing appears to have
 jumped over or nothing funky.
 
 At this point I am not sure what to think and what to do next. There is
 definitely something not going right during the exchanges.
 
 Anyone has been able to run a REMD simulation in an NPT ensemble without
 crashes? I would imagine someone has and something particular to my
 system
 is making it going wrong but I am really wondering what it could be. My
 feeling is that something relative to the box size or pressure is not
 going
 across but it might be something completely different, when the
 consecutive
 systems differ reasonably.
 
 However that would suggest that the manner the exchanges are made is
 severely wrong in some cases.
 
 Any help to resolve the problem would be greatly appreciated.
 
 XAvier.
 
 On Apr 26, 2013, at 9:21 AM, Mark Abraham mark.j.abra...@gmail.com
 wrote:
 
 On Thu, Apr 25, 2013 at 11:05 PM, XAvier Periole x.peri...@rug.nl
 wrote:
 
 
 Thanks for the answer. I'll check gmx4.5.7 and report back.
 
 I am not sure what you mean by GROMACS swaps the coordinates not the
 ensemble

Re: [gmx-users] issue in replica exchange

2013-05-02 Thread XAvier Periole

You mean working with or working on the code? 

I'll try gmx-4.6.1

On May 2, 2013, at 2:26 PM, Michael Shirts mrshi...@gmail.com wrote:

 Quick check here -- is 4.6 behaving correctly?  I actually spent some
 time working on REMD in 4.6, and it seems to be behaving  correctly in
 my hands with temperature and pressure control.
 
 Thanks for any additional info on this!
 
 On Thu, May 2, 2013 at 8:18 AM, Mark Abraham mark.j.abra...@gmail.com wrote:
 On Thu, May 2, 2013 at 12:58 PM, XAvier Periole x.peri...@rug.nl wrote:
 
 
 I saw that redmine report, which could be related but it seems to happen
 only for runs done outside the domain and particle decompositions.
 
 I'll fill up a red mine.
 
 Anything I could do to help speeding the fix?
 
 
 What'd be really nice is some thought on how one can demonstrate that the
 implementation of the exchange matches what would be expected from the
 theory. For T-exchange under NVT, it is sufficient to rescale velocities
 and quantities derived from them by the correct factor. That includes
 various things like T-coupling history and integrator half-step quantities
 (and does REMD with leap-frog make sense anyway?). For NPT, there's
 probably also some P-coupling quantities to scale, and the box to exchange.
 Anything I've missed? Hopefully virial contributions don't matter either
 way?
 
 Perhaps a decent first step is to hack the code to do a self exchange, by
 clearing the entire state and rebuilding with what would/should be received
 from an exchange with a hypothethetical replica in an identical
 pre-exchange state. Only if the code can do that (i.e. mdrun -reprod
 produces a trajectory indistinguishable from a run that does not attempt
 this self exchange) is it worth considering proper state exchanges, and the
 process of making the code do the former should illustrate what is required
 for the latter.
 
 Mark
 --
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Re: [gmx-users] issue in replica exchange

2013-05-02 Thread XAvier Periole

Some good news … 

The tpr files provided by Simone do NOT show abnormal behaviour! This good news 
:)) 

However after turning ON the particle decomposition option to mdrun (-pd) I got 
a warnings of water not being able to be settled and a crash. This was still 
with Simone's trips … I took that as a good sign! 

Then I went back to my system and changed the topology to be able to turn OFF 
the particle decomposition that I need to use due to a long bond … the system 
when right trough 650 ps with many exchanges without a complain. I would have 
to check the continuity in the energies, Temp and other but it seems to be 
quite clear:

The problem I am facing is located in the particle decomposition section of the 
code. 

I will fill a redmine and let see how to proceed from there. I won't be able to 
do this before middle of next week though.

Tks for your help,
XAvier.


On May 2, 2013, at 2:36 PM, Michael Shirts mrshi...@gmail.com wrote:

 Both.  So if 4.6.1 doesn't work, I want to know so we can patch it
 before 4.6.2 comes out.  If it does work, then there is probably stuff
 that can be backported.
 
 On Thu, May 2, 2013 at 8:32 AM, XAvier Periole x.peri...@rug.nl wrote:
 
 You mean working with or working on the code?
 
 I'll try gmx-4.6.1
 
 On May 2, 2013, at 2:26 PM, Michael Shirts mrshi...@gmail.com wrote:
 
 Quick check here -- is 4.6 behaving correctly?  I actually spent some
 time working on REMD in 4.6, and it seems to be behaving  correctly in
 my hands with temperature and pressure control.
 
 Thanks for any additional info on this!
 
 On Thu, May 2, 2013 at 8:18 AM, Mark Abraham mark.j.abra...@gmail.com 
 wrote:
 On Thu, May 2, 2013 at 12:58 PM, XAvier Periole x.peri...@rug.nl wrote:
 
 
 I saw that redmine report, which could be related but it seems to happen
 only for runs done outside the domain and particle decompositions.
 
 I'll fill up a red mine.
 
 Anything I could do to help speeding the fix?
 
 
 What'd be really nice is some thought on how one can demonstrate that the
 implementation of the exchange matches what would be expected from the
 theory. For T-exchange under NVT, it is sufficient to rescale velocities
 and quantities derived from them by the correct factor. That includes
 various things like T-coupling history and integrator half-step quantities
 (and does REMD with leap-frog make sense anyway?). For NPT, there's
 probably also some P-coupling quantities to scale, and the box to exchange.
 Anything I've missed? Hopefully virial contributions don't matter either
 way?
 
 Perhaps a decent first step is to hack the code to do a self exchange, by
 clearing the entire state and rebuilding with what would/should be received
 from an exchange with a hypothethetical replica in an identical
 pre-exchange state. Only if the code can do that (i.e. mdrun -reprod
 produces a trajectory indistinguishable from a run that does not attempt
 this self exchange) is it worth considering proper state exchanges, and the
 process of making the code do the former should illustrate what is required
 for the latter.
 
 Mark
 --
 gmx-users mailing listgmx-users@gromacs.org
 http://lists.gromacs.org/mailman/listinfo/gmx-users
 * Please search the archive at 
 http://www.gromacs.org/Support/Mailing_Lists/Search before posting!
 * Please don't post (un)subscribe requests to the list. Use the
 www interface or send it to gmx-users-requ...@gromacs.org.
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Re: [gmx-users] issue in replica exchange

2013-05-02 Thread XAvier Periole

I'll look at the 4.6.1 version next week, I could install it but I got a 
conflict between the environmental variable defining openMP variable but I 
turned it off during compilation … 

You could try to run on particle decomposition to see if you get a problem … it 
should one quite quick.

On May 2, 2013, at 2:36 PM, Michael Shirts mrshi...@gmail.com wrote:

 Both.  So if 4.6.1 doesn't work, I want to know so we can patch it
 before 4.6.2 comes out.  If it does work, then there is probably stuff
 that can be backported.
 
 On Thu, May 2, 2013 at 8:32 AM, XAvier Periole x.peri...@rug.nl wrote:
 
 You mean working with or working on the code?
 
 I'll try gmx-4.6.1
 
 On May 2, 2013, at 2:26 PM, Michael Shirts mrshi...@gmail.com wrote:
 
 Quick check here -- is 4.6 behaving correctly?  I actually spent some
 time working on REMD in 4.6, and it seems to be behaving  correctly in
 my hands with temperature and pressure control.
 
 Thanks for any additional info on this!
 
 On Thu, May 2, 2013 at 8:18 AM, Mark Abraham mark.j.abra...@gmail.com 
 wrote:
 On Thu, May 2, 2013 at 12:58 PM, XAvier Periole x.peri...@rug.nl wrote:
 
 
 I saw that redmine report, which could be related but it seems to happen
 only for runs done outside the domain and particle decompositions.
 
 I'll fill up a red mine.
 
 Anything I could do to help speeding the fix?
 
 
 What'd be really nice is some thought on how one can demonstrate that the
 implementation of the exchange matches what would be expected from the
 theory. For T-exchange under NVT, it is sufficient to rescale velocities
 and quantities derived from them by the correct factor. That includes
 various things like T-coupling history and integrator half-step quantities
 (and does REMD with leap-frog make sense anyway?). For NPT, there's
 probably also some P-coupling quantities to scale, and the box to exchange.
 Anything I've missed? Hopefully virial contributions don't matter either
 way?
 
 Perhaps a decent first step is to hack the code to do a self exchange, by
 clearing the entire state and rebuilding with what would/should be received
 from an exchange with a hypothethetical replica in an identical
 pre-exchange state. Only if the code can do that (i.e. mdrun -reprod
 produces a trajectory indistinguishable from a run that does not attempt
 this self exchange) is it worth considering proper state exchanges, and the
 process of making the code do the former should illustrate what is required
 for the latter.
 
 Mark
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Re: [gmx-users] issue in replica exchange

2013-05-02 Thread XAvier Periole

Are confirming that you reproduce the problem with gmx-4.6.1 or simply 
summarizing in case we lose track :))

On May 2, 2013, at 23:31, Michael Shirts mrshi...@gmail.com wrote:

 So to summarize -- the problem appears to be with particle decomposition.
 
 On Thu, May 2, 2013 at 4:15 PM, XAvier Periole x.peri...@rug.nl wrote:
 
 I'll look at the 4.6.1 version next week, I could install it but I got a 
 conflict between the environmental variable defining openMP variable but I 
 turned it off during compilation …
 
 You could try to run on particle decomposition to see if you get a problem … 
 it should one quite quick.
 
 On May 2, 2013, at 2:36 PM, Michael Shirts mrshi...@gmail.com wrote:
 
 Both.  So if 4.6.1 doesn't work, I want to know so we can patch it
 before 4.6.2 comes out.  If it does work, then there is probably stuff
 that can be backported.
 
 On Thu, May 2, 2013 at 8:32 AM, XAvier Periole x.peri...@rug.nl wrote:
 
 You mean working with or working on the code?
 
 I'll try gmx-4.6.1
 
 On May 2, 2013, at 2:26 PM, Michael Shirts mrshi...@gmail.com wrote:
 
 Quick check here -- is 4.6 behaving correctly?  I actually spent some
 time working on REMD in 4.6, and it seems to be behaving  correctly in
 my hands with temperature and pressure control.
 
 Thanks for any additional info on this!
 
 On Thu, May 2, 2013 at 8:18 AM, Mark Abraham mark.j.abra...@gmail.com 
 wrote:
 On Thu, May 2, 2013 at 12:58 PM, XAvier Periole x.peri...@rug.nl wrote:
 
 
 I saw that redmine report, which could be related but it seems to happen
 only for runs done outside the domain and particle decompositions.
 
 I'll fill up a red mine.
 
 Anything I could do to help speeding the fix?
 
 What'd be really nice is some thought on how one can demonstrate that the
 implementation of the exchange matches what would be expected from the
 theory. For T-exchange under NVT, it is sufficient to rescale velocities
 and quantities derived from them by the correct factor. That includes
 various things like T-coupling history and integrator half-step 
 quantities
 (and does REMD with leap-frog make sense anyway?). For NPT, there's
 probably also some P-coupling quantities to scale, and the box to 
 exchange.
 Anything I've missed? Hopefully virial contributions don't matter either
 way?
 
 Perhaps a decent first step is to hack the code to do a self exchange, 
 by
 clearing the entire state and rebuilding with what would/should be 
 received
 from an exchange with a hypothethetical replica in an identical
 pre-exchange state. Only if the code can do that (i.e. mdrun -reprod
 produces a trajectory indistinguishable from a run that does not attempt
 this self exchange) is it worth considering proper state exchanges, and 
 the
 process of making the code do the former should illustrate what is 
 required
 for the latter.
 
 Mark
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Re: [gmx-users] local pressure

2013-05-01 Thread XAvier Periole

The use of the original code is quite straightforward, the post processing is a 
bit more confusing but quite accessible. 

We have been using this code (the one available on the site) and related 
version in the lab and we definitely would find it very sad to not keep this 
feature available in GROMACS.

On May 1, 2013, at 2:34 AM, Justin Lemkul jalem...@vt.edu wrote:

 
 
 On 4/30/13 8:01 PM, Sikandar Mashayak wrote:
 Hi
 
 I found the branch of gromacs code called localpressure-4.0 at
 http://redmine.gromacs.org/projects/gromacs/repository/show?rev=localpressure-4-0.
 I am wondering whether this code can compute the spatial variation of
 pressure in given system. And if it does, how stable is this branch? Are
 there any known issues with it? And any particular reason this is not
 included in main gromacs releases?
 
 
 Lack of documentation has made it very difficult to use, it is extremely 
 slow, and no one ever asks about it except once every few years.  All of 
 those factors make it unlikely to ever incorporate into an actual release.  
 Given that the development process has gone on for years in the absence of 
 any real interest in the localpressure branch, it's probably more trouble 
 than it's worth to get it up and running effectively.
 
 -Justin
 
 -- 
 
 
 Justin A. Lemkul, Ph.D.
 Research Scientist
 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] local pressure

2013-05-01 Thread XAvier Periole


Well I am not the expert. O.H.S. Ollila, M. Louhivuori and E. Lindahl are :)).

The paper related to the use would be: 
Ollila et al, PRL 102, 078101 (2009)
Ollila et al, Biophysical Journal (100)1651–59

On May 1, 2013, at 5:48 PM, Sikandar Mashayak symasha...@gmail.com wrote:

 Thanks Xavier
 
 
 Can you please elaborate on how to use and post-process the local pressure
 version of gromacs? Do you have any examples or reference article?
 
 May be you can create a HowTo wiki as Justin suggested, it would be of
 great help.
 
 Thanks
 Sikandar
 
 
 On Wed, May 1, 2013 at 5:03 AM, Justin Lemkul jalem...@vt.edu wrote:
 
 
 
 On 5/1/13 5:12 AM, XAvier Periole wrote:
 
 
 The use of the original code is quite straightforward, the post
 processing is a bit more confusing but quite accessible.
 
 
 That would be a great topic for a wiki How-To.
 
 
 We have been using this code (the one available on the site) and related
 version in the lab and we definitely would find it very sad to not keep
 this feature available in GROMACS.
 
 
 I never said it would go away, but given the fact that there have been no
 updates to the git branch in over 3 years, it's simply unlikely that anyone
 has cared to move it forward.  If someone wants to update the code to be
 compatible with 4.6, that would be a welcome contribution.  Lack of any
 request for improvements and inclusion in an official release has likely
 led to the decline in interest from the development team.  If you want
 something included, you should file a feature request on
 redmine.gromacs.org - it's the only official way we keep track of fixes
 and features.  If it's not there, it likely won't get addressed until one
 of the developers has a compelling need to work on it.
 
 -Justin
 
 
 On May 1, 2013, at 2:34 AM, Justin Lemkul jalem...@vt.edu wrote:
 
 
 
 On 4/30/13 8:01 PM, Sikandar Mashayak wrote:
 
 Hi
 
 I found the branch of gromacs code called localpressure-4.0 at
 http://redmine.gromacs.org/**projects/gromacs/repository/**
 show?rev=localpressure-4-0http://redmine.gromacs.org/projects/gromacs/repository/show?rev=localpressure-4-0
 .
 I am wondering whether this code can compute the spatial variation of
 pressure in given system. And if it does, how stable is this branch? Are
 there any known issues with it? And any particular reason this is not
 included in main gromacs releases?
 
 
 Lack of documentation has made it very difficult to use, it is extremely
 slow, and no one ever asks about it except once every few years.  All of
 those factors make it unlikely to ever incorporate into an actual release.
 Given that the development process has gone on for years in the absence of
 any real interest in the localpressure branch, it's probably more trouble
 than it's worth to get it up and running effectively.
 
 -Justin
 
 --
 ==**==
 
 Justin A. Lemkul, Ph.D.
 Research Scientist
 Department of Biochemistry
 Virginia Tech
 Blacksburg, VA
 jalemkul[at]vt.edu | (540) 231-9080
 http://www.bevanlab.biochem.**vt.edu/Pages/Personal/justinhttp://www.bevanlab.biochem.vt.edu/Pages/Personal/justin
 
 ==**==
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 --
 ==**==
 
 Justin A. Lemkul, Ph.D.
 Research Scientist
 Department of Biochemistry
 Virginia Tech
 Blacksburg, VA
 jalemkul[at]vt.edu | (540) 231-9080
 http://www.bevanlab.biochem.**vt.edu/Pages/Personal/justinhttp://www.bevanlab.biochem.vt.edu/Pages/Personal/justin
 
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Re: [gmx-users] issue in replica exchange

2013-05-01 Thread XAvier Periole

Ok here is my current status on that REMD issue. 

For info: I use
Temperature: v-rescale, tau_t = 2.0 ps
Pressure: berendsen, tau_p = 5.0 ps, 
time step: dt=0.002 - 0.020 fs, 
COM removal on for bilayer/water separately

The symptoms: explosion of the system after 2-5 steps following the swap, first 
sign is a huge jump in LJ interactions and pressure. This jump seems to be 
absorbed by the box size and temperature when possible … see example I provided 
earlier. A large VCM (velocity centre of mass?) is often associated with the 
crash. But also pressure scaling more than 1% ...

1- the problem mentioned above remains in gmx-4.5.7 and it might actually got 
worse. I was able to run a 500 ns simulation with gmx405 using similar setup as 
for gmx457. The following point happened in gmx457.
2- it persists with a time step of 2 fs. Actually all tests performed in the 
following used dt=2fs.
3- if I perform an exchange that explodes within mdrun myself (externally to 
the remd gromacs by getting the gro file with the mdp adjusting the 
temperature) it goes all fine. 
4- the issue gets much worst when the consecutive replicas differ (different 
protein conformations and the box size etc) … explosion at first exchange. 
5- the use of parrinelo-raman does not help
6- cancelling the centre of mass removal does not remove the problem.
7- switching to NVT ensemble does not help but makes it worst (crash in 2 
steps). All exchanges accepted at first attempt crash with the message Large 
VCM(group SOL): -0.0XXX , -0.XXX, -0.16XXX, Temp-cm:6.55XXX
8- using a unique conformation (the same) for all replicas in the NVT REMD 
simulation after equilibration in the same NVT ensemble (for 1 ns) removes the 
problem. 
9- taking the equilibrated NVT conformations, equilibrate them in an NPT 
ensemble (1 ns) and let go the exchanges afterwards restores the problem … one 
exchange is not properly done at the second trial, while the first ones were 
fine. Well if errors were made that was with reasonable 
10- note also that the coarse grain I use is extremely forgiving, meaning you 
can perform really nasty transformations and run it further after simple 
minimisation … so even abrupt changes in temperatures should be fine and relax 
quickly. 
11- when looking at the conformations themselves nothing appears to have jumped 
over or nothing funky. 

At this point I am not sure what to think and what to do next. There is 
definitely something not going right during the exchanges. 

Anyone has been able to run a REMD simulation in an NPT ensemble without 
crashes? I would imagine someone has and something particular to my system is 
making it going wrong but I am really wondering what it could be. My feeling is 
that something relative to the box size or pressure is not going across but it 
might be something completely different, when the consecutive systems differ 
reasonably. 

However that would suggest that the manner the exchanges are made is severely 
wrong in some cases. 

Any help to resolve the problem would be greatly appreciated.

XAvier.

On Apr 26, 2013, at 9:21 AM, Mark Abraham mark.j.abra...@gmail.com wrote:

 On Thu, Apr 25, 2013 at 11:05 PM, XAvier Periole x.peri...@rug.nl wrote:
 
 
 Thanks for the answer. I'll check gmx4.5.7 and report back.
 
 I am not sure what you mean by GROMACS swaps the coordinates not the
 ensemble data. The coupling to P and T and not exchanged with it?
 
 
 The code in src/kernel/repl_ex.c:
 
 static void exchange_state(const gmx_multisim_t *ms, int b, t_state *state)
 {
/* When t_state changes, this code should be updated. */
int ngtc, nnhpres;
ngtc= state-ngtc * state-nhchainlength;
nnhpres = state-nnhpres* state-nhchainlength;
exchange_rvecs(ms, b, state-box, DIM);
exchange_rvecs(ms, b, state-box_rel, DIM);
exchange_rvecs(ms, b, state-boxv, DIM);
exchange_reals(ms, b, (state-veta), 1);
exchange_reals(ms, b, (state-vol0), 1);
exchange_rvecs(ms, b, state-svir_prev, DIM);
exchange_rvecs(ms, b, state-fvir_prev, DIM);
exchange_rvecs(ms, b, state-pres_prev, DIM);
exchange_doubles(ms, b, state-nosehoover_xi, ngtc);
exchange_doubles(ms, b, state-nosehoover_vxi, ngtc);
exchange_doubles(ms, b, state-nhpres_xi, nnhpres);
exchange_doubles(ms, b, state-nhpres_vxi, nnhpres);
exchange_doubles(ms, b, state-therm_integral, state-ngtc);
exchange_rvecs(ms, b, state-x, state-natoms);
exchange_rvecs(ms, b, state-v, state-natoms);
exchange_rvecs(ms, b, state-sd_X, state-natoms);
 }
 
 I mis-stated last night - there *is* exchange of ensemble data, but it is
 incomplete. In particular, state-ekinstate is not exchanged. Probably it
 is incomplete because the 9-year-old comment about t_state changing is in a
 location that nobody changing t_state will see. And serializing a complex C
 data structure over MPI is tedious at best. But that is not really an
 excuse for the non-modularity GROMACS has for many of its key data

Re: [gmx-users] Re: genbox box size problem

2013-04-30 Thread XAvier Periole

We have noticed that g_genbox issue with MARTINI but have not new able to 
understand where it actually comes from. It might be a bug or just a miss 
communication of the vdw radius with genbox that appears only with large 
spheres. 

On Apr 29, 2013, at 19:50, alex.bjorling alex.bjorl...@gmail.com wrote:

 Justin Lemkul wrote
 I have seen this exact problem posted before.  The coordinates of the
 water box 
 provided by MARTINI have some coordinate values that basically coincide
 across 
 the periodic box.  With genconf, you can apply the -dist option to space
 them 
 out slightly, then re-equilibrate before using the new configuration as
 input 
 into genbox.
 
 I don't think that's true. Stacking boxes with -nbox 3 3 3 (without -dist)
 gives a big box which you can minimize and equilibrate with no trouble. Both
 with and without -dist 0.21 0.21 0.21 (0.21 is a suitable MARTINI -vdwd for
 genbox), you get big water boxes which behave well. The problems start when
 you use them as solvents in genbox.
 
 Xavier's suggestion (stack, minimize, equilibrate, manually cut with a
 script) works fine, thanks for the suggestion.
 
 Seems to me there might be a bug in genbox, but I'm not the right person to
 make such claims.
 
 Alex
 
 
 
 --
 View this message in context: 
 http://gromacs.5086.x6.nabble.com/genbox-box-size-problem-tp5007753p5007768.html
 Sent from the GROMACS Users Forum mailing list archive at Nabble.com.
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Re: [gmx-users] genbox box size problem

2013-04-29 Thread XAvier Periole

genbox works best when the box size of the solute is defined as the same as of 
the water one used to solvate it. So you can build a water box with the 
dimensions you want and them use it. 

You can build a water box by using genconf -nbox and use a script to cut to the 
dimensions you need, minimize, equilibrate ... 

Using a bigger box size should work too but it might need to be 
positioned/centered correctly and the solute too ... 

On Apr 29, 2013, at 11:30, Alexander Björling alex.bjorl...@gmail.com wrote:

 Dear users,
 
 I am trying to solvate a MARTINI model, using a pre-equilibrated
 coarse-grained water box. This usually works fine with the following
 command.
 
 genbox -cs water-1bar-303K.gro -cp 01min.gro -o 02solv -vdwd 0.21
 
 When I recently increased the box size things started going wrong. As the
 simulation box got bigger than the (-cs) water box, the solvated structure
 ended up containing clear block-shaped regions of higher and lower solvent
 density. I obviously tried stacking the (-cs) box first to make it bigger
 than the box in the (-cp) file,
 
 genconf -f water-1bar-303K.gro -o water-1bar-303K_big.gro -nbox 3 3 3
 
 but the problem persisted. Waters actually coincide in the solvated
 structure, so energy minimization is obviously hopeless.
 
 Is genbox behaving unexpectedly or is this likely an input problem?
 Cheers,
 Alex
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Re: [gmx-users] Questions about the MFFA boundery implementation of Gromacs?

2013-04-27 Thread XAvier Periole

It is not clear what you are asking. Could you try to reformulate your 
problem/question?

Did you read the Louhivuori-PNAS papers? There are lots of details in the 
supplementary material. 

On Apr 27, 2013, at 6:43, song.yongshun song.yongs...@163.com wrote:

 Dear all:
 I was using the MFFA version of Gromacs which is provided by m.j.louhivuori 
 at http://md.chem.rug.nl/~mara/mffa.html.
 I have some quesition about this version:
 
 i.I saw the implementation of MFFA always with the flip-flop of lipid.Can I 
 apply the flip-flop with this MFFA version of Gromacs ?
 ii.I also saw the description of implementation of MFFA along only one 
 direction.Is this available in this MFFA version of Gromacs?
 
 
 Anyone who is familar with it help me.
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Re: [gmx-users] RE: Martini with PME, temp two low

2013-04-26 Thread XAvier Periole

nstlist of 2 is a be extreme! Did you try 5! It should be fine … but if your 
are happy that's ok :))

On Apr 26, 2013, at 12:37 PM, ABEL Stephane 175950 stephane.a...@cea.fr wrote:

 Hi Xavier, 
 
 I used a dt of 10 ps with nstlist of 2. In that case the Temp of the system 
 is stable and the energy well conserved (400 ns of run). I do know if it is 
 optimal but it works for my system. 
 
 Stephane
 
 
 
 --
 
 Message: 1
 Date: Fri, 26 Apr 2013 07:58:12 +0200
 From: XAvier Periole x.peri...@rug.nl
 Subject: Re: [gmx-users] Re: Martini with PME,  temp two low (ABEL
Stephane 175950)
 To: Discussion list for GROMACS users gmx-users@gromacs.org
 Message-ID: 6d1fd74e-91bb-4c0c-95ce-e863924dd...@rug.nl
 Content-Type: text/plain;   charset=us-ascii
 
 
 Good. Note however that we do get the right temperature with a dt=20fs with 
 Martini so you energy leak might be in the cutoff scheme or the system is 
 really badly equilibrated.
 
 On Apr 25, 2013, at 18:23, ABEL Stephane 175950 stephane.a...@cea.fr wrote:
 
 Xavier
 
 I have followed your suggestion and did a longer NPT equilibration with 
 smaller dt and ntlist values and It works. The Energy and Temp  reach to 
 stables values as i want.
 
 thank you again  for your help
 
 Stephane
 
 --
 
 Message: 2
 Date: Thu, 25 Apr 2013 14:17:00 +
 From: ABEL Stephane 175950 stephane.a...@cea.fr
 Subject: [gmx-users] Re: Martini with PME, temp two low
 To: gmx-users@gromacs.org gmx-users@gromacs.org
 Message-ID:
   3e39b768bb199548ab18f7289e7534af1a818...@exdag0-b0.intra.cea.fr
 Content-Type: text/plain; charset=us-ascii
 
 @ Vitaly
 of course. I know that. My system is neutral  but with charged particles 
 (AOT and Na+).
 
 @Xavier
 I will try your suggestion and equilibrate my system for a longer period
 
 Thanks again
 
 Stephane
 
 
 
 --
 
 Message: 1
 Date: Thu, 25 Apr 2013 15:52:09 +0200
 From: XAvier Periole x.peri...@rug.nl
 Subject: Re: [gmx-users] Martini with PME, temp two low
 To: Discussion list for GROMACS users gmx-users@gromacs.org
 Message-ID: 0a7b7d0a-b419-4d3d-826b-e6d61de6d...@rug.nl
 Content-Type: text/plain; charset=windows-1252
 
 
 Well ? 400 ps is rather small and you can expect deviations from so short 
 simulations if you start from an non-equilibrated system. I am not sure what 
 the void is but this indicates that your system might not be equilibrated ?
 
 You can try to decrease the time step and nstlist to see if you the drop of 
 temperature is due a flow of energy.
 
 On Apr 25, 2013, at 3:26 PM, ABEL Stephane 175950 stephane.a...@cea.fr 
 wrote:
 
 Hello Xavier,
 
 Thank you for your response.
 
 nstlist = 10 and the rlist = 1.0
 My mistake, i did not changes these values when i switched to PME,
 
 I have rerun the simulations for 400 ps in NPT with these changes and 
 plotted Epot and Temp vs Time The Epot and Temp values are not stables. The 
 average Temp of the system  is better than previously but fluctuate around 
 (294 K) instead of 298 K . Note i use gmx4.5.5 to do my calculations.
 
 I have also visualized my  system at the end of the NPT run, the  na+, 
 water, surfactant, octane molecules  form a slab with void
 
 What's wrong ?
 
 Stephane
 
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[gmx-users] issue in replica exchange

2013-04-25 Thread XAvier Periole

Hi,

I have been recently using the REMD code in gmx-407 and gmx-453 and got a few 
systems crashing for unclear reasons so far. The main tests I made are using 
gmx407 but it is all reproducible with gmx453. The crashing was also reproduced 
(not necessarily at the same time point) on several architectures. 

The system is made of a pair of proteins in a membrane patch and for which the 
relative orientation is controlled by non-native bond/angles/dihedrals to 
perform an umbrella sampling. I use the MARTINI force field but that might not 
be relevant here. 

The crashes occur following exchanges that do not seem to occur the correct way 
and preceded by pressure scaling warnings … indicative of a strong 
destabilisation of the system and eventual explosion. Some information seems to 
be exchanged inaccurately. 

Trying to nail down the problem I got stuck and may be some one can help. I 
placed a pdf file showing plots of bonded/nonbonded energies, temperatures, box 
size etc … around an exchange that does not lead to a crash (here: 
md.chem.rug.nl/~periole/remd-issue.pdf). I plotted stuff every step with the 
temperature colour coded as indicated in the first figure. 

From the figure it appears that the step right after the exchange there is a 
huge jump of Potential energy coming from the LJ(SR) part of it. Although there 
are some small discontinuities in the progression of the bond and angle energy 
around the exchange they seem to fine. The temperature and box size seem to 
respond to it a few step latter while the pressure seems to be affected right 
away but potentially as the Epot will affect the viral and thus the Pressure. 

The other potential clue is that the jumps reduce with the strength of the 
pressure coupling. A 1/2 ps tau_p (Berendsen) will lead to a crash while a 
5/10/20 ps won't. Inspection of the time evolution of the Epot, box … indicates 
that the magnitude of the jumps is reduced and the system ca handle the 
problem. 

One additional info since I first posted the problem (delayed by the file first 
attached but now given with a link) the problem is accentuated when the 
replicas differ in conformation. I am looking at the actual differences as 
you'll read this email.

That is as far as I could go. Any suggestion is welcome.

XAvier.
MD-Group / Univ. of Groningen
The Netherlands--
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Re: [gmx-users] Martini with PME, temp two low

2013-04-25 Thread XAvier Periole

Did you visualise the system? T in function of time? Epot in function of time? 

As a side note (not relevant for PME) the mix of nstlist = 10 and the rlist = 
1.0 is pretty bad! You want at least rlist=1.2 when nstlist=5 and rlist=1.4 if 
nstlist =10.

On Apr 25, 2013, at 1:10 PM, ABEL Stephane 175950 stephane.a...@cea.fr wrote:

 Hello all, 
 
 I am trying to test the martini force field with PME for a charged system 
 that contains na+, water, surfactant, octane molecules at 298K and P=0.1MPa. 
 My system works well, if i use the standard shift parameters (correct temp, 
 and pressure). But for for the simulation with PME , the temp of the system 
 decrease to  290 K. Below my *.mdp parameters for a NPT equil at 298K 
 
 
 integrator   = md
 dt   = 0.020
 nsteps   = 1 ; 200ps
 nstcomm  = 10
 comm-grps=
 ;refcoord_scaling = com
 
 nstxout  = 0
 nstvout  = 0
 nstfout  = 0
 nstlog   = 1000
 nstenergy= 100
 ;nstxtcout= 1000
 xtc_precision= 100
 ;xtc-grps =
 energygrps   = AOT W ION OCT
 
 nstlist  = 10
 ns_type  = grid
 pbc  = xyz
 rlist= 1.
 
 ; PME parameters
 coulombtype  = PME
 rcoulomb = 1.2
 rvdw = 1.2
 fourierspacing   = 0.12
 fourier_nx   = 0
 fourier_ny   = 0
 fourier_nz   = 0
 pme_order= 4
 
 tcoupl   = v-rescale
 tc-grps  = AOT_W_ION OCT
 tau_t= 1.0 1.0
 ref_t= 298 298
 Pcoupl   = berendsen
 Pcoupltype   = isotropic
 tau_p= 1.0
 compressibility  = 4.5e-5
 ref_p= 1.0
 
 ;gen_vel  = no
 ;gen_temp = 0
 ;gen_seed = 473529
 
 
 ; MARTINI and CONSTRAINTS
 ; for ring systems and stiff bonds constraints are defined
 ; which are best handled using Lincs.
 
 constraints  = none
 constraint_algorithm = Lincs
 unconstrained_start  = no
 lincs_order  = 4
 lincs_warnangle  = 3
 
 
 Results obtained with W/ PME 
 
   Statistics over 10001 steps using 1001 frames
 
   Energies (kJ/mol)
   Bond   G96AngleLJ (SR)   Coulomb (SR)   Coul. recip.
1.63789e+041.25195e+03   -4.02093e+05   -8.22079e+03   -4.86843e+04
  PotentialKinetic En.   Total EnergyTemperature Pressure (bar)
   -4.41367e+057.81801e+04   -3.63187e+052.90373e+02   -1.76470e+01
T-AOT_W_ION  T-OCT
2.90629e+022.90357e+02
 
 Results W:o PME
 
   Energies (kJ/mol)
   Bond   G96AngleLJ (SR)   Coulomb (SR)  Potential
1.60482e+041.24820e+03   -3.34608e+05   -7.33665e+02   -3.18046e+05
Kinetic En.   Total EnergyTemperature Pressure (bar)
8.02685e+04   -2.3e+052.98129e+02   -3.07123e+01
 
  Box-X  Box-Y  Box-Z
1.52926e+011.52926e+011.52926e+01
 
 
T-AOT_W_ION  T-OCT
2.98141e+022.98129e+02
 
 
 Did I miss something ?
 
 
 Note that for the moment i do not use the polarizable water model.
 
 Thanks for your help 
 
 Stephane
 
 
 
 
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Re: [gmx-users] Martini with PME, temp two low

2013-04-25 Thread XAvier Periole

Well … 400 ps is rather small and you can expect deviations from so short 
simulations if you start from an non-equilibrated system. I am not sure what 
the void is but this indicates that your system might not be equilibrated … 

You can try to decrease the time step and nstlist to see if you the drop of 
temperature is due a flow of energy. 

On Apr 25, 2013, at 3:26 PM, ABEL Stephane 175950 stephane.a...@cea.fr wrote:

 Hello Xavier, 
 
 Thank you for your response. 
 
 nstlist = 10 and the rlist = 1.0 
 My mistake, i did not changes these values when i switched to PME,
 
 I have rerun the simulations for 400 ps in NPT with these changes and plotted 
 Epot and Temp vs Time The Epot and Temp values are not stables. The average 
 Temp of the system  is better than previously but fluctuate around (294 K) 
 instead of 298 K . Note i use gmx4.5.5 to do my calculations.
 
 I have also visualized my  system at the end of the NPT run, the  na+, water, 
 surfactant, octane molecules  form a slab with void
 
 What's wrong ?
 
 Stephane 
 
 
 
 --
 
 Message: 5
 Date: Thu, 25 Apr 2013 13:34:21 +0200
 From: XAvier Periole x.peri...@rug.nl
 Subject: Re: [gmx-users] Martini with PME, temp two low
 To: Discussion list for GROMACS users gmx-users@gromacs.org
 Message-ID: 4632c83b-cd6f-4c92-b887-a1c39dff4...@rug.nl
 Content-Type: text/plain; charset=us-ascii
 
 
 Did you visualise the system? T in function of time? Epot in function of time?
 
 As a side note (not relevant for PME) the mix of nstlist = 10 and the rlist = 
 1.0 is pretty bad! You want at least rlist=1.2 when nstlist=5 and rlist=1.4 
 if nstlist =10.
 
 On Apr 25, 2013, at 1:10 PM, ABEL Stephane 175950 stephane.a...@cea.fr 
 wrote:
 
 Hello all,
 
 I am trying to test the martini force field with PME for a charged system 
 that contains na+, water, surfactant, octane molecules at 298K and P=0.1MPa. 
 My system works well, if i use the standard shift parameters (correct temp, 
 and pressure). But for for the simulation with PME , the temp of the system 
 decrease to  290 K. Below my *.mdp parameters for a NPT equil at 298K
 
 
 integrator   = md
 dt   = 0.020
 nsteps   = 1 ; 200ps
 nstcomm  = 10
 comm-grps=
 ;refcoord_scaling = com
 
 nstxout  = 0
 nstvout  = 0
 nstfout  = 0
 nstlog   = 1000
 nstenergy= 100
 ;nstxtcout= 1000
 xtc_precision= 100
 ;xtc-grps =
 energygrps   = AOT W ION OCT
 
 nstlist  = 10
 ns_type  = grid
 pbc  = xyz
 rlist= 1.
 
 ; PME parameters
 coulombtype  = PME
 rcoulomb = 1.2
 rvdw = 1.2
 fourierspacing   = 0.12
 fourier_nx   = 0
 fourier_ny   = 0
 fourier_nz   = 0
 pme_order= 4
 
 tcoupl   = v-rescale
 tc-grps  = AOT_W_ION OCT
 tau_t= 1.0 1.0
 ref_t= 298 298
 Pcoupl   = berendsen
 Pcoupltype   = isotropic
 tau_p= 1.0
 compressibility  = 4.5e-5
 ref_p= 1.0
 
 ;gen_vel  = no
 ;gen_temp = 0
 ;gen_seed = 473529
 
 
 ; MARTINI and CONSTRAINTS
 ; for ring systems and stiff bonds constraints are defined
 ; which are best handled using Lincs.
 
 constraints  = none
 constraint_algorithm = Lincs
 unconstrained_start  = no
 lincs_order  = 4
 lincs_warnangle  = 3
 
 
 Results obtained with W/ PME
 
  Statistics over 10001 steps using 1001 frames
 
  Energies (kJ/mol)
  Bond   G96AngleLJ (SR)   Coulomb (SR)   Coul. recip.
   1.63789e+041.25195e+03   -4.02093e+05   -8.22079e+03   -4.86843e+04
 PotentialKinetic En.   Total EnergyTemperature Pressure (bar)
  -4.41367e+057.81801e+04   -3.63187e+052.90373e+02   -1.76470e+01
   T-AOT_W_ION  T-OCT
   2.90629e+022.90357e+02
 
 Results W:o PME
 
  Energies (kJ/mol)
  Bond   G96AngleLJ (SR)   Coulomb (SR)  Potential
   1.60482e+041.24820e+03   -3.34608e+05   -7.33665e+02   -3.18046e+05
   Kinetic En.   Total EnergyTemperature Pressure (bar)
   8.02685e+04   -2.3e+052.98129e+02   -3.07123e+01
 
 Box-X  Box-Y  Box-Z
   1.52926e+011.52926e+011.52926e+01
 
 
   T-AOT_W_ION  T-OCT
   2.98141e+022.98129e+02
 
 
 Did I miss something ?
 
 
 Note that for the moment i do not use the polarizable water model.
 
 Thanks for your help
 
 Stephane
 
 
 
 
 --
 gmx-users mailing listgmx-users@gromacs.org
 http://lists.gromacs.org/mailman/listinfo/gmx-users
 * Please search the archive at 
 http://www.gromacs.org/Support

Re: [gmx-users] issue in replica exchange

2013-04-25 Thread XAvier Periole

Thanks for the answer. I'll check gmx4.5.7 and report back. 

I am not sure what you mean by GROMACS swaps the coordinates not the ensemble 
data. The coupling to P and T and not exchanged with it? That would explain 
what I see, but let see what 4.5.7 has to say first. 

Tks. 

On Apr 25, 2013, at 22:40, Mark Abraham mark.j.abra...@gmail.com wrote:

 Thanks for the good report. There have been some known issues about the
 timing of coupling stages with respect to various intervals between GROMACS
 events for some algorithms. There are a lot of fixed problems in 4.5.7 that
 are not specific to REMD, but I have a few lingering doubts about whether
 we should be exchanging (scaled) coupling values along with the
 coordinates. (Unlike most REMD implementations, GROMACS swaps the
 coordinates, not the ensemble data.) If you can reproduce those kinds of
 symptoms in 4.5.7 (whether or not they then crash) then there looks like
 there may be a problem with the REMD implementation that is perhaps evident
 only with the kind of large time step Martini takes?
 
 Mark
 
 
 On Thu, Apr 25, 2013 at 1:28 PM, XAvier Periole x.peri...@rug.nl wrote:
 
 
 Hi,
 
 I have been recently using the REMD code in gmx-407 and gmx-453 and got a
 few systems crashing for unclear reasons so far. The main tests I made are
 using gmx407 but it is all reproducible with gmx453. The crashing was also
 reproduced (not necessarily at the same time point) on several
 architectures.
 
 The system is made of a pair of proteins in a membrane patch and for which
 the relative orientation is controlled by non-native bond/angles/dihedrals
 to perform an umbrella sampling. I use the MARTINI force field but that
 might not be relevant here.
 
 The crashes occur following exchanges that do not seem to occur the
 correct way and preceded by pressure scaling warnings … indicative of a
 strong destabilisation of the system and eventual explosion. Some
 information seems to be exchanged inaccurately.
 
 Trying to nail down the problem I got stuck and may be some one can help.
 I placed a pdf file showing plots of bonded/nonbonded energies,
 temperatures, box size etc … around an exchange that does not lead to a
 crash (here: md.chem.rug.nl/~periole/remd-issue.pdf). I plotted stuff
 every step with the temperature colour coded as indicated in the first
 figure.
 
 From the figure it appears that the step right after the exchange there is
 a huge jump of Potential energy coming from the LJ(SR) part of it. Although
 there are some small discontinuities in the progression of the bond and
 angle energy around the exchange they seem to fine. The temperature and box
 size seem to respond to it a few step latter while the pressure seems to be
 affected right away but potentially as the Epot will affect the viral and
 thus the Pressure.
 
 The other potential clue is that the jumps reduce with the strength of the
 pressure coupling. A 1/2 ps tau_p (Berendsen) will lead to a crash while a
 5/10/20 ps won't. Inspection of the time evolution of the Epot, box …
 indicates that the magnitude of the jumps is reduced and the system ca
 handle the problem.
 
 One additional info since I first posted the problem (delayed by the file
 first attached but now given with a link) the problem is accentuated when
 the replicas differ in conformation. I am looking at the actual differences
 as you'll read this email.
 
 That is as far as I could go. Any suggestion is welcome.
 
 XAvier.
 MD-Group / Univ. of Groningen
 The Netherlands--
 gmx-users mailing listgmx-users@gromacs.org
 http://lists.gromacs.org/mailman/listinfo/gmx-users
 * Please search the archive at
 http://www.gromacs.org/Support/Mailing_Lists/Search before posting!
 * Please don't post (un)subscribe requests to the list. Use the
 www interface or send it to gmx-users-requ...@gromacs.org.
 * Can't post? Read http://www.gromacs.org/Support/Mailing_Lists
 -- 
 gmx-users mailing listgmx-users@gromacs.org
 http://lists.gromacs.org/mailman/listinfo/gmx-users
 * Please search the archive at 
 http://www.gromacs.org/Support/Mailing_Lists/Search before posting!
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--
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Re: [gmx-users] Re: Martini with PME, temp two low (ABEL Stephane 175950)

2013-04-25 Thread XAvier Periole

Good. Note however that we do get the right temperature with a dt=20fs with 
Martini so you energy leak might be in the cutoff scheme or the system is 
really badly equilibrated. 

On Apr 25, 2013, at 18:23, ABEL Stephane 175950 stephane.a...@cea.fr wrote:

 Xavier 
 
 I have followed your suggestion and did a longer NPT equilibration with 
 smaller dt and ntlist values and It works. The Energy and Temp  reach to 
 stables values as i want. 
 
 thank you again  for your help
 
 Stephane
 
 --
 
 Message: 2
 Date: Thu, 25 Apr 2013 14:17:00 +
 From: ABEL Stephane 175950 stephane.a...@cea.fr
 Subject: [gmx-users] Re: Martini with PME, temp two low
 To: gmx-users@gromacs.org gmx-users@gromacs.org
 Message-ID:
3e39b768bb199548ab18f7289e7534af1a818...@exdag0-b0.intra.cea.fr
 Content-Type: text/plain; charset=us-ascii
 
 @ Vitaly
 of course. I know that. My system is neutral  but with charged particles (AOT 
 and Na+).
 
 @Xavier
 I will try your suggestion and equilibrate my system for a longer period
 
 Thanks again
 
 Stephane
 
 
 
 --
 
 Message: 1
 Date: Thu, 25 Apr 2013 15:52:09 +0200
 From: XAvier Periole x.peri...@rug.nl
 Subject: Re: [gmx-users] Martini with PME, temp two low
 To: Discussion list for GROMACS users gmx-users@gromacs.org
 Message-ID: 0a7b7d0a-b419-4d3d-826b-e6d61de6d...@rug.nl
 Content-Type: text/plain; charset=windows-1252
 
 
 Well ? 400 ps is rather small and you can expect deviations from so short 
 simulations if you start from an non-equilibrated system. I am not sure what 
 the void is but this indicates that your system might not be equilibrated ?
 
 You can try to decrease the time step and nstlist to see if you the drop of 
 temperature is due a flow of energy.
 
 On Apr 25, 2013, at 3:26 PM, ABEL Stephane 175950 stephane.a...@cea.fr 
 wrote:
 
 Hello Xavier,
 
 Thank you for your response.
 
 nstlist = 10 and the rlist = 1.0
 My mistake, i did not changes these values when i switched to PME,
 
 I have rerun the simulations for 400 ps in NPT with these changes and 
 plotted Epot and Temp vs Time The Epot and Temp values are not stables. The 
 average Temp of the system  is better than previously but fluctuate around 
 (294 K) instead of 298 K . Note i use gmx4.5.5 to do my calculations.
 
 I have also visualized my  system at the end of the NPT run, the  na+, 
 water, surfactant, octane molecules  form a slab with void
 
 What's wrong ?
 
 Stephane
 
 --
 gmx-users mailing listgmx-users@gromacs.org
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Re: [gmx-users] Linear CG beads, grompp doesn't work

2013-01-02 Thread XAvier Periole

I think your original problem is that you define only one charge group for the 
entire molecule/polymer. You need to define each bead in a separate charge 
group and things will be fine :)) you do not have charges anyways. 

As far as I know angles have never made martini unstable but the conventional 
dihedral potential are not suited for martini or any flexible molecule. 

XAvier. 

On Jan 2, 2013, at 4:55, Justin Lemkul jalem...@vt.edu wrote:

 
 
 On 1/1/13 10:51 PM, Xu Dong Huang wrote:
 @Justin,
 
 Does the philosophy described in your tutorial apply to CG martini bead 
 models where 1 bead describes the entire CO2 atom? (If I were to do that, 
 assuming)
 
 Presumably.  As long as you satisfy the criteria mentioned in the tutorial 
 (moment of inertia and total mass), you should be able to get it to work.  
 I've never dealt with polymers and have very little personal experience with 
 CG models, so I don't know if there are other methodological issues that one 
 might encounter.
 
 -Justin
 
 -- 
 
 
 Justin A. Lemkul, Ph.D.
 Research Scientist
 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] Error with MARTINI depending by the box size

2012-12-11 Thread XAvier Periole


I have not followed the thread but concerning the solvation of a  
protein using genbox you need to:
1- use a box of water that has the exact size of the final box you  
want (you make it yourself using any tool you want) and you need to  
define the box size of the protein file as the one of the water box  
conformation. This is given on the last line of the gro file. Then  
genbox -cp -cs should work fine.
2- you need to use a water box size larger than the one you need. This  
solution is generally easier. You can generate a box using genconf - 
nbox option. And again define the box size in the protein conformation  
file and genbox will just do fine.


We generally use -vdwd 0.18. It is a good compromise for disturbing  
the system the least.


Note that these uses have been discussed on the MARTINI forum several  
times.


XAvier.

On Dec 11, 2012, at 9:05 AM, francesco oteri wrote:


Tanks to all for your advices,
I am going to check all the different aspect you suggested and I will
report the results as soon as possible.

Francesco


2012/12/11 Tsjerk Wassenaar tsje...@gmail.com


Hi,

Visualization is the key. If you check the structure right after  
genbox,
you should be able to notice something odd. Apparently genbox has a  
problem
with martini water, which probably means there is a problem with  
monoatomic
solvents. The problem has been noted before, b ut I'm a bit too  
lazy now to
check whether it was here or on the martini forum. Using a small  
box with a

single water molecule for filling will solve the problem.

Cheers,

Tsjerk


On Tue, Dec 11, 2012 at 12:06 AM, Mark Abraham mark.j.abra...@gmail.com

wrote:


On Mon, Dec 10, 2012 at 11:54 PM, Justin Lemkul jalem...@vt.edu  
wrote:





On 12/10/12 5:45 PM, francesco oteri wrote:


For Justin,
I need this water for one simple reason: less then 20nm doesn't

workAs

I said before



It seems you have identified the source of the problem, and it is
independent of box size.  I questioned the box size because it  
seemed
rather random and you had not shown any data for box sizes less  
than 19

nm,

so I was curious how you arrived at the need for 20 nm, more than

double

the size of your solute.

It would be interesting to see if you could identify a minimum  
box size

that does not require large numbers of solvent configurations to be

stacked

within the unit cell.  The only reason I could see for what you're
reporting is if neighboring solvent blocks somehow get crossed to

produce
overlap when they should simply be next to one another.  The  
larger the

box, the greater the probability that this happens.



Yeah, that's probably it. The water box has many waters with x

coordinates
down at 0.000 and near 10.901, with an x size of 10.902. So  
different box
sizes will randomly introduce unstable water configurations  
according to
whether stuff is too close. This water box is probably not suited  
to the
purpose - its box size might not include the half VDW radii  
outside the

water coordinates needed to pack stably.

Mark






2012/12/10 francesco oteri francesco.ot...@gmail.com

Hi Mark,

you are right respect the -vdwd 0.4: In MARTINI tutorials they

suggest

to
use 0.21. Since I still got errors with this procedure, I  
decided to

remove
water manually through vmd.

Looking carefully at the configurations, I found that the water

molecule
originating the error is exactly superimposed to an other  
molecule

so I
simply deleted it and the same error is reported for an other  
water

molecule.

Although I could scan all the pdb to detect all the superimposed

water
molecules, I believed genbox checked for this. Of course the  
original

box

does't contain superimposed molecules.



It is highly unusual for genbox to produce overlapping waters,  
but per

the

help description, only solute-solvent overlaps are checked, not
solvent-solvent, which would likely require enormous amounts of  
memory

(and

genbox already has memory issues).

-Justin

--
==**==


Justin A. Lemkul, Ph.D.
Research Scientist
Department of Biochemistry
Virginia Tech
Blacksburg, VA
jalemkul[at]vt.edu | (540) 231-9080
http://www.bevanlab.biochem.**vt.edu/Pages/Personal/justin

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


==**==

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Re: [gmx-users] REMD simulation

2012-11-19 Thread XAvier Periole


Well either you use more replicas or you reduce the temperature  
range ...

There is no way around!

On Nov 19, 2012, at 5:54 PM, Kenny Bravo Rodriguez wrote:


Dear All,

i am trying to performed REMD simulations using Gromacs.
My question is concerning the temperature distribution and the  
number of replica.
I need to run 24 replicas of my system with a temperature range of  
290-400 K. How can I select the temperatures values for each replica?
I tried the server http://folding.bmc.uu.se/remd/index.php but for  
my system it gives 50 replicas. If i try to take 24 evenly spaced  
values from the obtained list of temperature then

the replicas do not exchange at all.
I am using Gromacs 4.5.5 and my system has 6862 water molecules and  
535 atoms for the solute.


Thanks in advanced
Kenny

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Re: [gmx-users] Simulation of charged systems (2)

2012-11-02 Thread XAvier Periole


From what I remember from my earlier impressions ...  the equations  
are not correct when the system is not neutral. In your case the  
charge is significantly high ...


On Nov 2, 2012, at 9:36 AM, Felipe Pineda, PhD wrote:


Hi,

I recently sent a query, but it was probably not appealing enough to  
get some feedback. So I try again with a shorter one:


Is there any theoretical or technical objection against running an  
NPgammaT simulation on a charged (total charge = -36) membrane model  
(hydrated bipolar monolayer) using PME?


Many tanks in advance for your input.

Best,

Felipe

+---+
| Luis Felipe Pineda De Castro, PhD |
| Computational Chemist - Postdoc   |
| Linnaeus University   |
| SE-391 82 Kalmar  |
| Sweden - Sverige  |
+---+



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Re: [gmx-users] Martini FF for Sec structure changes...

2012-10-10 Thread XAvier Periole


Martini FF cannot model changes in secondary structure ... other CG FF  
can. You'll find them easily in the literature. Notably the ones from  
Deserno or Derreumaux.


On Oct 10, 2012, at 2:03 PM, rama david wrote:


Hi friends,

I planed to use the martini force-field for my simulation study of  
peptide.


The peptides are initially alpha-helix in nature. As they come  
together

they formed amyloid fibre( Antiparallel Beta structure).

Is it is possible to study the secondary structure backbone study by
martini force field.

I read in there tutorial that the Secondary structure is predefined
therefore they are statics through out the simulation.
Conformational changes that  produces  changes in Sec structure are  
out of
scope in martini. only  tertiary structure are free defined to  
change..



So what to do ???
How to use Martini FF to study secondary structure ???

Is there any way to use coarse grained FF to use for study in Sec.
structure???


With Best wishes and regards,
Rama David
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Re: [gmx-users] Martini FF for Sec structure changes...

2012-10-10 Thread XAvier Periole


Nope, but on other softwares.

On Oct 10, 2012, at 2:50 PM, rama david wrote:


Thank you for your reply,

Are these Cg can be used in Gromacs.

Thank you in advance.

With best wishes and regards,

Rama david

On Wed, Oct 10, 2012 at 6:13 PM, XAvier Periole x.peri...@rug.nl  
wrote:




Martini FF cannot model changes in secondary structure ... other CG  
FF

can. You'll find them easily in the literature. Notably the ones from
Deserno or Derreumaux.


On Oct 10, 2012, at 2:03 PM, rama david wrote:

Hi friends,


I planed to use the martini force-field for my simulation study of
peptide.

The peptides are initially alpha-helix in nature. As they come  
together

they formed amyloid fibre( Antiparallel Beta structure).

Is it is possible to study the secondary structure backbone study by
martini force field.

I read in there tutorial that the Secondary structure is predefined
therefore they are statics through out the simulation.
Conformational changes that  produces  changes in Sec structure  
are out of
scope in martini. only  tertiary structure are free defined to  
change..



So what to do ???
How to use Martini FF to study secondary structure ???

Is there any way to use coarse grained FF to use for study in Sec.
structure???


With Best wishes and regards,
Rama David
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Re: [gmx-users] Martini FF for Sec structure changes...

2012-10-10 Thread XAvier Periole


No, it does NOT!

HAve you red the paper?!

This implementation is an adoc representation to mimic specific  
sequences of short peptides! They do never for any secondary structure!


On Oct 10, 2012, at 3:05 PM, francesco oteri wrote:


Hi rama,
actually MARTINI has been further improved to allow secondary  
structure

change.
The title is:
*Improving Internal Peptide Dynamics in the Coarse-Grained MARTINI  
Model:

Toward Large-Scale Simulations of Amyloid- and Elastin-like Peptides*

and here there is a link to the paper:
http://dx.doi.org/10.1021/ct200876v

Francesco

2012/10/10 XAvier Periole x.peri...@rug.nl



Nope, but on other softwares.


On Oct 10, 2012, at 2:50 PM, rama david wrote:

Thank you for your reply,


Are these Cg can be used in Gromacs.

Thank you in advance.

With best wishes and regards,

Rama david

On Wed, Oct 10, 2012 at 6:13 PM, XAvier Periole x.peri...@rug.nl  
wrote:



Martini FF cannot model changes in secondary structure ... other  
CG FF
can. You'll find them easily in the literature. Notably the ones  
from

Deserno or Derreumaux.


On Oct 10, 2012, at 2:03 PM, rama david wrote:

Hi friends,



I planed to use the martini force-field for my simulation study of
peptide.

The peptides are initially alpha-helix in nature. As they come  
together

they formed amyloid fibre( Antiparallel Beta structure).

Is it is possible to study the secondary structure backbone  
study by

martini force field.

I read in there tutorial that the Secondary structure is  
predefined

therefore they are statics through out the simulation.
Conformational changes that  produces  changes in Sec structure  
are out

of
scope in martini. only  tertiary structure are free defined to  
change..



So what to do ???
How to use Martini FF to study secondary structure ???

Is there any way to use coarse grained FF to use for study in Sec.
structure???


With Best wishes and regards,
Rama David
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Re: [gmx-users] Martini lipid bilayer...

2012-10-09 Thread XAvier Periole


Well ... it always depends on what you want to do but the file on the  
link you give are the official website and they should be reliable :))


On Oct 9, 2012, at 12:04 PM, rama david wrote:


Hi Gromacs friends,

I am interested in Martini force-field and application in lipid  
bilayer.

I found the lipid bilayer at

http://md.chem.rug.nl/cgmartini/index.php/downloads/example-applications/66-dppc-membrane

is it is a reliable to use it after more equilibriation ( like 500  
ns  )


or I have to build my own bilayer 

Is any other link to get the martini lipids bilayer???


With best wishes and regards,
Rama David.
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Re: [gmx-users] using martinize.py to martinize two chains complex

2012-09-05 Thread XAvier Periole


You may want to try the forum on rte cgmartini.nl for more ...

In short:

try martinize.py -h it should give you options to separate the chain  
topologies. If it does not work that means your chains are not defined  
as two in the input.


Their is not direct manner to CG a lipid file ... the topology is easy  
to build though ... for the coordinate files you either start from an  
already existing file or you go through the reverse transformation  
tutorial. It is mainly used to get atomistic from CG but you can do  
the inverse ... the steps are identical and most importantly you learn  
how to build a topology with  a mapping section.


XAvier.

On Sep 5, 2012, at 11:53 PM, Lingyun Wang wrote:


Hi all,

There are two chains in the complex.pdb file, but martinize.py only  
recognize them as one chain. What can I do to generate two chains in  
the complex-martini.top file? My command is as following:


python martinize.py  -f complex.pdb -o complex-martini.top -x  
complex-martini.pdb



By the way, is any script to generate Martini topology and structure  
files for lipids available? If not, how can I martinize a lipids  
bilayer?. Thanks.


Lingyun
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Re: [gmx-users] using martinize.py to martinize two chains complex

2012-09-05 Thread XAvier Periole


I believe martinize looks for chain identifiers. There is a column for  
that in the PDB format.


The other solution is to proceed in two steps ... one chain at the  
time ...


On Sep 6, 2012, at 1:22 AM, Lingyun Wang wrote:


Hi XAvier,

Thank you for your reply.
I also tried  python martinize.py  -f complex.pdb -o complex- 
martini.top -x complex-martini.pdb -sep, but it still turns out the  
same result. There is Ter after each chain in the pdb, do I need  
other way to define that they are two chains? Thanks.


Best,
Lingyun

From: gmx-users-boun...@gromacs.org [gmx-users-boun...@gromacs.org]  
on behalf of XAvier Periole [x.peri...@rug.nl]

Sent: Wednesday, September 05, 2012 5:52 PM
To: Discussion list for GROMACS users
Subject: Re: [gmx-users] using martinize.py to martinize two chains  
complex


You may want to try the forum on rte cgmartini.nl for more ...

In short:

try martinize.py -h it should give you options to separate the chain
topologies. If it does not work that means your chains are not defined
as two in the input.

Their is not direct manner to CG a lipid file ... the topology is easy
to build though ... for the coordinate files you either start from an
already existing file or you go through the reverse transformation
tutorial. It is mainly used to get atomistic from CG but you can do
the inverse ... the steps are identical and most importantly you learn
how to build a topology with  a mapping section.

XAvier.

On Sep 5, 2012, at 11:53 PM, Lingyun Wang wrote:


Hi all,

There are two chains in the complex.pdb file, but martinize.py only
recognize them as one chain. What can I do to generate two chains in
the complex-martini.top file? My command is as following:

python martinize.py  -f complex.pdb -o complex-martini.top -x
complex-martini.pdb


By the way, is any script to generate Martini topology and structure
files for lipids available? If not, how can I martinize a lipids
bilayer?. Thanks.

Lingyun
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Re: [gmx-users] Elastic network model -building

2012-08-27 Thread XAvier Periole


There is no script generating an elastic network in Gromacs.

You could use the script that we developed in the context of the  
Martini CG model (cgmartini.nl) but it would be certainly easier for  
you to simply write a script that would rad the Clapha coordinates and  
define the ones that are within a cut-off distance of your choice and  
then write a list of bonds that you could add to a gromacs topology  
file ...


On Aug 26, 2012, at 3:34 PM, mohan maruthi sena wrote:


Hi all,
   I want to build elastic network model for a protein.  To
build an Elastic network model  , I consider only C-alpha atoms of the
protein. I want to make c-alpha atoms connect(make bond) with all the
other c-alpha atoms , if it falls within certain cut-off distance.
How can i do this?


Please suggest me a way,

Thanks,
Mohan.
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Re: [gmx-users] Elastic network model -building

2012-08-27 Thread XAvier Periole


On Aug 27, 2012, at 7:14 PM, mohan maruthi sena wrote:


Hi,
 Thanks for your reply. I have written a script which gives the
atoms with in certain cut-off distance from specified atom. I have
added this to topology , the problem is that it creates topology from
pdb but not the other way.

Not clear what the other way around is!


I use first pdb2gmx -f pdb -o gro -p top (command to generate
gro,top). I use this topology file and add the bonds in this  and use
this topology for further use.  Is this correct,?
I have no idea! It depends what you want to do! Doing like you  
describe you add a elastic network to a atomistic description ... if  
this is not the objective do something that would follow your idea!

,but still i could
not find bonds with other atoms when i load it in vmd. Please suggest
me a way.
VMD defines default bonds according to their distances in the  
structure you give. So between Calpha the distance is about 0.38  
nm ... if you use a dynamic bond description in VMD and select the  
Calphas ... a cutoff of 4.0 would show you the connections.


Thanks,
Mohan

On Mon, Aug 27, 2012 at 10:29 PM, XAvier Periole x.peri...@rug.nl  
wrote:


There is no script generating an elastic network in Gromacs.

You could use the script that we developed in the context of the  
Martini CG
model (cgmartini.nl) but it would be certainly easier for you to  
simply
write a script that would rad the Clapha coordinates and define the  
ones
that are within a cut-off distance of your choice and then write a  
list of

bonds that you could add to a gromacs topology file ...


On Aug 26, 2012, at 3:34 PM, mohan maruthi sena wrote:


Hi all,
  I want to build elastic network model for a protein.  To
build an Elastic network model  , I consider only C-alpha atoms of  
the
protein. I want to make c-alpha atoms connect(make bond) with all  
the

other c-alpha atoms , if it falls within certain cut-off distance.
How can i do this?


Please suggest me a way,

Thanks,
Mohan.
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Re: [gmx-users] Comparing amplitudes of motions in two MD simulations

2012-07-14 Thread XAvier Periole

rmsf is what you are looking for. g_rmsf should help. 



On Jul 14, 2012, at 16:23, Igor Druz idruz...@gmail.com wrote:

 Hello,
 
 I would like to compare amplitude of motion of a specific atom in two
 sets of MD simulations. Something like rms of displacements about the
 equilibrium position would do. In your experience, which gromacs
 analysis tools would be suitable for this? Any other insight into how
 this can be done best is appreciated.
 
 Thank you,
 Igor
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Re: [gmx-users] MARTINI parameters for dodecyl maltoside (DDM)

2012-05-21 Thread XAvier Periole


Thee are not yet parameters for DDM but indeed the parameters for both  
the head and the tail are defined separately. It would be very useful  
to combine them and start building a detergent parameter library ...  
the topologies would have to be tested against experimental and/or  
atomistic data. I believe there must be an enormous amount of data on  
the phase behavior of DDM and other thermodynamic data.


On May 21, 2012, at 3:35 PM, Dariush Mohammadyani wrote:

Sure, this is the way to make forcefield for your molecule. Also,  
please check literature.


Good luck,
Dariush



On Mon, May 21, 2012 at 9:26 AM, francesco oteri francesco.ot...@gmail.com 
 wrote:

Hi Dariush,
I've checked but it seems there no parameters for my detergent.

Actully there are parameters for the polar head and the lipidic  
tail, so it is worth trying to merge them

to have the correct representation!

Francesco

2012/5/21 Dariush Mohammadyani d.mohammady...@gmail.com
Have you checked MARTINI website?
http://md.chem.rug.nl/cgmartini/index.php/downloads/force-field-parameters

Dariush




Kind Regards,
Dariush Mohammadyani
Department of Structural Biology
University of Pittsburgh School of Medicine
Biomedical Science Tower 3
3501 Fifth Avenue
Pittsburgh, PA 15261
USA



On Sun, May 20, 2012 at 1:01 PM, francesco oteri francesco.ot...@gmail.com 
 wrote:

Dear gromacs users,
does someone of you know whether parameters for the detergent  
dodecyl-beta-maltoside

are avalaible in MARTINI forcefield?

Thank you in advance,
Francesco

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Cordiali saluti, Dr.Oteri Francesco

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Re: [gmx-users] dipole moment

2012-05-14 Thread XAvier Periole

Hi,

You do not need to use the polarizable martini water model to calculate the 
dipole of molecules. Or I am missing a point here!

g_dipole should do the work

XAvier. 

On May 13, 2012, at 15:11, dina dusti dinadu...@yahoo.com wrote:

 Dear Justin,
 
 Thank you very much from your response.
 
 Best Regards
 Dina
 
 From: Justin A. Lemkul jalem...@vt.edu
 To: dina dusti dinadu...@yahoo.com; Discussion list for GROMACS users 
 gmx-users@gromacs.org 
 Sent: Sunday, May 13, 2012 5:23 PM
 Subject: Re: [gmx-users] dipole moment
 
 
 
 On 5/13/12 8:41 AM, dina dusti wrote:
  Dear GROMACS Specialists,
  
  I have one system consists of water and two other molecules. I work by 
  MARTINI
  CG force field. I want to calculate dipole moment of molecules in water.
  May I ask you to help me, Please?
  
 
 I doubt you can.  Unless you are using version 2.P of the force field (which 
 contains polarizable water), MARTINI uses a single, uncharged particle to 
 represent water.  If there are no charges, there is no dipole.
 
 -Justin
 
 -- 
 
 Justin A. Lemkul, Ph.D.
 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] dipole moment

2012-05-14 Thread XAvier Periole


Interesting ...

do you have a reference for this?

XAvier.

On May 14, 2012, at 12:01 PM, Dommert Florian wrote:


On Mon, 2012-05-14 at 09:59 +0200, XAvier Periole wrote:



Hi,


You do not need to use the polarizable martini water model to
calculate the dipole of molecules. Or I am missing a point here!


g_dipole should do the work

XAvier.



Hi,


I want to point to another problem. If you simulate with a classical
force field, you usually have an effective set of partial charges.  
This

means polarization effects are often included in the partial charges.
This in turn requires an appropriate calculation of the dipoles. A
simple sum over the charges, like g_dipole or g_current does, is not
sufficient. The true dipoles are only obtained, if the results from  
the

MD are multiplied with a certain factor the is related to the
high-frequency limit of the dielectric constant, the electronic
dielectric constant. We have performed several studies on molecular
ionic liquids and showed, that with a set of bulk charges, the dipole
moments are reproduced correctly, if this electronic dielectric  
constant
is taken into account appropriate. Also for water or any other  
molecule,

the same arguments hold. For example, if TIP4P water is considered.
Calculating the dielectric constant gives a value around 50, which is
small compared to the exp. value of 80. However, if the correct  
dipoles
are considered, a simulated value of around 80 is the result. Hence,  
it

depends on the parametrization of the partial charges, how the dipole
moment or any related property has to be calculated.

If you are just interested in the static limit, an effective  
description

with static partial charges is sufficient in my opinion. However, as
soon as you are also interested in the time behavior, like the  
frequency

spectrum of the dielectric constant or conductivity, you consider the
electronic polarization explicitly with a corresponding force field,  
as

Justin mentioned.


Cheers,

Flo



On May 13, 2012, at 15:11, dina dusti dinadu...@yahoo.com wrote:




Dear Justin,


Thank you very much from your response.


Best Regards
Dina






From: Justin A. Lemkul jalem...@vt.edu
To: dina dusti dinadu...@yahoo.com; Discussion list for GROMACS
users gmx-users@gromacs.org
Sent: Sunday, May 13, 2012 5:23 PM
Subject: Re: [gmx-users] dipole moment




On 5/13/12 8:41 AM, dina dusti wrote:

Dear GROMACS Specialists,

I have one system consists of water and two other molecules. I

work by MARTINI

CG force field. I want to calculate dipole moment of molecules in

water.

May I ask you to help me, Please?



I doubt you can.  Unless you are using version 2.P of the force
field (which contains polarizable water), MARTINI uses a single,
uncharged particle to represent water.  If there are no charges,
there is no dipole.

-Justin

-- 

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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] jointly-couple lipids to theromstat - MARTINI force-field

2012-05-03 Thread XAvier Periole


The separation of groups for temperature control is originally  
necessary to avoid (or correct for) temperature gradient in the  
system, which occurs when systems parts have different frequencies of  
motions. Typically the water molecules and a protein would be  
separated to avoid the freezing of the protein and the heating up of  
the solvent.


It would not make much difference to couple the dppc and dppg lipid  
groups separately or together. To form a separate group you need a  
sufficient amount of particle to avoid large (and therefore more  
difficult to control) fluctuations. Ions are generally coupled to the  
solvent they are embedded into.


Anirban suggestion is fine.

On May 3, 2012, at 1:56 PM, Anirban Ghosh wrote:




On Thu, May 3, 2012 at 5:17 PM, Weingarth, M.H.  
m.h.weinga...@uu.nl wrote:

Hello,

I am a bit confused by a comment which I find in all MARTINI example  
md.mdp scripts concerning the tc-groups :


It is stated there to couple groups separately:

 MARTINI -Normal temperature and pressure coupling schemes can be  
used. It
; is recommended to couple individual groups in your system  
seperately


I am simulating a mixed dppc:dppg membrane (see below my  
parameters). Even these two different lipids-types should be coupled  
separately? (and how about Na+ (Qd particles) and water - also  
separately?)


I would greatly appreciate any comment on this issue.

Thanks a lot
Markus



my parameter:
; Temperature coupling:
tcoupl   = berendsen
; Groups to couple separately:
tc-grps  = DPPC DPPG W NAA Protein


Generally in membrane protein simulations different coupling groups  
are used to increase the accuracy of the calculations (more  
realistic). In your system you can make make three groups: Protein,  
Lipids(DPPC+DPPG) and Sol+Ions(Na+Qd)



-Anirban



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Re: [gmx-users] wham histograms

2012-04-23 Thread XAvier Periole


Not sure but you could compare with unbiased histogram constructed  
independently.


On Apr 23, 2012, at 11:55 AM, Gavin Melaugh wrote:


Hi all

Are the histograms from histo.xvg (output of g_wham) the biased or
unbiased distributions?

Cheers

Gavin
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Re: [gmx-users] martini coarse-grained

2012-04-10 Thread XAvier Periole


Where did you find the topology?

On Apr 10, 2012, at 10:44 AM, dina dusti wrote:


Dear GROMACS Specialists,

I have doubt about definition of tiofen ring in MARTINI CG force  
field. May I ask you to help me, Please?
I defined if as: SC4 and SC5, that SC5 is as S-C-C and SC4 is as C- 
C. Is it right?

Or should I change SC5 to C-S-C for .gro file?
And my definition of tiofen in .itp file it is as followed , Please  
say me that is it right?


;;  TIOFEN

[moleculetype]
; molname   nrexcl
  TIO 1

[atoms]
; idtyperesnr   residu  atomcgnrcharge
  1 SC4 1 TIO SI1 1 0
  2 SC5 1 TIO SI22 0

[constraints]
; i j   funct   length
  1 2 1 0.27

Because I for benzene see a triangle in ngmx program, but for this  
see a line. Please help me to correction of mistakes.

Thank you very much in advance.

Best Regards
Dina



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Re: [gmx-users] Exploding Protein with 4.6 and 4.5.5

2012-03-26 Thread XAvier Periole

Try to use constrains = all-bonds which is the way to use Gromos force fields. 

On Mar 26, 2012, at 12:30, SebastianWaltz 
sebastian.wa...@physik.uni-freiburg.de wrote:

 Dear Gromacs user,
 
 I try to simulate the human Villin head peace HP35 in approx. 6000 water
 molecules (spc) with the gromos ff ffG53a6. Using the 4.0.7 version the
 NPT equilibration for 5ns with position restraint protein (lincs) atoms
 and a integration step of 0.002 using the leap-frog integrator works
 just fine. Switching to the 4.5.5 or the 4.6 version with heterogeneous
 acceleration is leading to an exploding protein after a few ps. Changing
 the integration time step to 0.0002 delays the explosion for few ps but
 does not avoid it. The parameters in mdp file for the 4.6 version are
 the following:
 
 ;
 title= ttt
 cpp =  /lib/cpp
 include   = -I../top
 constraints = hbonds
 integrator   =  md
 cutoff-scheme=  verlet
 
 define =  -DPOSRES  
 ;constraint_algorithm = shake
 dt=  0.0002
 nsteps =  250   
 nstcomm=  10   
 nstxout   =  1000  
 nstvout   =  1000   
 nstfout=  1000
 nstlog =  1000  
 nstenergy   =  5000  
 nstxtcout =  10
 
 xtc_grps=  Protein
 
 nstlist=  25 
 ns_type =  grid
 rlist   =  1.2
 
 coulombtype  =  PME  
 rcoulomb=  1.2
 vdwtype  =  cut-off
 rvdw   =  1.2   
 fourierspacing=  0.12  
 pme_order =  6 
 optimize_fft=  yes
 pbc =  xyz
 Tcoupl =  v-rescale
 tc-grps=  Protein Non-Protein
 tau_t   =  0.1 0.1
 ref_t=  300 300
 
 energygrps  =  Protein Non-Protein
 
 Pcoupl =  berendsen
 tau_p   =  0.5
 compressibility =  4.5e-5
 ref_p =  1.0
 refcoord_scaling   =  all
 Pcoupltype=  isotropic
 gen_vel =  yes
 gen_temp =  300
 gen_seed  =  -1
 
 
 Any help is very welcomed.
 
 Dears sincerely,
 
 Sebastian
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Re: [gmx-users] About martini

2012-03-09 Thread XAvier Periole

Yes unfortunately the transformation is only inplemented in the version 
available on the martini page.

On Mar 9, 2012, at 10:30, francesca vitalini francesca.vitalin...@gmail.com 
wrote:

 Either you develop your own version of the mapping or I guess you have
 to use the old version...sorry, but I'm struggling with it right now
 and I understand that it can be quite problematic.
 Francesca
 
 2012/3/9 rama david ramadavidgr...@gmail.com:
 Dear GROMACS specialists,
   How to convert Coarse Grain Martini
 to   FG martini on Gromacs 4.5.4 version .
 ( And how to compile the source given in Martini
 home page with 4.5.4 version as they mention only
  Gromacs 3.3.1 version)
 
 Please give the valuable advice..
 
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Re: [gmx-users] g_fg2cg

2012-03-06 Thread XAvier Periole

Did you define the mapping in the atomistic topology? 



On Mar 6, 2012, at 10:57, dina dusti dinadu...@yahoo.com wrote:

 Dear Gromacs Specialists,
 
 I have one problem about g_fg2cg. I want convert structure of butanole in fg 
 to cg by g_fg2cg, but I take this error:
 
 Program g_fg2cg, VERSION 3.3.1
 Source code file: gmxfio.c, line: 735
 
 Range checking error:
 Variable fio has value -1. It should have been within [ 0 .. 1 ]
 Please report this to the mailing list (gmx-users@gromacs.org)
 
 May I ask you to help me, Please?
 Thank you very much in advance
 
 Best Regards
 Dina
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Re: [gmx-users] antifreeze particle in martini coarse-grained

2011-12-13 Thread XAvier Periole


It was a good idea to ask! You might want to try the MARTINI forum at  
the cgmartini.nl web site, though.


In short the way you did it will probably fill up the box with more  
water or antifreeze particle than necessary ...


As an alternative you may want to simply replace 10% of the existing  
waters into antifreeze particles. You need to change the name in the  
gro files and adapt the topology accordingly. Then an equilibration  
will disperse the WF particle pretty fast.


XAvier.

On Dec 13, 2011, at 2:56 PM, mohammad agha wrote:


Dear Prof.

I have a doubt about my way to add antifreeze water to my system,  
also I think my question looks silly but please help me for more  
certainty.
I changed W to WF in water.gro file of water that I downloaded  
from MARTINI site and named that antifreezewater.gro , and with  
below command added antifreeze water to my system:
# genbox -cp ---.gro -cs antifreezewater.gro -o .gro - 
maxsol 1000

Already I had added water.gro to my system with the same command.
May I know that I am right or wrong and if I'm wrong please say me  
the right way?


Thanks
Best Regards
Sara
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Re: [gmx-users] antifreeze particle in martini coarse-grained

2011-12-13 Thread XAvier Periole


You want to keep the conversation in the list so that others may  
benefit from it.


No. You need to place 1 W in the box and manually edit the gro  
file to change the last 1000 into WF but most importantly in the  
topology file generate two groups one with 9000 W and the other 1000 WF.

Your way may work but the original placement of the WF might be silly.

Do not separate the two groups in the mdp file for the temperature  
control. Leave them together.


On Dec 13, 2011, at 4:09 PM, mohammad agha wrote:


Dear Prof.

Thanks for your reply.

Yes, for example if I need 1 water, then I place 9000 water by  
genbox from water.gro file and 1000 antifreeze water from  
antifreezewater.gro that I changed W to WF in water.gro and I  
have in topology file:


[ molecules ]
solute   100
W9000
wf   1000

Then my way is correct?
also I have one group for WF in .mdp and index.ndx files, is it  
correct?


Best Regards
Sara




From: XAvier Periole x.peri...@rug.nl
To: mohammad agha mra...@yahoo.com; Discussion list for GROMACS  
users gmx-users@gromacs.org

Sent: Tuesday, December 13, 2011 5:34 PM
Subject: Re: [gmx-users] antifreeze particle in martini coarse-grained


It was a good idea to ask! You might want to try the MARTINI forum  
at the cgmartini.nl web site, though.


In short the way you did it will probably fill up the box with more  
water or antifreeze particle than necessary ...


As an alternative you may want to simply replace 10% of the existing  
waters into antifreeze particles. You need to change the name in the  
gro files and adapt the topology accordingly. Then an equilibration  
will disperse the WF particle pretty fast.


XAvier.

On Dec 13, 2011, at 2:56 PM, mohammad agha wrote:


Dear Prof.

I have a doubt about my way to add antifreeze water to my system,  
also I think my question looks silly but please help me for more  
certainty.
I changed W to WF in water.gro file of water that I downloaded  
from MARTINI site and named that antifreezewater.gro , and with  
below command added antifreeze water to my system:
# genbox -cp ---.gro -cs antifreezewater.gro -o .gro - 
maxsol 1000

Already I had added water.gro to my system with the same command.
May I know that I am right or wrong and if I'm wrong please say me  
the right way?


Thanks
Best Regards
Sara
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Re: [gmx-users] Martini force field: elastic network

2011-10-14 Thread XAvier Periole


The website has been updated to fit a CG tutorial  starting monday in  
Lausanne.
The manner of the construction you describe in your email is not the  
proper way to do it!


The new script is doing it properly.

If you want the old script to only generate the elastic network (as it  
seems from your email) you may have it or use the scripts from the  
ElNeDyn approach.


XAvier.

On Oct 14, 2011, at 5:58 PM, Li, Hualin wrote:


Dear all,

 I am using martini force field to generate elastic network  
for my protein. I generate a list of distance between all beads  
within a certain distance by:


genrestr -f  ***.gro -n index.ndx -constr -o constraints

   getting the constraints.itp file and will continue with the  
2nd step by using a script:


   ./select_restr.pl constraints.itp 0.5 0.9 500

  However, the martini forcefield developer seems to update  
their website yesterday and I can't find the select_restr.pl any  
more and in the new script they provide ( martinize.py),  -elastic
to write elastic bonds is not working yet.  Could some one provide  
me the old script   select_restr.pl please?


 Many thanks.

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Re: [gmx-users] MARTINI / all-atom mapping

2011-08-31 Thread XAvier Periole

Thanks Justin and Thomas for the helpful comments. Thomas pointed to the 
example I had in mind. I should have been more specific. 

It is obvious that we should make the mapping of molecules more easily 
accessible. 

Tks for the comments,
XAvier. 

On Aug 30, 2011, at 20:16, Thomas Piggot t.pig...@soton.ac.uk wrote:

 Hi Mike,
 
 If you download the rev_trans.tar.gz archive from the reverse transformation 
 tutorial on the Martini website 
 (http://md.chem.rug.nl/cgmartini/index.php/tutorial/reverse-transformation) 
 the mapping section at the end of the dppc.itp file provides the details of 
 the mapping for this lipid.
 
 Cheers
 
 Tom
 
 On 30/08/11 18:57, Michael Daily wrote: 
 
 Xavier,
 
 I did find the atom2cg.awk script on the downloads- tools of the martini 
 website, but there is no corresponding one for lipids.  In any case I can 
 probably figure out the mapping by trial and error, just based on inter-bead 
 distances, but it would be nice to have it officially documented.
 
 Mike
 
 On Tue, Aug 30, 2011 at 3:06 AM, XAvier Periole x.peri...@rug.nl wrote:
 
 it must be some example of mapping lipids on the website: cgmartini.nl
 
 On Aug 30, 2011, at 3:55 AM, Michael Daily wrote:
 
 Hi all,
 
 I am trying to reverse-map some martini lipids to united atom.  In order to 
 do this, I'd prefer to have an EXACT definition of the aa-to-cg mapping.  I 
 cannot find this, only an imprecise graphic, in the MARTINI paper; the 
 martini.itp file doesn't appear to list which heavy atoms are represented 
 by each CG bead either.  For example, I'm looking for something like:
 
 'NC3' : ['C1', 'C2', 'C3', 'N4', 'C5', 'C6'],
 'PO4' : ['O7', 'P8', 'O9', 'O10', 'O11','C12'],
 'GL1' : ['C13', 'O14', 'C15', 'O16'],
 'GL2' : ['C32', 'O33', 'C34', 'O35'],
 
 etc.
 
 For some atoms it's obvious which MARTINI groups they belong in, but others 
 on the borderline are not obvious.  For example, does C12 belong in PO4 or 
 GL1?
 
 Anybody have a master list like this?
 
 Thanks,
 Mike
 
 -- 
 
 Michael D. Daily
 Postdoctoral research associate
 Pacific Northwest National Lab (PNNL)
 509-375-4581
 (formerly Qiang Cui group, University of   
 Wisconsin-Madison)
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 Michael D. Daily
 Postdoctoral research associate
 Pacific Northwest National Lab (PNNL)
 509-375-4581
 (formerly Qiang Cui group, University of Wisconsin-Madison)
 
 -- 
 Dr Thomas Piggot
 University of Southampton, UK.
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Re: [gmx-users] MARTINI / all-atom mapping

2011-08-30 Thread XAvier Periole


it must be some example of mapping lipids on the website: cgmartini.nl

On Aug 30, 2011, at 3:55 AM, Michael Daily wrote:


Hi all,

I am trying to reverse-map some martini lipids to united atom.  In  
order to do this, I'd prefer to have an EXACT definition of the aa- 
to-cg mapping.  I cannot find this, only an imprecise graphic, in  
the MARTINI paper; the martini.itp file doesn't appear to list which  
heavy atoms are represented by each CG bead either.  For example,  
I'm looking for something like:


'NC3' : ['C1', 'C2', 'C3', 'N4', 'C5', 'C6'],
'PO4' : ['O7', 'P8', 'O9', 'O10', 'O11','C12'],
'GL1' : ['C13', 'O14', 'C15', 'O16'],
'GL2' : ['C32', 'O33', 'C34', 'O35'],

etc.

For some atoms it's obvious which MARTINI groups they belong in, but  
others on the borderline are not obvious.  For example, does C12  
belong in PO4 or GL1?


Anybody have a master list like this?

Thanks,
Mike

--

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Postdoctoral research associate
Pacific Northwest National Lab (PNNL)
509-375-4581
(formerly Qiang Cui group, University of Wisconsin-Madison)
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[gmx-users] Fwd: density error bars

2011-07-26 Thread XAvier Periole


You may have wanted to have sent the message to the gmx list!

XAvier.

Begin forwarded message:


From: nicoletta liguori fisico...@gmail.com
Date: July 26, 2011 5:28:29 PM MDT (CA)
To: x.peri...@rug.nl
Subject: density error bars

Hi,
I'm using Gromacs and its tools to sample some kind of membranes and  
characterize their features.

Actually I don't know what to do about error bars.
For example when I calculate the density mass distribution along the  
axis parallel to the normal to the
membrane surface I average on all trajectories using g_density_d on  
my set contained

in the .xtc file.
Considering that, for what I understood, it makes the average on  
time of the density, but without
adding any kind of error (there are no possibilities with this tool)  
I tried to check if there are other tools

available to calculate the error bars but seem not to exist!!
For example g_analyze reads directly the already averaged set of  
data (in this case) cause the only

possible input is a .xvg file!
So I was thinking to (not yet know how, is my first computational  
trial) to calculate the error with a simple
standard deviation (I was thinking to use matlab ), but to do this,  
I suppose that

I have to consider all the points indipendent, and to do this
I'd have to look at the autocorrelation function of density itself!
but how to do this??
there are again no tools available
how do you do when u deal with errors?
Thanks for attention and for the help
Nicoletta


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Re: [gmx-users] large error bars in PMF

2011-07-21 Thread XAvier Periole


One potential problem you have is that as Justin mentioned your minimum
is not well defined and certain much less well sampled than the long  
distances

windows. Small peptides (depends the size) may sample relevant phase
space to get reasonable convergence within 8 ns when free in solution;
in contact certainly not ...

How long is you peptide?

You might get a better estimate of your error by plotting all the pmfs  
you've
got through bootstrap (if this is the case) ... and get the errors  
based on the
pmfs aligned on the long distance value and not on the minimum which  
is
probably what you did ... if the minimum is not well defined then it  
does not

make sense.

On Jul 21, 2011, at 1:36 PM, Justin A. Lemkul wrote:




Rebeca García Fandiño wrote:

OK,
I will try a dodecahedral box and also to extend my actual  
simulations.
Could you give me some advice about starting to learn about 3D PMF?  
I have not seen this in the manual, and I have never used it  
before. I have only found your tutorial about how to calculate PMF  
in Gromacs 4...


In practice, there's basically nothing different between 3D and 1D.   
You specify the dimensions to which the biasing potential is applied  
with pull_dim or pull_vec (depending on the pull_geometry used).   
Right now you're calculating the PMF along the z-dimension only  
(pull_dim = N N Y), which may be appropriate for one-dimensional  
processes or those in which the reference group does not rotate much  
in the timeframe of the sampling.  Setting pull_dim = Y Y Y will  
apply the restraint in all dimensions.


-Justin


Thanks a lot again for your help.
Best wishes,
Rebeca.
 Date: Thu, 21 Jul 2011 15:16:52 -0400
 From: jalem...@vt.edu
 To: gmx-users@gromacs.org
 Subject: Re: FW: [gmx-users] large error bars in PMF



 Rebeca García Fandiño wrote:
 
 
  I am trying to achieve the binding energy of the dimer composed  
by the

  two small cyclic peptides, to compare it with experimental. What
  advantages would I have using 3D PMF instead only 1D for this  
calculation?


 Intuitively, two molecules diffuse through solution until they  
find one another,
 which to me sounds a lot like a 3D path. Further, using a  
dodecahedral box for
 your umbrella sampling removes the problems you're having with  
the peptides
 rotating. It sounds like you're trying to pull in one direction  
along a
 rectangular box, but the peptides are not playing nice. I feel  
like this

 discussion has come up at least once or twice before, though...

 -Justin

  Thanks a lot!
  Rebeca.
 
   Date: Thu, 21 Jul 2011 14:14:44 -0400
   From: jalem...@vt.edu
   To: gmx-users@gromacs.org
   Subject: Re: [gmx-users] large error bars in PMF
  
  
  
   Rebeca García Fandiño wrote:
Hi,
thanks a lot for your quick answer.
What I am trying to pull are two small peptides one from  
another (r_1

and r_2).
I did not understand very well your last suggestion: ...if  
you want
reasonable error bars you will not lots of well-converged  
data.

  
   Oops, that should have read you will *need* lots of well- 
converged

  data.
  
Do you mean I will need also more windows besides extending  
the

  simulations?
  
   I doubt you need more windows. Likely you just need more time  
in each.

  
I think the problem could be also that the peptides I am  
using

  rotate in
the box and they do not remain flat one respect to the  
other. They
gyrate freely and some parts of their structure interact  
along the

pulling...
  
   Interactions are part of the dissociation process and are not
  problematic per
   se. But if you're trying to obtain only a one-dimensional PMF  
then your

   rotation could be a problem. Is there some reason you need a
  one-dimensional
   PMF and not a three-dimensional PMF? What are you trying to  
achieve?

  
   -Justin
  
Thanks a lot again for your help.
Best wishes,
Rebeca.
   
   
   
   
   


From: rega...@hotmail.com
To: gmx-users@gromacs.org
Date: Thu, 21 Jul 2011 16:36:59 +
Subject: [gmx-users] large error bars in PMF
   
   
Hi,
I am trying to calculate the binding energy of two  
molecules using the

PMF (Umbrella Sampling method) and Gromacs 4.0.
Some weeks ago I have written to the list because changing  
the

  number of
windows used in the Umbrella Sampling calculations  
different results
were obtained, and I was suggested to extend my simulations  
since the

error bars associated to each windows were too high.
I have now extended my simulations from 1 ns to 8 ns,  
however, I

  cannot
see much different from the shorter calculations. I send  
you the
comparison of the two PMF including the error bars  
(attached).
Now I am using 50 windows, but the shorter simulations were  
done using
100 windows, so I don't think increasing the number of  
windows

  could 

Re: [gmx-users] large error bars in PMF

2011-07-21 Thread XAvier Periole


Well I do not know how g_wham is doing but it is likely that it does  
align

different pmf obtained through the bootstraap the their minimum.

Justin just answered. The other alternative is to inverse your distances
with the data files.

On Jul 21, 2011, at 2:57 PM, Rebeca García Fandiño wrote:


Thanks for your answer.
My peptide has 6 residues and it is cyclic.
I calculated the errors through bootstrap, using this:

g_wham -it tpr-files.dat -if pullf-files.dat -o -hist -unit kCal -b  
500 -n Bootstrap 200


Are the pmfs aligned on the minimum distance value? Is that the  
value by default? How could I calculate the errors based on the PMFs  
aligned on the long distance value?


Thanks a lot for all the help.

Best wishes,

Rebeca.


 From: x.peri...@rug.nl
 To: gmx-users@gromacs.org
 Subject: Re: [gmx-users] large error bars in PMF
 Date: Thu, 21 Jul 2011 14:33:28 -0600


 One potential problem you have is that as Justin mentioned your  
minimum

 is not well defined and certain much less well sampled than the long
 distances
 windows. Small peptides (depends the size) may sample relevant phase
 space to get reasonable convergence within 8 ns when free in  
solution;

 in contact certainly not ...

 How long is you peptide?

 You might get a better estimate of your error by plotting all the  
pmfs

 you've
 got through bootstrap (if this is the case) ... and get the errors
 based on the
 pmfs aligned on the long distance value and not on the minimum  
which

 is
 probably what you did ... if the minimum is not well defined then it
 does not
 make sense.

 On Jul 21, 2011, at 1:36 PM, Justin A. Lemkul wrote:

 
 
  Rebeca García Fandiño wrote:
  OK,
  I will try a dodecahedral box and also to extend my actual
  simulations.
  Could you give me some advice about starting to learn about 3D  
PMF?

  I have not seen this in the manual, and I have never used it
  before. I have only found your tutorial about how to calculate  
PMF

  in Gromacs 4...
 
  In practice, there's basically nothing different between 3D and  
1D.
  You specify the dimensions to which the biasing potential is  
applied

  with pull_dim or pull_vec (depending on the pull_geometry used).
  Right now you're calculating the PMF along the z-dimension only
  (pull_dim = N N Y), which may be appropriate for one-dimensional
  processes or those in which the reference group does not rotate  
much

  in the timeframe of the sampling. Setting pull_dim = Y Y Y will
  apply the restraint in all dimensions.
 
  -Justin
 
  Thanks a lot again for your help.
  Best wishes,
  Rebeca.
   Date: Thu, 21 Jul 2011 15:16:52 -0400
   From: jalem...@vt.edu
   To: gmx-users@gromacs.org
   Subject: Re: FW: [gmx-users] large error bars in PMF
  
  
  
   Rebeca García Fandiño wrote:
   
   
I am trying to achieve the binding energy of the dimer  
composed

  by the
two small cyclic peptides, to compare it with experimental.  
What

advantages would I have using 3D PMF instead only 1D for this
  calculation?
  
   Intuitively, two molecules diffuse through solution until they
  find one another,
   which to me sounds a lot like a 3D path. Further, using a
  dodecahedral box for
   your umbrella sampling removes the problems you're having with
  the peptides
   rotating. It sounds like you're trying to pull in one direction
  along a
   rectangular box, but the peptides are not playing nice. I feel
  like this
   discussion has come up at least once or twice before, though...
  
   -Justin
  
Thanks a lot!
Rebeca.
   
 Date: Thu, 21 Jul 2011 14:14:44 -0400
 From: jalem...@vt.edu
 To: gmx-users@gromacs.org
 Subject: Re: [gmx-users] large error bars in PMF



 Rebeca García Fandiño wrote:
  Hi,
  thanks a lot for your quick answer.
  What I am trying to pull are two small peptides one from
  another (r_1
  and r_2).
  I did not understand very well your last suggestion:  
...if

  you want
  reasonable error bars you will not lots of well-converged
  data.

 Oops, that should have read you will *need* lots of well-
  converged
data.

  Do you mean I will need also more windows besides  
extending

  the
simulations?

 I doubt you need more windows. Likely you just need more  
time

  in each.

  I think the problem could be also that the peptides I am
  using
rotate in
  the box and they do not remain flat one respect to the
  other. They
  gyrate freely and some parts of their structure interact
  along the
  pulling...

 Interactions are part of the dissociation process and are  
not

problematic per
 se. But if you're trying to obtain only a one-dimensional  
PMF

  then your
 rotation could be a problem. Is there some reason you  
need a

one-dimensional
 PMF and not a three-dimensional PMF? What are you trying to
  achieve?

 -Justin

  Thanks a lot again for your help.
  Best 

Re: [gmx-users] GPUs and umbrella sampling

2011-07-18 Thread XAvier Periole


Yes, include the harmonic restrain(s) directly into the topology. Then  
you may
convert the info (distance(s), angle(s)) into the g_wham format  
(which  I do not
know but should be reasonably easy) or use another script to get your  
PMF or

make you own ... it is possible.

On Jul 18, 2011, at 9:37 AM, Guido Polles wrote:


Hi everybody,
 I noticed that GPU version of gromacs do not support the pull code,
hence i suppose g_wham cannot be used to extract a PMF. I would like
to just ask if somebody could suggest or give any hint about the way
to do umbrella sampling and extract a PMF without pull code, so that I
will have an idea before I start diving deeper into the issue, make
mistakes and potentially write useless code.
Thanks in advance for any advice.
Guido Polles
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Re: [gmx-users] Residence time and trjorder

2011-07-13 Thread XAvier Periole


Mark is right g_dist can help you for this but there is no specific
tool calculating residence time ... I guess everyone dreams of
someone writing it :))

On Jul 13, 2011, at 2:28 AM, Mark Abraham wrote:


On 13/07/2011 5:52 PM, Carla Jamous wrote:


Dear Xavier,

my problem is the following:

I'm trying to figure out if a water molecule is present in a  
specific area around my protein and if so, which water molecule is  
that and how long does it stay in that place.


I think g_dist does this for a group containing a single water  
molecule. All you need to do write a script to iterate over each  
molecule, and then collate the statistics.


Mark

As you said, if I google residence time, here's the definition:  
Residence time (also known as removal time) is the average amount  
of time that a particle spends in a particular system.


But I don't find a tool to calculate this residence time in  
gromacs, so I'm trying to find a trick that can give me a  
pourcentage of the time of my simulation where a certain water  
molecule stays in the specific area of my protein.


Regards,
Carla

On Tue, Jul 12, 2011 at 5:51 PM, XAvier Periole x.peri...@rug.nl  
wrote:


Dear Boafu,

This sounds like a great tool!

Carla, note that once you've ordered the water molecules you loose
the continuity of their trajectories ... that is because you order  
them in

function of their distance to the protein.

I am not sure the definition you give will give you the answer to the
residence time. you can google residence time and proteins and see
what come out :))

XAvier.


On Jul 12, 2011, at 6:32 AM, Baofu Qiao wrote:

HI Carla,

I wrote a similar code, see attached. But it is written for my  
condition. You should modify it accordingly.


regards,
Baofu Qiao

On 07/12/2011 02:04 PM, Carla Jamous wrote:
Dear gmx-users,

I used trjorder in order to study the water molecules that are  
closer than 5 A from my protein.


trjorder -s structure.tpr -f traj.xtc -n prot_water.ndx -o  
ordered.pdb -nshell nshell_.xvg -r 0.5 -b 0 -e 5000


But now I need to analyse the residence time of a water molecule, I  
mean the number of times a single water molecule stays in a radius  
of 5 A of the protein and divide this number by the total number of  
conformations, in order to have a pourcentage value.


Please is there any gromacs tool able to do this calculation or  
else does anyone have an idea of how to do that?


Thank you

Carla

g_residence.c--
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Re: [gmx-users] Residence time and trjorder

2011-07-12 Thread XAvier Periole


Dear Boafu,

This sounds like a great tool!

Carla, note that once you've ordered the water molecules you loose
the continuity of their trajectories ... that is because you order  
them in

function of their distance to the protein.

I am not sure the definition you give will give you the answer to the
residence time. you can google residence time and proteins and see
what come out :))

XAvier.

On Jul 12, 2011, at 6:32 AM, Baofu Qiao wrote:


HI Carla,

I wrote a similar code, see attached. But it is written for my  
condition. You should modify it accordingly.


regards,
Baofu Qiao

On 07/12/2011 02:04 PM, Carla Jamous wrote:

Dear gmx-users,

I used trjorder in order to study the water molecules that are  
closer than 5 A from my protein.


trjorder -s structure.tpr -f traj.xtc -n prot_water.ndx -o  
ordered.pdb -nshell nshell_.xvg -r 0.5 -b 0 -e 5000


But now I need to analyse the residence time of a water molecule, I  
mean the number of times a single water molecule stays in a radius  
of 5 A of the protein and divide this number by the total number of  
conformations, in order to have a pourcentage value.


Please is there any gromacs tool able to do this calculation or  
else does anyone have an idea of how to do that?


Thank you

Carla


g_residence.c--
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Re: [gmx-users] Problem in followin MARTINI tutorial

2011-06-20 Thread XAvier Periole


Well, there must be some thing some where that you did the wrong way :))

You should try again from the start and may be try to post on the  
Martini website forum

www.cgmartini.nl

XAvier

On Jun 20, 2011, at 9:41 AM, Naba wrote:


Dear Users/Developers

I am trying to set a coarse-grained MD for the same protein  
(1UBQ.pdb) therein the MARTINI tutorial (http://md.chem.rug.nl/cgmartini/index.php/tutorial 
).
After the solvation by water-1bar-303K.gro I tried to minimize the  
system but it gives the following weired results.


grompp gives the following output:

checking input for internal consistency...
processing topology...
Generated 0 of the 465 non-bonded parameter combinations
Excluding 1 bonded neighbours molecule type 'Protein'
Excluding 1 bonded neighbours molecule type 'W'
processing coordinates...
double-checking input for internal consistency...
renumbering atomtypes...
converting bonded parameters...
initialising group options...
processing index file...
Analysing residue names:
There are:76Protein residues
There are:  5199  Other residues
Analysing Protein...
Analysing residues not classified as Protein/DNA/RNA/Water and  
splitting into groups...

Making dummy/rest group for T-Coupling containing 5362 elements
Making dummy/rest group for Acceleration containing 5362 elements
Making dummy/rest group for Freeze containing 5362 elements
Making dummy/rest group for Energy Mon. containing 5362 elements
Making dummy/rest group for VCM containing 5362 elements
Number of degrees of freedom in T-Coupling group rest is 16053.00
Making dummy/rest group for User1 containing 5362 elements
Making dummy/rest group for User2 containing 5362 elements
Making dummy/rest group for XTC containing 5362 elements
Making dummy/rest group for Or. Res. Fit containing 5362 elements
Making dummy/rest group for QMMM containing 5362 elements
T-Coupling   has 1 element(s): rest
Energy Mon.  has 1 element(s): rest
Acceleration has 1 element(s): rest
Freeze   has 1 element(s): rest
User1has 1 element(s): rest
User2has 1 element(s): rest
VCM  has 1 element(s): rest
XTC  has 1 element(s): rest
Or. Res. Fit has 1 element(s): rest
QMMM has 1 element(s): rest
Checking consistency between energy and charge groups...
This run will generate roughly 2 Mb of data
writing run input file...

But mdrun gives the following output:

Steepest Descents:
   Tolerance (Fmax)   =  1.0e+00
   Number of steps= 5000
Step=   14, Dmax= 1.2e-06 nm, Epot=  3.55783e+18 Fmax= inf,  
atom= 294

Stepsize too small, or no change in energy.
Converged to machine precision,
but not to the requested precision Fmax  1

Double precision normally gives you higher accuracy.
You might need to increase your constraint accuracy, or turn
off constraints alltogether (set constraints = none in mdp file)

writing lowest energy coordinates.

Back Off! I just backed up solvated.gro to ./#solvated.gro.1#

Steepest Descents converged to machine precision in 15 steps,
but did not reach the requested Fmax  1.
Potential Energy  =  3.5578291e+18
Maximum force =inf on atom 294
Norm of force =  1.0627526e+19

Maximum force is equal to infinity and hence I am afraid to proceed  
further. Can someone help me out?



Thanks in advance.

Nabajyoti Goswami

Senior Research Fellow
Bioinformatics Center, Sri Venkateswara College
University of Delhi South Campus
Benito Juarez Road, Dhaula Kuan
New Delhi 110021
India

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Re: [gmx-users] Domain Motion = How do get the rotational axis from eigenvectors ?

2011-05-28 Thread XAvier Periole

You should a have good read at the original papers. They are mentioned on the 
web site. They will answer all your questions. 

On May 28, 2011, at 6:03, Chih-Ying Lin chihying2...@gmail.com wrote:

 
 Hi
 I want to get the rotational axis about the protein domain motion. 
 From the DynDom website = DynDom is a program to determine domains, hinge 
 axes and hinge bending residues in proteins where two conformations are 
 available.
 
 Questions: 
 1. Do the hinge axes represent the rotational axis about the protein domain 
 motion ? 
 2. From its User created database, domains and hinge bending residues, 
 rotation angles and translation are created. 
 = The rotation angles must be defined as the angle of rotation between 
 two domains based on the hinge axes, right ?
 = The vector of the hinge axes is not given by DynDom website, or I did 
 not find it ???
 = Hinge axes could be obtained from hinge bending axes residues, right 
   If so, How 
 = How can I get the vector of the hinge axes with the results from 
 DynDom ???
 = I found some papers drawing the hinge axes, can Gromacs help me find 
 and draw the hinge axes 
 = From User created database in the DynDom website, it is showing 
 Sequence. What does sequence represent ???
 3. Should I install the program of DynDom and then g_dyndom can be functioned 
 ??? 
 (we need to install DSSP before using do_dssp) 
 4. From Gromacs manual = The purpose of this program (g_dyndom) is to 
 interpolate and extrapolate the rotation as found by DynDom. 
What does it mean to interpolate and extrapolate the rotation as found by 
 DynDom ?
 
 
 Thank you
 Lin
 
 
 
 
 
 
 Message: 1
 Date: Thu, 26 May 2011 19:54:29 -0700
 From: Chih-Ying Lin chihying2...@gmail.com
 Subject: [gmx-users] Domain Motion = How do get the rotational axis
fromeigenvectors ?
 To: gmx-users@gromacs.org
 Message-ID: banlktinje0fhg6e1dso8aj66_n16xnc...@mail.gmail.com
 Content-Type: text/plain; charset=iso-8859-1
 
 Hi
 I want to protein's domain motion.
 I use   g_covarandg_anaeig  to get the eigenvectors.
 How can i get the rotational axis of which protein do its domain motion from
 those eigenvectors?
 
 I found the papers and the authors plot its rotational axis of domain
 motion.
 How did they make it ?
 
 
 Thank you
 Lin
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 Message: 2
 Date: Fri, 27 May 2011 05:54:07 +0200
 From: Tsjerk Wassenaar tsje...@gmail.com
 Subject: Re: [gmx-users] Domain Motion = How do get the rotational
axis from   eigenvectors ?
 To: Discussion list for GROMACS users gmx-users@gromacs.org
 Message-ID: BANLkTinKF=-c5+M7op80Dy2VaFM=ml4...@mail.gmail.com
 Content-Type: text/plain; charset=ISO-8859-1
 
 Hi Lin,
 
 You don't get such axes directly from covariance analysis. If you want
 to know which rotations are associated with a certain eigenvector, you
 have to run a routine like dyndom (http://fizz.cmp.uea.ac.uk/dyndom/)
 on the extreme projections of your trajectory onto an eigenvector.
 
 Cheers,
 
 Tsjerk
 
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Re: [gmx-users] decomposing the energy

2011-05-14 Thread XAvier Periole


Two things you have to be careful about:
1- use trr trajectory files. xtc precision is not sufficient and it  
will give a lot of discrepancies at least for the bonded terms.
2- set the nstlist to 1 as the neiboring list should be undated for  
each frame and not every 5/10 as it is normally set in a regular mdp  
file.


On May 14, 2011, at 1:11 PM, Justin A. Lemkul wrote:




Ramachandran G wrote:

Hello gmx users:
 I did 1ns simulation for my system and have the trajectory and  
energy files.
Now i want to see the energy of some specific residues. So, i  
decompose(separated) the energy groups and edited the mdp file.
Using the mdp file, i created a new tpr file and rerun the mdrun  
using the trajectory file. But when i compared the total energy  
between the old and new one, it differs a lot.
I am doing some mistakes somewhere. Can anyone help me please.  
Thanks.


Maybe, maybe not.  Without seeing the .mdp settings and the data  
that you're looking at, all anyone can do is guess.  You also  
haven't stated what type of trajectory (i.e. .xtc or .trr) you're  
using as -rerun input.  If you're using an .xtc file, there is no  
velocity information, so any property related to velocities (most  
notably kinetic energy, but several others as well) will be zero.  I  
suspect this is probably where the discrepancy is, but it is not a  
problem.  Using energygrps is only useful for decomposing short- 
range nonbonded energy terms, nothing else.


-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] Surface area calculation

2011-05-11 Thread XAvier Periole


reference:
Eisenhaber F, Lijnzaad P, Argos P, Sander C,  Scharf M (1995) J.  
Comput. Chem. 16, 273-284.


On May 11, 2011, at 2:34 PM, Laura Leay wrote:


Can anyone explain in detail the method that gromacs uses to calculate
surface area? Which surface area is it calculating (e.g., connolley,
accessible)?

I am under the impression that the final result is given in nm^2. Is
this correct?


Carrying out the surface area calculation in gromacs using the OPLS  
all

atom force field I obtain a value of 4.43 nm^2  for methane (carbon =
opls_138, sigma = 0.35 and hydrogen = opls_140, sigma = 0.25) (CT-HC
ideal bond length = 0.109, e=284512). The command was

g_sas -f conf.gro -s topol.tpr -oa -or -tv -probe 0.2 -ndots 200 - 
nopbc


and the result was taken from resarea.xvg


I have written a program to calculate the geometric accessible surface
area using the van der waals radius of the atoms and a probe of a  
given

size. The surface is defined from the centre of the probe. Using the
above values for sigma I obtain a value for methane of 1.15 nm^2  
with a

probe diameter of 0.2 nm.

Obviously the two do not match and I am not sure why.

The individual atom areas for my molecule are:
C 0.22
H 0.24
H 0.23
H 0.22
H 0.24

Attached are the files used in the gromacs calculation along with the
output and my own program. If any one has any suggestions please let  
me

know.
 
area 
.xvg 
 
 
atomarea 
.xvg 
 
 
conf 
.gro 
 
grompp.mdpmethane.itpresarea.xvgtopol.topPIsurfaceOPLS.f90--

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Re: [gmx-users] Umbrella sampling

2011-03-31 Thread XAvier Periole


On Mar 31, 2011, at 11:53 AM, Gavin Melaugh wrote:


Hi All

I have generated several PMF curves for the one system using umbrella
sampling. In the first part of the curve (barrier region) I use a high
force constant with small intervals between the windows. The latter  
part

of the curve I use a lower force constant with larger window spacing.
Anyway I have a few issues that I need clarifying:
1 - Can you have too much overlap between windows?

no, there no such a thing of too much overlap :)) You could even put
two identical windows with same 100% overlap ... no problem.

2 - Does the distribution at each window have to centered around the
desired r0? (If not does this affect the free energy?)

The deviation of the distribution from the r0 is what dictates the
profile. The more away from the disired r0 the higher the free energy
of the system.

3- If you over sample one particular window, will it affect the curve?

There is no such a thing of over sampling ... the only thing you can
have is not enough sampling.


Many thanks

GAvin
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Re: [gmx-users] Umbrella sampling

2011-03-31 Thread XAvier Periole


You can present the data differently:
you have two windows at 0.78 nm giving different distribution.

That indicates these windows are not converged. Does not mean
that the others (0.80 nm) are converged :))

On Mar 31, 2011, at 12:20 PM, Gavin Melaugh wrote:


Hi Xavier

Thanks for the reply. With respect to your answer of my first query.
What if you had two windows practically on top of each other, but one
was not supposed to be there. e.g A window with r0 of 0.80 nm and
centred at 0.78 nm and a window with r0 of 0.78 nm centred at 0.78nm.

Gavin

XAvier Periole wrote:


On Mar 31, 2011, at 11:53 AM, Gavin Melaugh wrote:


Hi All

I have generated several PMF curves for the one system using  
umbrella
sampling. In the first part of the curve (barrier region) I use a  
high
force constant with small intervals between the windows. The  
latter part
of the curve I use a lower force constant with larger window  
spacing.

Anyway I have a few issues that I need clarifying:
1 - Can you have too much overlap between windows?

no, there no such a thing of too much overlap :)) You could even put
two identical windows with same 100% overlap ... no problem.

2 - Does the distribution at each window have to centered around the
desired r0? (If not does this affect the free energy?)

The deviation of the distribution from the r0 is what dictates the
profile. The more away from the disired r0 the higher the free energy
of the system.
3- If you over sample one particular window, will it affect the  
curve?

There is no such a thing of over sampling ... the only thing you can
have is not enough sampling.


Many thanks

GAvin
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Re: [gmx-users] Umbrella sampling

2011-03-31 Thread XAvier Periole


My bad, I red to quick and though you had three windows ...
you should follow Justin's advice.

On Mar 31, 2011, at 2:20 PM, Gavin Melaugh wrote:


Thanks Justin for the reply

Gavin

Justin A. Lemkul wrote:



Gavin Melaugh wrote:
Sorry I am not sure that I follow. Will the window with r0 =0.80  
giving
the distribution centred around 0.78nm not drive my free energy  
profile
up. If I remove this window prior to running g_wham the free  
energy goes

down. Should I increase the force constant so that the mean of the
window is 0.80nm (bearing in mind that this is near the barrier  
region).




If you have an incomplete or otherwise discontinuous free energy
profile, then you won't get a correct result, but it's not simply due
to oversampling one region.  It's that the oversampling results  
in
undersampling another region.  Increasing the force constant for  
the

window centered around 0.80 nm should work.

-Justin


Gavin
XAvier Periole wrote:

You can present the data differently:
you have two windows at 0.78 nm giving different distribution.

That indicates these windows are not converged. Does not mean
that the others (0.80 nm) are converged :))

On Mar 31, 2011, at 12:20 PM, Gavin Melaugh wrote:


Hi Xavier

Thanks for the reply. With respect to your answer of my first  
query.
What if you had two windows practically on top of each other,  
but one

was not supposed to be there. e.g A window with r0 of 0.80 nm and
centred at 0.78 nm and a window with r0 of 0.78 nm centred at  
0.78nm.


Gavin

XAvier Periole wrote:

On Mar 31, 2011, at 11:53 AM, Gavin Melaugh wrote:


Hi All

I have generated several PMF curves for the one system using
umbrella
sampling. In the first part of the curve (barrier region) I  
use a

high
force constant with small intervals between the windows. The  
latter

part
of the curve I use a lower force constant with larger window
spacing.
Anyway I have a few issues that I need clarifying:
1 - Can you have too much overlap between windows?
no, there no such a thing of too much overlap :)) You could  
even put

two identical windows with same 100% overlap ... no problem.
2 - Does the distribution at each window have to centered  
around the

desired r0? (If not does this affect the free energy?)
The deviation of the distribution from the r0 is what dictates  
the
profile. The more away from the disired r0 the higher the free  
energy

of the system.

3- If you over sample one particular window, will it affect the
curve?
There is no such a thing of over sampling ... the only thing  
you can

have is not enough sampling.

Many thanks

GAvin
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Re: [gmx-users] GROMACS 4.5 and MARTINI Force Field Installation

2011-03-28 Thread XAvier Periole


You can use any GROMACS version to run a simulation
with the Martini Force field. IT is only if you want to back-map
your system to an atomistic resolution that you'll have to
use the gmx331 modified version.

On Mar 27, 2011, at 8:25 PM, Edroaldo Lummertz da Rocha wrote:


Dear GROMACS users,

I am starting to setup a molecular dynamics simulation and I want to  
use the MARTINI force field. I was reading the tutorial in website: http://md.chem.rug.nl/cgmartini/index.php/tutorial/reverse-transformation 
 and I have a beginner question for you: How can I use the MARTINI  
in the GROMACS 4.5? I ask that because the link above provides a  
modified version of GROMACS to perform the mappings between Fine  
Grained and Coarse Grained structures. However, the package provided  
is the GROMACS 3.3.1 version and I don't want to change my GROMACS  
version. I search in CCL and GROMACS mailing list about this and I  
didn't find how to do that. Can you help me? Thanks so much.

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Re: [gmx-users] calcium diffuses away from the protein during MD

2011-03-03 Thread XAvier Periole

It is unfortunately often that cations on their binding sites in proteins are 
not stable. Either the site reorganize or the ion leaves. 

The problem is that ions parameters and especially double charged ones are 
difficult to parameterize. 

It is often that people use additional restrains (harmonic bonds, weak compared 
to regular ones) to maintain the ion bound. 

XAvier

On Mar 4, 2011, at 6:55, Sunita Patel sun...@mailhost.tifr.res.in wrote:

 
 Dear Users,
 
 I performed MD simulation on a calcium binding protein with bound calcium
 starting from the crystal structure using gromos96 forcefield with explicit
 solvent with NVT ensembles. I performed energy minimization of calcium bound
 protein with water and following this position restraint molecular dynamics
 was performed. Subsequently, MD was performed on the system. In a less
 than 100 ps the calcium ion diffuse away from protein. However, in the
 experiment (NMR and X-ray)the protein is stable in calcium bound form. 
 
 What could be the reason for this?
 
 How can this problem be fixed?
 
 Thanks.
 
 Sunita
 
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Re: [gmx-users] negative steps from tpbconv

2011-02-24 Thread XAvier Periole


Hi Jesper,

This occurs when you ask for a number of steps that exceed the
the size of an integer! I got the same problem recently ...

The only solution I found was to make a new mdp file where t0
is the old time and asking for the extension you need ... you can
give trr and edr files to grompp so the tpr file is a continuation of
earlier one ...

XAvier.

On Feb 24, 2011, at 11:50 AM, Jesper Sørensen wrote:


Hi,

I am trying to extend the run time in tpr file to include more steps  
using tpbconv…

This has worked well for a while, but now I get two errors…
One is that it writes “now -207466 steps”, which doesn’t make  
sense – why is this number negative…

Also, “You've simulated long enough. Not writing tpr file”

If I extend the simulation using the –nsteps flag, then it will  
write the tpr file, but still comes up with negative numbers whens  
starting mdrun with the file, which mdrun does not exactly like.


Output is a s follows:
READING COORDS, VELS AND BOX FROM TRAJECTORY ../ 
T305/512DPPC_9728W_305K_625ns.trr...


trn version: GMX_trn_file (single precision)
Readtrr frame   4166: step 212466 time 53116500.000

Using frame of step 212466 time 5.31165e+07
Extending remaining runtime of by 625000 ps (now -207466 steps)
You've simulated long enough. Not writing tpr file

Best regards,
Jesper
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Re: [gmx-users] negative steps from tpbconv

2011-02-24 Thread XAvier Periole


I am not sure the use of cpt would work! I might have tried and
got a problem since the cpt might define where it is going (nsteps) ...
to be tried!

@Tsjerk: I have not been able to use the nsteps set to -1 for some
reason it was telling it had ran enough! Any idea why would that be?

On Feb 24, 2011, at 1:01 PM, Tsjerk Wassenaar wrote:


Hi Jesper,

Using a .cpt file will also work with the modified .tpr file.
Maybe it is also worth considering using the -maxh option to mdrun,
with nsteps in the .mdp file set to -1 (run infinitely). That avoids
the hassle with extensions.

Cheers,

Tsjerk

2011/2/24 Jesper Sørensen li...@jsx.dk:

Hi Xavier,



That worked, thanks… Would it also work if I just gave the old  
state.cpt

file to mdrun?



Jesper



From: gmx-users-boun...@gromacs.org [mailto:gmx-users-boun...@gromacs.org 
]

On Behalf Of XAvier Periole
Sent: 24. februar 2011 12:19
To: Discussion list for GROMACS users
Subject: Re: [gmx-users] negative steps from tpbconv





Hi Jesper,



This occurs when you ask for a number of steps that exceed the

the size of an integer! I got the same problem recently ...



The only solution I found was to make a new mdp file where t0

is the old time and asking for the extension you need ... you can

give trr and edr files to grompp so the tpr file is a continuation of

earlier one ...



XAvier.



On Feb 24, 2011, at 11:50 AM, Jesper Sørensen wrote:

Hi,



I am trying to extend the run time in tpr file to include more  
steps using

tpbconv…

This has worked well for a while, but now I get two errors…

One is that it writes “now -207466 steps”, which doesn’t make  
sense –

why is this number negative…

Also, “You've simulated long enough. Not writing tpr file”



If I extend the simulation using the –nsteps flag, then it will  
write the
tpr file, but still comes up with negative numbers whens starting  
mdrun with

the file, which mdrun does not exactly like.



Output is a s follows:

READING COORDS, VELS AND BOX FROM TRAJECTORY
../T305/512DPPC_9728W_305K_625ns.trr...



trn version: GMX_trn_file (single precision)

Readtrr frame   4166: step 212466 time 53116500.000



Using frame of step 212466 time 5.31165e+07

Extending remaining runtime of by 625000 ps (now -207466 steps)

You've simulated long enough. Not writing tpr file



Best regards,

Jesper

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--
Tsjerk A. Wassenaar, Ph.D.

post-doctoral researcher
Molecular Dynamics Group
* Groningen Institute for Biomolecular Research and Biotechnology
* Zernike Institute for Advanced Materials
University of Groningen
The Netherlands
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Re: [gmx-users] Can g_wham support using different temperature for different windows?

2011-02-23 Thread XAvier Periole


On Feb 23, 2011, at 3:21 AM, Jianguo Li wrote:



Thank you  for the the useful information, XAvier.
My peptide is highly positively charged, 18 AA with +12 charges.  
Other of my group members told me their NMR experiment in water  
indicates the peptide conformation is very dynamics. Actually I also  
did peptide refolding using REMD in water, and I found it is  
flexible and has no stable structure in water, except some  
instantaneously helical structures. In addition, my peptide consists  
of two branches connected by unnatural peptide bond, so the backbone  
is discontinuous, and also because of the high charges, I assume the  
peptide doesn't form helcial structure in the negatively charged  
membrane. Therefore I didn't put any constraints in the peptide to  
keep the secondary structure of the peptide. I know there are  
assumptions in my model, but I have no other information to increase  
the accuracy of the model.  In fact, when I am doing REMD folding  
simulations using Gromos53a6 and CHARMM27 with cMap, I got different  
results. But the common thing is that both results seems to indicate  
the peptide is filexbile in water without stable secondary  
structure. Then I used MARTINI FF with flexible structure, just to  
find some general features.


I will try your suggestion, doing REMD in those bad windows.

And the reference you mentioned is very useful, I will take a look  
at them :-)


Another question: Suppose some other tools support using different  
temperatures in different windows, as you mentioned, if 500K is too  
high to have a significant contribution to the probability of 300K,   
can I do a series of simulation in a certain window with different  
temparatures (e.g. 300K, 350K, 400K,450K, 500K). In such cases, in  
each window, I need to do 5 simulations, which will be much cheaper  
than doing REMD in that window.
It would be computationally cheaper but this is assuming that you'd  
get the info you are looking for within these simulations and again  
the weight of the conformations from 400/450/500 K at 300 K is  
questionable. Note also that the conformations sampled at high  
temperature with position restrains on the lipids to avoid deformation  
will be difficult to interpret!


Cheers
Jianguo


From: XAvier Periole x.peri...@rug.nl
To: Discussion list for GROMACS users gmx-users@gromacs.org
Sent: Tuesday, 22 February 2011 21:18:12
Subject: Re: [gmx-users] Can g_wham support using different  
temperature for different windows?



A few notes:
- the original method (Kumar-JCC-1992) that inspired wham was actually
developed to mix different temperature simulations. It is however  
not clear

for the type of system you are simulating how much a 500K simulation
would be useful to improve the sampling at 300 K or so. The reason is
that the enthalpy difference between the two systems is so high that  
the
probability that a conformation from a 500K simulation would  
contribute
to sampling at 300K is really low. It would much more efficient for  
systems
with implicit solvent for which the energy of the system does not  
vary so

much with the temperature. One could look at Chodera-JCTC-2007
and ref therein for a few examples.
- I would think that a REMD simulation would be more useful. No need  
to
run 30 replicas to very hight temperature! A bilayer at 500K might  
get funny.


- Martini force field for flexible regions of protein should not be  
trusted ... or
really interpreted with a lot of reserve. The coil definition is  
simply something
flexible with absolutely no guaranty that it could be representing  
some thing
even close to reality, which we have only an approximate idea of  
what it is!


- A peptide in a bilayer has a very high chance to get into a  
helical conformation.

Do you think it is reasonable to keep it flexible?

- As noted by Justin and Chris, you definitely have a problem of  
convergence ...
I am not sure how many converged examples of PMFs of peptide  
crossing a
bilayer are out in the literature (Justin?) but from our experience  
with Martini
it does take an awful lot of time to really get convergence. For you  
system I
would expect at least a microsecond for the windows where sampling  
is an
issue. As an example, we saw significant differences on a PMF  
between two

simple helices up to 8 us ... and no charges were involved.

This might be a lot pessimistic but you should not get fooled by a  
CG model.
Martini is really good for a lot of things but other things should  
really but be

looked at carefully.

XAvier.

On Feb 22, 2011, at 9:12 AM, Jianguo Li wrote:


Sorry I forgot to attach my mdp files.

Here is the mdp file for pulling simulaition:
-




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Re: [gmx-users] Can g_wham support using different temperature for different windows?

2011-02-22 Thread XAvier Periole


A few notes:
- the original method (Kumar-JCC-1992) that inspired wham was actually
developed to mix different temperature simulations. It is however not  
clear

for the type of system you are simulating how much a 500K simulation
would be useful to improve the sampling at 300 K or so. The reason is
that the enthalpy difference between the two systems is so high that the
probability that a conformation from a 500K simulation would contribute
to sampling at 300K is really low. It would much more efficient for  
systems
with implicit solvent for which the energy of the system does not vary  
so

much with the temperature. One could look at Chodera-JCTC-2007
and ref therein for a few examples.
- I would think that a REMD simulation would be more useful. No need to
run 30 replicas to very hight temperature! A bilayer at 500K might get  
funny.


- Martini force field for flexible regions of protein should not be  
trusted ... or
really interpreted with a lot of reserve. The coil definition is  
simply something
flexible with absolutely no guaranty that it could be representing  
some thing
even close to reality, which we have only an approximate idea of what  
it is!


- A peptide in a bilayer has a very high chance to get into a helical  
conformation.

Do you think it is reasonable to keep it flexible?

- As noted by Justin and Chris, you definitely have a problem of  
convergence ...
I am not sure how many converged examples of PMFs of peptide  
crossing a
bilayer are out in the literature (Justin?) but from our experience  
with Martini
it does take an awful lot of time to really get convergence. For you  
system I

would expect at least a microsecond for the windows where sampling is an
issue. As an example, we saw significant differences on a PMF between  
two

simple helices up to 8 us ... and no charges were involved.

This might be a lot pessimistic but you should not get fooled by a CG  
model.
Martini is really good for a lot of things but other things should  
really but be

looked at carefully.

XAvier.

On Feb 22, 2011, at 9:12 AM, Jianguo Li wrote:


Sorry I forgot to attach my mdp files.

Here is the mdp file for pulling simulaition:
-



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Re: [gmx-users] removing pbc jumps from trajectory

2011-02-21 Thread XAvier Periole

You have to make sure of two things:

1- use a reference (gro or tpr) where the molecule is whole! The tpr is 
prefered since the molecules are defined. 

2- with such a reference and the option -mol you'll get a trajectory with the 
protein as a whole. 

On that trajectory you may apply more modifications: 
-nojump with generate a trajectory where the pbc are not applied so you can do 
msd analysis. Note that thisnis done by default in g_msd. 
- fitting with only translation removed (equivalent to centering but more 
stable. Centering works strangely)

XAvier.  

On Feb 21, 2011, at 8:52, Evelyne Deplazes depla...@student.uwa.edu.au wrote:

 Hi 
 
 I have a series of trajectories from a coarse grained simulation (Martini 
 force field) that I ran using gromacs 4.0.4. The system consists of a protein 
 embedded in a POPC bilayer solvated with water. During the simulation the 
 protein (most of time its actually *part* of the protein) jumps across the pb 
 into the neighboring box. I use a series of tcl scripts to analyse my 
 trajectories and for that purpose I need to remove that period boundary 
 jump and make the protein whole again. 
 
 I have tried the approach described on the gromacs website 
 http://www.gromacs.org/Documentation/Terminology/Periodic_Boundary_Conditions
 
 I also other combinations of -whole, -center and -pbc nojump of trjconv, 
 without any luck. Can anyone suggest how I can re-center the protein and 
 remove the pb jump ie make the protein whole
 
 Thanks 
 Evelyne 
 
 -- 
 Evelyne Deplazes
 
 PhD student 
 Theoretical Chemistry group
 University of Western Australia 
 
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Re: [gmx-users] Re: gmx-users Digest, Vol 82, Issue 150

2011-02-21 Thread XAvier Periole


ok this does not make sense! Did you check your tpr file?
the command 1) should give you a trajectory where the molecules
are whole but jumping across the boundaries ... if it does not that
means that the tpr is fucky!

Try to visualize your tpr in vmd ... night give you some insight on  
what is

going on!

You could also make a tpr file ... making sure things a fine :))

On Feb 21, 2011, at 9:45 AM, Evelyne Deplazes wrote:

I tried a couple of things according to your suggestions, but no  
luck so far


I used the following commands
1) trjconv  -f trajout_dt2000.xtc -s topol.tpr -pbc mol -o  
trajout_mol.xtc
2) trjconv  -f trajout_mol.xtc -s topol.tpr -pbc nojump  
trajout_nojump.xtc


no luck...If I use command 1) only the trajout_mol.xtc the protein  
is still split into to across 2 boxes ie it looks like it did not  
do anything to the trajectory
if I use 1) and 2) the system gets ripped apart. The system is no  
longer a box but a flat disk (very funky)



then I tried
trjconv  -f trajout_dt2000.xtc -s topol.tpr -pbc mol -fit  
translation -o trajout_fit.xtc
again...it looks like the trajectory did not change and the protein  
is still jumping out of the box


then I tried
trjconv  -f trajout_dt2000.xtc -s topol.tpr -pbc mol -trans -6 6 0 - 
o trajout_trans.xtc(the box is about 12 x 12)
now at least this command did something to the trajectory. The  
entire protein is now in the center of the box (rather than in the  
corner) but in the frames where the pb jump occurs the protein still  
jumps out of the box! it now simply jumps from the center to the  
next box rather than sliding across the border into the next box


On 21 February 2011 16:02, gmx-users-requ...@gromacs.org wrote:
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Today's Topics:

  1. Re: g_covar to calculate correlation of motion (Tsjerk Wassenaar)
  2. Re: g_covar to calculate correlation of motion (bipin singh)
  3. removing pbc jumps from trajectory (Evelyne Deplazes)
  4. Re: removing pbc jumps from trajectory (XAvier Periole)


-- Forwarded message --
From: Tsjerk Wassenaar tsje...@gmail.com
To: Discussion list for GROMACS users gmx-users@gromacs.org
Date: Mon, 21 Feb 2011 08:14:26 +0100
Subject: Re: [gmx-users] g_covar to calculate correlation of motion
Hi Bipin,

Try using a .gro or .pdb file as reference structure (-s). Only .tpr  
files are version specific.


Cheers,

Tsjerk



On Feb 21, 2011 8:05 AM, bipin singh bipinel...@gmail.com wrote:

Dear GMX users,
I want to calculate the correlated motion between atoms during the  
md simulation



for that purpose I am using g_covar(the one which is available  
under http://www.gromacs.org/Downloads/User_contributions/Other_software)




but it is not compatible with the GROMACS-4.5.3, so please suggest  
me the alternative way or does anyone have the modified g_covar for

GROMKACS-4.5.3.

--
-
Thanks and regards
Bipin Singh



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-- Forwarded message --
From: bipin singh bipinel...@gmail.com
To: Discussion list for GROMACS users gmx-users@gromacs.org
Date: Mon, 21 Feb 2011 13:17:48 +0530
Subject: Re: [gmx-users] g_covar to calculate correlation of motion
Hi,
Thanks for your suggestion.
While running the g_covar it is showing the error that  
aminoacids.dat is not found, so i have copied the  
residuetypes.dat(which i seems the new modified name for  
aminoacids.dat in current GROMACS version), then it prompts to  
choose the group for least square fit, which is not usual groups(i.e  
protein or C alpha groups etc.).please suggest where i have made  
mistake.


Choose a group for the least squares fit
Opening library file aminoacids.dat
WARNING 2 [file aminoacids.dat, line 1]:
  File aminoacids.dat is empty
Group 0 (  System) has 30585 elements
Group 1 ( GLU) has47 elements
Group 2 ( HIS) has86 elements
Group 3 ( ASN) has   224 elements
Group 4 ( PRO) has56 elements
Group 5 ( VAL) has   272 elements
Group 6 ( MET) has68 elements
Group 7 ( GLY) has   168 elements
Group 8 ( ILE) has

Re: [gmx-users] how many contacts has a certain atom at MD

2011-02-21 Thread XAvier Periole

g_dist
On Feb 21, 2011, at 11:32 AM, Olga Ivchenko wrote:


Dear Gromacs Users,

I would like to know if there is in gromacs an option how to  
calculate how many contacts has a certain atom i(n a molecules of  
interest) with water during the whole MD simulations (or at each  
step of MD).

Please could you advice me on this?

best,
Olga

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Re: [gmx-users] Simulation using Martini force field

2011-02-14 Thread XAvier Periole


Dear Regina,

You have two problems:
1- the parameterization of phosphorylated serine should be done
following the same philosophy of Martini. Check the Martini papers
to see how this is done. In short partitioning is of primary importance.
2- you want to simulate unfolded protein ... indeed there is evidently
no persistent structure in such system and therefore the choice for
secondary structure would be coil in the Martini force field.
However the definition of coil for Martini has not been parameterize
to reproduce anything even close to what an unfolded protein, assuming
that we know what it looks like :)) The Martini coil is simply  
something

flexible.

I am afraid Martini is just not ready for simulating unfolded proteins.
Any outcome of a simulation would have to be interpreted with CARE!

XAvier.

On Feb 14, 2011, at 2:09 PM, pol...@fh.huji.ac.il wrote:


Dear Gromacs users and developers,
I'm interested to run simulation of natively unstructured protein  
(casein), that can self assembly and create micelles, using Martini  
force field. The initial structure of the monomer was created and  
minimized using Sybyl. This protein includes also 4 phosporylated  
serines. I'm trying to understand how should I set my system. I  
started from the tutorial (http://md.chem.rug.nl/cgmartini/index.php/tutorial/ubiquitin-in-water 
) but I found that have no idea how to create a phosphorylated  
serine inCG structure (I have it in my initial pdb). In addition, I  
found that I need a secondary structure of the protein and I don't  
have something like this. Moreover, this protein doesn't have one. I  
will appreciated very much if somebody can help me and guide me a  
little.

Thank you very much in advance.
Regina


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Re: [gmx-users] Simulation using Martini force field

2011-02-14 Thread XAvier Periole


On Feb 14, 2011, at 7:24 PM, devicerandom wrote:


On 14/02/11 13:42, XAvier Periole wrote:


Dear Regina,

You have two problems:
1- the parameterization of phosphorylated serine should be done
following the same philosophy of Martini. Check the Martini papers
to see how this is done. In short partitioning is of primary  
importance.
2- you want to simulate unfolded protein ... indeed there is  
evidently

no persistent structure in such system and therefore the choice for
secondary structure would be coil in the Martini force field.
However the definition of coil for Martini has not been  
parameterize
to reproduce anything even close to what an unfolded protein,  
assuming
that we know what it looks like :)) The Martini coil is simply  
something

flexible.

I am afraid Martini is just not ready for simulating unfolded  
proteins.

Any outcome of a simulation would have to be interpreted with CARE!


Agree with Xavier. I am working exactly on a coarse grained generic  
FF that could allow this kind of simulations, but it's far from  
being production ready -not an easy task at all. :)

thanks for your support devicerandom!



XAvier.

On Feb 14, 2011, at 2:09 PM, pol...@fh.huji.ac.il wrote:


Dear Gromacs users and developers,
I'm interested to run simulation of natively unstructured protein
(casein), that can self assembly and create micelles, using Martini
force field. The initial structure of the monomer was created and
minimized using Sybyl. This protein includes also 4 phosporylated
serines. I'm trying to understand how should I set my system. I
started from the tutorial
(http://md.chem.rug.nl/cgmartini/index.php/tutorial/ubiquitin-in-water 
) but

I found that have no idea how to create a phosphorylated serine inCG
structure (I have it in my initial pdb). In addition, I found that I
need a secondary structure of the protein and I don't have something
like this. Moreover, this protein doesn't have one. I will  
appreciated

very much if somebody can help me and guide me a little.
Thank you very much in advance.
Regina


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Re: [gmx-users] Simulation using Martini force field

2011-02-14 Thread XAvier Periole


On Feb 14, 2011, at 11:43 PM, pol...@fh.huji.ac.il wrote:

Thank you very much for you reply. Can you please explain me why do  
i need secondary structure file at all and why secondary structure  
is pre-defined and thus static throughout a simulation? I didn't  
see that something like this defined for lipids.
Have look at the Martini paper for protein (JCTC-2009) you might find  
some stuff quite instructive in there :))


FYI lipids do not have secondary structure or something that would  
succgest they could have different interacting behavior in function of  
their conformation.
How do I use do_dssp to build the needed file? I saw that I need a  
topology file in rder to use do_dssp. Where can I find this topology  
file? I hope this is ok that I'm asking so many questions. Thank you  
very much for your help.

No problem it just shows how it was a good idea to make a tutorial :))
have look there cgmartini.nl

Regina
Quoting XAvier Periole x.peri...@rug.nl:



Dear Regina,

You have two problems:
1- the parameterization of phosphorylated serine should be done
following the same philosophy of Martini. Check the Martini papers
to see how this is done. In short partitioning is of primary  
importance.
2- you want to simulate unfolded protein ... indeed there is  
evidently

no persistent structure in such system and therefore the choice for
secondary structure would be coil in the Martini force field.
However the definition of coil for Martini has not been  
parameterize
to reproduce anything even close to what an unfolded protein,  
assuming
that we know what it looks like :)) The Martini coil is simply  
something

flexible.

I am afraid Martini is just not ready for simulating unfolded  
proteins.

Any outcome of a simulation would have to be interpreted with CARE!

XAvier.

On Feb 14, 2011, at 2:09 PM, pol...@fh.huji.ac.il wrote:


Dear Gromacs users and developers,
I'm interested to run simulation of natively unstructured protein  
(casein), that can self assembly and create micelles, using  
Martini force field. The initial structure of the monomer was  
created and minimized using Sybyl. This protein includes also 4  
phosporylated serines. I'm trying to understand how should I set  
my system. I started from the tutorial (http://md.chem.rug.nl/cgmartini/index.php/tutorial/ubiquitin-in-water 
) but I found that have no idea how to create a phosphorylated  
serine inCG structure (I have it in my initial pdb). In addition,  
I found that I need a secondary structure of the protein and I  
don't have something like this. Moreover, this protein doesn't  
have one. I will appreciated very much if somebody can help me and  
guide me a little.

Thank you very much in advance.
Regina


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Re: [gmx-users] WHAM with multiple force constants

2011-02-10 Thread XAvier Periole


On Feb 10, 2011, at 3:08 PM, jk...@ifr88.cnrs-mrs.fr wrote:


Hi,

I'm running an Umbrella Sampling analysis, with 1A steps in the  
reaction coordinate (distance) to estimate a PMF. However, owing to  
(high?) energetic barriers between my two proteins, some coordinates  
are not sampled. I intend to run simulations with stronger force  
constants to prevent my protein from fleeing to the nearest  
energetic minima.


So my question is : does  using different force constants to  
restrain the distance between my two proteins influences the PMF  
estimated by g_wham ?

No it does not assuming each window is equilibrated.


From what I understood, it doesn't seems so, as long as the  
distributions are well overlapped. But since I intend to invest a  
considerable amount of CPU time, a confirmation would be really  
apreciated !


Thanks,

Jonathan.




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Re: [gmx-users] Sampling windows

2011-01-05 Thread XAvier Periole


On Jan 5, 2011, at 4:08 PM, Gavin Melaugh wrote:


Dear all

I have generated a PMF curve for introducing a guest molecule into a
host molecule using the umbrella sampling method. The curve seems  
fine,

but there are no overlaps between histograms in the barrier region. To
circumvent this I have added more windows in this region and to ensure
sampling have increased the force constant only in this region. The
windows in this problematic region are now not equally spaced. Does  
this

matter for g_WHAM?

Nope it does not matter.

Could someone please reply to me on this matter as it
has been a sticking point for me for quite sometime?

Many thanks
Gavin
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Re: [gmx-users] Sampling windows

2011-01-05 Thread XAvier Periole


On Jan 5, 2011, at 5:01 PM, Gavin Melaugh wrote:


Hi Xavier

Many thanks for the reply. When I compare the two curves
Curve 1) lack of overlap in barrier region; force constant = 1000
Curve 2) with increased number of sampling windows with increased  
force

constant (note I have only increased the force constant of the windows
in the barrier region).
Force constant =1000, Force constant in barrier region  = 5000

The barrier increases due to better sampling in this region  
(expected),
but the rest of the curve in 2) is shifted upward compared to curve  
1).

Why is this so when the only difference is the increased number of
windows and force constant in one region?
the relative position of the regions on the left and right of your  
barrier

region is completely depending on the barrier region!

you may have overestimated the difference between bound/unbound states
because the energy barrier region was not sampled.

Note also that cure one is simply wrong so comparing to it is dangerous.

You have to be careful that you might still not have a converged  
sampling:

you might have overlap of your histograms on the reaction coordinate but
other degrees of freedom are not fully sampled ... that might result  
in a

funny and wrong profile. You might want to look at your simulations for
funny things ...



Gavin



XAvier Periole wrote:


On Jan 5, 2011, at 4:08 PM, Gavin Melaugh wrote:


Dear all

I have generated a PMF curve for introducing a guest molecule into a
host molecule using the umbrella sampling method. The curve seems  
fine,
but there are no overlaps between histograms in the barrier  
region. To
circumvent this I have added more windows in this region and to  
ensure

sampling have increased the force constant only in this region. The
windows in this problematic region are now not equally spaced.  
Does this

matter for g_WHAM?

Nope it does not matter.

Could someone please reply to me on this matter as it
has been a sticking point for me for quite sometime?

Many thanks
Gavin
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