[gmx-users] the total charge of system is not an integer

2011-03-31 Thread ahmet yıldırım
Dear users,

Before energy minimization step , I performed the preprosessing step using
grompp .
However, there are two note that :

*NOTE 1 [file topol.top, line 52]:*
  System has non-zero total charge: -1.50e+01

*NOTE 2 [file topol.top]:*
  The largest charge group contains 11 atoms.
  Since atoms only see each other when the centers of geometry of the charge
  groups they belong to are within the cut-off distance, too large charge
  groups can lead to serious cut-off artifacts.
  For efficiency and accuracy, charge group should consist of a few atoms.
  For all-atom force fields use: CH3, CH2, CH, NH2, NH, OH, CO2, CO, etc.
*
PS: *TRS and EDO are not aminoacid*

TRS.itp:*
..
[ moleculetype ]
; Name nrexcl
TRS  3

[ atoms ]
;   nr  type  resnr resid  atom  cgnr   charge mass
 1OA 1  TRS  O1 1   -0.119  15.9994
 2 H 1  TRS H13 10.032   1.0080
 3   CH2 1  TRS  C1 10.087  14.0270
 4  CCl4 1  TRS   C 20.055  12.0110
 5   CH2 1  TRS  C3 20.049  14.0270
 6OA 1  TRS  O3 2   -0.205  15.9994
 7 H 1  TRS H33 20.019   1.0080
 8NL 1  TRS   N 20.206  14.0067
 9 H 1  TRS  H2 20.004   1.0080
10 H 1  TRS  H3 20.004   1.0080
11 H 1  TRS  H1 20.004   1.0080
12   CH2 1  TRS  C2 20.050  14.0270
13OA 1  TRS  O2 2   -0.205  15.9994
14 H 1  TRS H23 20.019   1.0080
...

*EDO.itp*
...
[ moleculetype ]
; Name nrexcl
EDO  3

[ atoms ]
;   nr  type  resnr resid  atom  cgnr   charge mass
 1OA 1  EDO OAB 1   -0.111  15.9994
 2 H 1  EDO HAE 10.031   1.0080
 3   CH2 1  EDO CAA 10.080  14.0270
 4   CH2 1  EDO CAC 10.080  14.0270
 5OA 1  EDO OAD 1   -0.111  15.9994
 6 H 1  EDO HAF 10.031   1.0080
...
*
topol.top:*
..
; Include water topology
#include gromos43a1.ff/spc.itp
#include TRS.itp
#include EDO.itp
..
[ molecules ]
; Compound#mols
Protein_chain_A 1
Protein_chain_B 1
SOL   185
SOL   143
TRS1
EDO1
SOL 44125
*
Conf.gro:*
MTA/SAH NUCLEOSIDASE; 5 NUCLEOSIDASE
 5354
2GLN  N1   1.458  -1.158   0.739
2GLN H12   1.520  -1.083   0.763
...
  485HOHHW1 5333   0.221  -3.864  -2.291
  485HOHHW2 5334   0.303  -3.946  -2.407
1TRS  O1   1  -3.812  -0.471  -2.002
1TRS  H13  2  -3.865  -0.443  -1.922
1TRS  C1   3  -3.672  -0.469  -1.971
1TRS  C4  -3.635  -0.571  -1.863
1TRS  C3   5  -3.711  -0.547  -1.731
1TRS  O3   6  -3.694  -0.414  -1.679
1TRS  H33  7  -3.746  -0.404  -1.594
1TRS  N8  -3.673  -0.705  -1.911
1TRS  H2   9  -3.625  -0.725  -1.996
1TRS  H3  10  -3.771  -0.707  -1.927
1TRS  H1  11  -3.649  -0.774  -1.842
1TRS  C2  12  -3.483  -0.573  -1.840
1TRS  O2  13  -3.428  -0.445  -1.806
1TRS  H23 14  -3.470  -0.412  -1.722
1EDO  OAB  1   0.307  -2.792   0.149
1EDO  HAE  2   0.390  -2.826   0.104
1EDO  CAA  3   0.239  -2.901   0.212
1EDO  CAC  4   0.111  -2.851   0.281
1EDO  OAD  5   0.144  -2.763   0.388
1EDO  HAF  6   0.060  -2.731   0.432
   8.13100   7.04165  13.54850   0.0   0.0  -4.06550   0.0
0.0   0.0

How can I fixed these notes(note 1 and note 2)?

Thanks in advance
-- 
Ahmet YILDIRIM
-- 
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Re: [gmx-users] the total charge of system is not an integer

2011-03-31 Thread Tsjerk Wassenaar
Hi Ahmet,

As suggested, it's better to break up your molecule into smaller
charge groups. Note that charge groups don't need to have zero charge,
nor integer charge. In your case, I'd suggest two COH groups for EDO,
which will have zero net charge each, and for TRS I'd take the COH
groups as separate charge groups. I also note that the COH groups,
although chemically identical - H3NC(COH)3, right?-, have different
charges. That doesn't seem proper.

Hope it helps,

Tsjerk

2011/3/31 ahmet yıldırım ahmedo...@gmail.com:
 Dear users,

 Before energy minimization step , I performed the preprosessing step using
 grompp .
 However, there are two note that :

 NOTE 1 [file topol.top, line 52]:
   System has non-zero total charge: -1.50e+01

 NOTE 2 [file topol.top]:
   The largest charge group contains 11 atoms.
   Since atoms only see each other when the centers of geometry of the charge
   groups they belong to are within the cut-off distance, too large charge
   groups can lead to serious cut-off artifacts.
   For efficiency and accuracy, charge group should consist of a few atoms.
   For all-atom force fields use: CH3, CH2, CH, NH2, NH, OH, CO2, CO, etc.

 PS: TRS and EDO are not aminoacid

 TRS.itp:
 ..
 [ moleculetype ]
 ; Name nrexcl
 TRS  3

 [ atoms ]
 ;   nr  type  resnr resid  atom  cgnr   charge mass
  1    OA 1  TRS  O1 1   -0.119  15.9994
  2 H 1  TRS H13 1    0.032   1.0080
  3   CH2 1  TRS  C1 1    0.087  14.0270
  4  CCl4 1  TRS   C 2    0.055  12.0110
  5   CH2 1  TRS  C3 2    0.049  14.0270
  6    OA 1  TRS  O3 2   -0.205  15.9994
  7 H 1  TRS H33 2    0.019   1.0080
  8    NL 1  TRS   N 2    0.206  14.0067
  9 H 1  TRS  H2 2    0.004   1.0080
     10 H 1  TRS  H3 2    0.004   1.0080
     11 H 1  TRS  H1 2    0.004   1.0080
     12   CH2 1  TRS  C2 2    0.050  14.0270
     13    OA 1  TRS  O2 2   -0.205  15.9994
     14 H 1  TRS H23 2    0.019   1.0080
 ...

 EDO.itp
 ...
 [ moleculetype ]
 ; Name nrexcl
 EDO  3

 [ atoms ]
 ;   nr  type  resnr resid  atom  cgnr   charge mass
  1    OA 1  EDO OAB 1   -0.111  15.9994
  2 H 1  EDO HAE 1    0.031   1.0080
  3   CH2 1  EDO CAA 1    0.080  14.0270
  4   CH2 1  EDO CAC 1    0.080  14.0270
  5    OA 1  EDO OAD 1   -0.111  15.9994
  6 H 1  EDO HAF 1    0.031   1.0080
 ...

 topol.top:
 ..
 ; Include water topology
 #include gromos43a1.ff/spc.itp
 #include TRS.itp
 #include EDO.itp
 ..
 [ molecules ]
 ; Compound    #mols
 Protein_chain_A 1
 Protein_chain_B 1
 SOL   185
 SOL   143
 TRS    1
 EDO    1
 SOL 44125

 Conf.gro:
 MTA/SAH NUCLEOSIDASE; 5 NUCLEOSIDASE
  5354
     2GLN  N    1   1.458  -1.158   0.739
     2GLN H1    2   1.520  -1.083   0.763
 ...
   485HOH    HW1 5333   0.221  -3.864  -2.291
   485HOH    HW2 5334   0.303  -3.946  -2.407
     1TRS  O1   1  -3.812  -0.471  -2.002
     1TRS  H13  2  -3.865  -0.443  -1.922
     1TRS  C1   3  -3.672  -0.469  -1.971
     1TRS  C    4  -3.635  -0.571  -1.863
     1TRS  C3   5  -3.711  -0.547  -1.731
     1TRS  O3   6  -3.694  -0.414  -1.679
     1TRS  H33  7  -3.746  -0.404  -1.594
     1TRS  N    8  -3.673  -0.705  -1.911
     1TRS  H2   9  -3.625  -0.725  -1.996
     1TRS  H3  10  -3.771  -0.707  -1.927
     1TRS  H1  11  -3.649  -0.774  -1.842
     1TRS  C2  12  -3.483  -0.573  -1.840
     1TRS  O2  13  -3.428  -0.445  -1.806
     1TRS  H23 14  -3.470  -0.412  -1.722
     1EDO  OAB  1   0.307  -2.792   0.149
     1EDO  HAE  2   0.390  -2.826   0.104
     1EDO  CAA  3   0.239  -2.901   0.212
     1EDO  CAC  4   0.111  -2.851   0.281
     1EDO  OAD  5   0.144  -2.763   0.388
     1EDO  HAF  6   0.060  -2.731   0.432
    8.13100   7.04165  13.54850   0.0   0.0  -4.06550   0.0
 0.0   0.0

 How can I fixed these notes(note 1 and note 2)?

 Thanks in advance
 --
 Ahmet YILDIRIM

 --
 gmx-users mailing list    gmx-users@gromacs.org
 http://lists.gromacs.org/mailman/listinfo/gmx-users
 Please search the archive at
 http://www.gromacs.org/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




-- 
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

Re: [gmx-users] the total charge of system is not an integer

2011-03-31 Thread Mark Abraham

On 31/03/2011 5:18 PM, ahmet y?ld?r?m wrote:

Dear users,

Before energy minimization step , I performed the preprosessing step 
using grompp .

However, there are two note that :

*_NOTE 1 [file topol.top, line 52]:_*
  System has non-zero total charge: -1.50e+01


This is an integer. See 
http://en.wikipedia.org/wiki/Scientific_notation#E_notation and 
http://www.gromacs.org/Documentation/Floating_Point_Arithmetic



_*NOTE 2 [file topol.top]:*_
  The largest charge group contains 11 atoms.
  Since atoms only see each other when the centers of geometry of the 
charge

  groups they belong to are within the cut-off distance, too large charge
  groups can lead to serious cut-off artifacts.
  For efficiency and accuracy, charge group should consist of a few atoms.
  For all-atom force fields use: CH3, CH2, CH, NH2, NH, OH, CO2, CO, etc.


See Tsjerk's email.

Mark


*
PS: *TRS and EDO are not aminoacid*

_TRS.itp:_*
..
[ moleculetype ]
; Name nrexcl
TRS  3

[ atoms ]
;   nr  type  resnr resid  atom  cgnr   charge mass
 1OA 1  TRS  O1 1   -0.119  15.9994
 2 H 1  TRS H13 10.032   1.0080
 3   CH2 1  TRS  C1 10.087  14.0270
 4  CCl4 1  TRS   C 20.055  12.0110
 5   CH2 1  TRS  C3 20.049  14.0270
 6OA 1  TRS  O3 2   -0.205  15.9994
 7 H 1  TRS H33 20.019   1.0080
 8NL 1  TRS   N 20.206  14.0067
 9 H 1  TRS  H2 20.004   1.0080
10 H 1  TRS  H3 20.004   1.0080
11 H 1  TRS  H1 20.004   1.0080
12   CH2 1  TRS  C2 20.050  14.0270
13OA 1  TRS  O2 2   -0.205  15.9994
14 H 1  TRS H23 20.019   1.0080
...

_*EDO.itp*_
...
[ moleculetype ]
; Name nrexcl
EDO  3

[ atoms ]
;   nr  type  resnr resid  atom  cgnr   charge mass
 1OA 1  EDO OAB 1   -0.111  15.9994
 2 H 1  EDO HAE 10.031   1.0080
 3   CH2 1  EDO CAA 10.080  14.0270
 4   CH2 1  EDO CAC 10.080  14.0270
 5OA 1  EDO OAD 1   -0.111  15.9994
 6 H 1  EDO HAF 10.031   1.0080
...
_*
topol.top:*_
..
; Include water topology
#include gromos43a1.ff/spc.itp
#include TRS.itp
#include EDO.itp
..
[ molecules ]
; Compound#mols
Protein_chain_A 1
Protein_chain_B 1
SOL   185
SOL   143
TRS1
EDO1
SOL 44125
*_
Conf.gro:_*
MTA/SAH NUCLEOSIDASE; 5 NUCLEOSIDASE
 5354
2GLN  N1   1.458  -1.158   0.739
2GLN H12   1.520  -1.083   0.763
...
  485HOHHW1 5333   0.221  -3.864  -2.291
  485HOHHW2 5334   0.303  -3.946  -2.407
1TRS  O1   1  -3.812  -0.471  -2.002
1TRS  H13  2  -3.865  -0.443  -1.922
1TRS  C1   3  -3.672  -0.469  -1.971
1TRS  C4  -3.635  -0.571  -1.863
1TRS  C3   5  -3.711  -0.547  -1.731
1TRS  O3   6  -3.694  -0.414  -1.679
1TRS  H33  7  -3.746  -0.404  -1.594
1TRS  N8  -3.673  -0.705  -1.911
1TRS  H2   9  -3.625  -0.725  -1.996
1TRS  H3  10  -3.771  -0.707  -1.927
1TRS  H1  11  -3.649  -0.774  -1.842
1TRS  C2  12  -3.483  -0.573  -1.840
1TRS  O2  13  -3.428  -0.445  -1.806
1TRS  H23 14  -3.470  -0.412  -1.722
1EDO  OAB  1   0.307  -2.792   0.149
1EDO  HAE  2   0.390  -2.826   0.104
1EDO  CAA  3   0.239  -2.901   0.212
1EDO  CAC  4   0.111  -2.851   0.281
1EDO  OAD  5   0.144  -2.763   0.388
1EDO  HAF  6   0.060  -2.731   0.432
   8.13100   7.04165  13.54850   0.0   0.0  -4.06550   
0.0   0.0   0.0


How can I fixed these notes(note 1 and note 2)?

Thanks in advance
--
Ahmet YILDIRIM


-- 
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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[gmx-users] Re: gmx-users Digest, Vol 83, Issue 217

2011-03-31 Thread Raghuvir R S Pissurlenkar
  -1.679
   1TRS  H33  7  -3.746  -0.404  -1.594
   1TRS  N8  -3.673  -0.705  -1.911
   1TRS  H2   9  -3.625  -0.725  -1.996
   1TRS  H3  10  -3.771  -0.707  -1.927
   1TRS  H1  11  -3.649  -0.774  -1.842
   1TRS  C2  12  -3.483  -0.573  -1.840
   1TRS  O2  13  -3.428  -0.445  -1.806
   1TRS  H23 14  -3.470  -0.412  -1.722
   1EDO  OAB  1   0.307  -2.792   0.149
   1EDO  HAE  2   0.390  -2.826   0.104
   1EDO  CAA  3   0.239  -2.901   0.212
   1EDO  CAC  4   0.111  -2.851   0.281
   1EDO  OAD  5   0.144  -2.763   0.388
   1EDO  HAF  6   0.060  -2.731   0.432
  8.13100   7.04165  13.54850   0.0   0.0  -4.06550   0.0
0.0   0.0

How can I fixed these notes(note 1 and note 2)?

Thanks in advance
--
Ahmet YILDIRIM
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Re: [gmx-users] the total charge of system is not an integer

2011-03-31 Thread ahmet yıldırım
Dear Tsjerk,

I will ask you one thing but please do not get angry (I know you are not a
private tutor but I need your helps).

How do I apply on the files (EDO.itp and TRS.itp) that you said? (or can you
suggest a tutorial?)

Thanks

2011/3/31 Mark Abraham mark.abra...@anu.edu.au

  On 31/03/2011 5:18 PM, ahmet yıldırım wrote:

 Dear users,

 Before energy minimization step , I performed the preprosessing step using
 grompp .
 However, there are two note that :

 *NOTE 1 [file topol.top, line 52]:*
   System has non-zero total charge: -1.50e+01


 This is an integer. See
 http://en.wikipedia.org/wiki/Scientific_notation#E_notation and
 http://www.gromacs.org/Documentation/Floating_Point_Arithmetic

 *NOTE 2 [file topol.top]:*
   The largest charge group contains 11 atoms.
   Since atoms only see each other when the centers of geometry of the
 charge
   groups they belong to are within the cut-off distance, too large charge
   groups can lead to serious cut-off artifacts.
   For efficiency and accuracy, charge group should consist of a few atoms.
   For all-atom force fields use: CH3, CH2, CH, NH2, NH, OH, CO2, CO, etc.


 See Tsjerk's email.

 Mark


 *
 PS: *TRS and EDO are not aminoacid*

 TRS.itp:*
 ..
 [ moleculetype ]
 ; Name nrexcl
 TRS  3

 [ atoms ]
 ;   nr  type  resnr resid  atom  cgnr   charge mass
  1OA 1  TRS  O1 1   -0.119  15.9994
  2 H 1  TRS H13 10.032   1.0080
  3   CH2 1  TRS  C1 10.087  14.0270
  4  CCl4 1  TRS   C 20.055  12.0110
  5   CH2 1  TRS  C3 20.049  14.0270
  6OA 1  TRS  O3 2   -0.205  15.9994
  7 H 1  TRS H33 20.019   1.0080
  8NL 1  TRS   N 20.206  14.0067
  9 H 1  TRS  H2 20.004   1.0080
 10 H 1  TRS  H3 20.004   1.0080
 11 H 1  TRS  H1 20.004   1.0080
 12   CH2 1  TRS  C2 20.050  14.0270
 13OA 1  TRS  O2 2   -0.205  15.9994
 14 H 1  TRS H23 20.019   1.0080
 ...

 *EDO.itp*
 ...
 [ moleculetype ]
 ; Name nrexcl
 EDO  3

 [ atoms ]
 ;   nr  type  resnr resid  atom  cgnr   charge mass
  1OA 1  EDO OAB 1   -0.111  15.9994
  2 H 1  EDO HAE 10.031   1.0080
  3   CH2 1  EDO CAA 10.080  14.0270
  4   CH2 1  EDO CAC 10.080  14.0270
  5OA 1  EDO OAD 1   -0.111  15.9994
  6 H 1  EDO HAF 10.031   1.0080
 ...
 *
 topol.top:*
 ..
 ; Include water topology
 #include gromos43a1.ff/spc.itp
 #include TRS.itp
 #include EDO.itp
 ..
 [ molecules ]
 ; Compound#mols
 Protein_chain_A 1
 Protein_chain_B 1
 SOL   185
 SOL   143
 TRS1
 EDO1
 SOL 44125
 *
 Conf.gro:*
 MTA/SAH NUCLEOSIDASE; 5 NUCLEOSIDASE
  5354
 2GLN  N1   1.458  -1.158   0.739
 2GLN H12   1.520  -1.083   0.763
 ...
   485HOHHW1 5333   0.221  -3.864  -2.291
   485HOHHW2 5334   0.303  -3.946  -2.407
 1TRS  O1   1  -3.812  -0.471  -2.002
 1TRS  H13  2  -3.865  -0.443  -1.922
 1TRS  C1   3  -3.672  -0.469  -1.971
 1TRS  C4  -3.635  -0.571  -1.863
 1TRS  C3   5  -3.711  -0.547  -1.731
 1TRS  O3   6  -3.694  -0.414  -1.679
 1TRS  H33  7  -3.746  -0.404  -1.594
 1TRS  N8  -3.673  -0.705  -1.911
 1TRS  H2   9  -3.625  -0.725  -1.996
 1TRS  H3  10  -3.771  -0.707  -1.927
 1TRS  H1  11  -3.649  -0.774  -1.842
 1TRS  C2  12  -3.483  -0.573  -1.840
 1TRS  O2  13  -3.428  -0.445  -1.806
 1TRS  H23 14  -3.470  -0.412  -1.722
 1EDO  OAB  1   0.307  -2.792   0.149
 1EDO  HAE  2   0.390  -2.826   0.104
 1EDO  CAA  3   0.239  -2.901   0.212
 1EDO  CAC  4   0.111  -2.851   0.281
 1EDO  OAD  5   0.144  -2.763   0.388
 1EDO  HAF  6   0.060  -2.731   0.432
8.13100   7.04165  13.54850   0.0   0.0  -4.06550   0.0
 0.0   0.0

 How can I fixed these notes(note 1 and note 2)?

 Thanks in advance
 --
 Ahmet YILDIRIM



 --
 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




-- 
Ahmet YILDIRIM
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Re: [gmx-users] g_dipole: dipole moment autocorrelation function

2011-03-31 Thread Dommert Florian
On Wed, 2011-03-30 at 20:23 +0200, David van der Spoel wrote: 
 On 2011-03-30 20.16, Nilesh Dhumal wrote:
  Thanks.
  How can I take average.
 summing up and dividing by the number of sims.
 
  How much long I should run the simulation.
 until the average converges.
 
  Nilesh
 
  On Wed, March 30, 2011 12:59 pm, David van der Spoel wrote:
  On 2011-03-30 18.54, Nilesh Dhumal wrote:
 
  Hello,
 
 
  I am trying to calculate the dipole moment autocorrelation
  function for my system (ionic liquid). I am using gromacs 4.0.7 version.

Hello,

I think you will get into some trouble when you try to calculate an
autocorrelation function of property that is not continuous in time. In
an ionic liquid you have contributions of the molecular dipole and
contribution of the charged molecules to the dipole. The latter part is
unfortunately not continuous due to jumping of the molecules over the
PBCs. It depends what kind of property you want to calculate, but we
experienced that simulations in the range of 50-100ns are required to
reliably determine properties like the dielectric constant. The next
point is that you have to save your coordinates and velocities quite
often ( every 0.02ps we used)

Check corresponding literature for further advice.

Cheers,

Flo
 
 
  I run the simulation for 4 ns.  I run the following command to
  calculate the dipole moment autocorrelation function
 
  g_dipoles -f water.trr -s water.tpr -corr total -c
 
  The function is not geting converge to zero.
 
 
  I want to use this data for calculation of power spectra by fourier
  transfom of dipole moment autocorrelation function.
 
  Can you tell why its not geting converge to zero?
 
 
  You have to simulate at least a few 10s of ns for such slow liquids to
  converge. Alternatively you can average over many independent simulations
  (10s).
 
 
  Thanks
 
 
  Nilesh
 
 
 
 
 
 
  --
  David van der Spoel, Ph.D., Professor of Biology
  Dept. of Cell  Molec. Biol., Uppsala University.
  Box 596, 75124 Uppsala, Sweden. Phone: +46184714205.
  sp...@xray.bmc.uu.sehttp://folding.bmc.uu.se --
  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
 
 
 
 
 
 
 
 -- 
 David van der Spoel, Ph.D., Professor of Biology
 Dept. of Cell  Molec. Biol., Uppsala University.
 Box 596, 75124 Uppsala, Sweden. Phone:+46184714205.
 sp...@xray.bmc.uu.sehttp://folding.bmc.uu.se


-- 
Florian Dommert
Dipl. - Phys.

Institute for Computational Physics
University Stuttgart

Pfaffenwaldring 27
70569 Stuttgart

EMail: domm...@icp.uni-stuttgart.de
Homepage: http://www.icp.uni-stuttgart.de/~icp/Florian_Dommert

Tel.: +49 - (0)711 - 68563613
Fax.: +49 - (0)711 - 68563658


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Re: [gmx-users] the total charge of system is not an integer

2011-03-31 Thread Mark Abraham

On 31/03/2011 6:17 PM, ahmet yıldırım wrote:

Dear Tsjerk,

I will ask you one thing but please do not get angry (I know you are 
not a private tutor but I need your helps).


How do I apply on the files (EDO.itp and TRS.itp) that you said? (or 
can you suggest a tutorial?)


You'll need to become familiar with the file format, so that you know 
what all the columns of data mean, so you know where the charge groups 
are specified. Chapter 5 of the manual is your first port of call. If 
you have read that and still have questions about detail, please ask on 
the list :-)


Mark

2011/3/31 Mark Abraham mark.abra...@anu.edu.au 
mailto:mark.abra...@anu.edu.au


On 31/03/2011 5:18 PM, ahmet yıldırım wrote:

Dear users,

Before energy minimization step , I performed the preprosessing
step using grompp .
However, there are two note that :

*_NOTE 1 [file topol.top, line 52]:_*
  System has non-zero total charge: -1.50e+01


This is an integer. See
http://en.wikipedia.org/wiki/Scientific_notation#E_notation and
http://www.gromacs.org/Documentation/Floating_Point_Arithmetic


_*NOTE 2 [file topol.top]:*_
  The largest charge group contains 11 atoms.
  Since atoms only see each other when the centers of geometry of
the charge
  groups they belong to are within the cut-off distance, too
large charge
  groups can lead to serious cut-off artifacts.
  For efficiency and accuracy, charge group should consist of a
few atoms.
  For all-atom force fields use: CH3, CH2, CH, NH2, NH, OH, CO2,
CO, etc.


See Tsjerk's email.

Mark



*
PS: *TRS and EDO are not aminoacid*

_TRS.itp:_*
..
[ moleculetype ]
; Name nrexcl
TRS  3

[ atoms ]
;   nr  type  resnr resid  atom  cgnr   charge mass
 1OA 1  TRS  O1 1   -0.119  15.9994
 2 H 1  TRS H13 10.032   1.0080
 3   CH2 1  TRS  C1 10.087  14.0270
 4  CCl4 1  TRS   C 20.055  12.0110
 5   CH2 1  TRS  C3 20.049  14.0270
 6OA 1  TRS  O3 2   -0.205  15.9994
 7 H 1  TRS H33 20.019   1.0080
 8NL 1  TRS   N 20.206  14.0067
 9 H 1  TRS  H2 20.004   1.0080
10 H 1  TRS  H3 20.004   1.0080
11 H 1  TRS  H1 20.004   1.0080
12   CH2 1  TRS  C2 20.050  14.0270
13OA 1  TRS  O2 2   -0.205  15.9994
14 H 1  TRS H23 20.019   1.0080
...

_*EDO.itp*_
...
[ moleculetype ]
; Name nrexcl
EDO  3

[ atoms ]
;   nr  type  resnr resid  atom  cgnr   charge mass
 1OA 1  EDO OAB 1   -0.111  15.9994
 2 H 1  EDO HAE 10.031   1.0080
 3   CH2 1  EDO CAA 10.080  14.0270
 4   CH2 1  EDO CAC 10.080  14.0270
 5OA 1  EDO OAD 1   -0.111  15.9994
 6 H 1  EDO HAF 10.031   1.0080
...
_*
topol.top:*_
..
; Include water topology
#include gromos43a1.ff/spc.itp
#include TRS.itp
#include EDO.itp
..
[ molecules ]
; Compound#mols
Protein_chain_A 1
Protein_chain_B 1
SOL   185
SOL   143
TRS1
EDO1
SOL 44125
*_
Conf.gro:_*
MTA/SAH NUCLEOSIDASE; 5 NUCLEOSIDASE
 5354
2GLN  N1   1.458  -1.158   0.739
2GLN H12   1.520  -1.083   0.763
...
  485HOHHW1 5333   0.221  -3.864  -2.291
  485HOHHW2 5334   0.303  -3.946  -2.407
1TRS  O1   1  -3.812  -0.471  -2.002
1TRS  H13  2  -3.865  -0.443  -1.922
1TRS  C1   3  -3.672  -0.469  -1.971
1TRS  C4  -3.635  -0.571  -1.863
1TRS  C3   5  -3.711  -0.547  -1.731
1TRS  O3   6  -3.694  -0.414  -1.679
1TRS  H33  7  -3.746  -0.404  -1.594
1TRS  N8  -3.673  -0.705  -1.911
1TRS  H2   9  -3.625  -0.725  -1.996
1TRS  H3  10  -3.771  -0.707  -1.927
1TRS  H1  11  -3.649  -0.774  -1.842
1TRS  C2  12  -3.483  -0.573  -1.840
1TRS  O2  13  -3.428  -0.445  -1.806
1TRS  H23 14  -3.470  -0.412  -1.722
1EDO  OAB  1   0.307  -2.792   0.149
1EDO  HAE  2   0.390  -2.826   0.104
1EDO  CAA  3   0.239  -2.901   0.212
1EDO  CAC  4   0.111  -2.851   0.281
1EDO  OAD  5   0.144  -2.763   0.388
1EDO  HAF  6   0.060  -2.731   0.432
   8.13100   7.04165  13.54850   0.0   0.0  -4.06550  

[gmx-users] Help with Umbrella Sampling

2011-03-31 Thread Raghuvir R S Pissurlenkar
  -1.971
   1TRS  C4  -3.635  -0.571  -1.863
   1TRS  C3   5  -3.711  -0.547  -1.731
   1TRS  O3   6  -3.694  -0.414  -1.679
   1TRS  H33  7  -3.746  -0.404  -1.594
   1TRS  N8  -3.673  -0.705  -1.911
   1TRS  H2   9  -3.625  -0.725  -1.996
   1TRS  H3  10  -3.771  -0.707  -1.927
   1TRS  H1  11  -3.649  -0.774  -1.842
   1TRS  C2  12  -3.483  -0.573  -1.840
   1TRS  O2  13  -3.428  -0.445  -1.806
   1TRS  H23 14  -3.470  -0.412  -1.722
   1EDO  OAB  1   0.307  -2.792   0.149
   1EDO  HAE  2   0.390  -2.826   0.104
   1EDO  CAA  3   0.239  -2.901   0.212
   1EDO  CAC  4   0.111  -2.851   0.281
   1EDO  OAD  5   0.144  -2.763   0.388
   1EDO  HAF  6   0.060  -2.731   0.432
  8.13100   7.04165  13.54850   0.0   0.0  -4.06550   0.0
0.0   0.0

How can I fixed these notes(note 1 and note 2)?

Thanks in advance
--
Ahmet YILDIRIM
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Re: [gmx-users] g_dipole: dipole moment autocorrelation function

2011-03-31 Thread David van der Spoel

On 2011-03-31 09.25, Dommert Florian wrote:

On Wed, 2011-03-30 at 20:23 +0200, David van der Spoel wrote:

On 2011-03-30 20.16, Nilesh Dhumal wrote:

Thanks.
How can I take average.

summing up and dividing by the number of sims.


How much long I should run the simulation.

until the average converges.


Nilesh

On Wed, March 30, 2011 12:59 pm, David van der Spoel wrote:

On 2011-03-30 18.54, Nilesh Dhumal wrote:


Hello,


I am trying to calculate the dipole moment autocorrelation
function for my system (ionic liquid). I am using gromacs 4.0.7 version.


Hello,

I think you will get into some trouble when you try to calculate an
autocorrelation function of property that is not continuous in time. In
an ionic liquid you have contributions of the molecular dipole and
contribution of the charged molecules to the dipole. The latter part is
unfortunately not continuous due to jumping of the molecules over the
PBCs. It depends what kind of property you want to calculate, but we
experienced that simulations in the range of 50-100ns are required to
reliably determine properties like the dielectric constant. The next
point is that you have to save your coordinates and velocities quite
often ( every 0.02ps we used)

Check corresponding literature for further advice.


Thanks Florian, for pointing that out. I forgot about it in my previous 
mail. In order to compute the dielectric constant one could in principle 
apply constant electric fields at different strengths and then 
extrapolate to zero. Don't know whether that has been done.


Cheers,

Flo



I run the simulation for 4 ns.  I run the following command to
calculate the dipole moment autocorrelation function

g_dipoles -f water.trr -s water.tpr -corr total -c

The function is not geting converge to zero.


I want to use this data for calculation of power spectra by fourier
transfom of dipole moment autocorrelation function.

Can you tell why its not geting converge to zero?



You have to simulate at least a few 10s of ns for such slow liquids to
converge. Alternatively you can average over many independent simulations
(10s).



Thanks


Nilesh







--
David van der Spoel, Ph.D., Professor of Biology
Dept. of Cell   Molec. Biol., Uppsala University.
Box 596, 75124 Uppsala, Sweden. Phone:  +46184714205.
sp...@xray.bmc.uu.sehttp://folding.bmc.uu.se --
gmx-users mailing listgmx-users@gromacs.org
http://lists.gromacs.org/mailman/listinfo/gmx-users
Please search the archive at
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http://www.gromacs.org/Support/Mailing_Lists









--
David van der Spoel, Ph.D., Professor of Biology
Dept. of Cell  Molec. Biol., Uppsala University.
Box 596, 75124 Uppsala, Sweden. Phone:  +46184714205.
sp...@xray.bmc.uu.sehttp://folding.bmc.uu.se






--
David van der Spoel, Ph.D., Professor of Biology
Dept. of Cell  Molec. Biol., Uppsala University.
Box 596, 75124 Uppsala, Sweden. Phone:  +46184714205.
sp...@xray.bmc.uu.sehttp://folding.bmc.uu.se
--
gmx-users mailing listgmx-users@gromacs.org
http://lists.gromacs.org/mailman/listinfo/gmx-users
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Re: [gmx-users] the total charge of system is not an integer

2011-03-31 Thread Tsjerk Wassenaar
Hi Ahmet,

Why would I get angry? :) Sending a reply to the list will not usually
be taken as asking for private tutoring...

As Mark pointed out, you need to get familiar with the format of the
files. That's the first thing you should do if you get to the point of
needing to use non standard topologies. Read the manual, look at
existing files. As for the immediate question, under the [ atoms ]
section is a line indicating which column denotes what. You'd need to
modify the columns 'cgnr' (charge group number) and probably 'charge'.
For finding proper charge groups, in general you best draw your
molecule, with the charges added, and then see which atoms would
almost naturally group together.

TRS.itp:
..
[ moleculetype ]
; Name nrexcl
TRS  3

[ atoms ]
;   nr  type  resnr resid  atom  cgnr   charge mass
 1OA 1  TRS  O1 1   -0.119  15.9994
 2 H 1  TRS H13 10.032   1.0080
 3   CH2 1  TRS  C1 10.087  14.0270
 4  CCl4 1  TRS   C 20.055  12.0110
 5   CH2 1  TRS  C3 20.049  14.0270
 6OA 1  TRS  O3 2   -0.205  15.9994

Hope it helps,

Tsjerk



2011/3/31 ahmet yıldırım ahmedo...@gmail.com:
 Dear Tsjerk,

 I will ask you one thing but please do not get angry (I know you are not a
 private tutor but I need your helps).

 How do I apply on the files (EDO.itp and TRS.itp) that you said? (or can you
 suggest a tutorial?)

 Thanks

 2011/3/31 Mark Abraham mark.abra...@anu.edu.au

 On 31/03/2011 5:18 PM, ahmet yıldırım wrote:

 Dear users,

 Before energy minimization step , I performed the preprosessing step using
 grompp .
 However, there are two note that :

 NOTE 1 [file topol.top, line 52]:
   System has non-zero total charge: -1.50e+01

 This is an integer. See
 http://en.wikipedia.org/wiki/Scientific_notation#E_notation and
 http://www.gromacs.org/Documentation/Floating_Point_Arithmetic

 NOTE 2 [file topol.top]:
   The largest charge group contains 11 atoms.
   Since atoms only see each other when the centers of geometry of the
 charge
   groups they belong to are within the cut-off distance, too large charge
   groups can lead to serious cut-off artifacts.
   For efficiency and accuracy, charge group should consist of a few atoms.
   For all-atom force fields use: CH3, CH2, CH, NH2, NH, OH, CO2, CO, etc.

 See Tsjerk's email.

 Mark


 PS: TRS and EDO are not aminoacid

 TRS.itp:
 ..
 [ moleculetype ]
 ; Name nrexcl
 TRS  3

 [ atoms ]
 ;   nr  type  resnr resid  atom  cgnr   charge mass
  1    OA 1  TRS  O1 1   -0.119  15.9994
  2 H 1  TRS H13 1    0.032   1.0080
  3   CH2 1  TRS  C1 1    0.087  14.0270
  4  CCl4 1  TRS   C 2    0.055  12.0110
  5   CH2 1  TRS  C3 2    0.049  14.0270
  6    OA 1  TRS  O3 2   -0.205  15.9994
  7 H 1  TRS H33 2    0.019   1.0080
  8    NL 1  TRS   N 2    0.206  14.0067
  9 H 1  TRS  H2 2    0.004   1.0080
     10 H 1  TRS  H3 2    0.004   1.0080
     11 H 1  TRS  H1 2    0.004   1.0080
     12   CH2 1  TRS  C2 2    0.050  14.0270
     13    OA 1  TRS  O2 2   -0.205  15.9994
     14 H 1  TRS H23 2    0.019   1.0080
 ...

 EDO.itp
 ...
 [ moleculetype ]
 ; Name nrexcl
 EDO  3

 [ atoms ]
 ;   nr  type  resnr resid  atom  cgnr   charge mass
  1    OA 1  EDO OAB 1   -0.111  15.9994
  2 H 1  EDO HAE 1    0.031   1.0080
  3   CH2 1  EDO CAA 1    0.080  14.0270
  4   CH2 1  EDO CAC 1    0.080  14.0270
  5    OA 1  EDO OAD 1   -0.111  15.9994
  6 H 1  EDO HAF 1    0.031   1.0080
 ...

 topol.top:
 ..
 ; Include water topology
 #include gromos43a1.ff/spc.itp
 #include TRS.itp
 #include EDO.itp
 ..
 [ molecules ]
 ; Compound    #mols
 Protein_chain_A 1
 Protein_chain_B 1
 SOL   185
 SOL   143
 TRS    1
 EDO    1
 SOL 44125

 Conf.gro:
 MTA/SAH NUCLEOSIDASE; 5 NUCLEOSIDASE
  5354
     2GLN  N    1   1.458  -1.158   0.739
     2GLN H1    2   1.520  -1.083   0.763
 ...
   485HOH    HW1 5333   0.221  -3.864  -2.291
   485HOH    HW2 5334   0.303  -3.946  -2.407
     1TRS  O1   1  -3.812  -0.471  -2.002
     1TRS  H13  2  -3.865  -0.443  -1.922
     1TRS  C1   3  -3.672  -0.469  -1.971
     1TRS  C    4  -3.635  -0.571  -1.863
     1TRS  C3   5  -3.711  -0.547  -1.731
     1TRS  O3   6  -3.694  -0.414  -1.679
     1TRS  H33  7  -3.746  -0.404  -1.594
     1TRS  N    8  -3.673  -0.705  -1.911
     1TRS  H2   9  -3.625  -0.725  -1.996
     1TRS  H3  10  -3.771  -0.707  -1.927
     1TRS 

Re: [gmx-users] g_dipole: dipole moment autocorrelation function

2011-03-31 Thread Dommert Florian
On Thu, 2011-03-31 at 10:39 +0200, David van der Spoel wrote: 
 On 2011-03-31 09.25, Dommert Florian wrote:
  On Wed, 2011-03-30 at 20:23 +0200, David van der Spoel wrote:
  On 2011-03-30 20.16, Nilesh Dhumal wrote:
  Thanks.
  How can I take average.
  summing up and dividing by the number of sims.
 
  How much long I should run the simulation.
  until the average converges.
 
  Nilesh
 
  On Wed, March 30, 2011 12:59 pm, David van der Spoel wrote:
  On 2011-03-30 18.54, Nilesh Dhumal wrote:
 
  Hello,
 
 
  I am trying to calculate the dipole moment autocorrelation
  function for my system (ionic liquid). I am using gromacs 4.0.7 version.
 
  Hello,
 
  I think you will get into some trouble when you try to calculate an
  autocorrelation function of property that is not continuous in time. In
  an ionic liquid you have contributions of the molecular dipole and
  contribution of the charged molecules to the dipole. The latter part is
  unfortunately not continuous due to jumping of the molecules over the
  PBCs. It depends what kind of property you want to calculate, but we
  experienced that simulations in the range of 50-100ns are required to
  reliably determine properties like the dielectric constant. The next
  point is that you have to save your coordinates and velocities quite
  often ( every 0.02ps we used)
 
  Check corresponding literature for further advice.
 
 Thanks Florian, for pointing that out. I forgot about it in my previous 
 mail. In order to compute the dielectric constant one could in principle 
 apply constant electric fields at different strengths and then 
 extrapolate to zero. Don't know whether that has been done.
 

In the ionic liquids commmunity dielectric spectra of ILs are usually
calulated from equilibrium MD without application of an E-field. The
generalized dielectric constant is calculated and a Fourier Laplace
transformation finally allows to determine the full dielectric spectrum.
Schröder et. al from the University of Vienna have published some
articles about this topic. 

Cheers,
Flo

  Cheers,
 
  Flo
 
 
  I run the simulation for 4 ns.  I run the following command to
  calculate the dipole moment autocorrelation function
 
  g_dipoles -f water.trr -s water.tpr -corr total -c
 
  The function is not geting converge to zero.
 
 
  I want to use this data for calculation of power spectra by fourier
  transfom of dipole moment autocorrelation function.
 
  Can you tell why its not geting converge to zero?
 
 
  You have to simulate at least a few 10s of ns for such slow liquids to
  converge. Alternatively you can average over many independent simulations
  (10s).
 
 
  Thanks
 
 
  Nilesh
 
 
 
 
 
 
  --
  David van der Spoel, Ph.D., Professor of Biology
  Dept. of Cell   Molec. Biol., Uppsala University.
  Box 596, 75124 Uppsala, Sweden. Phone:   +46184714205.
  sp...@xray.bmc.uu.sehttp://folding.bmc.uu.se --
  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
 
 
 
 
 
 
 
  --
  David van der Spoel, Ph.D., Professor of Biology
  Dept. of Cell  Molec. Biol., Uppsala University.
  Box 596, 75124 Uppsala, Sweden. Phone: +46184714205.
  sp...@xray.bmc.uu.sehttp://folding.bmc.uu.se
 
 
 
 
 -- 
 David van der Spoel, Ph.D., Professor of Biology
 Dept. of Cell  Molec. Biol., Uppsala University.
 Box 596, 75124 Uppsala, Sweden. Phone:+46184714205.
 sp...@xray.bmc.uu.sehttp://folding.bmc.uu.se


-- 
Florian Dommert
Dipl. - Phys.

Institute for Computational Physics
University Stuttgart

Pfaffenwaldring 27
70569 Stuttgart

EMail: domm...@icp.uni-stuttgart.de
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[gmx-users] Umbrella sampling

2011-03-31 Thread Gavin Melaugh
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?
2 - Does the distribution at each window have to centered around the
desired r0? (If not does this affect the free energy?)
3- If you over sample one particular window, will it affect the curve?

Many thanks

GAvin
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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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[gmx-users] manually creating a topology file

2011-03-31 Thread Nishith Saurav Topno
Dear all,
I intend to run a simulation for a membrane protein. As per a tutorial, i
require a lipid bilayer and some (.itp) files for editing manually a toplogy
file for the lipid bilayer. Question is how do I choose the appropriate
lipid bilayer and its subsequent (.itp) file? Also, what are the required
necessary things to be edited. I intend to use teh OPLS-AA force field to
represent my protein

-- 
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Re: [gmx-users] Umbrella sampling

2011-03-31 Thread Gavin Melaugh
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] Help with Umbrella Sampling

2011-03-31 Thread Justin A. Lemkul



Raghuvir R S Pissurlenkar wrote:

Dear Justin

I removed the constrain on the DPPC molecules, however I find still 
LINCS errors are prominent

Any alterative can I try



Reduce the pull_rate.  If you pull too fast, your system cannot adapt properly 
to the collisions that are induced by the artificial force.


-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] manually creating a topology file

2011-03-31 Thread Mark Abraham
On 31/03/11, Nishith Saurav Topno  nto...@bicpu.edu.in wrote:
 Dear all,
 I intend to run a simulation for a membrane protein. As per a tutorial, i 
 require a lipid bilayer and some (.itp) files for editing manually a toplogy 
 file for the lipid bilayer. Question is how do I choose the appropriate lipid 
 bilayer and its subsequent (.itp) file? 
 

That depends on what you are modelling and what you are hoping to observe. 
There's no substitute for knowledge and learning about the biochemical system 
of interest, and how other people have approached similar problems, and what 
they learned.


 Also, what are the required necessary things to be edited. I intend to use 
 teh OPLS-AA force field to represent my protein
 

That sounds like you are pre-supposing the use of a particular tool. A better 
approach is to look at published studies similar to the one you propose, to 
learn from their apparent successes and failures, and to choose tools and 
methods accordingly.

Having chosen tools and methods, it is certain that you will need to spend time 
reading tutorials, documentation, published articles and asking questions of 
experts. Indeed, if you can't do this, then you should probably revisit those 
chocies of tools and methods, or even the proposed study.

Mark
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[gmx-users] gromacs/CPMD. Is LAM mandatory?

2011-03-31 Thread Elena Formoso
Dear all,
I am trying to do a QM/MM calculation with gromacs/CPMD. When I try to use a
parallel version of mdrun and CPMD I get a segmentation fault.
I have seen in the examples that LAM is used in runcpmd. It is mandatory for
parallel runs?

I do not have this problem when I run just CPMD in parallel

Regards


***
Elena
ETH Zürich and
Università della Svizzera Italiana, USI
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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] gromacs/CPMD. Is LAM mandatory?

2011-03-31 Thread Mark Abraham
On 31/03/11, Elena Formoso  elena.form...@phys.chem.ethz.ch wrote:
 Dear all,
 I am trying to do a QM/MM calculation with gromacs/CPMD. When I 
 try to use a parallel version of mdrun and CPMD I get a segmentation fault. 
 I have seen in the examples that LAM is used in runcpmd. It is mandatory for 
 parallel runs?
 

LAM is a deprecated library implementing the MPI standard. Whether it is 
necessary, or another MPI implementation is possible (or even preferable) is a 
question that should be answered in the documentation of the GROMACS-CPMD port. 
Is it?

Mark
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Re: [gmx-users] Umbrella sampling

2011-03-31 Thread Gavin Melaugh
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).

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/CPMD. Is LAM mandatory?

2011-03-31 Thread Christian Seifert
Hi Elena,

if you use GMX/CPMD in parallel, you can use any mpi implementation, but
you should start GMX on a single core and CPMD in parallel (via
runcpmd). You can not run both in parallel.

Greets,
Christian

On Thu, 2011-03-31 at 13:05 +0200, Elena Formoso wrote:
 Dear all,
 I am trying to do a QM/MM calculation with gromacs/CPMD. When I try to
 use a parallel version of mdrun and CPMD I get a segmentation fault. 
 I have seen in the examples that LAM is used in runcpmd. It is
 mandatory for parallel runs?
 
 I do not have this problem when I run just CPMD in parallel
 
 Regards
 
 
 ***
 Elena 
 ETH Zürich and
 Università della Svizzera Italiana, USI
 
 -- 
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-- 
M.Sc. Christian Seifert
Department of Biophysics
University of Bochum
ND 04/67
44780 Bochum
Germany
Tel: +49 (0)234 32 28363
Fax: +49 (0)234 32 14626
E-Mail: cseif...@bph.rub.de
Web: http://www.bph.rub.de

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Re: [gmx-users] gromacs/CPMD. Is LAM mandatory?

2011-03-31 Thread Elena Formoso
Thanks Christian
That is why it was not working. It is not possible to run both in parallel

Cheers

Elena



On Thu, Mar 31, 2011 at 1:14 PM, Christian Seifert 
cseif...@bph.ruhr-uni-bochum.de wrote:

 Hi Elena,

 if you use GMX/CPMD in parallel, you can use any mpi implementation, but
 you should start GMX on a single core and CPMD in parallel (via
 runcpmd). You can not run both in parallel.

 Greets,
 Christian

 On Thu, 2011-03-31 at 13:05 +0200, Elena Formoso wrote:
  Dear all,
  I am trying to do a QM/MM calculation with gromacs/CPMD. When I try to
  use a parallel version of mdrun and CPMD I get a segmentation fault.
  I have seen in the examples that LAM is used in runcpmd. It is
  mandatory for parallel runs?
 
  I do not have this problem when I run just CPMD in parallel
 
  Regards
 
 
  ***
  Elena
  ETH Zürich and
  Università della Svizzera Italiana, USI
 
  --
  gmx-users mailing listgmx-users@gromacs.org
  http://lists.gromacs.org/mailman/listinfo/gmx-users
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 http://www.gromacs.org/Support/Mailing_Lists/Search before posting!
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  www interface or send it to gmx-users-requ...@gromacs.org.
  Can't post? Read http://www.gromacs.org/Support/Mailing_Lists

 --
 M.Sc. Christian Seifert
 Department of Biophysics
 University of Bochum
 ND 04/67
 44780 Bochum
 Germany
 Tel: +49 (0)234 32 28363
 Fax: +49 (0)234 32 14626
 E-Mail: cseif...@bph.rub.de
 Web: http://www.bph.rub.de

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Re: [gmx-users] Umbrella sampling

2011-03-31 Thread Justin A. Lemkul



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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--


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


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[gmx-users] CUT-OFFs for GROMOS96 43a1...Reg

2011-03-31 Thread Kishore
Dear All,
I am running MD simulations of an Alcohol Dehydrogenase ( a tetramer) with
the bound NADPH in explicit solvent. I am employing GROMOS96 43a1 force
field for the simulations. I need a clarification on the CUT-OFFs applicable
for this force field. I have seen many people using *rvdw = 1.4*
and*rcoulomb = 1.0 ( short range vander-waals and elctrostatics
cut-offs)
*in all the .mdp files. In the tutorial I am following (Justin Lemkul's -
protein ligand complex)) he used *rvdw = 1.0* and *rcoulomb = 1.0* in case
of energy minimisation and* rvdw = 1.4* and *rcoulomb = 0.9* in case of
NVT/NPT equilibration and production MD run. So, someone please clarify me
what the widely accepted values for these two would be. If at all I should
use* rvdw = 1.4*, then should -d flag in editconf be atleast 1.4 or can it
be less than that in the case of PBC conditions enabled.
-- 
KRISHNA KISHORE@IIT-MADRAS
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Re: [gmx-users] Umbrella sampling

2011-03-31 Thread Gavin Melaugh
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] CUT-OFFs for GROMOS96 43a1...Reg

2011-03-31 Thread Justin A. Lemkul



Kishore wrote:

Dear All,
I am running MD simulations of an Alcohol Dehydrogenase ( a tetramer) 
with the bound NADPH in explicit solvent. I am employing GROMOS96 43a1 
force field for the simulations. I need a clarification on the CUT-OFFs 
applicable for this force field. I have seen many people using *rvdw = 
1.4* and* rcoulomb = 1.0 ( short range vander-waals and elctrostatics 
cut-offs) *in all the .mdp files. In the tutorial I am following (Justin 
Lemkul's - protein ligand complex)) he used *rvdw = 1.0* and *rcoulomb = 
1.0* in case of energy minimisation and* rvdw = 1.4* and *rcoulomb = 
0.9* in case of NVT/NPT equilibration and production MD run. So, someone 
please clarify me what the widely accepted values for these two would 
be. If at all I should use* rvdw = 1.4*, then should -d flag in editconf 


The latter.  EM is relatively insensitive to the cutoffs in my experience, so 
1.0 is fine there.  For the real MD, use the proper settings given in the 
production MD .mdp file.


be atleast 1.4 or can it be less than that in the case of PBC conditions 
enabled.


You simply have to ensure that your system's components never see one another. 
 In principle, you'd be safe setting -d 1.4 and have a maximum of 2.8 nm 
between periodic images.  That can result in a lot of wasted time doing 
calculations on distant water molecules when the box size gets extremely large. 
 If the box size/shape will not change much (as is the case for most 
well-equilibrated protein/water systems), you can get away with a shorter value 
of -d, maybe 1.0 or so.  Don't set it as low as 0.7 (such that the periodic 
distance is exactly 1.4 nm, equal to the cutoff), because then any small 
fluctuation can cause you problems.


-Justin


--
KRISHNA KISHORE@IIT-MADRAS



--


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] 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] g_dipole: dipole moment autocorrelation function

2011-03-31 Thread Nilesh Dhumal
Thanks Flo for detail reply.

Is it possible to put PBC off during calculation of dipole moment
autocorrelation function.

I will run the simulation for 50ns ans try to save trajectroy of 0.02ps.

Thanks

NIlesh

Nilesh

On Thu, March 31, 2011 5:38 am, Dommert Florian wrote:
 On Thu, 2011-03-31 at 10:39 +0200, David van der Spoel wrote:

 On 2011-03-31 09.25, Dommert Florian wrote:

 On Wed, 2011-03-30 at 20:23 +0200, David van der Spoel wrote:

 On 2011-03-30 20.16, Nilesh Dhumal wrote:

 Thanks.
 How can I take average.

 summing up and dividing by the number of sims.

 How much long I should run the simulation.

 until the average converges.

 Nilesh


 On Wed, March 30, 2011 12:59 pm, David van der Spoel wrote:

 On 2011-03-30 18.54, Nilesh Dhumal wrote:


 Hello,



 I am trying to calculate the dipole moment autocorrelation
 function for my system (ionic liquid). I am using gromacs
 4.0.7 version.


 Hello,


 I think you will get into some trouble when you try to calculate an
 autocorrelation function of property that is not continuous in time.
 In
 an ionic liquid you have contributions of the molecular dipole and
 contribution of the charged molecules to the dipole. The latter part
 is unfortunately not continuous due to jumping of the molecules over
 the PBCs. It depends what kind of property you want to calculate, but
 we experienced that simulations in the range of 50-100ns are required
 to reliably determine properties like the dielectric constant. The
 next point is that you have to save your coordinates and velocities
 quite often ( every 0.02ps we used)

 Check corresponding literature for further advice.


 Thanks Florian, for pointing that out. I forgot about it in my previous
  mail. In order to compute the dielectric constant one could in
 principle apply constant electric fields at different strengths and then
  extrapolate to zero. Don't know whether that has been done.


 In the ionic liquids commmunity dielectric spectra of ILs are usually
 calulated from equilibrium MD without application of an E-field. The
 generalized dielectric constant is calculated and a Fourier Laplace
 transformation finally allows to determine the full dielectric spectrum.
 Schröder et. al from the University of Vienna have published some
 articles about this topic.

 Cheers,
 Flo


 Cheers,


 Flo



 I run the simulation for 4 ns.  I run the following command
 to calculate the dipole moment autocorrelation function

 g_dipoles -f water.trr -s water.tpr -corr total -c

 The function is not geting converge to zero.



 I want to use this data for calculation of power spectra by
 fourier transfom of dipole moment autocorrelation function.

 Can you tell why its not geting converge to zero?



 You have to simulate at least a few 10s of ns for such slow
 liquids to converge. Alternatively you can average over many
 independent simulations (10s).



 Thanks



 Nilesh







 --
 David van der Spoel, Ph.D., Professor of Biology
 Dept. of Cell   Molec. Biol., Uppsala University.
 Box 596, 75124 Uppsala, Sweden. Phone:   +46184714205.
 sp...@xray.bmc.uu.sehttp://folding.bmc.uu.se -- gmx-users
 mailing listgmx-users@gromacs.org
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 --
 David van der Spoel, Ph.D., Professor of Biology
 Dept. of Cell  Molec. Biol., Uppsala University.
 Box 596, 75124 Uppsala, Sweden. Phone: +46184714205.
 sp...@xray.bmc.uu.sehttp://folding.bmc.uu.se




 --
 David van der Spoel, Ph.D., Professor of Biology
 Dept. of Cell  Molec. Biol., Uppsala University.
 Box 596, 75124 Uppsala, Sweden. Phone:   +46184714205.
 sp...@xray.bmc.uu.sehttp://folding.bmc.uu.se


 --
 Florian Dommert
 Dipl. - Phys.


 Institute for Computational Physics
 University Stuttgart


 Pfaffenwaldring 27
 70569 Stuttgart


 EMail: domm...@icp.uni-stuttgart.de
 Homepage: http://www.icp.uni-stuttgart.de/~icp/Florian_Dommert


 Tel.: +49 - (0)711 - 68563613
 Fax.: +49 - (0)711 - 68563658
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Re: [gmx-users] g_dipole: dipole moment autocorrelation function

2011-03-31 Thread Dommert Florian
On Thu, 2011-03-31 at 08:53 -0400, Nilesh Dhumal wrote: 
 Thanks Flo for detail reply.
 
 Is it possible to put PBC off during calculation of dipole moment
 autocorrelation function.

No, thats the problem, because the volume of the system will increase
and dipole density will decrease, this not what you want. However I've
written the tool g_current, that allows to calculate the dielectric
constant and terms of which it is composed. Read our paper (DOI:
10.1063/1.3030948), which describes the procedure and look at the help,
what the programm can do.

Cheers,

Flo

 
 I will run the simulation for 50ns ans try to save trajectroy of 0.02ps.
 
 Thanks
 
 NIlesh
 
 Nilesh
 
 On Thu, March 31, 2011 5:38 am, Dommert Florian wrote:
  On Thu, 2011-03-31 at 10:39 +0200, David van der Spoel wrote:
 
  On 2011-03-31 09.25, Dommert Florian wrote:
 
  On Wed, 2011-03-30 at 20:23 +0200, David van der Spoel wrote:
 
  On 2011-03-30 20.16, Nilesh Dhumal wrote:
 
  Thanks.
  How can I take average.
 
  summing up and dividing by the number of sims.
 
  How much long I should run the simulation.
 
  until the average converges.
 
  Nilesh
 
 
  On Wed, March 30, 2011 12:59 pm, David van der Spoel wrote:
 
  On 2011-03-30 18.54, Nilesh Dhumal wrote:
 
 
  Hello,
 
 
 
  I am trying to calculate the dipole moment autocorrelation
  function for my system (ionic liquid). I am using gromacs
  4.0.7 version.
 
 
  Hello,
 
 
  I think you will get into some trouble when you try to calculate an
  autocorrelation function of property that is not continuous in time.
  In
  an ionic liquid you have contributions of the molecular dipole and
  contribution of the charged molecules to the dipole. The latter part
  is unfortunately not continuous due to jumping of the molecules over
  the PBCs. It depends what kind of property you want to calculate, but
  we experienced that simulations in the range of 50-100ns are required
  to reliably determine properties like the dielectric constant. The
  next point is that you have to save your coordinates and velocities
  quite often ( every 0.02ps we used)
 
  Check corresponding literature for further advice.
 
 
  Thanks Florian, for pointing that out. I forgot about it in my previous
   mail. In order to compute the dielectric constant one could in
  principle apply constant electric fields at different strengths and then
   extrapolate to zero. Don't know whether that has been done.
 
 
  In the ionic liquids commmunity dielectric spectra of ILs are usually
  calulated from equilibrium MD without application of an E-field. The
  generalized dielectric constant is calculated and a Fourier Laplace
  transformation finally allows to determine the full dielectric spectrum.
  Schröder et. al from the University of Vienna have published some
  articles about this topic.
 
  Cheers,
  Flo
 
 
  Cheers,
 
 
  Flo
 
 
 
  I run the simulation for 4 ns.  I run the following command
  to calculate the dipole moment autocorrelation function
 
  g_dipoles -f water.trr -s water.tpr -corr total -c
 
  The function is not geting converge to zero.
 
 
 
  I want to use this data for calculation of power spectra by
  fourier transfom of dipole moment autocorrelation function.
 
  Can you tell why its not geting converge to zero?
 
 
 
  You have to simulate at least a few 10s of ns for such slow
  liquids to converge. Alternatively you can average over many
  independent simulations (10s).
 
 
 
  Thanks
 
 
 
  Nilesh
 
 
 
 
 
 
 
  --
  David van der Spoel, Ph.D., Professor of Biology
  Dept. of Cell   Molec. Biol., Uppsala University.
  Box 596, 75124 Uppsala, Sweden. Phone: +46184714205.
  sp...@xray.bmc.uu.sehttp://folding.bmc.uu.se -- 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
 
 
 
 
 
 
 
 
  --
  David van der Spoel, Ph.D., Professor of Biology
  Dept. of Cell  Molec. Biol., Uppsala University.
  Box 596, 75124 Uppsala, Sweden. Phone:   +46184714205.
  sp...@xray.bmc.uu.sehttp://folding.bmc.uu.se
 
 
 
 
  --
  David van der Spoel, Ph.D., Professor of Biology
  Dept. of Cell  Molec. Biol., Uppsala University.
  Box 596, 75124 Uppsala, Sweden. Phone: +46184714205.
  sp...@xray.bmc.uu.sehttp://folding.bmc.uu.se
 
 
  --
  Florian Dommert
  Dipl. - Phys.
 
 
  Institute for Computational Physics
  University Stuttgart
 
 
  Pfaffenwaldring 27
  70569 Stuttgart
 
 
  EMail: domm...@icp.uni-stuttgart.de
  Homepage: http://www.icp.uni-stuttgart.de/~icp/Florian_Dommert
 
 
  Tel.: +49 - (0)711 - 68563613
  Fax.: +49 - (0)711 - 68563658
  --
  gmx-users mailing listgmx-users@gromacs.org
  http://lists.gromacs.org/mailman/listinfo/gmx-users
 

[gmx-users] converting ILDN parameters to RB

2011-03-31 Thread Alan Wilter Sousa da Silva
Hi there,

Since ILDN dihedrals has some parameters with up to periodicity 6, I was
wondering if it's possible to convert it in RB with 6 coefficients. If so,
what would be the formula? For example, for converting the usual Amber99SB
to RB I have:

if phase in [0, 180]:

if kPhi  0: V[period] = 2 * kPhi * cal

if period == 1:

C[0] += 0.5 * V[period]

if phase == 0:

C[1] -= 0.5 * V[period]

else:

C[1] += 0.5 * V[period]

elif period == 2:

if phase == 180:

C[0] += V[period]

C[2] -= V[period]

else:

C[2] += V[period]

elif period == 3:

C[0] += 0.5 * V[period]

if phase == 0:

C[1] += 1.5 * V[period]

C[3] -= 2 * V[period]

else:

C[1] -= 1.5 * V[period]

C[3] += 2 * V[period]

elif period == 4:

if phase == 180:

C[2] += 4 * V[period]

C[4] -= 4 * V[period]

else:

C[0] += V[period]

C[2] -= 4 * V[period]

C[4] += 4 * V[period]

So, as you can see, I can handle up to 4 periods (C[5] is always 0, but not
with ILDN and I need to add C[6] rules as well).

Any ideas? Many thanks in advance,

Alan
-- 
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Bioinformatician, UniProt - PANDA, EMBL-EBI
CB10 1SD, Hinxton, Cambridge, UK
+44 1223 49 4588
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[gmx-users] couple-moltype for two molecules

2011-03-31 Thread Luca Bellucci
Dear all,
I tryed to use couple-moltype=Protein Ligand directive   
to annihilate both protein and ligand molecules using free energy method.
I realized that couple-moltype key works for only one molecule type.
Is it right? 

To perform the same annihilation I used
couple-moltype=Protein to annihilate the protein and dual topology
 formalism (definied in itp file) to annihilate the ligand.
Are these commands able to work together?
Thanks
Luca
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[gmx-users] couple-moltype for two molecules

2011-03-31 Thread Luca
Dear all,
I tryed to use couple-moltype=Protein Ligand directive   
to annihilate both protein and ligand molecules using free energy method.
I realized that couple-moltype key works for only one molecule type.
Is it right? 

To perform the same annihilation I used
couple-moltype=Protein to annihilate the protein and dual topology
 formalism (definied in itp file) to annihilate the ligand.
Are these commands able to work together?
Thanks
Luca
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[gmx-users] couple-moltype for two molecules

2011-03-31 Thread Luca Bellucci
Dear all,
I tryed to use couple-moltype=Protein Ligand directive   
to annihilate both protein and ligand molecules using free energy method.
I realized that couple-moltype key works for only one molecule type.
Is it right? 

To perform the same annihilation I used
couple-moltype=Protein to annihilate the protein and dual topology
 formalism (definied in itp file) to annihilate the ligand.
Are these commands able to work together?
Thanks
Luca
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Re: [gmx-users] converting ILDN parameters to RB

2011-03-31 Thread Alan Wilter Sousa da Silva
I know it's supported.

I was just investigating the possibility since I build acpype to create
topologies for gromacs, but also it converts from amber to gromacs (like
amb2gmx.pl), and so I was wondering about RB with 6 coefficients since
multiple proper dihedrals is only supported for gmx 4.5 and above.

But I don't want to fuss about it. If to forget about GMX 4.0.x and below is
the way, so it will be.

Thanks,

Alan

On 31 March 2011 16:08, David van der Spoel sp...@xray.bmc.uu.se wrote:

 On 2011-03-31 15.27, Alan Wilter Sousa da Silva wrote:

 Hi there,

 Since ILDN dihedrals has some parameters with up to periodicity 6, I was
 wondering if it's possible to convert it in RB with 6 coefficients. If
 so, what would be the formula? For example, for converting the usual
 Amber99SB to RB I have:

 ILDN is already supported in the latest gromacs releases, by simply using
 multiple proper dihedrals. Why would you want to change it?



 if phase in [0, 180]:

 if kPhi  0: V[period] = 2 * kPhi * cal

 if period == 1:

 C[0] += 0.5 * V[period]

 if phase == 0:

 C[1] -= 0.5 * V[period]

 else:

 C[1] += 0.5 * V[period]

 elif period == 2:

 if phase == 180:

 C[0] += V[period]

 C[2] -= V[period]

 else:

 C[2] += V[period]

 elif period == 3:

 C[0] += 0.5 * V[period]

 if phase == 0:

 C[1] += 1.5 * V[period]

 C[3] -= 2 * V[period]

 else:

 C[1] -= 1.5 * V[period]

 C[3] += 2 * V[period]

 elif period == 4:

 if phase == 180:

 C[2] += 4 * V[period]

 C[4] -= 4 * V[period]

 else:

 C[0] += V[period]

 C[2] -= 4 * V[period]

 C[4] += 4 * V[period]


 So, as you can see, I can handle up to 4 periods (C[5] is always 0, but
 not with ILDN and I need to add C[6] rules as well).

 Any ideas? Many thanks in advance,

 Alan
 --
 Alan Wilter SOUSA da SILVA, DSc
 Bioinformatician, UniProt - PANDA, EMBL-EBI
 CB10 1SD, Hinxton, Cambridge, UK
 +44 1223 49 4588



 --
 David van der Spoel, Ph.D., Professor of Biology
 Dept. of Cell  Molec. Biol., Uppsala University.
 Box 596, 75124 Uppsala, Sweden. Phone:  +46184714205.
 sp...@xray.bmc.uu.sehttp://folding.bmc.uu.se
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Bioinformatician, UniProt - PANDA, EMBL-EBI
CB10 1SD, Hinxton, Cambridge, UK
+44 1223 49 4588
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Re: [gmx-users] converting ILDN parameters to RB

2011-03-31 Thread David van der Spoel

On 2011-03-31 17.19, Alan Wilter Sousa da Silva wrote:

I know it's supported.

I was just investigating the possibility since I build acpype to create
topologies for gromacs, but also it converts from amber to gromacs (like
amb2gmx.pl http://amb2gmx.pl), and so I was wondering about RB with 6
coefficients since multiple proper dihedrals is only supported for gmx
4.5 and above.
Unfortunately RB only goes to 5 and it would be a pain to support more 
since the tpr format would have to be updated. The current solution with 
the type 9 dihedrals is a royal pain in the neck too. I've actually 
written a script that converts the present rtp files to contain *all* 
bonded interactions explicitly (with parameters), and it replaces the 9 
type dihedrals with multiple 1 type dihedrals (lots of them with all 
zeros, LOL).


But I don't want to fuss about it. If to forget about GMX 4.0.x and
below is the way, so it will be.

Thanks,

Alan

On 31 March 2011 16:08, David van der Spoel sp...@xray.bmc.uu.se
mailto:sp...@xray.bmc.uu.se wrote:

On 2011-03-31 15.27, Alan Wilter Sousa da Silva wrote:

Hi there,

Since ILDN dihedrals has some parameters with up to periodicity
6, I was
wondering if it's possible to convert it in RB with 6
coefficients. If
so, what would be the formula? For example, for converting the usual
Amber99SB to RB I have:

ILDN is already supported in the latest gromacs releases, by simply
using multiple proper dihedrals. Why would you want to change it?



if phase in [0, 180]:

if kPhi  0: V[period] = 2 * kPhi * cal

if period == 1:

 C[0] += 0.5 * V[period]

if phase == 0:

 C[1] -= 0.5 * V[period]

else:

 C[1] += 0.5 * V[period]

elif period == 2:

if phase == 180:

 C[0] += V[period]

 C[2] -= V[period]

else:

 C[2] += V[period]

elif period == 3:

 C[0] += 0.5 * V[period]

if phase == 0:

 C[1] += 1.5 * V[period]

 C[3] -= 2 * V[period]

else:

 C[1] -= 1.5 * V[period]

 C[3] += 2 * V[period]

elif period == 4:

if phase == 180:

 C[2] += 4 * V[period]

 C[4] -= 4 * V[period]

else:

 C[0] += V[period]

 C[2] -= 4 * V[period]

 C[4] += 4 * V[period]


So, as you can see, I can handle up to 4 periods (C[5] is always
0, but
not with ILDN and I need to add C[6] rules as well).

Any ideas? Many thanks in advance,

Alan
--
Alan Wilter SOUSA da SILVA, DSc
Bioinformatician, UniProt - PANDA, EMBL-EBI
CB10 1SD, Hinxton, Cambridge, UK
+44 1223 49 4588



--
David van der Spoel, Ph.D., Professor of Biology
Dept. of Cell  Molec. Biol., Uppsala University.
Box 596, 75124 Uppsala, Sweden. Phone:  +46184714205.
sp...@xray.bmc.uu.se mailto:sp...@xray.bmc.uu.se
http://folding.bmc.uu.se
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--
Alan Wilter SOUSA da SILVA, DSc
Bioinformatician, UniProt - PANDA, EMBL-EBI
CB10 1SD, Hinxton, Cambridge, UK
+44 1223 49 4588




--
David van der Spoel, Ph.D., Professor of Biology
Dept. of Cell  Molec. Biol., Uppsala University.
Box 596, 75124 Uppsala, Sweden. Phone:  +46184714205.
sp...@xray.bmc.uu.sehttp://folding.bmc.uu.se
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[gmx-users] Umbrella sampling

2011-03-31 Thread chris . neale
can you show us your mdp and the pmf and the histograms for the data  
that you put into wham? It's a lot easier to diagnose with the real  
data.


In the general case where umbrellas are spaced equally along your  
reaction coordinate, sampling overlap between umbrellas will always  
decrease anywhere the PMF is concave down, such as your barrier  
region. I would suggest adding windows at every 0.005 nm spanning the  
region that you consider to have a sampling problem (e.g. 0.76 to 0.83  
?) and use a much stronger force constant here (e.g. 2-3 times as  
strong as you used for umbrellas with 0.02 nm spacing). You have  
identified a problem, so my suggestion is to not bother fiddling with  
adding one extra replica but sample that region to death with strong  
force constants. I presume that this will not impact your overall  
efficiency too much if the reaction coordinate is long overall.


Finally, you will need to evaluate the convergence of your PMF overall  
and perhaps of this region in particular, especially if you want to  
know the dG to cross it or between two low energy states on either  
side of it.


Chris.

-- original message --


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).

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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[gmx-users] Umbrella Sampling

2011-03-31 Thread Gavin Melaugh
Hi Chris many thanks again for the advise. I have, or at least I thought
have sampled my barrier region to death, but as I say some histograms
may not be centred around r0. I will proceed with what you suggest.
Please find attached a picture of the histograms, the corresponding
profile, and a sample mdp file that I use.



groprofile.agr.gz
Description: GNU Zip compressed data


hist.agr.gz
Description: GNU Zip compressed data
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Re: [gmx-users] Umbrella sampling

2011-03-31 Thread Gavin Melaugh
Here is also the sample .mdp file

chris.ne...@utoronto.ca wrote:
 can you show us your mdp and the pmf and the histograms for the data
 that you put into wham? It's a lot easier to diagnose with the real data.

 In the general case where umbrellas are spaced equally along your
 reaction coordinate, sampling overlap between umbrellas will always
 decrease anywhere the PMF is concave down, such as your barrier
 region. I would suggest adding windows at every 0.005 nm spanning the
 region that you consider to have a sampling problem (e.g. 0.76 to 0.83
 ?) and use a much stronger force constant here (e.g. 2-3 times as
 strong as you used for umbrellas with 0.02 nm spacing). You have
 identified a problem, so my suggestion is to not bother fiddling with
 adding one extra replica but sample that region to death with strong
 force constants. I presume that this will not impact your overall
 efficiency too much if the reaction coordinate is long overall.

 Finally, you will need to evaluate the convergence of your PMF overall
 and perhaps of this region in particular, especially if you want to
 know the dG to cross it or between two low energy states on either
 side of it.

 Chris.

 -- original message --


 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).

 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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umbrella114.mdp
Description: application/mdp
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[gmx-users] Umbrella Sampling

2011-03-31 Thread chris . neale
looks fine to me, no need to do that extra sampling that I suggested  
since it appears that you already did this -- benefits of seeing real  
data ;). If you want to understand why your histograms are not always  
centered at r0 (note that this is just fine) then you should read more  
about US, WHAM, and how to bias/debias the data for US (I am sure that  
there are textbooks around that explain this). The only case in which  
all of your histograms will be centered at their respective r0 is when  
the underlying PMF is exactly flat.


Chris.

-- original message --

Hi Chris many thanks again for the advise. I have, or at least I thought
have sampled my barrier region to death, but as I say some histograms
may not be centred around r0. I will proceed with what you suggest.
Please find attached a picture of the histograms, the corresponding
profile, and a sample mdp file that I use.

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--

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Re: [gmx-users] Umbrella Sampling

2011-03-31 Thread Gavin Melaugh
Cheers Chris

If I remove the red histogram (the first of the wider distributions),
which should be centred around 0.80nm but is actually centred around
0.78 nm; and add in some more histograms with higher force constants the
profile changes slightly. It seems that  g_wham is very sensitive to
these subtleties. How do I know which curve is correct? I have about six
such curves that differ slightly in this manner.

Gavin

chris.ne...@utoronto.ca wrote:
 looks fine to me, no need to do that extra sampling that I suggested
 since it appears that you already did this -- benefits of seeing real
 data ;). If you want to understand why your histograms are not always
 centered at r0 (note that this is just fine) then you should read more
 about US, WHAM, and how to bias/debias the data for US (I am sure that
 there are textbooks around that explain this). The only case in which
 all of your histograms will be centered at their respective r0 is when
 the underlying PMF is exactly flat.

 Chris.

 -- original message --

 Hi Chris many thanks again for the advise. I have, or at least I thought
 have sampled my barrier region to death, but as I say some histograms
 may not be centred around r0. I will proceed with what you suggest.
 Please find attached a picture of the histograms, the corresponding
 profile, and a sample mdp file that I use.

 -- next part --
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 --




modifiedhist.xvg.gz
Description: GNU Zip compressed data


modified.agr.gz
Description: GNU Zip compressed data
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Re: [gmx-users] Heat of vap

2011-03-31 Thread Elisabeth
in your mail:

On 30 March 2011 15:30, Justin A. Lemkul jalem...@vt.edu wrote:



 Elisabeth wrote:

 Dear all,

 I intend to obtain vaporization heat per volume for a /pure alkane
 system/.  Here is the steps I am taking. Please correct me.

 1- Obtain total energy of system (kinetic+potential) and divide by number
 of molecules to obtain energy per mol of molecules. g_energy -f *.edr -nmol
 XXX
 2- Obtain total energy of a single molecule (use pbc).
 3- Subtract step 2 from step 1.
 4- Divide by simulation box volume.

 My questions is:

 in step 2 : what should be the box size? The same size as in 1 or it does
 not matter? (step 1 is done for the actual denstiy)


 More troubling, how does one define the energy of a molecule?  If you use
 any sort of long-range algorithms (especially PME, but also dispersion
 correction), you can't simply decompose the system like this.

 Thanks Justin and David.

I have been trying to find the article in which this has been presented. If
you have time Please see page 5937, right column, equation 11. I think I
made a mistake and I dont have to include kinetic energy, Only nonboded
energies!?

http://pubs.acs.org/doi/pdfplus/10.1021/jp0707539



 In the derivation of recent Gromos96 parameter sets, the heat of
 vaporization is quite simple:

 DHvap = Ugas - Uliq + RT


1- So  Uliq is the total energy or only potential (no kinetic)
2- How can I compute Ugas? I have liquid now...


  Thank you,
 Regards,


 --
 

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

 

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Re: [gmx-users] Heat of vap

2011-03-31 Thread Justin A. Lemkul



Elisabeth wrote:



in your mail:

On 30 March 2011 15:30, Justin A. Lemkul jalem...@vt.edu 
mailto:jalem...@vt.edu wrote:




Elisabeth wrote:

Dear all,

I intend to obtain vaporization heat per volume for a /pure
alkane system/.  Here is the steps I am taking. Please correct me.

1- Obtain total energy of system (kinetic+potential) and divide
by number of molecules to obtain energy per mol of molecules.
g_energy -f *.edr -nmol XXX
2- Obtain total energy of a single molecule (use pbc).
3- Subtract step 2 from step 1.
4- Divide by simulation box volume.

My questions is:

in step 2 : what should be the box size? The same size as in 1
or it does not matter? (step 1 is done for the actual denstiy)


More troubling, how does one define the energy of a molecule?  If
you use any sort of long-range algorithms (especially PME, but also
dispersion correction), you can't simply decompose the system like this.

Thanks Justin and David.

I have been trying to find the article in which this has been presented. 
If you have time Please see page 5937, right column, equation 11. I 
think I made a mistake and I dont have to include kinetic energy, Only 
nonboded energies!?


http://pubs.acs.org/doi/pdfplus/10.1021/jp0707539



What is cohesive energy and how does it relate to the quantity you're trying to 
calculate?


 


In the derivation of recent Gromos96 parameter sets, the heat of
vaporization is quite simple:

DHvap = Ugas - Uliq + RT


1- So  Uliq is the total energy or only potential (no kinetic)


Potential.


2- How can I compute Ugas? I have liquid now...



Run a simulation in the gas phase.

-Justin



Thank you,
Regards,


-- 



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



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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] Heat of vap

2011-03-31 Thread David van der Spoel

On 2011-03-31 18.52, Elisabeth wrote:



in your mail:

On 30 March 2011 15:30, Justin A. Lemkul jalem...@vt.edu
mailto:jalem...@vt.edu wrote:



Elisabeth wrote:

Dear all,

I intend to obtain vaporization heat per volume for a /pure
alkane system/.  Here is the steps I am taking. Please correct me.

1- Obtain total energy of system (kinetic+potential) and divide
by number of molecules to obtain energy per mol of molecules.
g_energy -f *.edr -nmol XXX
2- Obtain total energy of a single molecule (use pbc).
3- Subtract step 2 from step 1.
4- Divide by simulation box volume.

My questions is:

in step 2 : what should be the box size? The same size as in 1
or it does not matter? (step 1 is done for the actual denstiy)


More troubling, how does one define the energy of a molecule?  If
you use any sort of long-range algorithms (especially PME, but also
dispersion correction), you can't simply decompose the system like this.

Thanks Justin and David.

I have been trying to find the article in which this has been presented.
If you have time Please see page 5937, right column, equation 11. I
think I made a mistake and I dont have to include kinetic energy, Only
nonboded energies!?
Either Epot or Etot. It does not matter if you simulate at the same 
Temp. You could also consider using the enthalphy (gmx 4.5 and higher).


http://pubs.acs.org/doi/pdfplus/10.1021/jp0707539

In the derivation of recent Gromos96 parameter sets, the heat of
vaporization is quite simple:

DHvap = Ugas - Uliq + RT


1- So Uliq is the total energy or only potential (no kinetic)
2- How can I compute Ugas? I have liquid now...


Thank you,
Regards,


--


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



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Dept. of Cell  Molec. Biol., Uppsala University.
Box 596, 75124 Uppsala, Sweden. Phone:  +46184714205.
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[gmx-users] adding a new residue in the ff

2011-03-31 Thread Anna Marabotti
Hi folks,
I have a problem with a strange residue into a PDB file. It is a
cysteinesulfonic acid, in which the -SH moiety of the Cys residue is
replaced by -SO3. This modified residue is essential for the activity of
this protein, therefore I must keep it into the protein. So, I'm trying to
add this new residue to the force field (I'm planning to use the 43a1ff
already modified for lipids in the past). Since I have Gromacs 4.5.3 I
copied the ff directory on my local dir, then I attempted to modify the
aminoacids.rtp file and other files following instructions in the section
Adding a residue to a force field. In order to have some hints on OCS
topology, I used PRODRG, at least to have some indication on atom, bonds and
angle types, but in the .itp file obtained from PRODRG there are several
data for which I don't find the corresponding element in the ffbonded.itp
file. For example, I don't see any equivalent for the CB - SG - OD1 angle.
Probably I should add them to the ffbonded.itp file, but I'm unsure how to
do it.  Is there an order to follow, or can I simply add a new element at
the end of the [ angle ] section? Can anyone give me some hint to do it
correctly, and more generally to manage correctly the whole problem? 
Thanks a lot
Anna Marabotti
 
__
Anna Marabotti, Ph.D.
Laboratory of Bioinformatics and Computational Biology
Institute of Food Science - CNR
Via Roma, 64
83100 Avellino
Phone: +39 0825 299651
Fax: +39 0825 781585
E-mail: amarabo...@isa.cnr.it
Skype account: annam1972
Web site: http://bioinformatica.isa.cnr.it/anna/anna.htm
 
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(Roberto Benigni, about Roberto Saviano)
 
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Re: [gmx-users] Heat of vap

2011-03-31 Thread Elisabeth
On 31 March 2011 12:58, Justin A. Lemkul jalem...@vt.edu wrote:



 Elisabeth wrote:



 in your mail:


 On 30 March 2011 15:30, Justin A. Lemkul jalem...@vt.edu mailto:
 jalem...@vt.edu wrote:



Elisabeth wrote:

Dear all,

I intend to obtain vaporization heat per volume for a /pure
alkane system/.  Here is the steps I am taking. Please correct me.

1- Obtain total energy of system (kinetic+potential) and divide
by number of molecules to obtain energy per mol of molecules.
g_energy -f *.edr -nmol XXX
2- Obtain total energy of a single molecule (use pbc).
3- Subtract step 2 from step 1.
4- Divide by simulation box volume.

My questions is:

in step 2 : what should be the box size? The same size as in 1
or it does not matter? (step 1 is done for the actual denstiy)


More troubling, how does one define the energy of a molecule?  If
you use any sort of long-range algorithms (especially PME, but also
dispersion correction), you can't simply decompose the system like
 this.

 Thanks Justin and David.

 I have been trying to find the article in which this has been presented.
 If you have time Please see page 5937, right column, equation 11. I think I
 made a mistake and I dont have to include kinetic energy, Only nonboded
 energies!?

 http://pubs.acs.org/doi/pdfplus/10.1021/jp0707539


 What is cohesive energy and how does it relate to the quantity you're
 trying to calculate?

 It is delta Hvap/volume. It is directly related to Hvap. What is happening
 is that they are calculating nonbonded energy of some chains, divide by
 number of chains and substract from nonbonded energy of a single chain in
 vacuum. These are the steps I wrote in my first post but I think I should
 not have included kinetic and should just look at LJ-SR and Coulomb-SR.


I am using PME..If I remember correctly LR is included in Coulomb-SR and can
not get decomposed? But I dont think this doesnt matter since if I am to
take nonbonded energies this should not hurt,,,

Please comment ...




In the derivation of recent Gromos96 parameter sets, the heat of
vaporization is quite simple:

DHvap = Ugas - Uliq + RT


 1- So  Uliq is the total energy or only potential (no kinetic)


 Potential.


  2- How can I compute Ugas? I have liquid now...


 Run a simulation in the gas phase.


Sorry, but how can I do this? :( I have box of molecules with density of
actual liquid..How can I shift to gas phase ..I mean how many molecules I
need to keep in the box..

Many thanks...


 -Justin


Thank you,
Regards,


-- 

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

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



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 --
 

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

 
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[gmx-users] How to compile the template.c when GMX is builded with cmake

2011-03-31 Thread Bert
Dear all,

When GMX is builded with cmake, how to compile the template.c? I used
to make the template.c by the command make -f MakefileXXX, but it
can not work in version 4.5. Thanks for your suggestions.

Best regards,
Bert
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Re: [gmx-users] Heat of vap

2011-03-31 Thread Justin A. Lemkul



Elisabeth wrote:



On 31 March 2011 12:58, Justin A. Lemkul jalem...@vt.edu 
mailto:jalem...@vt.edu wrote:




Elisabeth wrote:



in your mail:


On 30 March 2011 15:30, Justin A. Lemkul jalem...@vt.edu
mailto:jalem...@vt.edu mailto:jalem...@vt.edu
mailto:jalem...@vt.edu wrote:



   Elisabeth wrote:

   Dear all,

   I intend to obtain vaporization heat per volume for a /pure
   alkane system/.  Here is the steps I am taking. Please
correct me.

   1- Obtain total energy of system (kinetic+potential) and
divide
   by number of molecules to obtain energy per mol of molecules.
   g_energy -f *.edr -nmol XXX
   2- Obtain total energy of a single molecule (use pbc).
   3- Subtract step 2 from step 1.
   4- Divide by simulation box volume.

   My questions is:

   in step 2 : what should be the box size? The same size as
in 1
   or it does not matter? (step 1 is done for the actual
denstiy)


   More troubling, how does one define the energy of a molecule?  If
   you use any sort of long-range algorithms (especially PME,
but also
   dispersion correction), you can't simply decompose the system
like this.

Thanks Justin and David.

I have been trying to find the article in which this has been
presented. If you have time Please see page 5937, right column,
equation 11. I think I made a mistake and I dont have to include
kinetic energy, Only nonboded energies!?

http://pubs.acs.org/doi/pdfplus/10.1021/jp0707539


What is cohesive energy and how does it relate to the quantity
you're trying to calculate?

It is delta Hvap/volume. It is directly related to Hvap. What is
happening is that they are calculating nonbonded energy of some
chains, divide by number of chains and substract from nonbonded
energy of a single chain in vacuum. These are the steps I wrote in
my first post but I think I should not have included kinetic and
should just look at LJ-SR and Coulomb-SR.


I am using PME..If I remember correctly LR is included in Coulomb-SR and 
can not get decomposed? But I dont think this doesnt matter since if I 
am to take nonbonded energies this should not hurt,,,


Please comment ...



PME energies are from nonbonded interactions.  The mesh energy is written to the 
Coul-recip term in the .edr file.  If there is some other Coul (LR) term, it 
is because you're using a twin-range cutoff such that rcoulomb  rlist, which I 
do not believe is correct when using PME.


 

 
   In the derivation of recent Gromos96 parameter sets, the heat of

   vaporization is quite simple:

   DHvap = Ugas - Uliq + RT


1- So  Uliq is the total energy or only potential (no kinetic)


Potential.


2- How can I compute Ugas? I have liquid now...


Run a simulation in the gas phase.


Sorry, but how can I do this? :( I have box of molecules with density of 
actual liquid..How can I shift to gas phase ..I mean how many molecules 
I need to keep in the box..




Make a box with an equivalent number of molecules separated by some large amount 
of space (i.e. 50 nm or so).  Set pbc=no and all cutoffs to zero.  I'm basing 
this on Gromos96 parameterization, but I don't know what your target force field is.


-Justin


Many thanks...


-Justin


   Thank you,
   Regards,


   -- 

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

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

   

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Justin A. Lemkul
Ph.D. Candidate
ICTAS Doctoral Scholar
MILES-IGERT Trainee
Department of Biochemistry
  

Re: [gmx-users] Heat of vap

2011-03-31 Thread David van der Spoel

On 2011-03-31 19.11, Elisabeth wrote:



On 31 March 2011 12:58, Justin A. Lemkul jalem...@vt.edu
mailto:jalem...@vt.edu wrote:



Elisabeth wrote:



in your mail:


On 30 March 2011 15:30, Justin A. Lemkul jalem...@vt.edu
mailto:jalem...@vt.edu mailto:jalem...@vt.edu
mailto:jalem...@vt.edu wrote:



Elisabeth wrote:

Dear all,

I intend to obtain vaporization heat per volume for a /pure
alkane system/.  Here is the steps I am taking. Please
correct me.

1- Obtain total energy of system (kinetic+potential) and
divide
by number of molecules to obtain energy per mol of
molecules.
g_energy -f *.edr -nmol XXX
2- Obtain total energy of a single molecule (use pbc).
3- Subtract step 2 from step 1.
4- Divide by simulation box volume.

My questions is:

in step 2 : what should be the box size? The same size
as in 1
or it does not matter? (step 1 is done for the actual
denstiy)


More troubling, how does one define the energy of a
molecule?  If
you use any sort of long-range algorithms (especially PME,
but also
dispersion correction), you can't simply decompose the
system like this.

Thanks Justin and David.

I have been trying to find the article in which this has been
presented. If you have time Please see page 5937, right column,
equation 11. I think I made a mistake and I dont have to include
kinetic energy, Only nonboded energies!?

http://pubs.acs.org/doi/pdfplus/10.1021/jp0707539


What is cohesive energy and how does it relate to the quantity
you're trying to calculate?

It is delta Hvap/volume. It is directly related to Hvap. What is
happening is that they are calculating nonbonded energy of some
chains, divide by number of chains and substract from nonbonded
energy of a single chain in vacuum. These are the steps I wrote in
my first post but I think I should not have included kinetic and
should just look at LJ-SR and Coulomb-SR.


I am using PME..If I remember correctly LR is included in Coulomb-SR and
can not get decomposed? But I dont think this doesnt matter since if I
am to take nonbonded energies this should not hurt,,,

Please comment ...

It is simple.
Compute Epot with all normal liquid options (PME, Dispcorr etc.).
Compute Epot for a gas phase molecule without any cutoffs
Apply equation below.
For OPLS/AA we obtain close to 98% correlation between experiment and 
simulation (paper submitted).



In the derivation of recent Gromos96 parameter sets, the heat of
vaporization is quite simple:

DHvap = Ugas - Uliq + RT


1- So Uliq is the total energy or only potential (no kinetic)


Potential.


2- How can I compute Ugas? I have liquid now...


Run a simulation in the gas phase.


Sorry, but how can I do this? :( I have box of molecules with density of
actual liquid..How can I shift to gas phase ..I mean how many molecules
I need to keep in the box..

Many thanks...


-Justin


Thank you,
Regards,


-- 

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

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



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


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[gmx-users] Umbrella Sampling

2011-03-31 Thread chris . neale

your comment:

which should be centred around 0.80nm

is flawed, as i mentioned earlier. also, it is not g_wham that is  
sensitive but the convergence and sampling of phase space that is  
sensitive. don`t remove any data. do evaluate your convergence.  
without convergence measures, a pmf is worse than useless.


chris.

-- original message --

Cheers Chris

If I remove the red histogram (the first of the wider distributions),
which should be centred around 0.80nm but is actually centred around
0.78 nm; and add in some more histograms with higher force constants the
profile changes slightly. It seems that  g_wham is very sensitive to
these subtleties. How do I know which curve is correct? I have about six
such curves that differ slightly in this manner.

Gavin

chris.ne...@utoronto.ca wrote:

[Hide Quoted Text]
looks fine to me, no need to do that extra sampling that I suggested
since it appears that you already did this -- benefits of seeing real
data ;). If you want to understand why your histograms are not always
centered at r0 (note that this is just fine) then you should read more
about US, WHAM, and how to bias/debias the data for US (I am sure that
there are textbooks around that explain this). The only case in which
all of your histograms will be centered at their respective r0 is when
the underlying PMF is exactly flat.

Chris.

-- original message --

Hi Chris many thanks again for the advise. I have, or at least I thought
have sampled my barrier region to death, but as I say some histograms
may not be centred around r0. I will proceed with what you suggest.
Please find attached a picture of the histograms, the corresponding
profile, and a sample mdp file that I use.


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Re: [gmx-users] adding a new residue in the ff

2011-03-31 Thread Tsjerk Wassenaar
Hi,

 It would probably be easier, faster, and more accurate to just use most of
 the parameters for Cys rather than try to have PRODRG re-create a
 (potentially flawed) model of your compound.  The only new parameters are
 related to SO3, so the rest should be identical to the Cys residue.

That's not a good idea. It'll only do for the backbone. The charge of
CB will be quite different, as well as the CA-CB-SG angle, and for the
rest there's nothing similar even.

 This is where parameterization becomes a chore - when there's nothing
 analogous to what you're doing.  Proper Gromos96 parameterization
 methodology would dictate that you generate an analogous compound (i.e.,
 methyl sulfonic acid) and adjust its parameters such that it reproduces
 various condensed-phase thermodynamic and physical properties (DeltaG of
 solvation, liquid density, heat of vaporization).  Proper derivation is
 quite time-consuming.  Perhaps someone has already done this work and it is
 published.  If you're unlucky, you've got to do it all yourself.

That's a good idea :)

Cheers,

Tsjerk



-- 
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] adding a new residue in the ff

2011-03-31 Thread Justin A. Lemkul



Tsjerk Wassenaar wrote:

Hi,


It would probably be easier, faster, and more accurate to just use most of
the parameters for Cys rather than try to have PRODRG re-create a
(potentially flawed) model of your compound.  The only new parameters are
related to SO3, so the rest should be identical to the Cys residue.


That's not a good idea. It'll only do for the backbone. The charge of
CB will be quite different, as well as the CA-CB-SG angle, and for the
rest there's nothing similar even.



Gah, that's what I meant.  Thanks for pointing that out!  I guess I've stated so 
many times (and published on the fact) that PRODRG charges are useless that I'm 
no longer even quoting myself...


-Justin


This is where parameterization becomes a chore - when there's nothing
analogous to what you're doing.  Proper Gromos96 parameterization
methodology would dictate that you generate an analogous compound (i.e.,
methyl sulfonic acid) and adjust its parameters such that it reproduces
various condensed-phase thermodynamic and physical properties (DeltaG of
solvation, liquid density, heat of vaporization).  Proper derivation is
quite time-consuming.  Perhaps someone has already done this work and it is
published.  If you're unlucky, you've got to do it all yourself.


That's a good idea :)

Cheers,

Tsjerk





--


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Ph.D. Candidate
ICTAS Doctoral Scholar
MILES-IGERT Trainee
Department of Biochemistry
Virginia Tech
Blacksburg, VA
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[gmx-users] Web site issues (Search, Redmine)

2011-03-31 Thread Lutz Maibaum
I ran into some issues with the Gromacs web site:

1. I tried to register an account on the bug tracker
(http://redmine.gromacs.org/account/register). Upon entering my
information, I get the odd error message Email notifications is not
included in the list. Perhaps this is related to
http://www.redmine.org/issues/7138 ?

2. Trying to figure out what's going on, I wanted to check the mailing
list archive. Searching for redmine on
http://www.gromacs.org/Support/Mailing_Lists/Search gives strange
results (just a few emails that are listed dozens of times).

I hope this helps to track some of these things down.

Best,

  Lutz
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[gmx-users] implicit solvent GB force table

2011-03-31 Thread Chi-cheng Chiu
Hi,
I have been tracking the code for implicit solvent,
i.e. src/mdlib/genborn.c
According to the gromacs paper on implicit solvent, J Comp Chem 31:2593,
2010, the GB force is tabulated in the X = Rij Ci Cj dimension.
However, the tabulated function, which I think is stored in fr-gbtab, is
only used in the function gb_bonds_tab().
I could not find the function of X applied in the calc_gb_chainrule()
function. Does the gbtab applied on dvda and dadx elsewhere? Thanks in
advance!

regards,

Chi-cheng
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[gmx-users] Spatially Varying External Force

2011-03-31 Thread Apoorv Kalyankar
Hello,

Is there a way we can apply a spatially varying external force in
GROMACS. I went through the manual if anything like this is possible
but couldn't find anything.
Any help is appreciated.

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

2011-03-31 Thread Per Larsson
Hi!

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

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

Cheers
/Per

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

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

2011-03-31 Thread Luca Bellucci
Dear all,
I tried to use couple-moltype=Protein Ligand directive   
to annihilate both protein and ligand molecules using free energy method.
I realized that couple-moltype key works for only one molecule type.
Is it right? 

To perform the same annihilation I used
couple-moltype=Protein to annihilate the protein and dual topology
 formalism (definied in itp file) to annihilate the ligand.
Are these commands able to work together?
Thanks
Luca
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Re: [gmx-users] Web site issues (Search, Redmine)

2011-03-31 Thread Rossen Apostolov

Hi Lutz,

On 3/31/11 9:06 PM, Lutz Maibaum wrote:

I ran into some issues with the Gromacs web site:

1. I tried to register an account on the bug tracker
(http://redmine.gromacs.org/account/register). Upon entering my
information, I get the odd error message Email notifications is not
included in the list. Perhaps this is related to
http://www.redmine.org/issues/7138 ?


I moved the server a few days ago and haven't done one of the migration 
steps. Could you check again and let me know (offline is OK) if it 
doesn't work?



2. Trying to figure out what's going on, I wanted to check the mailing
list archive. Searching for redmine on
http://www.gromacs.org/Support/Mailing_Lists/Search gives strange
results (just a few emails that are listed dozens of times).


That's strange indeed, will fix it.


I hope this helps to track some of these things down.


Thanks a lot for reporting!

Cheers,
Rossen


Best,

   Lutz


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[gmx-users] Taking difference of forces in two trajectories

2011-03-31 Thread Sikandar Mashayak
Hi

I want to test two test potentials compared to reference potential.

I have md trajectories from reference potential. So I do mdrun -rerun with
two different test potentials and get two separate trajectory files. Now I
want to compute difference between forces acting on each atom in each frame
due to different test potentials. Is there any way where two trajectories
with same position values but different forces can be used to get third .trr
file with forces which are difference of first two?

thanks
sikandar
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Re: [gmx-users] Taking difference of forces in two trajectories

2011-03-31 Thread Justin A. Lemkul



Sikandar Mashayak wrote:

Hi

I want to test two test potentials compared to reference potential. 

I have md trajectories from reference potential. So I do mdrun -rerun 
with two different test potentials and get two separate trajectory 
files. Now I want to compute difference between forces acting on each 
atom in each frame due to different test potentials. Is there any way 
where two trajectories with same position values but different forces 
can be used to get third .trr file with forces which are difference of 
first two?




I don't think you can make mdrun calculate differences in two existing 
trajectories, but you can extract forces using g_traj and take the difference 
between the two output files.  The file sizes may get extremely large for either 
long trajectories or many atoms.


-Justin


thanks
sikandar



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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] Taking difference of forces in two trajectories

2011-03-31 Thread Sikandar Mashayak
hey thanks for the explanation..

 for some constraints I need to have the difference of forces in the .trr
format so that I have position,velocity and force error values in one single
.trr file. , I dont think g_traj would help me getting that.. is there any
other option?

On Thu, Mar 31, 2011 at 4:44 PM, Justin A. Lemkul jalem...@vt.edu wrote:



 Sikandar Mashayak wrote:

 Hi

 I want to test two test potentials compared to reference potential.
 I have md trajectories from reference potential. So I do mdrun -rerun with
 two different test potentials and get two separate trajectory files. Now I
 want to compute difference between forces acting on each atom in each frame
 due to different test potentials. Is there any way where two trajectories
 with same position values but different forces can be used to get third .trr
 file with forces which are difference of first two?


 I don't think you can make mdrun calculate differences in two existing
 trajectories, but you can extract forces using g_traj and take the
 difference between the two output files.  The file sizes may get extremely
 large for either long trajectories or many atoms.

 -Justin

  thanks
 sikandar


 --
 

 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] Taking difference of forces in two trajectories

2011-03-31 Thread Justin A. Lemkul



Sikandar Mashayak wrote:

hey thanks for the explanation..

 for some constraints I need to have the difference of forces in the 
.trr format so that I have position,velocity and force error values in 
one single .trr file. , I dont think g_traj would help me getting that.. 
is there any other option?




I don't think there is currently any tool that can do this.  With the xdrfile 
library, though, you might be able to write your own program that can do it.


-Justin

On Thu, Mar 31, 2011 at 4:44 PM, Justin A. Lemkul jalem...@vt.edu 
mailto:jalem...@vt.edu wrote:




Sikandar Mashayak wrote:

Hi

I want to test two test potentials compared to reference potential.
I have md trajectories from reference potential. So I do mdrun
-rerun with two different test potentials and get two separate
trajectory files. Now I want to compute difference between
forces acting on each atom in each frame due to different test
potentials. Is there any way where two trajectories with same
position values but different forces can be used to get third
.trr file with forces which are difference of first two?


I don't think you can make mdrun calculate differences in two
existing trajectories, but you can extract forces using g_traj and
take the difference between the two output files.  The file sizes
may get extremely large for either long trajectories or many atoms.

-Justin

thanks
sikandar


-- 



Justin A. Lemkul
Ph.D. Candidate
ICTAS Doctoral Scholar
MILES-IGERT Trainee
Department of Biochemistry
Virginia Tech
Blacksburg, VA
jalemkul[at]vt.edu http://vt.edu | (540) 231-9080
tel:%28540%29%20231-9080
http://www.bevanlab.biochem.vt.edu/Pages/Personal/justin


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Department of Biochemistry
Virginia Tech
Blacksburg, VA
jalemkul[at]vt.edu | (540) 231-9080
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[gmx-users] VDW parameters: Martini Forcefield + Implicit Solvation

2011-03-31 Thread emendez
Greetings,

I am trying to do Martini Forcefield + Implicit solvation model for a
large system and I need to supply parameters for the
[ implicit_genborn_params ]
section. Which I have not found.

The syntax is

Atomtype sar st pi gbr hct

Can anybody provide me a clue about where I can find these parameters?

Regards

Eduardo Mendez
University of Calgary

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Re: [gmx-users] VDW parameters: Martini Forcefield + Implicit Solvation

2011-03-31 Thread Mark Abraham

On 1/04/2011 9:29 AM, emen...@ucalgary.ca wrote:

Greetings,

I am trying to do Martini Forcefield + Implicit solvation model for a
large system and I need to supply parameters for the
[ implicit_genborn_params ]
section. Which I have not found.

The syntax is

Atomtype sar st pi gbr hct

Can anybody provide me a clue about where I can find these parameters?


Manual section 5.3.5 describes the parameters.

Mark
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[gmx-users] RE: VDW parameters: Martini Forcefield + Implicit Solvation

2011-03-31 Thread emendez
Thanks for your promt reply Mark.
Of course I know what is the format, that is implied in my question
what I would like to know is if anybody has the specific parameters for
the amber forcefield. I will try using the gbr parameters from the sigma
in the  LJ potentials, but  I am not sure about the proper hct (or the
other numbers) hence I am inquiring about this,

Cheers.

Eduardo Mendez

 Greetings,

 I am trying to do Martini Forcefield + Implicit solvation model for a
 large system and I need to supply parameters for the
 [ implicit_genborn_params ]
 section. Which I have not found.

 The syntax is

 Atomtype sar st pi gbr hct

 Can anybody provide me a clue about where I can find these parameters?



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[gmx-users] Installtion of gromacs-4.5.3

2011-03-31 Thread parichita parichita
Hi...
I am try to istalling gromacs -4.5.3 on AMD phenom II.
I am following the installtions protocols, 1 St i have installed the fftw3.2.2,
./configure --enable-threads --enables-floats --enables-sse
make 
make install

then I am doing the cmake. 
cd gromacs-4.5.3
mkdir exec
cd exec
cmake ../

After cmake the make -j 6 gives me an error

Linking C shared library libmd.so
/usr/bin/ld: /usr/local/lib/libfftw3f.a(tensor.o): relocation R_X86_64_32 
against `.rodata.str1.1' can not be used when making a shared object; recompile 
with -fPIC
/usr/local/lib/libfftw3f.a: could not read symbols: Bad value
collect2: ld returned 1 exit status
make[2]: *** [src/mdlib/libmd.so.6] Error 1
make[1]: *** [src/mdlib/CMakeFiles/md.dir/all] Error 2
make: *** [all] Error 2

please suggest me what I should do next...

with regards


Parichita Mazumder  
 Research Fellow 
C/O Dr. Chaitali Mukhopadhayay 
Department of Chemistry 
University of Calcutta 
92,A P C Road 
Kolkata-79 
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[gmx-users] VDW parameters: Martini Forcefield + Implicit Solvation

2011-03-31 Thread emendez
I meant to say, the MARTINI parameters,

regards

E

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Re: [gmx-users] Installtion of gromacs-4.5.3

2011-03-31 Thread Roland Schulz
Hi,

this question has been answered often. Please check the archive before
posting.

Roland

On Thu, Mar 31, 2011 at 8:01 PM, parichita parichita 
parichitamajum...@yahoo.co.in wrote:

 Hi...
 I am try to istalling gromacs -4.5.3 on AMD phenom II.
 I am following the installtions protocols, 1 St i have installed the
 fftw3.2.2,
 ./configure --enable-threads --enables-floats --enables-sse
 make
 make install

 then I am doing the cmake.
 cd gromacs-4.5.3
 mkdir exec
 cd exec
 cmake ../

 After cmake the make -j 6 gives me an error

 Linking C shared library libmd.so
 /usr/bin/ld: /usr/local/lib/libfftw3f.a(tensor.o): relocation R_X86_64_32
 against `.rodata.str1.1' can not be used when making a shared object;
 recompile with -fPIC
 /usr/local/lib/libfftw3f.a: could not read symbols: Bad value
 collect2: ld returned 1 exit status
 make[2]: *** [src/mdlib/libmd.so.6] Error 1
 make[1]: *** [src/mdlib/CMakeFiles/md.dir/all] Error 2
 make: *** [all] Error 2

 please suggest me what I should do next...

 with regards


 Parichita Mazumder
 Research Fellow
 C/O Dr. Chaitali Mukhopadhayay
 Department of Chemistry
 University of Calcutta
 92,A P C Road
 Kolkata-79
 India.

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[gmx-users] dipole moment of a charged peptide

2011-03-31 Thread Sanku M
Hi,
   I have a long-chain peptide which has a net charge of  +5 . I was wondering 
whether the g_dipole will give any reasonable dipole moment for a molecule with 
a net charge. Is there any suggestion I should follow regarding calculation of 
dipole-moment of a charged molecule .
 I found that in the manual it is mentioned that 'For molecules with a net 
charge, the net charge is subtracted atcenter of mass of the molecule.'.  I did 
not understand what it means. I am using gromacs-4.0.7.
Sanku



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[gmx-users] Groups in mdp file

2011-03-31 Thread Sai Pooja
Hi,

This is regarding the energygroups that one can use in the mdp file for
tracking energy. Are these the groups defined in the index file?

I want to know if I can define a subset of atoms in the index file and track
its energy.

Pooja

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Re: [gmx-users] Installtion of gromacs-4.5.3

2011-03-31 Thread Mark Abraham

On 1/04/2011 11:01 AM, parichita parichita wrote:

Hi...
I am try to istalling gromacs -4.5.3 on AMD phenom II.
I am following the installtions protocols, 1 St i have installed the 
fftw3.2.2,

./configure --enable-threads --enables-floats --enables-sse



That's not how you successfully configured FFTW. Two of your flags do 
not work, for three separate uses of wrong words.



make
make install

then I am doing the cmake.
cd gromacs-4.5.3
mkdir exec
cd exec
cmake ../

After cmake the make -j 6 gives me an error

Linking C shared library libmd.so
/usr/bin/ld: /usr/local/lib/libfftw3f.a(tensor.o): relocation 
R_X86_64_32 against `.rodata.str1.1' can not be used when making a 
shared object; recompile with -fPIC




I have updated the 
http://www.gromacs.org/Downloads/Installation_Instructions to cover this 
issue.


Mark


/usr/local/lib/libfftw3f.a: could not read symbols: Bad value
collect2: ld returned 1 exit status
make[2]: *** [src/mdlib/libmd.so.6] Error 1
make[1]: *** [src/mdlib/CMakeFiles/md.dir/all] Error 2
make: *** [all] Error 2

please suggest me what I should do next...

with regards


Parichita Mazumder
Research Fellow
C/O Dr. Chaitali Mukhopadhayay
Department of Chemistry
University of Calcutta
92,A P C Road
Kolkata-79
India.



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Re: [gmx-users] Groups in mdp file

2011-03-31 Thread Mark Abraham

On 1/04/2011 1:30 PM, Sai Pooja wrote:

Hi,
This is regarding the energygroups that one can use in the mdp file 
for tracking energy. Are these the groups defined in the index file?


Yes, the groups are defined there (or created by default if an index 
file is not supplied) and specified as energy groups in the .mdp file.


I want to know if I can define a subset of atoms in the index file and 
track its energy.


Yes. Whether it means anything is another matter.

Mark
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Re: [gmx-users] RE: VDW parameters: Martini Forcefield + Implicit Solvation

2011-03-31 Thread Mark Abraham

On 1/04/2011 10:57 AM, emen...@ucalgary.ca wrote:

Thanks for your promt reply Mark.
Of course I know what is the format, that is implied in my question


Leaving things to implication is risky. People do misunderstand, 
unfortunately. Fault in such cases varies :-) If what you actually want 
is gbr and hct parameters for Martini atom types, everyone can use their 
time better if you ask specifically about that.



what I would like to know is if anybody has the specific parameters for
the amber forcefield. I will try using the gbr parameters from the sigma
in the  LJ potentials, but  I am not sure about the proper hct (or the
other numbers) hence I am inquiring about this,


That manual section mentions the reference sources for these parameters, 
which is why I referred to it. Whether there's any established procedure 
for implicit solvation with Martini is probably a question for 
literature search and speaking with the Martini developers.


Mark


Cheers.

Eduardo Mendez


Greetings,

I am trying to do Martini Forcefield + Implicit solvation model for a
large system and I need to supply parameters for the
[ implicit_genborn_params ]
section. Which I have not found.

The syntax is

Atomtype sar st pi gbr hct

Can anybody provide me a clue about where I can find these parameters?





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Re: [gmx-users] Groups in mdp file

2011-03-31 Thread Sai Pooja
On Thu, Mar 31, 2011 at 10:41 PM, Mark Abraham mark.abra...@anu.edu.auwrote:

 On 1/04/2011 1:30 PM, Sai Pooja wrote:

 Hi,
 This is regarding the energygroups that one can use in the mdp file for
 tracking energy. Are these the groups defined in the index file?


 Yes, the groups are defined there (or created by default if an index file
 is not supplied) and specified as energy groups in the .mdp file.


 I want to know if I can define a subset of atoms in the index file and
 track its energy.


 Yes. Whether it means anything is another matter.


Well the idea is to modify the hamiltonian for only a subset of atoms and
apply hamiltonian replica exchange. I was hoping defining energy group could
be a good way to apply this(obv it would requires other changes too).


 Mark
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Re: [gmx-users] Groups in mdp file

2011-03-31 Thread Mark Abraham

On 1/04/2011 2:06 PM, Sai Pooja wrote:



On Thu, Mar 31, 2011 at 10:41 PM, Mark Abraham 
mark.abra...@anu.edu.au mailto:mark.abra...@anu.edu.au wrote:


On 1/04/2011 1:30 PM, Sai Pooja wrote:

Hi,
This is regarding the energygroups that one can use in the mdp
file for tracking energy. Are these the groups defined in the
index file?


Yes, the groups are defined there (or created by default if an
index file is not supplied) and specified as energy groups in the
.mdp file.


I want to know if I can define a subset of atoms in the index
file and track its energy.


Yes. Whether it means anything is another matter.

Well the idea is to modify the hamiltonian for only a subset of atoms 
and apply hamiltonian replica exchange. I was hoping defining energy 
group could be a good way to apply this(obv it would requires other 
changes too).


Describing the overall objective is usually a good idea. Sometimes one's 
candidate for a solution is not best and someone else knows it :-) Here, 
energy groups are the only reasonable solution.


Mark
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