From chemistry-request@server.ccl.net Tue Jul  9 03:56:42 2002
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From: "Tamas E. Gunda" <tamasgunda@tigris.klte.hu>
To: "Luciana Marinelli" <luci@novel7.farmacia.unina.it>, <chemistry@ccl.net>
References: <3D29C50E.CCD1338F@novel7.farmacia.unina.it>
Subject: Re: CCL:problem with mol2topdb script
Date: Tue, 9 Jul 2002 09:57:00 +0200
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Luciana,

The sybyl2 file looks quite strange - I mean the atoms and residues are
scrambled, bonds between chains etc.
The sum of partial charges is -104.18. Is it surely correct?
The file was produced by Sybyl, if I understood well. Have you tried to
re-read the file into Sybyl? Is it OK then?
Regards

Dr. Tamas E. Gunda
Research Group for Antibiotics
Hungarian Academy of Sciences
University of Debrecen, POBox 36
H-4010 Debrecen, Hungary
tamasgunda@tigris.klte.hu


----- Original Message -----
From: "Luciana Marinelli" <luci@novel7.farmacia.unina.it>
To: <chemistry@ccl.net>
Sent: Monday, July 08, 2002 18:59
Subject: CCL:problem with mol2topdb script


> hallo,
> I am a new AUTODOCK user, I have problem with mol2topdb script.
> I am working on a silicon graphics with an operating system: IRIX64
> Release 6. I have download the new one version of autodock.
> I have downloaded my protein from PDB and I have added H and charges by
> sybyl as you explain in the user guide, than I saved it as mol2 file,
> but when I try to run the script that should convert the mol2 file into
> the pdbq I have this output:
> % mol2topdbq 1L5G.pdb
> gawk - Command not found
> %
>
>


From chemistry-request@server.ccl.net Tue Jul  9 04:16:08 2002
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Date: Tue, 9 Jul 2002 10:16:03 +0200 (METDST)
From: An Van Looy <avalo@ruca.ua.ac.be>
To: chemistry@ccl.net
Subject: distributed multiopole analysis of the molecule NF3
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Hello

I have a problem. I want to do a distributed multipole analysis with the
program GAMESS for the
molecule NF3, but what do I do with the free electronpair: ingnore, dummy
... 

I tried to do it the same way as for example CF4, SiF4 (this means ignore
the free electronpair)

First I optimize the structure of the molecule with G98.
Then I make my Gamess inputfile. in $data, I give a C1 symmetry and the
(G98) coordinates of the molecule. 

This is then my Gamess inputfile ...

 $contrl scftyp=rhf mplevl=2 $end
 $system memory=4000000 $end
 $basis gbasis=n311 ngauss=6 ndfunc=1 diffsp=.true. $end
 $guess guess=huckel $end
 $stone
 ATOMS
 $end
 $data
 distributed multipole
 C1
 N    7      0.000000          0.477297          0.000000
 F    9     -1.230673         -0.124400          0.000000
 F    9      0.615337         -0.123416          1.066030
 F    9      0.615337         -0.123416         -1.066030
 $end


I tried to use a dummy in the structure for the free electronpair. To me
it seems that I have to do something with the free electronpair. But the
calculation does not do anything with the dummy It gets no multipoles at
all. This was the used input-file

...
 $stone                                                                         
 ATOMS                                                                          
 POINT     0.000000    0.000000    1.000000    DUMMY
...
 C1
 N          7        0.000000    0.000000    0.000000                           
 F          9        1.197378    0.000000   -0.573989                           
 F          9       -0.598689   -1.036960   -0.573989                           
 F          9       -0.598689    1.036960   -0.573989                           
 $end

How can I calculate the DMA for NF3, which way is the right one ? Is there
someone who can help me ?

Thanks !

An


    --- *** ---

An Van Looy
avalo@ruca.ua.ac.be
Ph.D student
researchgroup Prof B.J. van der Veken
RUCA - University of Antwerp
BELGIUM




From chemistry-request@server.ccl.net Tue Jul  9 07:45:31 2002
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Date: Tue, 09 Jul 2002 13:41:29 +0200
From: Vlad Cojocaru <Vlad.Cojocaru@mpi-bpc.mpg.de>
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Hi!
  I am trying (using Gaussian 94) to estimate the differences between 
hydrogen bonding between A-T and 2-amino purine-T. I also have other 
base analogues with which I want to do the same.
  Would you please indicate me some references or some advices about the 
approach for such kind of studies?
  Thanks a lot in advance,
vlad

-- 
Vlad Cojocaru 
Max Planck Institut for Biophysical Chemistry 
Deparment: 060 
Am Fassberg 11, 37077 Goettingen, Germany 
tel: ++49-551-201.1389 
e-mail: Vlad.Cojocaru@mpi-bpc.mpg.de  




From chemistry-request@server.ccl.net Tue Jul  9 09:14:05 2002
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Date: Tue, 09 Jul 2002 14:13:41 +0100
From: Krzysztof Radacki <K.Radacki@ic.ac.uk>
Organization: Imperial College, London
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Subject: gaussian problems
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Dear all,
I have two question and one information concerning gaussian.

1)
I wanted to perform an optimization with possibly slowest  changing
of geometry. The command line was as:
#P OPT=(Redundant,CalcAll,StepSize=1,TIGHT) INT=(GRID=99590)

I got an error:

  QPERR --- A SYNTAX ERROR WAS DETECTED IN THE INPUT LINE.
 #P OPT=(REDUNDANT,CALCALL,STEPSIZE=1,TIG
                           '

What's wrong? On p.129 of User's reference one can find description 
of StepSize in Opt and I can't see why it shouldn't work.



2)
However calculation of IR was already sometimes discussed on CCL I 
still have uneasy feeling. An example.
I have a molecule with trigonal bipiramide (D3h) structure. I know 
however that minimum is distorted - both axial ligands are moved out 
of Z-axis in direction of one equatorial ligand (f.e.: ax-ax angle 160) 
and the equatorial are still co-planar (C2v).
(I hope that you can imagin it from my description).

Now: If I would distorte D3h structure to C2v with ax-ax angle 175 deg
and optimized geometry with frozen ax-ax, should IR calculation have 
a one imaginary freq. narrowing ax-ax angle or not? If it gives me no 
Imag - hwat does it mean?

One can find in books that vibrational analysis should be performed 
only on stationary point - if not it's meaningless. What sense has it 
if one makes such restriction? If I want to be sure that I'm in minimum
should I repaet all symmetry bounded calculation (like above D3h)
with NoSymm?



3)
Last week I wanted to calculated some quite complicated 
molecules like CO or CCH2 and various level of theory.
Everything was fine with DFT and MP2 but the same inputs
didn't work for CCSD and CCSD(T).
The input like:

%MEM=1000MB
%NPROC=2
%SAVE
%CHK=CO-CCSD

#P OPT=(CART,TIGHT) POP=FULL CCSD/6-311G(D,P)  Gues=Read

carbon monoxid

0 1
 C         0.000000000000      0.000000000000      0.000000000000
 O         0.000000000000      0.000000000000      1.126962524921

produced an error:

 Symbolic Z-matrix:
 Charge =  0 Multiplicity = 1
 C                     0.        0.        0. 
 O                     0.        0.        1.12696 
 Leave Link  101 at Fri Jul  5 17:23:43 2002, MaxMem=   13107200 cpu:       0.2
 (Enter /usr/local/SW/g98/l114.exe)

 NEF-NEF-NEF-NEF-NEF-NEF-NEF-NEF-NEF-NEF-NEF-NEF-NEF-NEF-NEF-NEF-NEF-NEF-
 NUMERICAL EIGENVECTOR FOLLOWING MINIMUM SEARCH
 INITIALIZATION PASS


 ************************************************
 ** ERROR IN INITNF. NUMBER OF VARIABLES (  0) **
 **   INCORRECT (SHOULD BE BETWEEN 1 AND 50)   **
 ************************************************


 Error termination via Lnk1e in /usr/local/SW/g98/l114.exe.


I was supprised that gaussian was looking for z-matrix even if I wrote
opt=cart.  I've repeated the calculation with opt=z-matrix and geometry:

 C 
 O    1   r1

 r1  =  1.126962524921

and gaussian succeed with Normal Termination. So probably I've found small
bug.


Thanks a lot in advance and best reagrds
Krzysztof


-- 
Dr. K.Radacki
Department of Chemistry
Catalysis and Advanced Materials Section
Imperial College, London

From chemistry-request@server.ccl.net Tue Jul  9 09:40:32 2002
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Date: Tue, 9 Jul 2002 15:40:31 +0200 (CEST)
From: Jan Heurich <heurich@tkm.physik.uni-karlsruhe.de>
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To: <chemistry@ccl.net>
Subject: gold basis set
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Hi everybody,

I am planning to carry out some electronic structure calculations
including gold atoms. In particular it would be great if ehty could be
carried out with a minimal basis set in the sense that the inner 68
electrons are all lumped into an ECP and only the "valence" s,p,d-shells
are treated on the level of a gaussian basis set.

The only basis set which I have found and which fulfills these
requirements has a maximum angular momentul lmax of 4 in its ECP.
However, unfortunately TURBOMOLE (which I would like to use) cannot deal with this
apparently so I wonder if there are any other basis sets for gold out
there which could do the job...?

Thanks in advance

Jan Heurich

*********************************************************************
Jan Heurich                 mail: heurich@tfp.physik.uni-karlsruhe.de
Adlerstr. 18a               Tel: ++49 (0)721/3504774  (privat)
76133 Karlsruhe             Tel: ++49 (0)721/608-6363 (Uni)

        WWW: http://www-tfp.physik.uni-karlsruhe.de/~heurich


From chemistry-request@server.ccl.net Tue Jul  9 10:35:45 2002
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Date: Tue, 9 Jul 2002 07:35:39 -0700
From: Laura Brovold <brovold@SDSC.EDU>
To: Krzysztof Radacki <K.Radacki@ic.ac.uk>
cc: CCL <chemistry@ccl.net>
Subject: Re: CCL:gaussian problems
In-Reply-To: <3D2AE185.499E2254@ic.ac.uk>
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I can answer the first one - as I had the same problem recently.

The ability to use a reduced step size is present in the program,
but the keyword is not properly connected. To use a reduced step size,
use "IOp(1/8=N)", where N has the same meaning as the N in stepsize=N.
Additionally, you should add the option "NoTrustUpdate" to the opt
keyword. So, your input should contain
"#p opt=(Redundant,CalcAll,TIGHT,notrustupdate) iop(1/8=1)"...

Cheers,
Laura

---------------------------------------------------------------------------------
Laura Gregerson (Brovold)
UCSD/SDSC MC-0505
9500 Gilman Dr.
La Jolla, CA 92093-0505
(858)531-2172  fax:
http://www.sdsc.edu/~lgregers/laura.html


On Tue, 9 Jul 2002, Krzysztof Radacki wrote:

> Dear all,
> I have two question and one information concerning gaussian.
>
> 1)
> I wanted to perform an optimization with possibly slowest  changing
> of geometry. The command line was as:
> #P OPT=(Redundant,CalcAll,StepSize=1,TIGHT) INT=(GRID=99590)
>
> I got an error:
>
>   QPERR --- A SYNTAX ERROR WAS DETECTED IN THE INPUT LINE.
>  #P OPT=(REDUNDANT,CALCALL,STEPSIZE=1,TIG
>                            '
>
> What's wrong? On p.129 of User's reference one can find description
> of StepSize in Opt and I can't see why it shouldn't work.
>
>
>
> 2)
> However calculation of IR was already sometimes discussed on CCL I
> still have uneasy feeling. An example.
> I have a molecule with trigonal bipiramide (D3h) structure. I know
> however that minimum is distorted - both axial ligands are moved out
> of Z-axis in direction of one equatorial ligand (f.e.: ax-ax angle 160)
> and the equatorial are still co-planar (C2v).
> (I hope that you can imagin it from my description).
>
> Now: If I would distorte D3h structure to C2v with ax-ax angle 175 deg
> and optimized geometry with frozen ax-ax, should IR calculation have
> a one imaginary freq. narrowing ax-ax angle or not? If it gives me no
> Imag - hwat does it mean?
>
> One can find in books that vibrational analysis should be performed
> only on stationary point - if not it's meaningless. What sense has it
> if one makes such restriction? If I want to be sure that I'm in minimum
> should I repaet all symmetry bounded calculation (like above D3h)
> with NoSymm?
>
>
>
> 3)
> Last week I wanted to calculated some quite complicated
> molecules like CO or CCH2 and various level of theory.
> Everything was fine with DFT and MP2 but the same inputs
> didn't work for CCSD and CCSD(T).
> The input like:
>
> %MEM=1000MB
> %NPROC=2
> %SAVE
> %CHK=CO-CCSD
>
> #P OPT=(CART,TIGHT) POP=FULL CCSD/6-311G(D,P)  Gues=Read
>
> carbon monoxid
>
> 0 1
>  C         0.000000000000      0.000000000000      0.000000000000
>  O         0.000000000000      0.000000000000      1.126962524921
>
> produced an error:
>
>  Symbolic Z-matrix:
>  Charge =  0 Multiplicity = 1
>  C                     0.        0.        0.
>  O                     0.        0.        1.12696
>  Leave Link  101 at Fri Jul  5 17:23:43 2002, MaxMem=   13107200 cpu:       0.2
>  (Enter /usr/local/SW/g98/l114.exe)
>
>  NEF-NEF-NEF-NEF-NEF-NEF-NEF-NEF-NEF-NEF-NEF-NEF-NEF-NEF-NEF-NEF-NEF-NEF-
>  NUMERICAL EIGENVECTOR FOLLOWING MINIMUM SEARCH
>  INITIALIZATION PASS
>
>
>  ************************************************
>  ** ERROR IN INITNF. NUMBER OF VARIABLES (  0) **
>  **   INCORRECT (SHOULD BE BETWEEN 1 AND 50)   **
>  ************************************************
>
>
>  Error termination via Lnk1e in /usr/local/SW/g98/l114.exe.
>
>
> I was supprised that gaussian was looking for z-matrix even if I wrote
> opt=cart.  I've repeated the calculation with opt=z-matrix and geometry:
>
>  C
>  O    1   r1
>
>  r1  =  1.126962524921
>
> and gaussian succeed with Normal Termination. So probably I've found small
> bug.
>
>
> Thanks a lot in advance and best reagrds
> Krzysztof
>
>
> --
> Dr. K.Radacki
> Department of Chemistry
> Catalysis and Advanced Materials Section
> Imperial College, London
>
> -= This is automatically added to each message by mailing script =-
> CHEMISTRY@ccl.net -- To Everybody  | CHEMISTRY-REQUEST@ccl.net -- To Admins
> Ftp: ftp.ccl.net  |  WWW: http://www.ccl.net/chemistry/   | Jan: jkl@ccl.net
>
>
>
>
>




From chemistry-request@server.ccl.net Tue Jul  9 11:40:25 2002
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From: Konrad Hinsen <hinsen@cnrs-orleans.fr>
To: chemistry@ccl.net
Subject: Annoucement: nMOLDYN 2.0

                       nMOLDYN 2.0
                       ===========

nMOLDYN is an interactive analysis program for Molecular Dynamics
simulations. It is especially designed for the computation and
decomposition of neutron scattering spectra, but also computes
other quantities.

The current release 2.0 of nMOLDYN can compute the following quantities:

    Quantities related to neutron scattering:
    * coherent intermediate scattering function
    * memory function for coherent scattering function
    * dynamic structure factor
    * incoherent intermediate scattering function
    * elastic incoherent structure factor

    Other quantities:
    * mean-square displacement
    * velocity autocorrelation function
    * memory function for velocity autocorrelation function
    * density of states
    * angular velocity autocorrelation function (and its spectrum)
    * reorientational correlation function

nMOLDYN has both a graphical user interface that is easy to use, and a
command-line interface for experienced users. The latter is also
appropriate for situations in which the graphical interface cannot be
used for technical reasons (network restrictions etc.)

For more information and for downloading nMOLDYN, see

    http://dirac.cnrs-orleans.fr/nMOLDYN/

-- 
-------------------------------------------------------------------------------
Konrad Hinsen                            | E-Mail: hinsen@cnrs-orleans.fr
Centre de Biophysique Moleculaire (CNRS) | Tel.: +33-2.38.25.56.24
Rue Charles Sadron                       | Fax:  +33-2.38.63.15.17
45071 Orleans Cedex 2                    | Deutsch/Esperanto/English/
France                                   | Nederlands/Francais
-------------------------------------------------------------------------------

From chemistry-request@server.ccl.net Tue Jul  9 13:10:15 2002
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Date: Tue, 09 Jul 2002 19:11:15 +0200
From: =?iso-8859-1?Q?=C1ngy=E1n=20J=E1nos?= <angyan@lctn.uhp-nancy.fr>
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Subject: Announcement: Optimally Partitioned Electric Properties - OPEP
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         ===============================================
         OPEP: Optimally Partitioned Electric Properties
         ===============================================
 
OPEP (Optimal Partitioning of Electric Properties) is a suite of 
Fortran programs, featuring a Tcl/Tk graphical user interface to
facilitate the fit of electric charges and multipoles, as well 
as models of distributed polarizabilities. It relies upon two 
alternative fitting procedures, a least-squares approach and a
statistical analysis of the distributed electric components. The
goal of OPEP is to provide compact and flexible models of distributed
multipoles and polarizabilities, that can be used in a variety of
applications, among which the design of molecular mechanical force
fields.

OPEP main functionalities include:

- handle molecular symmetry;
- allow to constrain the molecular charge, or the charge borne by
  user-defined fragments;
- automated generation  of local frames of reference for fitting 
  multipolar properties;
- models of distributed polarizabilities, including charge-flow
  polarizabilities;
- visualization of both the molecular structures and their local 
  frames of reference through an interface with XMakemol;
- automated generation of input files for Gaussian computations 
  of electrostatic potential and induction energy grids.

OPEP is a free software, distributed under the GNU General Public
License.

For more information and download, refer to:

http://www.lctn.uhp-nancy.fr/Opep/

Comments and requests for additional information can be addressed to:

mailto:opep@lctn.uhp-nancy.fr

-----------------------------------------------------------------
ÁNGYÁN János                   SRSMC  UMR 7565
Directeur de Recherche au CNRS Laboratoire de Chimie théorique
Janos.Angyan@lctn.uhp-nancy.fr BP. 239
tel: +33-(0)3.83.68.43.80      Université Henri Poincaré
fax: +33-(0)3.83.68.43.71      54506 Vandoeuvre-lès-Nancy FRANCE
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From chemistry-request@server.ccl.net Tue Jul  9 10:21:02 2002
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From: "George Hall" <georgehalli@hotmail.com>
To: chemistry@ccl.net
Subject: CHELPG
Date: Tue, 09 Jul 2002 14:20:56 +0000
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Hi everybody,

I wonder if some could point me out what are the differences between Chelpg 
charges and Mulliken.

Would you please indicate me some references or some advices about the 
aproach for these kind of charges.

Thanks a lot in advance.

George Hall.


_________________________________________________________________
Chat with friends online, try MSN Messenger: http://messenger.msn.com



From chemistry-request@server.ccl.net Tue Jul  9 15:50:44 2002
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From: "Dr. N. SUKUMAR" <nagams@rpi.edu>
Organization: Rensselaer Polytechnic Institute
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Date: Tue, 09 Jul 2002 15:50:39 EDT
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Subject: Re: CCL:CHELPG
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Mulliken charges are asigned by apportioning the electrons in the overlap
region between two atoms (two center overlap integrals) equally between the
atoms, which are then added to the net atomic populations (from the
one-center overlap integrals). Like most such schemes, it is an arbitrary
scheme for assigning charges (since "atomic charges" are not unambiguously
defined, at least outside of Bader's AIM theory).

If one wants to reproduce the electrostatic effects of the electron charge
distribution in a molecule with reasonable accuracy, without arbitrary
parametrization, one can employ either:
* a distribution of point charges (i.e. monopoles) fitted to the
electrostatic potential -- this is exactly what the CHELPG procedure does;
or
* a distribution of monopoles, dipoles, quadrupoles and higher-order
multipoles -- we have implemented this in a version of our RECON algorithm:
Whitehead, Sukumar and Breneman, submitted to J. Comp. Chem.

The original reference for CHELPG (CHarges from ELectrostatic Potentials
Grid) is:

"Determining Atom-Centered Monopoles from Molecular Electrostatic
Potentials.  The Need for High Sampling Density in Formamide Conformational
Analysis"
J. Comput. Chem., 11, 361-373 (1990) Curt M. Breneman and Kenneth B. Wiberg



Dr. N. Sukumar
http://www.drugmining.com/
Rensselaer Department of Chemistry

On Tue, 09 Jul 2002 14:20:56 +0000 "George Hall" wrote:

> 
> Hi everybody,
> 
> I wonder if some could point me out what are the differences between
> Chelpg 
> charges and Mulliken.
> 
> Would you please indicate me some references or some advices about the 
> aproach for these kind of charges.
> 
> Thanks a lot in advance.
> 
> George Hall.
> 
> 
> _________________________________________________________________
> Chat with friends online, try MSN Messenger: http://messenger.msn.com
> 
> 
> 
> -= This is automatically added to each message by mailing script =-
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> Admins
> Ftp: ftp.ccl.net  |  WWW: http://www.ccl.net/chemistry/   | Jan:
> jkl@ccl.net
> 



From chemistry-request@server.ccl.net Tue Jul  9 14:26:59 2002
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From chemistry-request@server.ccl.net Tue Jul  9 15:14:10 2002
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From: "Shobe, Dave" <dshobe@sud-chemieinc.com>
Subject: RE: CHELPG
To: "'George Hall'" <georgehalli@hotmail.com>, "'CCL'" <chemistry@ccl.net>
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Mulliken charges are assigned to atoms based on the "usage" of the atoms'
basis functions in the molecular orbitals that are calculated.  It is known
as a quick-and-dirty way of assigning charges, but one that doesn't
necessarily have any physical meaning.  Mulliken charges are notoriously
basis-set dependent.  

CHELPG charges are based on the electrostatic field generated by the
molecule.  It is a best-fit method; the set of charges produced by the
CHELPG method are the point charges that would produce an electric field
which is as similar as possible to the molecule's.  Accordingly, if you need
the charges for molecular-mechanics calculations which include electrostatic
interactions, CHELPG is arguably the best for that purpose.

There are other methods of assigning atomic charges.  GAPT charges are based
on the derivative of the molecular dipole moment WRT the atomic positions.
AIM charges are based on the division of 3-dimensional space among the atoms
in the molecule, according to a surface that has certain mathematical
properties.  NBO charges are similar to Mulliken charges, but the orbitals
are transformed into "natural" orbitals, which fixes some of the basis-set
dependency of the Mulliken method.  

--David Shobe
Süd-Chemie Inc.
phone (502) 634-7409
fax     (502) 634-7724
email  dshobe@sud-chemieinc.com

Don't bother flaming me: I'm behind a firewall.



-----Original Message-----
From: George Hall [mailto:georgehalli@hotmail.com]
Sent: Tuesday, July 09, 2002 10:21 AM
To: chemistry@ccl.net
Subject: CCL:CHELPG



Hi everybody,

I wonder if some could point me out what are the differences between Chelpg 
charges and Mulliken.

Would you please indicate me some references or some advices about the 
aproach for these kind of charges.

Thanks a lot in advance.

George Hall.


_________________________________________________________________
Chat with friends online, try MSN Messenger: http://messenger.msn.com



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From chemistry-request@server.ccl.net Tue Jul  9 16:56:17 2002
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Date: Tue, 9 Jul 2002 15:56:10 -0500 (EST)
From: Alice NgarKit Ko <ako@cse.nd.edu>
To: chemistry@ccl.net
Subject: charmm IO error
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Hi,
I generated a equil1.trj file and wanted to extract some information from
it.  But I got the following error.

eor/uio: [1010] off end of record
logical unit 11, named 'equil1.trj'
lately: reading sequential unformatted external IO
Abort

My input file is:
...
! Convert the files
open unit 11 read file name equil1.trj
open unit 1 write file name equil1A_1.dcd
merge coor firstu 11 nunit 1 skip 1 outputu 1 
begin 21000 stop 25000 sele segid A .and. resid 1:180 end

Anyone knows what that error means?  My trajectory file is about 6MB
large.  When I ran the simulation, the energy file was written out okay
and the output of charmm said normal termination.

Thanks

Alice


