From chemistry-request@server.ccl.net Tue Feb 27 19:50:28 2001
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Date: Tue, 27 Feb 2001 17:47:58 -0700
To: chemistry@ccl.net
From: Hans Martin Senn <senn@ucalgary.ca>
Subject: Re: CCL:planewawe methods
Cc: Armando Juan Navarro Vazquez <qoajnv@usc.es>


>Dear All
>Can anyone point me to reviews on Car-Parrinello and in general planewawe
>methods. I did a search on CA but wihtout too much success

These are some topical reviews on Car-Parrinello ab initio MD. The 
last one is the most comprehensive I am aware of, containing lots of 
references and touching other AIMD methods as well.

D. K. Remler, P. A. Madden, "Molecular dynamics without effective 
potentials via the Car-Parrinello approach", Mol. Phys. 1990, 70, 
921-966.

M. C. Payne, M. P. Teter, D. Allan, T. A. Arias, J. D. Joannopoulos, 
"Iterative minimizations techniques for ab initio total-energy 
calculations: molecular dynamics and conjugate gradients", Rev. Mod. 
Phys. 1992, 64, 1045-1097.

G. Kresse, J. Furthm=FCller, "Efficiency of ab-initio total energy 
calculations for metals and semiconductors using a plane-wave basis 
set", Comp. Materials Science 1996, 6, 15-50.

M. E. Tuckerman, J. P. Ungar, T. von Rosenvinge, M. L. Klein, "Ab 
Initio Molecular Dynamics Simulations", J. Phys. Chem. 1996, 100, 
12878-12887.

D. Marx, J. Hutter, "Ab initio molecular dynamics: Theory and 
implementation", in Modern Methods and Algorithms of Quantum 
Chemistry, J. Grotendorst (Ed.), NIC Series Vol. 1, Proceedings of 
the Winterschool, J=FClich (Germany), 21-25 February 2000, John von 
Neumann Institute of Computing, J=FClich, 2000, pp. 301-449.
(Available as PDF or PS at http://www.fz-juelich.de/wsqc/proceedings.html)


Cheers,

Hans
-- 
.....................................................
Dr. Hans Martin Senn            Phone  +1 403 220 3232
University of Calgary           Fax    +1 403 289 9488
Department of Chemistry         E-Mail senn@ucalgary.ca
2500 University Drive N.W.
Calgary, Alberta
Canada, T2N 1N4

From chemistry-request@server.ccl.net Tue Feb 27 23:40:56 2001
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Date: Wed, 28 Feb 2001 09:57:12 +0530 (IST)
From: Rajarshi Guha <rajarshi@presidency.com>
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To: CompuChem List <chemistry@ccl.net>
Subject: file format?
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Hi,
  I was using the software package DTMM (for windows) to draw some
molecules. After saving them I see that it uses a .mol suffix. But babel
does'nt seem able to convert them. I've been using the mol or mol2 types
Could anybody tell me what file format DTMM uses?
TIA

------------------------------------------------------------------------
Rajarshi Guha                       | Genius is pain.
Dept. of Chemistry		    |
IIT Kharagpur.                      |         -- John Lennon
		                    |
email: rajarshi@presidency.com      |
       rajarshi@cts.iitkgp.ernet.in |
web  : www.psynet.net/jijog         |
-------------------------------------------------------------------------



From chemistry-request@server.ccl.net Wed Feb 28 04:06:47 2001
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Date: Tue, 27 Feb 2001 22:34:30 +0100
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Hi CCL'ers,

One simple short question:

Can the total percentage of non-Lewis orbitals (electron density in
antibonding Lewis orbitals) in molecules (in NBO analysis) treated as
electron delocalization effect or conjugation level over all molecule ?


Best regards to all
Arturas Z.


From chemistry-request@server.ccl.net Wed Feb 28 04:31:12 2001
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From: "Tamas E. Gunda" <tamasgunda@tigris.klte.hu>
To: "Rajarshi Guha" <rajarshi@presidency.com>, <chemistry@ccl.net>
References: <Pine.LNX.4.32.0102280955230.29447-100000@cts.iitkgp.ernet.in>
Subject: Re: CCL:file format?
Date: Wed, 28 Feb 2001 10:32:50 +0100
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Dear Rajarshi,

You mean the DTMM = Desktop Molecular Modeller? I have an older version and it uses a simplified format of CSSR.
Don't be confused with the .mol suffix: a number of very different file formats uses this suffix.

Open the file with any text editor. If the beginning looks similarly like this:

                                         1.000   1.000   1.000
                       90.000  90.000  90.000
  60

  61 C       0.28000  -3.13070  -3.30400    2   6  32   0   0   0   0   0
  62 C       1.61320  -3.51880  -3.09460    1   3  33   0   0   0   0   0

then it is CSSR file. 

Hope this helps

Tamas

------------
Dr Tamas E. Gunda
Research Group for Antibiotics of the Hungarian Acad. Sci.
University of Debrecen, POBox 36
H-4010 Debrecen, Hungary
tel.: (+36-52) 512 900/2472
fax: (+36-52) 512 914
e-mail: tamasgunda@tigris.klte.hu
home-page: www.klte.hu/~gundat/gunda.htm

----- Original Message ----- 
From: Rajarshi Guha <rajarshi@presidency.com>
To: CompuChem List <chemistry@ccl.net>
Sent: Wednesday, February 28, 2001 5:27 AM
Subject: CCL:file format?


> Hi,
>   I was using the software package DTMM (for windows) to draw some
> molecules. After saving them I see that it uses a .mol suffix. But babel
> does'nt seem able to convert them. I've been using the mol or mol2 types
> Could anybody tell me what file format DTMM uses?
> TIA
> 
> ------------------------------------------------------------------------
> Rajarshi Guha                       | Genius is pain.



From chemistry-request@server.ccl.net Wed Feb 28 04:34:48 2001
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Dear CCLers

I've just encountered an extremely annoying and I think unusual error:
Yesterday I ran a GAMESS (PC-version) calculation which used ECP for Ag
via ECP=READ in $CONTRL and specifying the ECP in $ECP as
AG-ECP GEN 28 3
and the SBKJC parameters
and everything went just fine

Today I did another inputfile (added 3 more Ag:s) and now I get

          --------------
          ECP POTENTIALS
          --------------
 **** ERROR READING VARIABLE IZCORE   CHECK COLUMN 15
  1      ----- f potential    
-----                                             

....V....1....V....2....V....3....V....4....V....5....V....6....V....7....V....8

whatever I try. Any suggestions ? The IZCORE is at the same place as it
was yesterday...

/P


-- 

Dr. Patrik Johansson
Act. Lecturer
Materials Physics
Chalmers University of Technology
patrikj@fy.chalmers.se

From chemistry-request@server.ccl.net Wed Feb 28 05:54:04 2001
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On Wed, 28 Feb 2001, Tamas E. Gunda wrote:

>   You mean the DTMM = Desktop Molecular Modeller?  I have an older
>   version and it uses a simplified format of CSSR.  Don't be confused
>   with the .mol suffix: a number of very different file formats uses
>   this suffix.

That is very useful information:  babel will convert from dtmm format, 
treating it as cssr.  However, I have just tried converting an .xyz file
to .cssr format using babel, and find that dtmm will not read the resulting
file.

  Bruce

Bruce.Tattershall@newcastle.ac.uk
    Dr. B.W. Tattershall    Department of Chemistry
    University of Newcastle    Newcastle upon Tyne
    England


From chemistry-request@server.ccl.net Wed Feb 28 06:58:52 2001
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Dear CCLers

With respect to my prior email:

The ECP works if I name all atoms Ag1, Ag2 etc
and then in $ECP Ag1-ECP GEN 28 3, Ag2-ECP GEN 28 3 etc
This does however not seem in line with the manual.

Anyway, now it works & sorry for waisting time.

/Patrik

-- 

Patrik Johansson
Scientist
Materials Physics
Chalmers University of Technology
patrikj@fy.chalmers.se

From chemistry-request@server.ccl.net Wed Feb 28 05:23:23 2001
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On Wed, 28 Feb 2001, Rajarshi Guha wrote:

>   I was using the software package DTMM (for windows) to draw some
> molecules. 
> Could anybody tell me what file format DTMM uses?

The answer appears to be 'a very fussy one'.  My experience is that the
file format, while it is plain text, has to have the numbers in strictly
defined column positions.

For a modest sized molecule, it is easy to get from dtmm format by using
a text editor to hand edit the file to .xyz format, which can then be   
translated using babel or molden.  You just need a text editor which
preferably can do rectangular block copy, delete etc., i.e. is designed for
column-oriented text.

To go to dtmm format, I eventually became desperate enough to write a
program, todtmm.for, which I attach as plain text.  This reads a coordinates
file which is in relatively free format, so can easily be generated from
an .xyz file by hand editing.  This format is described in the program
comments.

My coordinates file format was originally designed for input to my
programs bangl and tangl, to tabulate bond lengths and angles, and
torsion angles, respectively.  I also attach these programs, in case
they are of any use to you.  They produce identical results to the
distance or angle tables in Gaussian output, or individual measurements
using molden (but different to Rasmol or the Chime plugin, which seem to
suffer from rounding errors).

No guarantees given!  Bangl and tangl have been in use for many years,
but todtmm is much less tested, as I have now given up using dtmm in favour
of software which can read mdl .mol files etc.

Bruce Tattershall

Bruce.Tattershall@newcastle.ac.uk
    Dr. B.W. Tattershall    Department of Chemistry
    University of Newcastle    Newcastle upon Tyne
    England


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---559023410-758783491-983355577=:6362--


From chemistry-request@server.ccl.net Wed Feb 28 08:31:25 2001
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Date: Wed, 28 Feb 2001 08:31:30 -0500
From: Dave Young<dave.young@springmail.com>
To: chemistry@ccl.net
Reply-To: dave.young@springmail.com
Subject: new book
Sender: dave.young@springmail.com
Message-ID: <Springmail.105.983367090.0.78980700@www.springmail.com>
X-Originating-IP: 209.196.125.101

Hi,

A number of CCL members have asked about the book I have been writing.  It is now in print and available from Wiley.  Here is the publisher's description.  

COMPUTATIONAL CHEMISTRY
Applying Computational Techniques to Real-World Problems

David Young, Cytoclonal Pharmaceutics, Dallas

0-471-33368-9		Pub Date: 2/16/01		416 pages		$69.95

As the field of computational chemistry continues to expand, experimental chemists are expected to know how to utilize techniques that are becoming available at the desktop level through commercial software packages. This book provides a much-needed basic guide to computational chemistry software and tools available today.  A practical, easily accessible reference for chemists, this text focuses on accurately applying computational chemistry techniques to everyday chemistry problems.  Techniques for handling problem cases, such as SCF convergence problems, are also discussed.

To order, please call (800) 225-5945 or visit http://www.amazon.com/exec/obidos/ASIN/0471333689
It is also available through Barnes & Noble (http://www.barnesandnoble.com/), which has the table of contents listed on the web.


Dave Young
dave.young@springmail.com


From chemistry-request@server.ccl.net Wed Feb 28 08:51:01 2001
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Message-ID: <3A9D0154.E52D67C3@mail.fct.unl.pt>
Date: Wed, 28 Feb 2001 13:47:00 +0000
From: "J.Aires de Sousa" <jas@mail.fct.unl.pt>
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To: CHEMISTRY@ccl.net
Subject: Java applets for neural networks
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JATOON has been developed as Java applets for training and applying
neural networks. In version 1.0 three architectures have been
implemented: Kohonen self-organizing maps, counter-propagation neural
networks, and back-propagation neural networks.

Some features of JATOON are:
        . simple and intuitive GUI
        . 'life' visualization of maps during training
        . monitoring of BPG NN training by continuous evaluation
          of a test set
        . prediction and mapping of new objects after training

I'm currently accepting proposals of projects that would use JATOON for
cheminformatics or bioinformatics applications, or for teaching neural
networks.

The authors of the selected projects will have free access to the
software. I will consider the development of adapted versions for
specific requirements of the projects.

Please contact me for more details.

-- 
Dr. Joao Aires de Sousa

e-mail:jas@mail.fct.unl.pt
www: http://www.dq.fct.unl.pt/qoa/jas/

Departamento de Quimica, Fac. Ciencias e Tecnologia,
Univ. Nova de Lisboa, 2825 - 114 Caparica, Portugal


From chemistry-request@server.ccl.net Wed Feb 28 10:02:26 2001
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Date: Wed, 28 Feb 2001 10:02:18 -0500
From: Tom Halgren <halgren@schrodinger.com>
To: Gary Breton <gbreton@berry.edu>
cc: CHEMISTRY@ccl.net, jweiser@anterio.com
Subject: Re: CCL:Question concerning Spartan molecular modeling software
In-Reply-To: <B6C15374.1328%gbreton@berry.edu>
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Hi -

The problem for axial vs. equatorial chlorocyclohexane addressed in your 
message is known and is documented in my 1999 JCC paper (T. A. Halgren,
"MMFF VII. Characterization of MMFF94, MMFF94s, and Other Widely Available
Force Fields for Conformational Energies and for Intermolecular-
Interaction Energies and Geometries), J. Comput. Chem. 1999, 20, 730-748).
In particular, Table II on p. 734 shows the axial form to be wrongly
preferred by MMFF by 0.35 kcal/mol, whereas the equatorial form should be
preferred by 0.5 kcal/mol.  In the paper, I attributed this error to the
lack of inclusion of any halocyclohexanes in the parameterization of
MMFF94.  

There are occasions in which Spartan/MMFF results are themselves
erroneous.  For example, Table I of the 1999 JCC paper by Rousseau and
Mathieu (Vol 21, p. 367) contains a number of apparent failings of MMFF94,
nearly all of which are due to its erroneous implementation in Spartan.
However, the poor result for Spartan/MMFF on chlorocyclohexane is a valid
finding.

Had I remained at Merck, there would by now be a "MMFF99" that would have
included appropriate data on conformational energies of halocycloalkanes.
Instead, that data, and much additional data on conformational energies I 
had collected for the reparameterization of MMFF, is being used in
a reparameterization and extension of OPLS-AA that Schrodinger intends to
offer this fall.  This new version, which we are calling OPLS-AA_2001,
will have a vastly broader parameterization for conformational energies
and for intermolecular interactions than does any existing force field,
including MMFF94.  At the same time. it will retain the good performance
of OPLS-AA for condensed-phase properties.

As for MMFF, my paper notes that the halocycloalkane failing is a
relatively rare one, and that other methods examined (CFF95, CVFF, CHARMm,
CHARMM in part, AMBER*, OPLS*, MM2*, and MM3*) on the whole do far worse, 
though some to correctly predict axial vs. equatorial chlorocycohexane.

					- Tom Halgren  

--------------------------------------------------------------------------
Thomas A. Halgren                              
Chief Technical Officer                    voice: 201-433-2014 x 106   
Schrodinger, Inc.                          fax:   201-433-2065
One Exchange Place, Suite 604              e-mail: halgren@schrodinger.com
Jersey City, NJ 07302                      www.schrodinger.com
--------------------------------------------------------------------------

On Tue, 27 Feb 2001, Gary Breton wrote:

> Thanks to all that responded to my question concerning the molecular
> mechanics FF in PC SpartanPro.  I received many responses that corroborated
> my finding that when utilizing MMFF94 (as contained within Spartan), the
> chlorine in chlorocyclohexane is found to be more stable in the axial
> position rather than the equatorial position (contrary to experimental
> findings, and the general rule that substituents prefer the equatorial
> position in order to eliminate 1,3-diaxial interactions present in the axial
> position).  I also received a response from Wavefunction which some of you
> may be interested in.  I have summarized the responses since a few who
> responded asked me to do so.
> 
> I should note:  I carried out the same type of calculation utilizing
> methylcyclohexane instead of chlorocyclohexane and DID obtain the expected
> result (apparently MMFF94 being parametized for this application).  Also,
> when I performed an ab initio 3-21G* calculation on the MM minimized
> structures of the axial and equatorial chair conformers of
> chlorocyclohexane, I DID obtain the expected result.  It would appear
> therefore (to this beginner) that the safest route would be to utilize
> MMFF94 to obtain starting geometries for ab initio (or maybe semi-empirical
> or DFT) energy calculations rather than to read too much into the "steric"
> energies provided by MMFF94.
> 
> Again, thanks for your help and best regards!
> 
> Gary Breton
> Berry College
> 
> ************************************************************
> 
> Wavefunction's response:
> 
> It appears like MMFF94 does not correctly predict the known energy
> difference.  My guess is MMFF94 has the Cl-H 1-4 term repulsive (positive
> energy), in
> both conformations.  In going from the axial two of the 1-4/Cl-H contacts
> are
> replaced by two 1-5 repulsive terms.  And the weight of the 1-5 contact is
> smaller than expected.  More likely the weight of the 1-4 term is too high,
> but in most 1-4
> cases the is partly canceled by a 1-4 torsion term.
>     In general the VdW parameters are the hardest to fit using mechanics
> method.
> (Usually MP2 level is considered good.)  For one, the functional form 6-12,
> 7-14-buffered, exp-6 etc. are very crude approximations.   And the
> parameterization
> depends  highly on the parametizing method.  In Halgren's MMFF94 he put
> priority on:
> 
>   1) Geometry
>   2) intra-molecular torsion term's and conformation
>   3) the near part of the VdW term (thus his buffered 7-14 VdW term).
> 
> To this effect MMFF has a very highly tuned torsional profile which does
> as good as I know for conformations on a broad range of molecules.
> (Until a recent flurry of papers describing the importance of polarization
> terms in getting good conformations which all the force fields you've
> mentioned
> have ignored.)  This heavy tuning of torsional terms has led to some
> non-optimal
> non-bonded terms.
>     Another example of this is hydrogen bonds.  While Halgren has done
> extensive work to get geometries of a large set of systems correct using
> only charges and a buffered 7-14 term, as well as some energetics for these
> systems, cases where there are strained H-Bonds fail because there
> are just not enough terms to model the correct behavior at intermediate
> distances, (where polarization dominates).
> ****************************************************
> 
> Responses from others:
> 
> 1.  To me this force field seems more oriented towards providing good
> geometries than energies. (we use MMFF geometries mostly to carry out
> single-point calculations in view of estimating formation enthalpies).
> 
> 2.  What is the experimental difference in energies?  Most force fields can
> easily be in error by a kcal or two, and assuming that the experimental
> difference is in that range all this result tells you is that the
> developers probably didn't consider that specific compound when
> developing the force field.  A useful article on what sorts of
> conformational errors to expect is JACS volume 119, pages 5908-5920
> (1997). 
> 
> 3.  in principle this is the drawback of any molecular
> mechanics method, you cannot make prediction with them, just reproduce the
> type of molecule they have been parametrised with...
> 
> 4. I performed the calculation using SYBYL.  Several force fields are
> installed on the version that I am presently using.
> 1) MMFF94 with MMFF94 charges
> equatorial conformer 1.408 kcal
> axial conformer 1.061 kcal
> This differs in detail from your result.  The author of the MMFF94
> has published a test set.  That might be worth trying
> in order to discover if Spartan has a faithful implementation
> of MMFF94.
> 2) Tripos force field without charges
> equatorial conformer 0.749 kcal
> axial conformer 0.945 kcal
> 3) Tripos force field with Gasteiger charges
> equatorial conformer 0.787 kcal
> axial conformer 1.123 kcal
> 4)I haven't had time to explore an ab initio calculation.
> In all case the energy difference is rather small.
> Can you trust a modeling calculation in this case?
> I am an experimentalist and naturally have a bias towards
> data from microwave spectroscopy, NMR spectroscopy, and electron
> diffraction.  In determining 3D structures from NMR data,
> I combine modeling calculations with experimental constraints
> that I obtain from nuclear Overhauser effect measurements.
> 
> 
> 
> 
> 
> > From: Gary Breton <gbreton@berry.edu>
> > Date: Fri, 23 Feb 2001 12:37:53 -0500
> > To: <CHEMISTRY@ccl.net>
> > Subject: CCL:Question concerning Spartan molecular modeling software
> > 
> > Hello folks,
> > 
> > I hope at least some of you have some experience with PC Spartan Pro.  I
> > recently purchased several copies of the software and began testing it with
> > some routine molecular mechanics (MMFF94) calculations.  Amazingly, when I
> > computed the energy of chlorocyclohexane with the Chlorine in the equatorial
> > position ( 1.4 kcal/mol) it was of HIGHER energy than when the Cl was axial
> > (1.1 kcal/mol).  This is contrary to experiment.  I ran the same calculation
> > utilizing CambridgeSoft's Chem3D, with Hyperchem (MM+), and MOLGEN (MM2) and
> > received the proper result (i.e., Cl prefers to be equatorial in the chair
> > conformation) and the calculated energy differences were consistent with the
> > experimental values.
> > 
> > Has anyone else observed this? is it a result of the force field? Am I doing
> > something wrong in Spartan that I am NOT doing in the other packages?  If it
> > is the force field, can I replace the parameters contained within Spartan?
> > 
> > Thanks for your help!
> > 
> > Gary W. Breton
> > Department of Chemistry
> > Berry College
> > PO Box 495016
> > Mount Berry, GA 30149
> > 
> > 
> > 
> > 
> > 
> > 
> > 
> > 
> > 
> 
> 
> 
> -= This is automatically added to each message by mailing script =-
> CHEMISTRY@ccl.net -- To Everybody  | CHEMISTRY-REQUEST@ccl.net -- To Admins
> MAILSERV@ccl.net -- HELP CHEMISTRY or HELP SEARCH
> CHEMISTRY-SEARCH@ccl.net -- archive search    |    Gopher: gopher.ccl.net 70
> Ftp: ftp.ccl.net  |  WWW: http://www.ccl.net/chemistry/   | Jan: jkl@ccl.net
> 
> 
> 
> 
> 
> 



From chemistry-request@server.ccl.net Wed Feb 28 09:25:49 2001
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Reply-To: "benny" <fengy@mail.ustc.edu.cn>
From: "benny" <fengy@mail.ustc.edu.cn>
To: <chemistry@ccl.net>
Subject: summary of large rwf spliting
Date: Wed, 28 Feb 2001 22:19:17 +0800
Organization: ustc

Dear CCL Members:
  
According your advice, I have solved the large rwf spling problem.
ere is my adding line.

%RWF=f1,2000MB,f2,2000MB,f3,2000MB

or

%RWF=f1,240MW,f2,240MW,f3,240MW

the default path is the current directory.

You may give the path, such as

%RWF=/home/lboc/tmp1/f1,2000MB,/home/lboc/tmp2/f2,2000MB

Here is the summary. thanks to everyone.

THE original problem is:

    I use Gaussian A.7 to do MP2 frequency calculation.My workstation's
configuration is 30G hard disk and 780M memory. However,when I calculate
a system with 7 heavy atoms using MP2/6-31+g**, The calcualtion will stop
with the following message: 
 
Erroneous write during file extend. write 114687 instead of 4096
Probably out of disk space.

I have split the scratch file as the following:

      %rwf=f1,2GB,f2,2GB

However,the calculation still stop after the first file(f1) exceed 2.1G,while
f2 do not contain any data. Does anyone have the similar experience and how
to deal with the problem?
Thanks a lot!
Yours

-----------------------------
REPLY from Matthias is:
in former versions of Gaussian, the memory limit in the %rwf line
_must_ be in words. I'm not sure about G98 Rel.A7.
I also used in all cases slightly less than 2 GB for each file,
as example:
%RWF=/scratch/f1.rwf,200000000,/scratch/f2.rwf,230000000,/scratch/f3.rwf,-1

Maybe this helps.

Matthias

------------------------------
REPLY from Paul is:
I had this pb some times. It seemed to me that it was a file system
limitation : they must not
exceed 2GB.... but with G98, I discovered that most of the times, I had to put
the limit well below, around
1.5GB or 1.6GB.

  Hope this helps,
Paul.


Fleurat-Lessard Paul                        | fleurat@lpct.u-bordeaux.fr   
Laboratoire de Physico Chimie Moleculaire,  | Phone: (33)(0)5 56 84 63 09
Universite Bordeaux I, 33400 Talence, FRANCE| Fax : (33)(0) 5 56 84 66 45

------------------------------
REPLY from Roy is:
You may need to add a decimal point to the numbers. I had problems with 2
and 2.0GB rwf files. Try makin the rwf files 1.8GB.

Roy Jensen

-------------------------
REPLY from Tapas is:
Check the limit of filesize using command "limit"  (in AIX), ulimit (TrueUnix).
Change it to unlimited.

Tapas Kar, Ph. D
Department of Chemistry & Biochemistry
Utah State University
Logan, UT 84322-0300

Tel: 435-797-7230
Fax: 435-797-3390
Email: tapaskar@cc.usu.edu
       tapas@risky3.chem.usu.edu

---------------------------
REPLY from Cust. is:
While formally files up to 2GB can be used there is overhead which is
makes some of this unavailable.  I find that 240MW is safe for all calculations
so

%rwf=f1,240mw,f2,240mw
#  ... MaxDisk=480mw

should get you past the 2GB limit.

  Note that MP2 frequencies cannot restrict things to the MaxDisk limit
but you will get a note on the smallest disk required. I suspect for this
case that two files will be sufficient but you should consider defining
more to be on the safe side since you have enough.  The maximum is 8 files
for about 16GB and if you shorten the file names to a single character
you will be able to fit it all on one 80 character line.

-----------------
REPLY from Prof.Curt is

Have you tried the Gaussian route card option MP2=semidirect?  I think
you need to reduce your scratch / rwf usage to get around these
limitations.  You may also have run up against an old OS limitation on
file size.

Curt Breneman
RPI Chemistry

---------------------
REPLY from Pedro is
Hi
try SCF=Direct Maxdisk=4200Mb or the maximum available

hope it helps

 Pedro Salvador Sedano             |
 Ph.D. Student                     | I'll stare the sundown
 Institut de Quimica Computacional |  until my eyes go blind...
 Universitat de Girona             |  I won't change direction
 Campus Montilivi 17071            |   and I won't change my mind.
 Girona  Spain                     |
 e-mail: perico@stark.udg.es       |
 WWW: http://stark.udg.es/~perico  |
 Telf: +34 972 418358              |


---------------------
REPLY from Thomas is
splitting th rw-file is probably without any success unless you have
some restrictions concerning the maximum filesize at your system. First
you should try the option: MP2(VeryStingy) and have a look if using
MP2(FullDirect) works. Then there are some other possible problems. See
if the MaxDisk-option in the Default.Route file is set. If you do not
find a Default.Route file then there are no MaxDisk restrictions. But as
far as my experience goes to allocate 4GB for the rw-file is very often
insufficient. If you can try %rwf=f1,20GB. Last but not least you should
see what's the size of your f1 and f2 at the error termination of your
job. If both are 2GB then you need to allocate more disk space otherwise
there is another problem.
Hope could help you


--------------
REPLY from Borislav is
I think you should try with %rwf=f1,240MW,f2,240MW. 

                                    Boris


===========================================================================

  Boris Kovacevic                       Phone: (385) (1) 4561-117
  Quantum chemistry group               Fax:   (385) (1) 4561-118
  Institut Rudjer Boskovic              e-mail: boris@spider.irb.hr
  Bijenicka 54, 10000 Zagreb            http:
  Croatia


----------------
REPLY from Thomas is
sorry I did not read the last sentences of your mail. I know this
problem. First try
%rwf=f1,2GB,f2,2GB,
The last comma is important! If that doesn't work try

%rwf=f1,230MW,f2,2GB,

But why do you split your rw-file and why don't you allocate
%rwf=f1,2GB  ???
Please tell me if you have any success.

Greetings
Thomas


-----------------



From chemistry-request@server.ccl.net Wed Feb 28 11:07:34 2001
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Date: Wed, 28 Feb 2001 21:23:09 +0530 (IST)
From: Rajarshi Guha <rajarshi@presidency.com>
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Hi,
  are there any sites on the web or any books where I could get, say the
minimum energy conformation of a molecule or the actual bond
lengths/angles etc etc.
Actually I was looking for data on cyclopropane carboxylic acid - but I
don't have much idea on where to start.

TIA

-------------------------------------------------------------------------
Rajarshi Guha                       | "My Ethicator machine must  have
Dept. of Chemistry		    |  had a built-in moral compromise
IIT Kharagpur.                      |  spectral phantasmatron! I'm
		                    |  a genius."
email: rajarshi@presidency.com      |
       rajarshi@cts.iitkgp.ernet.in |             Calvin
web  : www.psynet.net/jijog         |
-------------------------------------------------------------------------



From chemistry-request@server.ccl.net Wed Feb 28 12:06:56 2001
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Reply-To: "Hui-Hsu (Gavin) Tsai" <hxt10@po.cwru.edu>
From: "Hui-Hsu (Gavin) Tsai" <hxt19@po.cwru.edu>
To: <CHEMISTRY@ccl.net>
Subject: electron transfer theory/electronic coupling
Date: Wed, 28 Feb 2001 12:14:55 -0500


Dear CCLers:

I have one following question about electron transfer theory...

I have started to explore the electron transfer theory and did some
literature searches.

I mainly focused on electronic coupling and photoinduced systems.

My search shows that the methods (electronic coupling) span from simple
models such as expoential decay of distance, to Huckel theory, the
integration of donor and acceptor ground states, and to very complicated
integration of donor and acceptor configuration interactions. 

Because there are too many theories and models, it is very difficult to
judge which method is more reliable or flexible, which method is famous
or has been standarized,. or which method can utilize computational
software such as Gaussian98 to help the integration of electronic
coupling?

Is there any one who can share your experiences with me? comments and
suggestions are welcome and appreciated. 

Sincerely,

Gavin 



From chemistry-request@server.ccl.net Wed Feb 28 15:32:50 2001
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Date: Wed, 28 Feb 2001 21:32:48 +0100
From: Silmar Andrade do Monte <silmar@tbi.univie.ac.at>
To: chemistry@ccl.net
Subject: Reply:ET theory/Electronic coupling
Message-ID: <20010228213248.A5633@rohling>
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	Dear Gavin,

	For me it is always a pleasure to discuss about Electron Transfer.
First, ET is a dynamic process, then should be treated by time-dependente
quantum mechanics. As far as I know the easiest way to do this is by using
the Fermi's Golden rule, which is a consequence of first-order time
dependent perturbation theory. 
	In a two-state model, the first step is to identify the two
relevant states for this model, i.e, the one with charge localized on the
donor and the one with charge localized on the acceptor. These two states
are called diabatic. The matrix element responsible for the transition
between these two states is composed of a electronic coupling + terms
concerning variation of diabatic states with nuclear coordinates(reaction
coordinate). The most common electron transfer theories use the two
following assumptions: 
(i) The electronic coupling(Tab) is >> than the other therms.
(ii) Tab(Q)=Tab(Q*), i.e, the value of Tab is constant and is equal to the
one obtained for the transition state (TS). This is de Franck-Condon
factorization.
	These two points are very well explained in an excellent Review by
Patrick Bertrand(I don't have the reference now, but tomorrow i will send
it to you).
	I am not an expert in ET theory, but in my point of view the best
way to understand it is by application in simple systems. Consider the
molecule of H4+ with nuclear symmetry D2h(rectangle). The two diabatic
states are the following:

	|+  |   and  |   |+       For a reaction path with paralell
aproximation between the
	|   |        |   |

 the H2+ and H2 molecules this configuration corresponds to the TS. The
question now is how to obtain the electronic coupling. These two states are
non-orthogonal and can only be obtained by the method of localized
orbitals(of Boys for example). The expression for Tab is
		Tab = (Hab-HaaSab)/(1-S**2)
In a normal calculation with Gaussian the SCF solution is a
charge-delocalized one. This solution is called ADIABATIC and actually is a
combination of the two charge-localized solutions. In order to obtain the
charge-localized solutions it is necessary BREAKS THE SYMMETRY of the
electronic wavefunction. Actually, these two solutions have
symmetry(electronic) C2v. In practice these two solutions are only
necessary if you want to obtain the matrix elements Hab and Sab. This can
be done by the non-orthogonal CI method and the method of corresponding
orbitals of Lowdin(I can give you the references if you want).

For obtaining Tab are several levels of aproximation. In a one-electron
level 2Tab corresponds to the difference E(HOMO)-E(HOMO-1). Increasing the
accuracy you can perform a CI only with HOMO-1 -> HOMO excitation, and
finally you can include more excitations in the CI, relaxing(MCSCF) or not
the orbitals.
	The exponential decay of Tab(with distance between the two H2
molecules in the example) is a consequence of a the tunneling model, and
spite its simple character is observed in many situations. Including a
bridge between D and A often diminushes the rate of decay of Tab with
distance, and there are some rules for the best bridges.
	Finally for bigger, assymetric systems the major difficulty is to
reach the transition state, but once reached these methods can be applied
as well.

	Well, that is all for the moment and we can continue this
discussion anytime you want.
		The best regards,
							Silmar.  


From chemistry-request@server.ccl.net Wed Feb 28 19:20:55 2001
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Message-ID: <000e01c0a1e4$a5094f00$33ac0441@sttln1.wa.home.com>
From: "Mark A. Thompson" <markt158@home.com>
To: <CHEMISTRY@ccl.net>
Subject: ArgusLab 2.0 released
Date: Wed, 28 Feb 2001 16:14:55 -0800

(Apologies if you already received this)

ArgusLab 2.0 is released and freely licensed.  You can=20
download it from:

http://www.planaria-software.com

Briefly: ArgusLab is a molecular modeling program that
runs on Windows 98, NT, and 2000.  It includes several
semi-empirical methods including INDO/s for excited
states, Molecular mechanics for the entire periodic table,
and EHT for the entire periodic table.  Also, it includes
an 3D molecule builder.

Please register if you download the program.  The more
people who use it, the more we are inclined to continue
giving it away for free and to fix bugs.

Enjoy,
Mark Thompson


email:  info@planaria-software.com
web:   http://www.planaria-software.com


