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An Electronic conference for discussing recent developments in
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From ccluser@chu.chem.nthu.edu.tw  Wed Mar 26 22:32:02 1997
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Subject: H2 dissociation by UHF and DFT in G94?
To: chemistry@www.ccl.net
Date: Thu, 27 Mar 97 10:51:21 TAIST




 Dear CCL members,
          I tried to get energies of h2 (H atoms are seperated by 2 and 10
          angstrom) by UHF/6-31g**, b3lyp/6-31g** and svwn/6-31g**,
          and all are set in singlet state, then I got energies as following,
          2 angstrom,
          UHf/6-31g**    -0.9167408
          b3lyp/6-31g**  -0.9959347
          svwn/6-31g**   -0.9167408

          10 angstrom,
          UHf/6-31g**    -0.7241629
          b3lyp/6-31g**  -0.8923662
          svwn/6-31g**   -0.4588643
         I am so surprising at these results, does it mean these three 
         methods can't describe the PES of h2 dissociation exactly? and
         we can't calculate TS involving H2 formation or dissociation? 
-- 
=====================================================================
  Chiu-Ling Lin                 | E-mail: lin@chu.chem.nthu.edu.tw
  Department of chemistry       |         
  National Tsing Hua University |  Phone: 886-35-721634 
  Hsinchu, Taiwan 30043         |    Fax: 886-35-711082
=====================================================================


From noy@einstein.sc.mahidol.ac.th  Thu Mar 27 11:32:13 1997
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From: "Dr. Teerakiat Kerdcharoen" <noy@einstein.sc.mahidol.ac.th>
Message-Id: <199703280530.WAA14674@einstein.sc.mahidol.ac.th>
Subject: Getting Started with Gaussian
To: chemistry@www.ccl.net
Date: Thu, 27 Mar 1997 22:30:40 -0700 (GMT+7)
In-Reply-To: <199703261553.KAA29504@alchemy.chem.utoronto.ca> from "E. Lewars" at Mar 26, 97 10:53:03 am



>  H Y Jeong recently asked how he could get started using programs like
> Gaussian.
> 
> 1 General information on computational chemistry:
>   "Quantum Chemistry", by Ira N. Levine, 4th ed., Prentice Hall, 1991.
>   Very good introduction to QC, with problems (some answered). Chapters 15 and,
>   especially, 16 and 17 give a nice, brief overview of current computational


May I added some here. A good new book just coming out to the shelf from
Addison Wesley Longman Limited does worth your money. The title catches
your eyes easily as "Molecular Modelling: Principles and Applications".
The author is Andrew R. Leach and ISBN is 0-582-23933-9.

Teerakiat
----------------------------------------------------------------------------
Teerakiat Kerdcharoen, Ph.D.
Address:      Department of Physics, Mahidol University, Bangkok 10400
Phone:        2461381  FAX  2461381
Cellular:     01-4906089
E-mail:       noy@einstein.sc.mahidol.ac.th, noy@atc.atccu.chula.ac.th
Homepage:     http://www.sc.mahidol.ac.th/noy/       
Research:     Computer Aided Molecular Design (CAMD)
-----------------------------------------------------------------------------


From dgregory@msi.com  Thu Mar 27 12:32:12 1997
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To: chemistry@www.ccl.net
From: dgregory@msi.com (Don Gregory)
Subject: Re: CCL:How to prevent protein moving during dynamics?




Hi Yun,
If I read between your lines, my guess is that you have one very large
sphere of surrounding water, with the protein in the middle ... ?
and that when you did the SBMD the protein "diffused" to the boundary?
Realize that the boundary potential has a lower-energy-well component
in it, and that as one 'approaches' the boundary there is actually a bit of
attraction,
as there would be to numerous water molecules that the boundary is
"representing"
but then as one goes further and further into the boundary, there is a steep
repulsive component, to keep molecules inside the boundary.
So what you seeing is entierly .... understandable, if not desirable.
I would think your only two alternatives at this point, would be to artifically
restrain the protein, there are some ways one could think about doing this,
but they all have the caveat of artificiallity.  Some possibilities here might
be the use of a droplet potential, or to add in a "dummy" atom at the center
of your sphere, fix it, and put some weak distance constraints between it and
some atoms near the center of the protein.
Of course, you could also use a bigger sphere of water.
Neither of these are optimal; in any case, it sounds like "starting" over in
some manner will  likely be necessary.
Don Gregory

At 6:08 AM 3/27/97, Yun Tang wrote:
>Hi, everyone
>
>I tried to perform protein dynamics with deformable stochastic boundary
>using CHARMM program. But during the dynamics process, the protein
>gradually moved to the water sphere boundary and finally touched the
>boundary. That meant I had to do it once more.
>
>Does anyone also meet this problem and how do you deal properly with it?
>I mean how to prevent the protein moving during dynamics! Any
>suggestions are appreciated!
>
>Thanks in advance and happy holiday to everyone!
>
>Yun Tang
>
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>             Web: http://www.ccl.net/chemistry.html

Dr. Don Gregory (dgregory@msi.com)
Molecular Simulations Inc.
9685 Scranton Rd.
San Diego, CA  92121
(619) 546-5331     http://www.msi.com




From SMILLER@RARUSRAEXS1.prius.jnj.com  Thu Mar 27 14:39:29 1997
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Date: Thu, 27 Mar 1997 13:35:58 -0500
From: "Miller, Susan [PRI]" <SMILLER@RARUSRAEXS1.prius.jnj.com>
Subject: Summary of answers to QSAR question
To: "'chemistry@www.ccl.net'" <chemistry@www.ccl.net>
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Dear CCL'ers,

   Following is a summary of the replies I received to my question about
how 
long it should take to perform a QSAR analysis of 120 compounds. First
is
the original question and then come the answers. Thanks very much to all
who replied.

Dear CCL'ers'

   I am about to start doing some QSAR on a set of 120 compounds. How
long should I expect it to take to overlay all 120 compounds and adjust
their
conformations, to achieve maximal overlap? A range of times or an
approximate number of hours will make a fine answer. Thanks alot.


                                    Susan

gee, wouldn't that depend on what software and methods
you're using?

[7m[5m
 ___         _ http://ellington.pharmacy.arizona.edu/~bear  O-topo-O 
(___        |.)           bear@.pharmacy.arizona.edu    5'  :      : .*
 ___)OARING |_)EAR,    UA Pharmacy 404, Tucson 85721     |'*.    .*'| |
 Computer Modeling for Medicinal Chemistry; SAR CAMD     | | *.,* | | |
 Protein/DNA Structural Biology; Cancer Biochemistry    3',DNA helix|.*
 Pharmacognosy, Herbs, Nutrition,  Natural Dentistry       '***'  '**
[0m      

It depends on a lot of things.  If these are near analogs, where a
common
scaffold has the same numbering, a Sybyl spl (there is one called align,
or at
least I have one) will do a rough atom-to-atom alignment in a matter of
a minute
or so.  If the structures are dissimilar, a manual use (in Sybyl) of the
orient
command will give you a very rough alignment in probably 30 or 40
minutes,
depending on how good you are with the keyboard.  If you want to do
something
fancy, like alignments based on similarity of the ESP. . .this gets to
be time
consuming.  If you are also taking into account multiple conformations,
or
tweaking the alignment given a first-pass CoMFA-QSAR. . .you just have
to try
it.

I infer from your address (prius.jnj) that you are with Johnson and
Johnson.
Debbie Loughney (sp?) is well versed in Sybyl.  Have you discussed this
with
her?

Viel Vergnuegung!
Steve Bowlus

Hi there,

It depends on the machine power, qsar software, compound size, parameter
selecting .....Generally, as I am doing now for about 100 compounds(MW.
300) using a PowerMac8100 with CAChe Project leader, one month or 500
hrs
around is the common expense. Maybe I am lazy.

Any QSAR topic I am interesting in.

Yours,

Canping Pan
---------------------------------
E-mail: pan_canp@agr.kyushu-u.ac.jp
Tel: 092-611-7122(H)
       092-642-2858(O)
Fax: 092-642-2864
http://133.5.200.42/pan.html


Hi Susan,
I am afraid your question is impossible to answer considering the 
background information you supplied. None.

First you need a very well planned working strategy.
Do you now anything about the target protein. That is, do you now 
anything about the ligand-target protein interactions? 
How flexible are your compounds? You need to perform conformational 
analyses on most of them.
You must align low energy conformations from all compounds. This is 
the most crucial step in order to obtain a reliable 3D QSAR model.

Having all compounds aligned the most time consuming part is over and 
the real fun begins. 

Cheers
/jonas


My company offers two products that you may find VERY useful.  The first
is 
AMPAC, a semiempirical quantum mechanical package along with an easy to
use 
graphical user interface.  The second is CODESSA, and advanced QSAR/QSPR
program that does much of what you are currently doing manually
automatically 
when paired with AMPAC.  There are a number of reference papers in the 
literature describing the sorts of correlations that are possible, and
one of 
them (#1 below) sounds somewhat like what you want to do.  If you are 
interested and will send me your regular mail address, I'll be happy to
send 
some propaganda in the way of brochures along.  Also, perhaps we can
arrange a 
demo if you think that you might be further intrigued.  Let me know.

Best regards, Andy Holder

=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=
                    DR. ANDREW HOLDER
                         President
 
Semichem, Inc.            ||  Internet Addr: aholder@cctr.umkc.edu
7128 Summit               ||  Phone Number:  (913) 268-3271
Shawnee, KS,  66216       ||  FAX Number:    (913) 268-3445
=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=
 


Dear CCL'ers,

  You have all rightly pointed out that I did not provide sufficient
background
information for an answer to my question. I will provide it now (I
hope):

   I am doing everything manually, from the overlays to the
conformational
searches. The compounds I am aligning fall into about half a dozen 
structural categories (by my reckoning), within which there is not great
structural variation but among which there is little similarity. There
are 
large flat fused ring structures and spiro compounds, single phenyl
rings
with long aliphatic chains on either side (in some cases branched, in
others, not) and pairs and larger sets of phenyl and non-aromatic rings
connected by
aliphatic chains and other moieties.

   I hope this clarifies the earlier question somewhat. Thanks for your
replies,
both future and those already sent.


                                              Susan


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Dear Susan,

Please, post a summary with your answers. Which software are you using
to do the QSAR study?

Thanks,

Ezequiel


If you know the corresponding points then this is pretty easy. The
cheapest way is to do ensemble distance geometry. I would use the most
constrained analogue of each class. Generate 100 ensembles with that
contain the chosen member of each class. Minimize the structures. Then
see which ensembles (1) still match & how well and (2) contain mainly
low energy conformations. You will discover either that you have only
a few solutions (good) or 50 or so different solutions which will tell
you that you will never have a unique choice of conformations so you
might as well just pick one set and move on. Ensemble distance geometry
is available in DGEOM from QCPE.

Sheridan, R. P.; Nilakantan, R.; Dixon, J. S.; Venkataraghavan, R.,  J.
Med. Chem. 1986, 29, 899-906. "The Ensemble Approach to Distance
Geometry:  Application to the Nicotinic Pharmacophore".

If you don't know what atoms correspond in the different structures,
you can run a bunch of DGEOM runs to see which give solutions. Or,
you can use DISCO, an option with Sybyl.

Martin, Y. C.; Bures, M. G.; Danaher, E. A.; DeLazzer, J.; Lico, I.;
Pavlik, P. A.,  J. Comput.-Aided Mol. Design 1993, 7, 83-102. "A Fast
New Approach to Pharmacophore Mapping and its Application to
Dopaminergic and Benzodiazepine Agonists".

It shouldn't take you a month to do what you want, except that you are
apparently learning in the process with no good tutor. How do you plan
to do the QSAR? 

Yvonne Martin, Senior Project Leader
Computer Assisted Molecular Design Project
D-47E, AP10 2fl
Abbott Laboratories
100 Abbott Park Road
Abbott Park, IL 60064-3500
Phone: 847 937-5362
FAX: 847 937-2625
yvonne.c.martin@abbott.com


Susan,

For the situation you have described, I highly recommend SEAL, an
automatic
alignment program, available from QCPE for a  small fee.  Forget manual
alignments - it will take forever!  With SEAL, you can align all 120 of
your
molecules (even if you have ~20 conformations of each) in <= a few
hours.

Good luck.

Mary

/***************************
*                          *
*     Mary Bradley         *
* Senior Research Scientist*
* Rhone-Poulenc Ag Company *
*                          *
* bradleym@mindspring.com  *
*                          *
***************************/
***********************************
Mary Bradley                      *
email: mbradley@mindspring.com    *
fone & fax: (919) 572-6599        *
***********************************


Dear Suzan

I don't know what you mean by hand... Could you tell me what are the
modelling softwares available in you lab ?

I see two problems to face : Conformer generation (it seems that you
have very flexible compounds) and conformer fitting.

I would suggest you to start with the more rigid compounds, do a
conformational search (systematic, random, high temperature dynamic as
you want or as you can). Keep structures in a range of 10-20 kCal above
the minima (don't forget to investigate ring conformation).

Then make hypothesis on what would be the pharmacophore (charged atom,
hydrogen donnors or acceptors, aromatics, lipophilic groups etc...) or
any common points available in your series or reported in literature.

Then measure some key distances between these elements and try to
cluster the molecules according to these parameters (with SAS) or make
some sorts with excel to identify the common pharmacophore if you don't
have any specific softwares to do that.

Once you have identified the best clusters then you can superimpose the
best conformations.

Concerning the more flexible molecules, don't spend time to generate
conformers but simply check that you can simply superimpose one
reasonable conformation to the previously identified pharmacophore.

To my opinion, and without any additional information, you have to plan
some months to do the job.

Hope this helps

Don't hesitate to contact me for help

Francois

------------------------------------------------------------------------
--
Dr. Francois CROIZET - Riom Laboratoires CERM - Chemistry Dept. (CMC) -
ZI de la Varenne, Rue H. Goudier, BP 140 - 63203 RIOM Cedex - FRANCE -
Phone: (33) 473 33 49 70 - Fax: (33) 473 33 49 97
E-mail: f.croizet@organon.akzonobel.nl
========================================================================
==

For automated overlay of two molecule with conformational flexibility on
PC, PowerFit may be useful. You can go to our web site to download a 
fully functional program to evaluate. Currently only Windows 95 and NT 
version is available for download.

For automated overlay of two molecule with conformational flexibility on
PC, PowerFit may be useful. You can go to our web site to download a 
fully functional program to evaluate. Currently only Windows 95 and NT 
version is available for download.


Ms. (Dr.?) Miller:

For the past few days, I have been following with interest
your postings to the CCL concerning QSAR.  (BTW, I haven't
seen (most of) the responses to you show up in my mail, so I'm 
assuming they're going directly to you.)  Since I do molecular
modeling and algorithm design, I haven't felt competent to
comment on your questions.  After your last posting, however,
I feel compelled to register extreme surprise (and to stick
my nose in where it doesn't belong :-).

Why, pray tell, would your mentor even suggest doing _all_
of the overlays by hand???  There is certainly value to
doing a small, random set of overlays by hand, just to
confirm that the results make sense.  However, if you're
needing to do anything more than a couple of handfuls of
compounds, noninteractive fitting seems the only way to
go.  Otherwise, you end up wasting enormous amounts of
human time doing things a mindless computer was invented
for.  On the other hand, if you're using Tripos software,
I guess noninteractive isn't really a choice anyways?

Ah well, good luck with your project.  I hope you're able
to finish in something approximating a reasonable amount
of time.

Sorry for butting into the middle of your more substantive
discussion with people who actually do QSAR...

Marti Head



%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%

Martha S. Head, Ph.D. (Marti)
Center for Advanced Research in Biotechnology
9600 Gudelsky Drive
Rockville MD 20850
voice: (301)738-6104
email: mhead@indigo18.carb.nist.gov

%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%

Hi all,

  Thanks again for all of your responses. I will post a summary in a
couple
of days when the discussion is over. All of the responses I've received
so
far have come to CCL and not to my personal mailbox, but if it is
desired,
I can still post a compilation of the responses.

  I forgot to mention 2 very important facts:

   1) I am using SYBYL and have no access to anything else, save the
       free software on the net. I cannot use that however, for the
second 
       reason.

   2) My mentor insists that I do the overlays by hand, that is, by
using
       the fit module in SYBYL and picking points, with the mouse, to
fit.
       I must also do torsion adjustments by hand, that is, by choosing
       a torsion angle for each bond and applying it, using either the
twist
       widget in the upper left corner of the screen or the modify
torsion
       command.  


                                           Susan


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Susan,
The superimposition procedure is performed due to that the 3D 
structure of the target protein is not known. You seek atoms or 
mutual points on your ligands that are most likely to interact with 
target protein. However, very often your fits will be much better if 
you also allow extension vectors to act as a fit point. For example, 
a basic nitrogen may interact through its lone pair of electrons or, 
if it is protonated, through the proton. Therefore, if you apply 
extension vectors in the direction of the lone pair of electrons 
, and use this vector as a fit point, much more reliable fits will 
occur. You use a UNIX machine and I suggest that you use Apollo or a 
similar program for this. Even SYBYL has a module.

Your mentor does not allow you to perform conformational searches on 
your ligands? Then why bother at all. This is, one of the most 
crucial steps in 3D QSAR, especially if your ligands are flexible.
In SYBYL I suggest you to use the random search procedure!

The conformational search and the alignment proecedures are tedious 
and cost a lot of time, but must be performed rationally and 
thoroughly.

Succes
/jonas


++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
Jonas Nilsson                e-mail: j.nilsson@farm.rug.nl
Univ. Centre for Pharmacy       tel: +31(0)503633302
Dept. of Med. Chemistry         fax: +31(0)503636908
Antonius Deusinglaan 1
NL-9713 AV Groningen
The Netherlands
http://pc131.farm.rug.nl/main.htm
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++


(In reply to your message dated Tuesday 11, March 1997)

-- 
Something of interest for QSAR work.
Accord for Excel can be used for structure relationships and Activities.

Check out 

WWW.synopsys.co.uk


   Take care, all.

                                         Susan



From jtgolab@amoco.com  Thu Mar 27 18:32:13 1997
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From: jtgolab@amoco.com (Joe Golab)
Date: Thu, 27 Mar 1997 16:44:42 -0600
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To: CHEMISTRY@www.ccl.net
Subject: Summary of responses to "CCL: IRIX 6.2+ and MSC's XMOL"
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3/27/97

RE: Summary of responses to "CCL: IRIX 6.2+ and MSC's XMOL"

>-- Original Question

>! Dear CCL:
>!
>! Recently, we upgraded our Silicon Graphics equipment to IRIX 6.2.  After
>! that, Xmol stopped working (% xmol - Exec format error) because Xmol uses
>! the COFF binary format.  According to Xmol's creators (Minnesota's SC),
>! "There are not plans to produce a new XMol distribution".
>!
>! We have been looking for an alternative to Xmol.  So far, we haven't had
>! much luck to duplicate Xmol's "Extras/Animate" feature.  We have found that
>! feature very useful when looking at optimization runs, IRC runs, etc.  The
>! animation button basically reads and displays a series of geometries from an
>! Xmol input file.
>!
>! Can anyone suggest an alternative software product for UNIX machines?
>! We have tried Rasmol and have not had any luck getting it to do animation
>! using a series of separate geometries.  (Which should not be taken as a slam
>! to Rasmol which we have found useful for Web presentations.)
>!
>! If any replies are received, I'll post the summary.  Thank you.
>!
>! --
>!
>! :Joe
>!  jtgolab@amoco.com
>!  (630) 961-7878  <SOCON 231 7878>


>-- Executive Summary

 1) Source Code to Xmol is not available (to the best of my knowledge).  It
    was only distributed via executable code.  I (for one) wish one of the
    commerical software vendors would investigate the possibility of
    distributing a working copy of Xmol.  As far as I know, MSC has no plans
    for it beyond what is on their web site now.
    (Hint, Hint, Knudge, Knudge, Wink, Wink - Know what I mean?)

 2) Suggested Replacements
    a) VMD      - http://www.ks.uiuc.edu/Research/vmd/
    b) MOLDEN   - http://www.caos.kun.nl/~schaft/molden/molden.html
    c) Chime    - http://www.mdli.com/chemscape
    d) gOpenMol - http://laaksonen.csc.fi/gopenmol/gopenmol.htmls


>-- Response

*> Hi again Joe.  I don't use Xmol, but would the MOLDEN program do what
*> you need?  I use it to visualize geometry optimizations, vibrational
*> frequencies, and orbitals from Gaussian and sometimes GAMESS.  It's
*> free and has a web page:
*> http://www.caos.kun.nl/~schaft/molden/molden.html
*>
*> Good luck!
*>
*> ----------------------------------------------
*> Dr. Karl K. Irikura
*> Physical and Chemical Properties Division
*> National Institute of Standards and Technology
*> Gaithersburg, MD  20899
*> voice: 301-975-2510	fax: 301-975-3670
*> e-mail: karl.irikura@nist.gov
*> ----------------------------------------------

>-- Response

*> try using Chime as a plugin of a web page. It allows animations.
*> You only will have to set up a web page to do the embedding.
*>
*> Chemscape Chime is free downloadable from http://www.mdli.com/chemscape
*>
*> Rene P.F. Kanters
*> Chemistry Project Specialist
*> Chemistry Department
*> University of Richmond VA 23173
*>
*> phone: (804) 287-6873
*> email: rkanters@richmond.edu
*> www:   http://www.richmond.edu/~rkanters
*>        http://www.science.richmond.edu/~kanters

>-- Response

*> You might want to try VMD, just released to the public on Mar 25. It's
*> homepage is http://www.ks.uiuc.edu/Research/vmd/
*>
*> David E. Reichert, Ph.D.
*> Mallinckrodt Inst. of Radiology
*> Div. Radiation Sciences
*> phone: (314)362-8461
*> fax: (314)362-9940
*> e-mail: reichertd@mirlink.wustl.edu

>-- Response

*> I use vmd to display dynamics (results from MD and normal modes).
*> I think vmd can use Xmol's xyz files, however I never tried that.
*> Instead, I wrote a little program that generates dcd files that
*> vmd can read. You are welcome to have it, if you want.
*> I found that vmd makes very fast and very pretty animation.
*> I you don't know where to find vmd on the net, I cal dig it up for you.
*>
*> Hope that helps,   Gert
*>
*> Gert von Helden
*> Dept. of molecular and Laser Physics, University of Nijmegen, Netherlands
*> e-mail: gertvh@sci.kun.nl, phone: (+31) 24 3652179, fax: (+31) 24 3653311

>-- Response

*> Did you tried the molden software ?
*> I use it on IRIX6.2 but you should have gaussian output.
*> Is it your case
*>
*> Dorothee Berthomieu
*> **************************************************
*> Laboratoire des Materiaux et Procedes Membranaires
*> UMR CNRS 5635
*> Ecole Nationale Superieure de Chimie de Montpellier
*> 8, rue de l'Ecole Normale
*> 34296 MONTPELLIER cedex 5
*> Tel : (33) 467 14 43 40
*> Telecopie :   (33) 467 14 43 47
*> email : bertho@crit1.univ-montp2.fr
*> http://www.dr13.cnrs.fr/lmpm/fequ.html#DEPOCVD

>-- Response

*> Have you tried MolDen?  It can read various file types (e.g. Gaussian
*> output) and animate things like structures and vibrational modes.
*>
*> Nick
*>
*> ============================================================================
*>   Nicholas A. Nystrom, Ph.D.              Pittsburgh Supercomputing Center
*>   Scientific Specialist                   Mellon Institute Building
*>   email: nystrom@psc.edu                  4400 Fifth Avenue
*>   voice: +1 412-268-1592 fax: -5832       Pittsburgh, PA  15213    USA
*> ============================================================================

>-- Response

*>         Can't you get the xmol source code? All you should
*>   need to do is to rebuild the executable. If the program
*>   is being distributed form an academic center, I would
*>   be surprised if they would not hand out the source.
*>
*>        Good luck,
*>
*>        Randy
*>
*> All opinions expressed here are mine, not my employer's
*>
*> /////////////////////////////////////////////////////////////////////////
*> \\ Randy J. Zauhar, PhD             | E-mail: zauhar@tripos.com        //
*> \\ Tripos, Inc.                     |       : zauhar@fastrans.net      //
*> \\ 1699 S. Hanley Rd., Suite 303    |  Phone: (314) 647-1099 Ext. 3382 //
*> \\ St. Louis, MO 63144              |                                  //
*> /////////////////////////////////////////////////////////////////////////
*> **                                                                     **
*> **  "If you have conceptions of things that you can have no conception **
*> **   of, then the conception and the thing appear to co-incide."       **
*> **   --- C.G. Jung                                                     **
*> *************************************************************************

>-- Response

*> Joe, I assume the source for XMol was never distributed?  Does anybody own
*> it currently?  If they're not going to make a new distribution, what's
*> happening to the program?
*>
*> All that's required is a recompile on an appropriate SGI...
*>
*> Joe
*>
*> --
*>
*> Joe Leonard                       Phone: +1 314 647 8837 x3204
*> Tripos, Inc.                      Fax:   +1 314 647 9241
*> 1699 S. Hanley Rd.                email: jle@tripos.com
*> St. Louis, MO 63144 USA           after-hours: jle@world.std.com

>-- Response

*> We went through exactly the same process. We're presently using the package
*> VMD. You can obtain a copy via http://www.ks.uiuc.edu/Research/vmd/ . It can
*> read in multi-frame XYZ files. Might be worth a try....
*>
*> Regards,
*> Mike
*>
*> -------------------------------------------------------------------
*> |    Mike Fearn,              Tel : UK (01684) 896536             |
*> |    Room PA101,	      Fax : UK (01684) 896150             |
*> |    D.R.A, Malvern,                                              |
*> |    Worcs. WR14 3PS          Email : hp003@dra.hmg.gb            |
*> -------------------------------------------------------------------

>-- Response

*> There are certainly a lot of options. Let me suggest one further:
*>
*> The gOpenMol program at:
*>
*> http://laaksonen.csc.fi/gopenmol/gopenmol.htmls
*>
*> Regards,
*>
*> -leif laaksonen
*>
*> -------------------------------------------------------------------
*> Leif Laaksonen                     |
*> Center for Scientific Computing    | Phone:      358 9 4572378
*> P.O. Box 405                       | Mobile:     358 400425203
*> FIN-02101 Espoo                    | Telefax:    358 9 4572302
*> FINLAND                            | Mail:  Leif.Laaksonen@csc.fi
*> -------- URL: http://laaksonen.csc.fi/leif.laaksonen.html ---------

>-- Response

*>    This seems to be a common question lately as more and more
*> people upgrade to 6.x .  You might want to look at our visualization
*> program, VMD, at http://www.ks.uiuc.edu/Research/vmd/ .  It was
*> developed for, amoung other things, the visualization of MD
*> trajectories.
*>
*>   I doesn't read XYZ files directly, but if you have Babel
*> installed (http://mercury.aichem.arizona.edu/babel.html) it VMD
*> will call it and to the conversion to a set of PDB files automatically,
*> then read them in.  To the user, you wouldn't even notice the exchange.
*>
*> 						Andrew
*> 						dalke@ks.uiuc.edu

-- 

:Joe
 jtgolab@amoco.com
 (630) 961-7878  <SOCON 231 7878>

 +----------------------------------------------------+
 | Profanity - the one language all programmers know. |
 | After all, why do you think they call it a cursor? |
 +----------------------------------------------------+


From ccl@www.ccl.net  Sun Mar 30 07:32:47 1997
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http://www.geocities.com/Tokyo/5243/index.htm (frames)
http://www.geocities.com/Tokyo/5243home_en.htm (no frames - english)
http://www.geocities.com/Tokyo/5243home_de.htm (no frames - german)

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Tel. +49 931 701814


From schiffer@h1tw0036.hoechst.com  Fri Apr  4 02:33:53 1997
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From: "Dr. Heinz Schiffer" <schiffer@h1tw0036.hoechst.com>
Organization: Hoechst Corporate Research & Technology
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To: "M.Govender" <GOVENDEM@che.und.ac.za>,
        Computational Chemistry List <chemistry@www.ccl.net>
Subject: Re: CCL:Temperature Calculations
References: <B4B0414C43@che.und.ac.za>
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M.Govender wrote:
> 
> Dear Netters,
> 
> I am interested in obtaining Rotational and Vibrational
> temperature calculations on spherical top molecules. Can anyone
> provide any info as to what programs are available?...
> 
> Many Thanks
> Magan

Hi Magan,

Look at Donald A. McQuarrie, Statistical Mechanics, Harper & Row 1976.
All the relevant formulars are there. The vibrational temperature
of the normal frequency nu_j is 

	Theta_nu_j = h * nu_j / k
 
The rotational temperatures of a general polyatomic molecule are :

	Theta_A = A / k
	Theta_B = B / k
	Theta_C = C / k

A, B, and C are the rotational constants in Joule. Normally they
are given in cm**(-1), that is as A_quer = A / ( h * c ). A, B, and
C are defined as 

	A = h**2 / ( 8 * pi**2 * I_A )
	B = h**2 / ( 8 * pi**2 * I_B )
	C = h**2 / ( 8 * pi**2 * I_C )

I_A, I_B, and I_C are the principle moments of inertia. You can get 
them by diagonalizing the moments of inertia tensor. The formalas in
the McQuarrie book on page 134 are wrong : I_xy is missing a negative
sign : I_xy = - sum_j .... and in the formulas for A_quer, B_quer, and
C_quer the pi should be squared, see above.

Ciao,
Heinz	
-- 
Dr. Heinz Schiffer		Phone   ++49-69-305-2330
Hoechst CR&T			Fax     ++49-69-305-81162
Scientific Computing, G864	Email   schiffer@h1tw0036.hoechst.com
65926 Frankfurt am Main		        schiffer@msmwia.hoechst.com

From ccl@www.ccl.net  Mon Mar 31 11:33:02 1997
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To: chemistry@ccl.net
From: William Welsh <wwelsh@jinx.umsl.edu>
Subject: band structures in 3D




Dear Netters,

Can someone point me to programs available for calculating electronic band
structures in 1-, 2-, and 3- dimensions?  I remember a few years back that a
program known as VEH (Valence Effective Hamiltonian) was capable of doing
this, but there may be others (or updated versions of VEH).  I would be
interested in both semi-empirical and ab initio programs.

Thanks ... Prof. Bill Welsh
Dept. of Chemistry
University of Missouri-St. Louis



From macrae@rikaxp.riken.go.jp  Mon Mar 31 21:33:06 1997
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Date: Tue, 01 Apr 1997 11:11:45 JST
From: "R. M. Macrae" <macrae@rikaxp.riken.go.jp>
To: CHEMISTRY@www.ccl.net
Message-ID: <009B2215.F2A511D3.52@rikaxp.riken.go.jp>
Subject: degenerate open shells





Dear CCL subscribers

Looking in the archive I saw some discussion from some considerable
time back (around 1993) on the topic of G92 calculations on linear 
systems with x,y degenerate open shells, the point being that UHF
gives the wrong result apparently even if nonstandard guess orbitals
are used. (In some other programs apparently one can generate 
fractional occupancies with equally populated x and y components 
and this constraint will be retained throughout the calculation.)
ROHF, on the other hand, will not of course give correct
spin-dependent properties. There didn't seem to be a satisfactory 
outcome to this discussion at the time (unless, of course, i missed it). 

My question is, then: is there a satisfactory solution or workaround
to this problem either in G92 or G94?

Sincerely

Rod

* Rod Macrae  * Muon Science Laboratory * macrae@rikaxp.riken.go.jp *


From keruu@ifm.liu.se  Tue Apr  1 11:33:15 1997
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Date: Tue, 1 Apr 1997 18:13:04 +0200
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To: chemistry@www.ccl.net
Subject: Release of free quantum chemistry program: Dalton
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Content-MD5: 3Wwb5CD0UIR4duQfew8kFA==





                          ANNOUNCEMENT


We are happy to announce the release of the Dalton quantum chemistry
program, Release 1.0 (1997) to the computational chemistry/physics
community. Dalton is a complete, powerful quantum chemistry program
for the calculation of molecular properties with SCF, MP2 or MCSCF
wave functions. The  strengths of the program are mainly in the areas
of magnetic and (frequency-dependent) electric properties, and for
studies of molecular potential energy surfaces, both for static and
dynamical investigations, as well as stable algorithms for converging
large MCSCF wave functions (also excited states).

The program is distributed freely to all academic users, although we
require all users to sign a copyright and license agreement.


For more complete information on how to obtain a copy of the program,
more information about what the program can and can not do, please
check out our homepage at
http://www.kjemi.uio.no/software/dalton/dalton.html, or send an e-mail
to dalton-admin@kjemi.uio.no.



The complete author list of the program is:  

T.Helgaker, H.J.Aa.Jensen, P.Joergensen, J.Olsen, K.Ruud, H.AAgren,
T.Andersen, K.L.Bak, V.Bakken, O.Christiansen, P.Dahle, E.K.Dalskov,
T.Enevoldsen, B.Fernandez, H.Heiberg, H.Hettema, D.Jonsson,
S.Kirpekar, R.Kobayashi, H.Koch, K.V.Mikkelsen, P.Norman, M.J.Packer,
T.Saue, P.R.Taylor, and O.Vahtras



On behalf of the authors,


Kenneth
_______________________________________________________________________________
Kenneth Ruud, Ph.D.-student in Chemical Physics at the Department of Chemistry,
University of Oslo, Norway.         E-mail: kenneth.ruud@kjemi.uio.no

I don't know what the computer language of the year 2000 will look like, but
I know it will be called FORTRAN.
_______________________________________________________________________________




From ccl@www.ccl.net  Thu Apr  3 12:33:42 1997
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From: Leonardo Demaria <demaria@sissa.it>
Message-Id: <199704031726.TAA31876@shannon.sissa.it>
Subject: STO two-center overlap integrals.
To: chemistry@ccl.net
Date: Thu, 3 Apr 1997 19:26:10 +22310718 (MET_DST)
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Hi everybody, 
	
	I need to calculate STO two-center overlap integrals between s and
p type orbitals for general n. Does any one know about a Fortran 77
subroutine that does this task?

	I thank you all in advance.

			Best regards,

				Leonardo De Maria


From John_Beckerle@quickmail.clemson.edu  Thu Apr  3 12:33:49 1997
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Date: 3 Apr 1997 12:23:29 -0500
From: "John Beckerle" <John_Beckerle@quickmail.clemson.edu>
Subject: "Best" Multiprocessor Platf
To: "List CCL" <CHEMISTRY@www.ccl.net>
X-Mailer: Mail*Link SMTP-QM 3.0.2




We are seriously considering investing in a multiprocessor compute server.
The candidates include the IBM SP2, SGI Origin2000, Sun Ultra HPC, DEC
Alphaserver and other similar machines.  We are probably looking at something
on the order of 8 processors and 2GB of memory, although expandability and
upgradability are important.  The system is supposed to serve a variety of
engineering and scientific high performance computing needs, not just
computational chemistry.

I would like to poll the collective experience of CCL as to what is the best
platform, and even more importantly, which platforms should be avoided for
computational chemistry applications.  I am interested in hearing about real
experience with software availability, incompatibilities, and performance
surprises (including effective use of parallelism), both good and bad.  We are
interested in the full range of computational chemistry applications including
SCF and MD. 

I would like to stress that I am looking for good and bad experiences with
effectively using any of these multiprocessor machines and the roadblocks
others have encountered.  I am not so interested in relatively minor
differences in performance of the individual CPUs, benchmarks, etc.  I want to
know if they can be used effectively without miracles.

I am already familiar with the extensive evaluation of workstation performance
by Martyn Guest, as well as Milan Hodoscek's comparison for parallel MD
speedups.

As I don't subscribe to CCL at this time, please respond directly to:
beckerj@clemson.edu

I will summarize to the list if their is interest.

John Beckerle
Clemson University
beckerj@clemson.edu





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Date: Thu, 3 Apr 1997 16:23:24 -0500
To: CHEMISTRY@ccl.net
Subject: Comp. Chem. Reception at ACS in San Francisco
Cc: chaka@lubrizol.com






                  RECEPTION ANNOUNCEMENT

INDUSTRIAL APPLICATIONS OF COMPUTATIONAL CHEMISTRY RECEPTION 

    American Chemical Society Meeting in San Francisco

                Sunday evening, 6 - 9 pm
                    April 13, 1997
                      ANA Hotel
                 Metropolitan I Suite

      "Bring Your Unsolved Problems to the Experts"


At the reception there will be an opportunity to informally present a 
poster and/or 2 minute oral presentation about an unsolved problem
you wish to discuss with your colleagues.  Then mingle with the experts
from industry and academia and enjoy the refreshments!


***********************************************************************
            RECEPTION AND SYMPOSIUM ARE SPONSORED BY

                      IBM CORPORATION

                 MOLECULAR SIMULATIONS, INC.
***********************************************************************

For more information, please contact the organizers:

Anne Chaka                   Rick Ross
The Lubrizol Corp.           PPG Industries
chaka@lubrizol.com           rbross@ppg.com
216-943-1200 x2027           412-492-5359


************SYMPOSIUM TECHNICAL PROGRAM************************

The Symposium on Industrial Applications of Computational Chemistry in the Computers 
in Chemistry Division comprises seven sessions from Sunday morning, April 13, through 
Wedensday morning, April 16.   The sessions are as follows:
       Materials Properties
       Polymers
       Catalysis
       Automotive, Coatings, and the Petroleum Industry
       Molecular Properties
       Process Simulation
       Solvation and Surfactants




Sunday Morning
       Industrial Applications of Computational Chemistry:  Materials Properties
       Moscone Center Room 123, Exhibit Level

       9:00--22. Computational materials science applications at the Hughes Research 
Laboratories. M. F.
       Gyure, R. N. Schwartz .  Hughes Research Labs
       9:30--23. Glass-densification under 193-nm laser exposure:Experiment and theory. D. 
C. Allan, C.
       Smith, N. F. Borrelli, T. P. Seward III .  Corning Incorporated
       10:00--24. Industrial applications of polymorph prediction. F. J. Leusen 
       10:30--25. Local density-functional theory study of paramagnetic ion-doped BaLiF3 
for information
       storage applications. F. Tsobnang, I. Lado, A. Le Mhaut, J. C. Fayet .  Universite du 
Maine
       11:00--26. Industrial applications of computational materials science:Current status and 
future directions.
       S. J. Mumby .  Molecular Simulations
       11:30--27. A framework for approaching industrial problems by molecular simulation. 
J. M. Newsam.  Molecular Simulations

       Sunday Afternoon
       Industrial Applications of Computational Chemistry:  Polymers
       Moscone Center Room 123, Exhibit Level

       1:30--48. Molecular modeling of polymers. S. H. Jacobson.  Hoechst Celanese
       2:00--49. Applications of molecular dynamics to the study of thermal degradation in 
polymers. M. R.
       Nyden. NIST
       2:30--50. Prediction of stress-strain curves of semicrystalline polymers with rubbery 
amorphous phase. J.
       Bicerano, N. Grant, J. Seitz, K. Pant, Dow Chemical
       3:00--51. Physical properties of PEN by amorphous cell simulation. J. M. O'Reilly, 
D. R. Perchak.  Eastman Kodak.
       3:30--52. Acyl and alkyl attack in the imidization reaction of poly(methyl methacrylate) 
(PMMA):A
       computational study. S. Fitzwater.  Rohm and Haas 
       4:00--53. Rational design of next generation polycarbonates. C. W. Ulmer II, D. A. 
Smith, N. Teich,
       K. Miaskiewicz, P. Nagy, B. G. Sumpter, D. W. Noid.  The DAS Group
       4:30--54. Density functional study of initiators for polymerization of -caprolactones. 
P. W-C. Kung,
       N. Tanpipat, J. Andzelm.  Molecular Simulations

Sunday Evening Reception 6:00-9:00 pm
Industrial Applications of Computational Chemistry Reception
RBring Your Unsolved or Almost Solved Problems to the ExpertsS
Optional Informal Poster and/or 2 minute oral presentation for your topic, then mingle with 
the experts and enjoy the refreshments


       Monday Morning
       Industrial Applications of Computational Chemistry:  Catalysis
       Moscone Center Room 120, Exhibit Level

       9:00--65. A computational study of the nature of Ti(IV) active sites in mesoporous 
titanosilicate catalysts.
       P. E. Sinclair, C. R. A. Catlow, G. Sankar, J. M. Thomas, T. Maschmeyer.  The 
Royal Institution of Great Britain.
       9:30--66. Activation of carbon-hydrogen bonds at transition-metal surfaces. S. 
Clemendot, C. Guerra,
       Z. Liu, J. Harris 
       10:00--67. Modeling of homogeneous catalysis by density-functional molecular 
dynamics. P. M. Margl,
       T. K. Woo, L. Deng, T. Ziegler, P. E. Bl&umlochl 
       10:30--68. Combined quantum mechanical/molecular mechanics (QM/MM) studies of 
homogeneous
       catalysis: Static and ab initio molecular dynamics investigations. T. K. Woo, P. M. 
Margl, L. Deng, T.
       Ziegler 
       11:00--69. Catalysts and sorbents:Industrial modeling applications and opportunities. 
C. M. Freeman,
       A. M. Gorman, C. M. K&umlolmel 
       11:30--70. New reactors based on heat-tense catalytic surfaces. V. I. Anikeev, N. A. 
Kuzin, A. V.
       Gudkov 

       Monday Afternoon
       Industrial Applications of Computational Chemistry:  Automotive, Coatings, and 
Petroleum
       Moscone Center Room 130, Exhibit Level

       1:30--104. Universal behavior in adhesion. J. R. Smith 
       2:00--105. Theoretical results on the mechanism of catalytic NO decomposition over 
Cu zeolites. W. F.
       Schneider, K. C. Hass, R. Ramprasad, J. B. Adams 
       2:30--106. Computational studies of the photochemistry of benzotriazole UV 
stabilizers. K. C. Hass,
       W. F. Schneider, C. M. Estevez, R. D. Bach 
       3:00--107. Theoretical study of the reaction of the chlorine atom with hydrocarbons. 
A. M. Chaka 
       3:30--108. Computational chemistry applications in an industrial coatings research 
laboratory. R. B.
       Ross 
       4:00--109. A joint QSAR project between LZ and Purdue University employing neural 
networks and first
       principles modeling. D. T. Daly, A. M. Chaka, V. Venkatasubramanian, A. 
Sundarum, J. Carruthers 
       4:30--110. Thermodynamical study of factors influencing polysulfides C-S and S-S 
bonds heterolytic scissions,  Presulfiding agents  for the oil refinery industry.
 J. Joffre, C. Moreau, J. C. Duchet, J. Leglise 

       Tuesday Morning
       Industrial Applications of Computational Chemistry:  Molecular Properties
       Moscone Center Room 130, Exhibit Level

       9:00--144. High-performance electronic structure methods: Practicable techniques. G. 
Fitzgerald 
       9:45--145. Accurate thermochemistry:The parameterized multireference perturbation 
PMPx approach. M.
       Dupuis, K. Hirao, M. Yamanishi 
       10:15--146. Theoretical insight into the scaling of third-order nonlinear optical 
properties for polyenes and
       cyanines. B. M. Pierce 
       10:45--147. Binding energy calculations of HIV-2 protease inhibitors. P. H. Lee, G. 
M. Maggiora, W.
       J. Howe, K. W. Watenpaugh, P. K. Tomich, B. Honig 
       11:15--148. Experimental and theoretical studies of LED-compatible fluorogenic K+ 
sensing molecules.
       S-H. Chou, J. G. Bentsen, E. M. Cross, C. C. Nagel, J. E. Trend 

       Tuesday Afternoon
       Industrial Applications of Computational Chemistry:  Process Simulation
       Moscone Center Room 110, Exhibit Level

       2:00--173. Industrial applications of modeling. N. Quirke 
       2:45--174. Making better technical business decisions with chemistry modeling. J. T. 
Golab, M. R.
       Green 
       3:15--175. Calculating chemical reaction equilibria using the reaction ensemble 
method. W. R. Smith, I.
       Nezbeda, M. Strnad 
       3:45--176. Kinetic parameters for hydrocarbon conversion reactions. J. K. Perry, W. 
A. Goddard III,
       A. Patel, N. Reynolds, J. Shinn, R. Frazier 
       4:15--177. Kinetic theory of transport in molecular sieve catalysts. S. M. Auerbach 
       4:45--178. Mathematical modeling of gas-phase catalytic copolymerization of 
propylene with ethylene in a
       system with two reactors. V. I. Anikeev 

       Wednesday Morning
       Industrial Applications of Computational Chemistry:  Solvation and Surfactants
       Moscone Center Room 110, Exhibit Level

       9:00--296. Mesoscale dynamics of polymer surfactant solutions. J. G. E. M Fraaije, 
B. A. C. van
       Vlimmeren, N. M. Maurits 
       9:30--297. Correlation modeling of surfactants and surface active molecules in 
solution. M. J. Doyle, D.
       Rogers 
       10:00--298. Direct methods for calculating lipophilicity:Application to industrial 
chemicals. S. A. Best, K.
       M. Merz Jr., C. H. Reynolds 
       10:30--299. Molecular modeling studies of solvent solubility parameters and their 
components. D. Rigby

       11:00--300. Parameterization and validation of atomic nonbonded parameters. H. Sun 
       11:30--301. Materials modeling on the corporate intranet. J. D. Honeycutt 




From CHZLIN@usthk.ust.hk  Fri Apr  4 03:33:54 1997
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 04 Apr 1997 15:12:28 +0800
Date: Fri, 04 Apr 1997 15:12:28 +0800
Subject: Seeking assistance
To: chemistry@www.ccl.net
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Dear Colleagues,

We did MP2 calculation for a metal complex using G94. The job went through 
the SCF stage successfully, but it immediately failed after l906.exe has 
started with the message:

 Logic failure, MDV=     7440563 NBuf=         -10 but FulOut=F

Anyone has ever come across this kind of error message? 
I'd be very grateful if anyone could provide assistance.

Thanks.
Zhenyang LIN
Chemistry/HKUST

From h.rzepa@ic.ac.uk  Fri Apr  4 03:39:58 1997
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Subject: ANNOUNCE: ECTOC-3 Organometallic Conf. Abstracts


We would be grateful if you could bring to the attention of any
"organometallic" chemists in your organisation who might be interested
in submitting an article or poster to the  ECTOC-3 conference that the
registration process for abstracts is now open;

http://www.ch.ic.ac.uk/ectoc/ectoc-3/ectoc_sub.html

The deadline for submitting an abstract is  April 25th, 1997.

full details are on http://www.ch.ic.ac.uk/ectoc/ectoc-3/

Dr Henry Rzepa,  Dept. Chemistry,  Imperial College,  LONDON SW7 2AY;
rzepa@ic.ac.uk; Tel  (44) 171 594 5774; Fax: (44) 171 594 5804.
URL: http://www.ch.ic.ac.uk/rzepa/ 



From vrc@ems.ncl.res.in  Fri Apr  4 04:33:54 1997
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Date: Fri, 4 Apr 1997 14:13:24 +0530 (IST)
From: Dr V R Choudhari <vrc@ems.ncl.res.in>
To: "Dr. Bruno Manunza" <bruno@antas.agraria.uniss.it>
cc: castejon@kbw350.chem.yale.edu, chemistry@www.ccl.net
Subject: Re: CCL:real memory checking on IBM-errata-
In-Reply-To: <Pine.A32.3.91.970331222022.9218A-100000@antas.agraria.uniss.it>
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I guess "top" command would do the trick
or df -k in kilobytes or df -u

with regards
sivadinarayana
naa@ems.ncl.res.in


On Mon, 31 Mar 1997, Dr. Bruno Manunza wrote:

> 
> 
>  On Sun, 30 Mar 1997 castejon@kbw350.chem.yale.edu wrote:
>  
>  > 
>  > Hi everyone.
>  > 
>  > 	I have a simple question. Does anyon know how to check how
>  > 	much physical memory a computer has by using a unix command.
>  > 	I have an IBM RS/6000. Iknow how much memory it has but I want
>  > 	to be able to check it.
>  > 
>  > 
> 
> 
> Dear Henry, sorry for my previous misleading message, and let me 
> apologize for this errata
> 
> The right answer is: lsdev -C -c memory	
>   
> bye
> Bruno
> 
> > 
> > Dr Bruno Manunza
> > DISAABA (Dept. of Agricultural Environm. Sci)
> > University of Sassari
> > V.le Italia 39
> > 07100 Sassari, ITALY
> > phone: 39 79 229215
> > fax:   39 79 229276
> > e-mail: bruno@antas.agraria.uniss.it
> > e-mail: bruno@tharros.dipchim.uniss.it
> > e-mail: gx6bot81@cray.cineca.it
> > web: http://antas.agraria.uniss.it
> > 
> > 
> > -------This is added Automatically by the Software--------
> > -- Original Sender Envelope Address: bruno@antas.agraria.uniss.it
> > -- Original Sender From: Address: bruno@antas.agraria.uniss.it
> > CHEMISTRY@www.ccl.net: Everybody | CHEMISTRY-REQUEST@www.ccl.net: Coordinator
> > MAILSERV@www.ccl.net: HELP CHEMISTRY or HELP SEARCH | Gopher: www.ccl.net 73
> > Anon. ftp: www.ccl.net   | CHEMISTRY-SEARCH@www.ccl.net -- archive search
> >              Web: http://www.ccl.net/chemistry.html 
> > 
> > 
> 
> -------This is added Automatically by the Software--------
> -- Original Sender Envelope Address: bruno@antas.agraria.uniss.it
> -- Original Sender From: Address: bruno@antas.agraria.uniss.it
> CHEMISTRY@www.ccl.net: Everybody | CHEMISTRY-REQUEST@www.ccl.net: Coordinator
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> Anon. ftp: www.ccl.net   | CHEMISTRY-SEARCH@www.ccl.net -- archive search
>              Web: http://www.ccl.net/chemistry.html 
> 

From Sylvie.Joanteguy@univ-pau.fr  Fri Apr  4 09:33:55 1997
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Message-Id: <199704041342.PAA59434@crisv3.univ-pau.fr>
Subject: electronic correlation
To: chemistry@www.ccl.net
Date: Fri, 4 Apr 1997 15:42:03 +0200 (MET DST)
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Dear CCL,

My question is short: What's exactely the electronic correlation (dynamic and no dynamic correlation)?

	Many thanks for your help

				Sylvie Joanteguy

From david.decorte@unifr.ch  Fri Apr  4 09:35:37 1997
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Date: Fri, 04 Apr 1997 16:19:05 +0100
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Organization: Universite de Fribourg
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Hello,

A few days ago I posted the following problem.

> Hello, 
> 
> I've got a small g94 problem. When doing a Scan=Opt calculation, the
> calculation stops after the first optimisation and does not perform a
> scan....No error messages are listed... Does anybody know how to prevent
> this problem?
> Kind regards,
>                               David

Here is a condensated version of the answer I received. 
The Scan=Opt keyword doesn't work! So it's better to perform an
Opt=Addredundant or an Opt=Z-matrix calculation.

It works.....
Thanks to everybodz who responded to my mail.

				David

-- 
David De Corte				
Institute of Inorganic Chemistry	Tel: 0041-26-300.87.52(49)
University Fribourg			Fax: 0041-26-300.97.38
CH-1700 Switzerland			mailto:David.Decorte@unifr.ch
http://www.unifr.ch/

From schiffer@h1tw0036.hoechst.com  Fri Apr  4 10:34:01 1997
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        Computational Chemistry List <chemistry@www.ccl.net>
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Sylvie.Joanteguy@univ-pau.fr wrote:
> 
> Dear CCL,
> 
> My question is short: What's exactely the electronic correlation (dynamic and no dynamic correlation)?
> 
>         Many thanks for your help
> 
>                              Sylvie Joanteguy

Hi Sylvie,
the definition of the correlation energy is

	E_corr = E_exact - E_HF

E_exact is the exact nonrelativistic energy eigenvalue of the
electronic Schroedinger equation. E_HF is the corresponding 
Hartree-Fock energy (basis set limit !). That definition goes
back to Loewdin. Sinanoglu was the first who introduced the terms
'dynamic' and 'non-dynamic' correlation, the latter one arises
because of degeneracies or near-degeneracies of electronic systems.
A good and very recent discussion of this subject can be found in the
paper

Daniel K. W. Mok, Ralf Neumann, and Nicholaus C. Handy
J. Phys. Chem. 100 (1996) 6225-6230

Ciao,
Heinz 
-- 
Dr. Heinz Schiffer		Phone   ++49-69-305-2330
Hoechst CR&T			Fax     ++49-69-305-81162
Scientific Computing, G864	Email   schiffer@h1tw0036.hoechst.com
65926 Frankfurt am Main		        schiffer@msmwia.hoechst.com

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****************************************************************************

   The National Center for Supercomputing Applications and
         Gaussian, Inc. are pleased to announce:

     Quantum Chemistry for Engineers and Chemists in the
                Chemical Process Industry

 Date:      June 3-6, 1997

 Location:  National Center for Supercomputing Applications
            Urbana-Champaign, IL

 The National Center for Supercomputing Applications (NCSA) in conjunction
 with Gaussian, Inc. are pleased announce a workshop tuned to address the
 needs of researchers in the chemical process industry who need to add
 electronic structure methods to their arsenal of research tools.

 State of the art electronic structure methods and main stream chemical
 process industry (CPI) applications are converging at a rapid pace.
 Computational models now have the accuracy and reliability to predict
 physical properties at costs and time frames competitive with experimental
 approaches.  This course will lay out the methods of electronic structure
 theory and describe how to extract physical properties from calculations.
 While this workshop is oriented to chemical engineering topics we encourage
 you to consider sending chemist/chemical engineer teams to gain optimal
 benefit.


      Instructors:

        Dr. Michael J. Frisch               Gaussian, Inc.
        Prof. Phillip Westmoreland          Univ. of Massachusetts
        Prof. Matthew Neurock               Univ. of Virginia
        Dr. Douglas J. Fox                  Gaussian, Inc.

      Tentative Agenda Topics:

        Computational Chemistry: A CPI Perspective
        Introduction to Electronic Structure Theory
        Predicting Thermodynamics with Model Chemistries
        Geometry Optimization Techniques
        Electron Correlation Methods
        Density Functional Theory Methods
        Theoretical Methods for Optical and UV Spectra
        Predicting Molecular Properties
        Continuum Models for Solvation
        Case Studies: Electronic Structure Methods in Process Design
                    : Model Assessment for Physical Properties


 There will be hands-on sessions each day between the morning and  afternoon
 lectures.  Additional hands-on sessions will be available until the building
 closes. Workshop participants will be provided with use of an SGI
 workstation to complete exercises, experiment and/or conduct short research
 topics.  Each workshop participant will also be provided a copy of the
 lecture notes, a copy of Exploring Chemistry with Electronic Structure
 Methods (2nd. Ed.)  and a copy of the Gaussian 94 User's Reference.

 For Application please contact:

        Workshop Coordinator
        Gaussian, Inc.
        Carnegie Office Park
        Bldg. 6, Suite 230
        Pittsburgh, PA  15106 USA

  Additional information can be obtained from

        Telephone: (412) 279-6700
        Fax:       (412) 279-2118
        Email:     info@gaussian.com


 DEADLINES:

        Receipt of Registration Materials:      May 2, 1997


 This notice is sent without warranty of any kind, expressed or implied
 by Gaussian, Inc. or NCSA.  Gaussian is a registered trademark of 
 Gaussian, Inc.

****************************************************************************

From korkin@qtp.ufl.edu  Fri Apr  4 13:33:59 1997
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Date: Fri, 4 Apr 1997 13:32:54 -0500 (EST)
From: Anatoli Korkin <korkin@qtp.ufl.edu>
Reply-To: Anatoli Korkin <korkin@qtp.ufl.edu>
Subject: Re: CCL:electronic correlation
To: Sylvie.Joanteguy@univ-pau.fr
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> 
> Dear CCL,
> 
> My question is short: What's exactely the electronic correlation (dynamic and 
no dynamic correlation)?
> 
> 	Many thanks for your help
> 
> 				Sylvie Joanteguy
> 


Dear Silvie,

As you as a short question, I will give you a short answer :-)

The definition of the electronic correlation is simple -
it is what you get above single-determinant SCF method. Of course, you
should remeber that your result depends of the basis set you use.
Only full CI with infinite number of basis functions will give
you an exact solution for the energy and the wave fuction within 
Born-Oppenheimer approximation.

The definition of the dymanic and non-dynamic correlation is less
accurate. If you have a good SCF solution, and you do a perturbation
calculation on top of it, your correction to the energy, structure and
other properties is considered to be an effect of dynamic correlation.
If you need a few determinants to get a good first approximation for the
wave function, it is what people call non-dynamic correlation.
Of course, the destingtion between "good" and "bad" is rather uncertain,
as it happens to all qualitative concepts.

The coupled cluster (CC) method [1] provides both dynamic and non-dynamic
correlation effects, and if the number of electrons is equal to
the level of CC (e.g. CCSDT for 3 electrons) you will get the total correlation,
as the full CI does.

Anatoli Korkin

[1] see, for example, R.J. Bartlett & J.F. Stanton, Applications of
Post-Hartree-Fock Methods: A Tutorial, in Reviews in Computational
Chemistry, Vol. 5, VCH Publishers, 1994)



