From chemistry-request@server.ccl.net Tue Apr 17 07:02:03 2001
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From: "Petr Toman" <toman@imc.cas.cz>
To: chemistry@ccl.net
Date: Tue, 17 Apr 2001 13:02:10 +0200
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Subject: G98 and atomic coordinates printing
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Dear CCLers,
Gaussian 98 prints the atomic coordinates in input (Z-matrix) orientation 
by default only if the number of atoms is less or equal 20.
Does anybody know how can I force G98 to print the coordinates in all 
cases.

Thanks in advance,
Petr Toman



From chemistry-request@server.ccl.net Mon Apr 16 19:51:13 2001
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Date: Mon, 16 Apr 2001 16:51:12 -0700 (PDT)
From: eric hu <erichu_linux@yahoo.com>
Subject: Re: CCL:molscript Makefile.complete for redhat 7.0
To: Andrew Dalke <dalke@acm.org>
Cc: chemistry@ccl.net
In-Reply-To: <008c01c0c4bc$a3223e40$0301a8c0@josiah>
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Content-Type: multipart/mixed; boundary="0-1303455736-987465072=:57623"

--0-1303455736-987465072=:57623
Content-Type: text/plain; charset=us-ascii
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Here is my Makefile.complete as an attachment file.

--- Andrew Dalke <dalke@acm.org> wrote:
> >I'm trying to compile molscript 2.1.2 on the redhat
> >7.0. There's always an error about clib/clib.a. I
> >wonder if any of you have the Makefile. Thanks!
> 
> I can't help you with that since I don't have
> molscript.  
> However, as a point for future reference, if you had
> included the error message in your mail you might
> have gotten a response from people who know how to
> solve the problem in the general sense, since it
> might not be a molscript specific error.
> 
>                     Andrew
>                     dalke@acm.org
> 
> 


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RkxBR1MpIiBPUEVOR0xDTElCT0JKPSIkKE9QRU5HTENMSUJPQkopIgoK

--0-1303455736-987465072=:57623--


From chemistry-request@server.ccl.net Tue Apr 17 08:58:06 2001
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From: Tobias =?iso-8859-1?Q?Br=FCggemann?= 
	<tobbes@citrin.chemie.uni-dortmund.de>
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To: Petr Toman <toman@imc.cas.cz>
CC: chemistry@ccl.net
Subject: Re: CCL:G98 and atomic coordinates printing
References: <200104171102.NAA08150@linus.imcm.cas.cz>
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Petr Toman wrote:
> 
> Dear CCLers,
> Gaussian 98 prints the atomic coordinates in input (Z-matrix) orientation
> by default only if the number of atoms is less or equal 20.
> Does anybody know how can I force G98 to print the coordinates in all
> cases.
> 
> Thanks in advance,
> Petr Toman
> 
> -= This is automatically added to each message by mailing script =-
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Hi,

try the IOP(99/14=1). It shuld print the final z-matrix at the end of
the output.

Tobias Brüggemann


From chemistry-request@server.ccl.net Tue Apr 17 12:38:45 2001
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Date: Tue, 17 Apr 2001 12:44:16 -0400
From: elewars <elewars@trentu.ca>
Subject: SUMMARY: POTENTIAL E SURFACE, MARCELIN
To: chemistry@ccl.net
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2001 April 17

Here are the answers to this question:
=========
In his textbook "Physical Chemistry", Fourth Ed. (1972), on page 377,
Walter J. Moore (author of the definitive biography of Erwin
Schroedinger, 1989) says: "The idea that a chemical reaction can be
represented by [a potential energy surface] was suggested by Marcelin in
1915..." and gives this reference:
Marcelin, Ann. Phys., 3, 158 (1915).

(1) Who was Marcelin, and what was his initial(s) (A. Marcelin, B.
Marcelin, ...)?
(2) What was Ann. Phys. in 1915--Annalen der Physik, or Annales de
Physique, or what?

If anyone....
=========
THE ANSWERS:

I thank those who responded: Matt Thompson, Adam Hixson, and Konrad
Hinsen. I summarize the answers here and give the responses below.

R. Marcelin published in Annales de Physique, 1915, 3, 120-231 (!) a
very long paper (perhaps a dissertation) which evidently created much of
transition-state theory about 20 years before the much-better-known work
of Eyring and coworkers. The section most relevant to potential energy
surfaces seems to start on page 158.

Rudolph Marcus, in his Nobel Prize (1992) speech recognizes Marcelin's
work as a milestone: "...Marcelin's classic 1915 theory which came
within one small step of the Transition State Theory of 1935."

Marcelin was apparently killed in 1915, in World War I.

Thanks again to all (below) who responded.

E. Lewars
-----
-----

#1
Matt Thompson:

Dr. Lewars, here is some info on R. Marcelin, Ann. Phys., 3, 152 (1915).

It is R. Marcelin from "Annales de Physique" and the paper is titled
(sorry for no accents):

"Contribution a l'etude de la cinetique physico-chimique"

It spans pp. 120 - 231.

Page 152 is in Chapter II, Section IV.

The chapter is titled:

"La formule synthetique precedemment obtenue se presente comme une
consequence tres directe de la theorie de l'equipartition."

The section is:

"La formule synthetique obtenue dans le Chapitre precedent est une
consequence du theoreme de Boltzmann-Gibbs."

Essentially, the paper just about had all of transition state theory
correct.  Almost.  I know Rudy Marcus feels it is a very important
paper, see his Nobel biography at
http://www.nobel.se/chemistry/laureates/1992/marcus-autobio.html

Matt Thompson
--
******************************************************************
"And isn't sanity really just a one-trick pony, anyway?  I mean,
all you get is one trick, rational thinking, but when you're good
and crazy, ooh ooh ooh, the sky's the limit!" -- The Tick
******************************************************************
The Matt Thompson -- thompsma@colorado.edu
                     http://ucsub.colorado.edu/~thompsma/Home.html

=======
#2
Adam Hixson

The reference is R. Marcelin Annales de physique
3 120-231 1915.

It is the length of a dissertation, but there
is a footnote on the first page:

Tue' a` l'ennemi en sept 1914.

Died in WWI, apparently.  Apparently a student of
P. Duhem, of Gibbs-Duhem fame.


Adam Hixson
Department of Chemistry and Biochemistry
The University of Oklahoma     chixson@chemdept.chem.ou.edu
620 Parrington Oval            hixsonc@yahoo.com
Norman, OK 73069
==========
#3
Konrad Hinsen

[This  clears up the journal name (Annales ...), but Google seems to
have got the initial wrong--EL]

Just typing the reference into Google yielded a page with a more
complete reference:

  A. Marcelin, Ann. Phys. (Paris), 3, 158 (1915).

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

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

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
















=========



From chemistry-request@server.ccl.net Tue Apr 17 11:05:54 2001
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From: "Scott L. Anderson" <anderson@chem.utah.edu>
To: <chemistry@ccl.net>
Subject: visualization software
Date: Tue, 17 Apr 2001 09:06:42 -0600

Version 2.0 of the gOpenMol visualization package has been released by Leif
Laaksonen and can be downloaded at http://www.csc.fi/~laaksone/gopenmol/
Versions are available for Win 95/98/ME/2000, Linux, SGI Irix, and Compaq OSF1.


gOpenMol is designed to allow visualization of molecules, MOs, densities,
etc., as well as animations of vibrations, MD simulations etc.  It can read
results from a wide variety of quantum chemistry and simulation programs.
gOpenMol also includes many tools for analyzing structures and trajectories.



New features include:

Handling up to 100,000 atoms

Additional controls for trajectory/MD visualization and analysis (including
   variable animation speed)

Ability to define clip planes to allow you to cut away part of a molecule or
   orbital to see the interior structure

Ability to define arbitrarily oriented planes for displaying contours (of
   MOs, etc)

Additional import filters for new quantum chemistry, MM, and MD programs (23
   at last count)



You can find a tutorial that illustrates the features and operations of the
program at 
        http://www.chem.utah.edu/chemistry/faculty/anderson/gopen.html
The tutorial now includes a section on use of Tcl/Tk scripts to automate
gOpenMol.  The scripts can be used to deal with repeated tasks, and can
also be used to produce animated presentations, etc.

Prof. Scott L. Anderson / Chemistry Dept.
315 S. 1400 E. Rm 1216 / U. of Utah
Salt Lake City, UT  84112
(801)585-7289       FAX: (801)581-8433
www.chem.utah.edu/chemistry/faculty/anderson/anderson.html


From chemistry-request@server.ccl.net Tue Apr 17 11:41:01 2001
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From: "Hui-Hsu \(Gavin\) Tsai" <hxt10@po.cwru.edu>
To: <CHEMISTRY@ccl.net>
Subject: "all electron" basis set for second row transition metal
Date: Tue, 17 Apr 2001 11:45:10 -0400

Hi CCLers,

I have searched different sources for an "all electron" basis set
higher than 3-21G for second row transition metal and Ce.
I mainly focused on Zr and Ce so far.

If they do exist, I would appreciate knowing where to find it?
Any comment is welcome.

Gavin

From chemistry-request@server.ccl.net Tue Apr 17 13:47:34 2001
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This is becoming a FAQ, but the two main sources:

http://www.emsl.pnl.gov:2080/forms/basisform.html   Gaussian Basis Set
Order Form.  Huzinaga WTBS, Partridge Uncontracted, etc.

"Gaussian Basis Sets for Molecular Calculations" Huzinaga, S. (ed).
Otherwise known as the "Green Book".

						-fred

					Frederick P. Arnold, Jr.
					NUIT, Northwestern U.
					f-arnold@northwestern.edu




From chemistry-request@server.ccl.net Tue Apr 17 17:18:24 2001
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From: Bernd Schubert <bernd.schubert@student.uni-halle.de>
To: chemistry@ccl.net
Subject: Re: CCL:gaussian and hollerith string Summury
Date: Tue, 17 Apr 2001 23:18:00 +0200
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On Monday 9 April 2001 I asked how to define the maximum allowed symmetry in 
Gaussian.

I got two replies to my answer and the problem is completely solved (thanks 
both for their reply).

The maximum allowed symmetry might be specified by using the undocumented 
keyword symm(pg=pointgroup). 
For example: symm(pg=cs)

If someone wants to use iop(2/19) for defining then the required number can 
be determinated by using the following procedure:

1.) The hollerith string is a 4 byte string
2.) the string must be written from the right to the left, unused characters 
are replaced by space
for example for the cs group: <SPACE>  <SPACE>  <S> <C>
3.) The characters are replaced by hexadecimal numbers of the ascii table
for my example giving: 20 20  53 43
4.) The resulting hex. number (20205343) is translated into a decimal number 
giving: 538989379
5.) This decimal number can be used for iop(2/19)
for my example: iop(2/19=538989379)

By using a lower symmetry than the molecule has there might be several equal 
symmetry planes possible to use as main symmetry plane. 
IOP(2/20) is needed to define which one is the main symmetry plane.


--------------------------------------------------------------------------
Here are the 2 answers I got:


From: Stefan Fau <fau@qtp.ufl.edu>

Hi Bernd,

I ran across the problem of Hollerith strings
in connection with symmetry in Gaussian some
years ago. Unfortunately I lost access to the
handbook in which I wrote down the solution ...

As far as I remember, the Hollerith string is a
hexadecimal representation of the characters
in the symmetry label. I think it went like this:
" C2v", characters 32, 67, 50 and 118 of the
ASCII character table. In hexadecimal this
corresponds to 20, 43, 32, 76 giving the
Hollerith string "20433276".

This string depends on which character set is
default on your computer. You can find out
using the FORTRAN command char('C'). I'm
not sure anymore if the Hollerith string expects 8
hexadecimal numbers and about small or capital
characters.

If it doesn't work at first, better look into the
source code ...

Stefan

P.S.: please post the final solution to CCL when
you find it, so it gets into the archives.
______________________________________________________________________
Dr. Stefan Fau                    |      fau@qtp.ufl.edu
Quantum Theory Project     |     (352) 392-6714
University of Florida
Gainesville, FL 32611-8435

------------------------------------------------------------------------------
From: "Cust. Service Jim" <csj@gaussian.com>

Dear Bernd,
   There is an undocumented feature that will get around your
iop(2/19=2HCS) problem, and that is to use something like "symm=(pg=cs)". 
This will read in the point group you requested. As for opt(2/20), this is
necessary when it is ambiguous how the symmetry will be reduced. For
example, if your initial structure is C4V and you request a reduction of
symmetry to CS, the program wants to know which of the symmetry planes in
the C4V point group you'd like as the CS plane. 

Regards,

Jim Hess
------------------------------------------------------------------------------


