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From: ahirasim@agr.kyushu-u.ac.jp (Akinori Hirashima)
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Dear Netters:

Anybody who needs to access data base such as Cambridge Crystallographic
Data Centre,
please visit the following www site.

http://csdvx2.ccdc.cam.ac.uk/

Thanks.



====================================
        $BJ?Eg!!L@K!(B (Akinori Hirashima)$B!!!!!!!!!!!!!!!!!!!!!!!!!!!!(B
        $B6e=#Bg3XG@3XItG@7]2=3X2J!!!!!!(B
        $B")(B812-81$B!!J!2,;TEl6hH":j(B6-10-1$B!!!!!!!!!!!!!!!!!!(B
        Department of Agricultural Chemistry
        Kyushu University
        Fukuoka 812-81, Japan
        Phone: (+81)92 - 641 - 1101 ext. 6205$B!!(B 
        Fax:  (+81)92 - 632 - 1960
        E-Mail: ahirasim@agr.kyushu-u.ac.jp 
=====================================


From kris@bionmr1.rug.ac.be  Thu Sep  7 02:58:52 1995
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Date: Thu, 7 Sep 1995 08:55:59 +0200 (MDT)
From: Kris Boulez <kris@bionmr1.rug.ac.be>
Subject: Re: CCL:CCL:Java chemistry applets?
To: wdi@eros.ccc.uni-erlangen.de
Cc: chemistry@www.ccl.net
In-Reply-To: <9509061940.ZM1277@schiele>
Message-Id: <Pine.3.89.9509070801.B9877-0100000@bionmr1.rug.ac.be>
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On Wed, 6 Sep 1995, Wolf-Dietrich Ihlenfeldt wrote:

> 
> On Sep 6, 10:06, Hinsen Konrad wrote:
> > Subject: CCL:Java chemistry applets?
> >
	[ part about Java deleted ]
> >
	[ part about Python deleted ]
> >
> 
	[ part about E (prononounced awe) deleted ]
> 
	[ part about tcl/tk deleted ]

  To add one more language : Perl. It's used in the big majority off CGI 
scripts on the WWW and is a great general programming language. There is 
a beta-version of safe-perl and work is underway for a perl/tk browser. 
For a comparison of perl versus the abovementioned languages look at 
ftp://ftp.perl.com/pub/perl/versus/ 
  This is just to show that there are more (and much more widely used) 
languages around. So I think the suggestion of Henry Rzepa to use a 
stand-alone program (Rasmol is great software and free) for molecular 
visualisation is the way to go.

Kris,
----
Kris Boulez		(Kris.Boulez@rug.ac.be)
Biomolecular NMR unit	<http://bionmr1.rug.ac.be/~kris>
University of Ghent, Belgium


From jkl@ccl.net  Thu Sep  7 05:43:54 1995
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Date: Thu, 7 Sep 1995 11:47:31 +0100
To: chemistry@ccl.net
From: bouyer@ext.jussieu.fr (Frederic BOUYER)
Subject: Harris functional


Hi everybody,

I was wondering what is the Harris functional, in the DFT context, and what
are the main differences with the functionals used in programs (DGauss,
deMon, DMol, ADF, ...). Any comments would be appreciated and/or a summary.

Thank you in advance.

Frederic Bouyer


____________________________________________________________________
Frederic BOUYER
Laboratoire d'Electrochimie et de Chimie Analytique
Equipe "Reactivite en Milieux Ioniques Liquides" (G. PICARD)
ENSCP
11, rue Pierre et Marie Curie
75231 PARIS Cedex 05
FRANCE
Tel : (33)-1-43-54-53-84 ou (33)-1-44-27-67-51 ou (33)-1-44-27-66-94
Fax : (33)-1-44-27-67-50
E-mail : bouyer@ext.jussieu.fr
http://alcyone.enscp.jussieu.fr/  created, in progress ...
http://alcyone.enscp.jussieu.fr/Pages/LECA/GP/FB/



From csron@wicc.weizmann.ac.il  Thu Sep  7 06:28:55 1995
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From: Ron Edgar <csron@wicc.weizmann.ac.il>
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Subject: summary - algorithms for basic molecule manip..
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First I would like to thank all who replied, in retrospect, my question
was too general and I guess this held back some people with specific 
answers to a specific  problem.  If after reading the replies you
think you can add - by all means please do.

my original question was:

I'm writing a C++ library to deal with atoms/molecules. In the
good tradition of trying to avoid re-inventing the wheel I would
appreciate any references (or source) to algorithms for basic operations 
which can be applied to groups of atoms defined in Cartesian OR fractional
coordinate systems, e.g. torsion and "bend" angles, rotations 
along an arbitrary vector, etc. 

Also I would be interested in means of finding internal molecular 
symmetries for a given set of coordinates.

Please reply directly to me, I will summarize to the group.

Thanks,
	Ron

-------------------------------------------------------------------
Message 6/14  From Leslie Glasser 

Organization:  CHEMISTRY -  WITS UNIVERSITY
To: Ron Edgar <csron@wicc.weizmann.ac.il>
Date:          Tue, 5 Sep 1995 12:13:43 GMT + 2:00

Dear Ron:

You will find the vector algebra for some of the operations in which
you might be interested in my article "Molecular Geometry and
Substituent Ganeration: a MathCAD Program", Comp. Chem., 17(1),
107-8 (1993).

Leslie ==============================================================
(Prof.) Leslie Glasser                     Dept. of Chemistry    
E-mail: glasser@aurum.chem.wits.ac.za      Univ. of Witwatersrand     
Tel: Intl + 27 11 716-2070                 P. O. WITS 2050            
Fax: Intl + 27 11 339-7967                 South Africa               
Home Pages:  University      http://sunsite.wits.ac.za
             Chemistry       http://www.chem.wits.ac.za
====================================================================== 

Message 4/14  From Craig Taverner                           

X-Sender: craig@zaphod.gh.wits.ac.za

I have a C (ANSI) program I'm been writing for some time, that contains 
calculations that may be of some use:

It is called "steric", and is primarily for organometalic chemistry.
It is for the calculation of linear cone angles (Tolman), solid angles,
angles of overlap and molecular volumes (rough fast Monte Carlo) 
for steric interactions in ligands and molecules.
Code that may be of interest:
 . bond search using vdW radii
 . group search using recursive bond trace for individual molecules 
and seperate ligands bonded to central metal atom.
 . fractional to cartesian transform
 . some vector manipulations of data (basic and specific).
 . fully dynamically allocated linked lists to describe all molecular 
features (seperate molecules, atoms and bonds).
 . various others I cannot think of now.

If you're interested, I'll be glad to try and provide some code.  My 
program has been written to be easily expanded with new functions, but 
I'm not sure that that will make it easy to provide the current code in a 
general library format.  Unfortunately I never got to learn C++ to 
facilitate that sort of feature.

Cheers, Craig

"If God had meant us to be naked, we would have been born that way."

Craig Taverner
Structural Chemistry, University of the Witwatersrand, South Africa

-----------------------------------------------------------------
Message 3/14  From Matt Stahl                                


Date: Tue, 5 Sep 1995 11:25:58 -0700 (MST)

Ron,
	You may want to check out:

    Computers & Chemistry.  18(4):371-376, 1994 

	This paper contains an algorithm for automatic point group
determination. 
	I have various and sundry routines for internal->cartesian
conversion, bond angle, and torsion angle adjustments (rotation about a
bond).  I can give you sources, but they need to be linked with the BABEL
library.  Actually, babel may also be a good place to look for vector and
matrix routines.  If you are interested in playing with the code i have
(crude, uncommented C) let me know.

matt

~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~
Matthew Stahl, Ph.D.			| 
Department of Chemistry			| I'd rather be right half of the
University of Arizona			| time than half right all the
Tucson, AZ  85721			| time.
matt@synthesis.chem.arizona.edu		|	-Malcom S. Forbes
~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~

Message 2/14  From Hinsen Konrad                             Sep 6, 95 10:13:09 am -0400


Date: Wed, 6 Sep 1995 10:13:09 -0400

I have written some C++ code that takes internal coordinate specifications
(e.g. a Z matrix, but also more flexible forms) and turns them into
Cartesian coordinates. I never had the time to finish this properly;
it works, but error checking is minimal.

-------------------------------------------------------------------------------
Konrad Hinsen                     | E-Mail: hinsenk@ere.umontreal.ca
Departement de chimie             | Tel.: +1-514-343-6111 ext. 3953
Universite de Montreal            | Fax:  +1-514-343-7586
C.P. 6128, succ. A                | Deutsch/Esperanto/English/Nederlands/
Montreal (QC) H3C 3J7             | Francais (phase experimentale)
-------------------------------------------------------------------------------


From ferenc@rchsg8.chemie.uni-regensburg.de  Thu Sep  7 09:45:13 1995
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Date: Thu, 7 Sep 95 15:38:37 +0200
From: Ferenc.Molnar@chemie.uni-regensburg.de (Ferenc Molnar)
Message-Id: <9509071338.AA01245@rchsg8.chemie.uni-regensburg.de>
To: CHEMISTRY@www.ccl.net
Subject: normal modes summary



Dear Netters:

Some days ago I posted the following question:

> I have a (maybe trivial) question concerning the calculation
> of normal modes in MOPAC.
> 
> The diagonalization of the force matrix (in mass weighted
> coordinates) leaves you with a set of eigenvalues and normal 
> coordinates.
> 
> The eigenvalue number k correspond to (w_k)^2, where the w_ks
> are the vibrational frequencies, this means:
> 
>  (w_k)^2=K_k/M_k 
> 
> K_k: force constant of the kth normal mode
> M_k: reduced mass of the k_th normal mode
> 
> Now my question is, if (w_k)^2 determines only the ratio
> of K_k and M_k, then how are the reduced masses, reported
> in the "vibrational analysis" section of the MOPAC output 
> file, calculated? Is there a convention, which "fraction" of
> (w_k)^2 to use for K_k and which for M_k?

Some people asked me for a summary, so here it is.
It consist only of one message.

I want to thank Jimmy Stewart very much for his reply.
It really answered the question!

> The reduced mass is like atomic charges, in that it is not an observable,
> however, for specific systems - mainly homonuclear diatomics - the reduced 
> mass does have meaning.   The reduced mass definition used in MOPAC can be
> understood as follows:
> 
> Each vibration can be modelled by a mass, M_k, at the end of a spring of
> force constant K_k, attached to an infinite mass.
> 
>   Inf   |       K_k        M_k
>   Mass  |
>         |^^^^^^^^^^^^^^^^^^O
>         |
>         |
> 
> The contribution to the mass is proportional to the amount each atom
> contributes to the normal mode, and is proportional to the fraction of
> the atomic mass contributed by each atom.
> 
> Put in more formal terms, the contribution of each atom to the effective mass
> of a vibration is proportional to the product of the intensity on that
> atom times the mass-weighted intensity.
> 
>  rho = sum_A <c_A|c_A><c_A|M_A|c_A> = sum_A (c_A_x**2+c_A_y**2+c_A_z**2)**2*M_A
> 
> where c_A are the coefficients of the normal modes.  
> 
> 
> 
> Consider H2: c_1 = 0.7071*H_1+0.7071*H_2
> 
>      rho_1 = 0.7071**4*1 + 0.7071**4*1 =0.5
> 
> Consider M-H, M being an atom of very large mass, say 1000:
> 
>              c_1 = 0.0316*M+0.9995*H
> 
>      rho_1 = 0.0316**4*1000 + 0.9995**4*1 = 0.9990
> 
> [0.0316 ~ sqrt(1/1000); 0.9995 ~sqrt(1-1/1000)]
> 
> Consider N2: c_1 = 0.7071*N_1+0.7071*N_2
> 
>      rho_1 = 0.7071**4*14+0.7071**4*14 = 7.0
> 
> 
> Jimmy Stewart

Best Regards,
Ferenc


Ferenc Molnar

---------------------------------------------------------------------------
Institut fuer Physikalische und Theoretische Chemie
- Lehrstuhl Prof. Dick -                   Tel.:  (+49) 941 943-4466 /-4486
Universitaet Regensburg                    Fax.:  (+49) 941 943-4488
Universitaetsstrasse 31
D-93053 Regensburg
Deutschland / Germany
---------------------------------------------------------------------------
EMail (SMTP):  Ferenc.Molnar@chemie.uni-regensburg.de
---------------------------------------------------------------------------
 Those who do not archive the past are condemned to retype it!
  -- Garfinkel & Spafford, Practical Unix Security
---------------------------------------------------------------------------


From MARSHALL@cas.unt.edu  Thu Sep  7 09:58:58 1995
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From: "Dr. P. Marshall (Chemistry ext 2294)" <marshall@unt.edu>
Organization:  University of North Texas
To: chemistry@www.ccl.net
Date:          Wed, 6 Sep 1995 15:46:31 CST6CDT
Subject:       QM code for spin-orbit coupling?
Priority: normal
X-Mailer: Pegasus Mail for Windows (v2.0-WB3)
Message-Id: <3ABEC4C4C6C@cas.unt.edu>


Dear Netters:
I am looking for an easy to use ab initio package
capable of computing spin-orbit splittings for halogenated 
radicals. Any pointers/help will be greatly appreciated (I know 
what GAMESS can do). If there is sufficient interest, I'll summarize 
the responses.
Thanks in advance,  Paul

-------------
Paul Marshall                            marshall@unt.edu
Associate Professor             University of North Texas
Dept. of Chemistry, PO Box 5068, Denton, Texas 76203-0068
tel (817) 565-2294                     fax (817) 565-4318

From jkl@ccl.net  Thu Sep  7 10:05:44 1995
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From: kessi@psizi1.psi.ch (Alain Kessi)
Message-Id: <9509071347.AA13552@psizi1.psi.ch>
To: chemistry@ccl.net
Subject: Re: CCL:Harris functional
In-Reply-To: <v01510100ac747ca95ba5@[134.157.11.12]>
X-Mailer: [XMailTool v3.1.2b]


Frederic Bouyer (bouyer@ext.jussieu.fr) wrote:
> I was wondering what is the Harris functional, in the DFT context, and what
> are the main differences with the functionals used in programs (DGauss,
> deMon, DMol, ADF, ...). Any comments would be appreciated and/or a summary.

The Harris functional is an alternative formulation to the Kohn-Sham
total energy functional. It is therefore not an alternative to the
exchange and correlation functionals such as the Perdew and Wang functional,
but uses such parametrizations as parts of its total energy expression
(just like the Kohn-Sham total energy formulation does).

As explained in the DSolid manual, the Harris functional is stationary at
the same density as the Kohn-Sham total energy functional and can therefore
be used instead for the SCF calculation. It has two advantages as compared
to the Kohn-Sham scheme. First, the density does not need to be
V-representable. Second, the curvature of the Harris functional about
the stationary point is smaller than the curvature of the Kohn-Sham
functional, so convergence is faster. Actually, the Harris functional was
originally developed for single-shot calculations rather than SCF convergence,
and for many purposes, the accuracy after the first iteration may be
sufficient.

DMol (and its periodic boundary conditions implementation DSolid) uses
the Harris functional.

--
Alain Kessi (alain.kessi@psi.ch)
Paul Scherrer Institut, Zuerich, Switzerland

From jkl@ccl.net  Thu Sep  7 10:14:03 1995
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To: chemistry@ccl.net
Subject: NBODel Utility on G92 
Date: Thu, 07 Sep 95 16:00:40 +0100
X-Mts: smtp


Dear Netters,

I would like to know how can be done a NBO Fock matrix deletion procedure on 
G92, particularly by setting some NBO Fock matrix elements to zero and 
reevaluating the energy. G92 manual refers to NBO separate manual, but 
unfortunately I have no access to that one. Which methodology do I have to 
follow? An example G92 input data would be most welcome, as well as any 
suggestion on the theme.

 Many thanks for you help,

G. Suner
------------------------------------------------------------------------ 
Dr Guillermo A. Suner; Dep. de Quimica, UNIVERSITAT DE LES ILLES BALEARS
E-07071-Palma de Mallorca, SPAIN.
E-mail: guillem@gauss.uib.es    Tel: + 34 71 173498  Fax: + 34 71 173426 
WWW URL: http://www.uib.es/depart/dqu/dquo/suner.html

From laidig@pg.com  Thu Sep  7 10:29:02 1995
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From: laidig@pg.com (Bill Laidig)
Message-Id: <9509071011.ZM3403@morpheus.na.pg.com>
In-Reply-To: Ferenc.Molnar@chemie.uni-regensburg.de (Ferenc Molnar)
        "CCL:M:normal modes summary" (Sep  7,  3:38pm)
References: <9509071338.AA01245@rchsg8.chemie.uni-regensburg.de>
X-Mailer: Z-Mail (3.2.1 6apr95 MediaMail)
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All,

In a recent C&E News article an approximate electronic structure method
called MEDLA by Prof. P.G. Mezey was discussed. I was asked by my boss if
this really was the greatest invention since sliced bread as the article
implied. Since I am not familar with this method I was wondering if any
of you have thoughts on the subject. Also, is this technique similar
to Yang's divide-and-conquer approach? I will summarize to the list if
I get any responses. Bill

-- 
******************************************************************************
*    "Like jewels in a crown, the precious stones glittered in the queen's   *
*     round metal hat." - Jack Handey                                        *
*                                                                            *
*     Bill Laidig                                                            *
*     The Procter & Gamble Co.             tel 513-627-2857 fax - 1233       *
*     Miami Valley Laboratories            laidig@pg.com (preferred)         *
*     P.O. Box 538707                      wd_laidig@pg.com                  *
*     Cincinnati, OH 45253-8707            laidig@qtp.ufl.edu                *
******************************************************************************

From kessi@psizi1.psi.ch  Thu Sep  7 11:28:58 1995
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To: chemistry@www.ccl.net
Subject: [Q] Empty force field for pure electrostatics
X-Mailer: [XMailTool v3.1.2b]


Hi everybody,

After doing a DFT calculation on a molecule, I would like to look at the
purely electrostatic effects. Is there an easy way to do this
using the Discover software? Since I'm not very familiar with defining
my own force fields, could somebody point out to me what parts of the
*.frc file I need to change/drop/add so the only interactions which
will be taken into account will be the Coulomb interactions between the
point charges?

In addition, how can I assign the charges to the atoms using Mulliken
charges computed in DMol/DSolid? What intermediate file format would
I need to create and read into Insight? If I write a car/mdf pair of
files and read in the molecule from them, will the charges read from the
mdf file be used?

I realize that it's overkill to use Discover for the job. Maybe
someone can point me to a public domain code for point charge
electrostatics (periodic and molecular)?

Thanks for any help! Best regards,

Alain

--
Alain Kessi (alain.kessi@psi.ch)
Paul Scherrer Institut, Zuerich, Switzerland

From paul@tammy.harvard.edu  Thu Sep  7 12:59:03 1995
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Date: Thu, 7 Sep 95 12:48:59 -0400
From: paul@tammy.harvard.edu (Paul Lyne)
Message-Id: <9509071648.AA05488@tammy.harvard.edu>
To: chemistry@www.ccl.net
Subject: CADPAC
Cc: paul@tammy.harvard.edu


Hi,

Does anybody have a makefile for CADPAC for the HPUX
or DECALPHA computers?

Thanks in advance,

Paul

From gotwals@mcnc.org  Thu Sep  7 13:59:04 1995
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To: chemistry@www.ccl.net
From: gotwals@mcnc.org (Bob Gotwals)
Subject: CCL:Computational Chemistry Web Course


The North Carolina Supercomputing Center (NCSC), a part of the non-profit
advanced technologies group known as MCNC, located in Research Triangle
Park,NC, is pleased to offer an on-line course entitled  "Computational
Chemistry for Chemistry Educators". This course is intended for secondary,
community college and undergraduate educators of chemistry, as well as
graduate students who are interested in chemistry education.  The course
syllabus and registration information can be viewed by setting your World Wide
Web browser to this URL:

http://www.mcnc.org/HTML/ITD/NCSC/ccsyllabus.html

Description of the workshop:

The goal of this course is to introduce chemistry educators to
computational techniques in quantum chemistry.  The course is intended as
an enrichment activity, designed to help educators understand the use of
high-performance computing tools and their role in chemical research.
Educators are not expected to integrate these technologies into their
teaching activities, but the course will offer discussions on how this
might be accomplished for those educators interested in doing so.

Using commercial third-party software (Gaussian94 and MOPAC) resident on
the North Carolina Supercomputing Center's Cray Y-MP supercomputer,
educators will investigate, using computational tools,techniques, and
technologies,  a number of chemical properties, such as single-point
energies, geometry optimizations, frequency calculations, potential energy
surfaces, and thermochemical properties.

Participants will also have the opportunity to complete a number of case
studies for potential use in the classroom.

Prerequisites:

Participants must have access to the Internet via the World Wide Web (WWW),
preferably using Netscape 1.1.  Text-based access (i.e., via lynx) is
inadequate.  Access assumes electronic mail capabilities.  Participants who
have Internet connections through America Online or other non-Internet
service are advised to ensure good Web connectivity prior to registering.

Educators should also have a basic background in quantum chemistry and
atomic structure.  Completion of a basic course in physical chemistry at
the undergraduate level is the appropriate level.  A solid mathematics
background, particularly in calculus, is helpful but not mandatory.
Participants should also have basic computer literacy skills:  use of a
word processor, basic understanding of the concepts of an operating system,
keyboarding skills, etc.  A UNIX background is helpful but not required. No
programming skills are required.  Prospective participants who wish to
discuss their qualifications PRIOR to registering are encouraged to do so
with the instructor.

Workshop Logistics:

The course is designed as a self-paced "seminar" series, consisting of 15
sessions.  Each week, a new topic and assignment will be posted to the
World Wide Web.  Students need to complete the reading and assignment, ask
questions via electronic mail, and submit their work via email to the
course instructor.  Students will be able to interact via an email
discussion list (listserv).  All reading materials and resources are
available electronically, although the use of a basic physical chemistry
textbook (Atkins is recommended) is strongly advised.

Access to the lessons and the supercomputer will begin on October 3, 1995,
and will close on February 16, 1996.  The course instructor will be
available for electronic support during that period.

The fee for this activity is $150.  Tuition includes access to all Web
materials, addition to the class discussion group maililing list, and
computing time on the supercomputer.   As there is limited enrollment,
participants are asked to give considerable consideration to their
commitment PRIOR to registering for this activity.  The course will require
time (roughly four to five hours per week), effort, and intellectual
energy.  At this point, no grades or continuing education credit is
available; however, certificates of completion with an accompanying
descriptive letter are provided to all course "graduates".

To register for this course, complete the form below and email it to Robert
R. Gotwals (gotwals@mcnc.org).  There is limited enrollment in this course.
Registration is on a first-come, first-serve basis.

Please feel free to send questions about this course to gotwals@mcnc.org

Tentative Schedule:

Session 1:  Overview of Computational Chemistry;  Overview of the Cray Y-MP
and the UNIX operating system

Session 2:  Logging On;  Using Gaussian94 on the Cray supercomputer;
creating and submitting G94 input files

Session 3:  Basis sets and approximations;  Input file options;
Calculating Single Point Energies

Session 4:  Single Point Energies. Analyzing output files

Session 5:  Case Study:  Energies of Isomers

Session 6:  Geometry Optimizations I

Session 7:  Geometry Optimizations II

Session 8:  Preparing Geometry Inputs

Session 9:  Frequency Calculations I

Session 10:  Frequency Calculations II

Session 11:  Potential Energy Scans

Session 12:  Case Study/Teaching Module:  Problem Development and Investigation

Session 13:  Case Study/Teaching Module:  Lab Writeup and Instructor Guide

Session 14:  Overview of other tools for computational chemistry; Classroom
integration

Session 15:  "Final Exam";  Course Wrap-up / Evaluation

******************************************************************
                    "Computational Chemistry for Chemistry Educators"
                                Registration Form



Last Name:                         First Name:

Position:

Phone:

Curriculum Area:

Primary Courses Taught (intro, AP Chem., etc.)



School:                                           District( if appropriate):

School Address:




FAX:

E-mail Address:

Degree(s):       BS [ ]       MS [ ]       Doctorate [ ]       Other [ ]

Subject area(s) of degree(s):

Years of Teaching Experience:   1-5 [ ]   6-10 [ ]   11-15 [ ]   >16 [ ]

Years of Technology Experience: 1-5 [ ]   6-10 [ ]   11-15 [ ]

Do you own your own computer system?       Yes [ ]      No [ ]

If yes, indicate the hardware platform:

Describe the hardware you will use to access the Web lessons:



Describe your Web connection (Dialup SLIP or PPP, America Online, etc.)



Describe your chemistry, mathematics, and computing background (coursework,
workshops, experiences, etc.)











Return this registration form to Robert R. Gotwals, Jr.(gotwals@mcnc.org)
or by FAX (919) 248-1101.

We are unable to process credit card payments.  Send tuition check or PO
(payable to MCNC) to:


                        Robert R. Gotwals, Jr.
                        Course Instructor

                                -OR-

                        Faye McLean Ellis
                        Course Registrar
                        North Carolina Supercomputing Center
                        3021 Cornwallis Road
                        Research Triangle Park, NC 27709



















From monty@seminole.chem.wisc.edu  Thu Sep  7 15:14:04 1995
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Date: Thu, 7 Sep 95 14:05:34 CDT
From: "J. Monty Wright" <monty@chem.wisc.edu>
Subject: Re: CCL:G:NBODel Utility on G92
To: CHEMISTRY@www.ccl.net, guillem@gauss.uib.ES
CC: weinhold@chem.wisc.edu
X-Mailer: LeeMail 2.0.4
Message-Id: <AC74ACAF@seminole.chem.wisc.edu.>


I passed G. Suner's question on to Prof. Frank Weinhold, author of NBO, and his 
reply follows:

Q:
>I would like to know how can be done a NBO Fock matrix deletion procedure on 
>G92, particularly by setting some NBO Fock matrix elements to zero and 
>reevaluating the energy. G92 manual refers to NBO separate manual, but 
>unfortunately I have no access to that one. Which methodology do I have to 
>follow? An example G92 input data would be most welcome, as well as any 
>suggestion on the theme.

A:
Gaussian, Inc. should provide a copy of the NBO manual on request.
NBO Fock matrix deletions are described in Sec. B.5  There are nine
separate deletion types, for deleting everything from entire
orbitals to selected blocks of intermolecular matrix elements.
A simple example of the syntax for deleting 3 Fock matrix elements is:

   $DEL
     DELETE 3 ELEMENTS  1 15  3 19  23 2
   $END

All $DEL keylists need the POP=NBODel keyword on the route card.  FW
*********************************************************************

                      J.M.-Monty- Wright
             Research Assistant (C.R. Landis Labs)
  Molecular Modelling and Solution Structure Determination
            in Support of Rational Catalyst Design



From jkl@ccl.net  Thu Sep  7 17:29:03 1995
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From: h9290218@hkusua.hku.hk (Danny Yau)
Message-Id: <9509071829.AA01140@hkusua.hku.hk>
Subject: Conference which held in NOV. or Dec. in 1995
To: chemistry@ccl.net
Date: Fri, 8 Sep 1995 02:29:30 +0800 (HKT)
Cc: h9290218@hkusua.hku.hk (Danny Yau)
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Dear Netters,

	Would anyone know that are there any computational chemistry
	conferences(included Monte-Carlo simulation, Molecular dynamic,
	theoretical calculation etc.) will be held in November or
	December 1995 in U.S.A or Canada? 
	Even some sort of chemistry conference which include the above topic is
	also welcome. I would be much appreciated if you could provide those
	information to me.
	Thanks in advance.

Best wishes,
-- 
Danny H.L.Yau                   email: h9290218@hkursc.hku.hk   
Department of chemistry,           or  h9290218@hkuxb.hku.hk
The University of Hong Kong.		

From jkl@ccl.net  Thu Sep  7 18:44:03 1995
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Message-ID: <n1401634374.22520@qmail.fullerton.edu>
Date: 7 Sep 1995 15:31:16 -0800
From: "Steve Hardinger" <steve_hardinger@qmail.fullerton.edu>
Subject: Animations and Spartan
To: "CCL" <chemistry@ccl.net>
X-Mailer: Mail*Link SMTP-QM 3.0.2


                      Subject:                              Time:  3:40 PM
  OFFICE MEMO         Animations and Spartan                Date:  9/7/95

Hello CClers...

I've been working with trying to animate the rotaion of n-butane with Spartan.
 Everything works very well, but I would like to improve the presentation. 
I'd like to know (1) can I change the speed at which the frames are presented,
and (2) how can I get the view to stay the saem, i.e, always along the c2-c3
bond axis?

Any suggestions will be helpful.  I'll post a summary if it all works out.


Steve Hardinger
California State University Fullerton
shardinger@fullerton.edu


From iiv@mmlds1.pha.unc.edu  Thu Sep  7 18:59:04 1995
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Date: Thu, 7 Sep 1995 19:02:42 -0400 (EDT)
From: Iosif Vaisman <iiv@mmlds1.pha.unc.edu>
To: chemistry@www.ccl.net
Cc: Naomi Siew <SIEW@vms.huji.ac.il>
Subject: Re: Side-chain conformation data bank
Message-Id: <Pine.ULT.3.91.950907185521.11267G-100000@mmlds1.pha.unc.edu>
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> I am looking for a bank of side chain conformations.
> Can anyone help me with that?

> Thank-you very much,
> Naomi Siew
> siew@vms.huji.ac.il

Roland Dunbrack's backbone-dependent rotamer library is available at 
http://www.cmpharm.ucsf.edu/public/resources.html

   The backbone-dependent rotamer library and a program for its use provide 
a fast means of predicting sidechain conformation from backbone phi and psi 
values. These methods can be used for homology modeling and structure 
refinement by x-ray and NMR.

  References: 
R. L. Dunbrack Jr. and M. Karplus. "Backbone-dependent Rotamer Library 
for Proteins: Application to Side-chain prediction." J. Mol. Biol. vol. 
230, 543-574 (1993).

R. L. Dunbrack Jr. and M. Karplus. "Conformational analysis of the
backbone-dependent rotamer preferences of protein sidechains." Nature 
Structural Biology, 1, 334-340 (1994).



Iosif Vaisman
UNC - Chapel Hill

From jkl@ccl.net  Thu Sep  7 20:14:04 1995
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Date: Thu, 7 Sep 95 17:11:14 -0700
From: hcj@mazda.wavefun.com (Harry C. Johnson)
Message-Id: <9509080011.AA07591@mazda.wavefun.com>
To: steve_hardinger@qmail.fullerton.edu
Cc: chemistry@ccl.net
In-Reply-To: <n1401634374.22520@qmail.fullerton.edu> (steve_hardinger@qmail.fullerton.edu)
Subject: Re: CCL:Animations and Spartan
Reply-To: hcj@wavefun.com


>>>>> "Steve" == Steve Hardinger <steve_hardinger@qmail.fullerton.edu> writes:

    Steve> I've been working with trying to animate the rotaion of
    Steve> n-butane with Spartan.  Everything works very well, but I
    Steve> would like to improve the presentation.  I'd like to know
    Steve> (1) can I change the speed at which the frames are
    Steve> presented, and (2) how can I get the view to stay the saem,
    Steve> i.e, always along the c2-c3 bond axis?

1) There is no current way to control the speed of the animations.  If
the animation is too fast (the usual case) you can generate more
conformers which will produce a smoother animation, or get a slower
machine 8^)  Also the addition of surfaces will often slow things down
considerably, so there is often a trade off between the rate of
animation of the structure alone, and the structure with surfaces.

Future versions of Spartan will most likely include some mechanism for
controlling the animation rate directly.

2) When animating a series of conformations it is usually desirable to
specify the 'NOMOVE' keyword in the setup dialog of the appropriate
energy calculation method (mechanics, semi-empirical, or ab initio).
Without NOMOVE the optimization methods will re-orient the molecule in
an attempt to recognize symmetry within the molecule.  It is usually
also desirable to specify 'ENFORCE' and 'DUPLCHECK=NONE' in the
conformational analysis setup as well.  This prevents the particular
dihedral of interest from changing as a result of optimization
(enforce), and also turns off duplicate checking.

Hope this helps!
-Harry

+-----------------------+------------------+-------------------------+
|Harry C. Johnson IV    |  ______________  | E-Mail: hcj@wavefun.com |
|Computational Chemist  |  \  _________	/  | Phone:  (714)955-2120   |
|Wavefunction Inc.      |   \ \\\\\\\\/	   | Fax:    (714)955-2118   |
|18401 Von Karman       |    \ \\\\\/	   |                         |
|Suite 370              |     \	\\/        | "Seems to me its all    |
|Irvine, CA 92715       |      \/	   |  just chemistry" - RUSH |
+-----------------------+------------------+-------------------------+




From jkl@ccl.net  Thu Sep  7 20:44:06 1995
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 id <01HV03Y4GPI8019GFX@NAUVAX.UCC.NAU.EDU>; Thu,
 07 Sep 1995 17:35:53 -0700 (MST)
Date: Thu, 07 Sep 1995 17:35:53 -0700 (MST)
Subject: Cyclodextrin Z matrix or structures
To: chemistry@ccl.net
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Greetings to all!

A colleague of mine wishes to do some calculations on cyclodextrins.  To
those who are unfamiliar with these molecules, they are cyclic sugar-
containing systems with either six (alpha-cyclodextrin), seven (beta-
cyclodextrin), or eight (gamma-cyclodextrin) sugar residues.

Thus, my colleague would like to find either atomic coordinates or a
workable Z-matrix for these molecules.  If anyone out there can assist
him, please reply to me, and, while passing along the information to my
colleague, I shall post the results to the CCL as well.

Thanks in advance for any assistance given!

Robert W. Zoellner, Ph.D.
Associate Professor of Chemistry
zoellner@nauvax.ucc.nau.edu

From markm@portal.vpharm.com  Thu Sep  7 23:29:07 1995
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From: markm@portal.vpharm.com (Mark Murcko)
Message-Id: <9509080308.AA16453@portal.vpharm.com>
Subject: metabolism sites in aromatic rings
To: chemistry@www.ccl.net
Date: Thu, 7 Sep 1995 23:08:29 -0500 (EDT)
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I know this is a widely-studied field, and I am currently
in the midst of collecting references, but I thought it
would also be wise to tap the Collective Wisdom of the group
on the following topic: 

What molecular orbital methods have been DEMONSTRATED to do 
the best job of explaining/predicting/rationalizing the 
positions on aromatic rings which undergo different types 
of metabolic events?  For example, P450 or xanthine oxidase 
oxidation, etc.  Any help appreciated.

/ Mark (markm@vpharm.com)

From markm@portal.vpharm.com  Thu Sep  7 23:40:39 1995
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From: markm@portal.vpharm.com (Mark Murcko)
Message-Id: <9509080301.AA16439@portal.vpharm.com>
Subject: Summary of metal-bound water pKa data
To: chemistry@www.ccl.net
Date: Thu, 7 Sep 1995 23:01:50 -0500 (EDT)
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Here is a summary of the responses to my recent question about 
the pKa of waters bound to metals in proteins.  Thanks to all
who contributed!

/ Mark (markm@vpharm.com)

=================================
From: lasse@KVLVAX.kvl.dk (Lars Hemmingsen)

concerning your question about pKa's of metalbound water in proteins:

For the zinc enzyme horse liver alcohol dehydrogenase I can give you the 
following values (NAD+/NADH is a coenzyme, which binds close to the metal)

LADH-H2O: pKa=9.2,   LADH-NAD+-H2O: pKa=7.6, LADH-NADH-H2O: 11.2
(Kvassmann and Pettersson 1980 Eur. J. Biochem., 103, 565-575 
and Kvassmann and Pettersson 1987 Eur. J. Biochem., 166, 167-172.

and for the same enzyme with the zinc ion exchanged with cadmium:
LADH-H2O: pKa=11.0, LADH-NAD+-H2O: pKa=9.2, LADH-NADH-H2O: Not measured
(Hemmingsen et al. 1995 Biochemistry, 35, 7145-7153.

Furthermore pKa's have been measured, by the group of professor Michael
Zeppezauer in Saarbrucken, for the same enzyme with the zinc ion
exchanged with cobalt (the references and numbers are in the Biochemistry
reference). If you want more pKa-values I would suggest that you contact
the poeple in Saarbrucken, Germany (fax: +49 681 302 2097)

=================================
>From HMARQUES@AURUM.CHEM.WITS.AC.ZA Thu Aug 17 00:40:22 1995 (Helder Marques)

We compared the pKa of H2O bound to a hemepeptide to pKas in 
hemoproteins in J. Inorg. Biochem, 27, 245-254 (1986)

=================================
From: Steve Cabaniss <SCABANIS@KENTVM.KENT.EDU>

     The hydrolysis constant of a metal can be written as an acid dissociation
constant, comparable to the  Ka for any 'normal' acid.  The pKa's can thus be
looked up in any standard compendium (i.e., Smith and Martell).  I believe the
most authoritative review is "Hydrolysis of Cations" by Baes and Mesmer.
(Of course, this is all simple aqueous solution chemistry, not the active sites
 of proteins.)  Fe(III) thus 'induces' a water pKa of 2-3.

=================================
From: vg857@dewar.pnl.gov (Yajun Zheng)

 You asked about references concerning pK's of metal-coordinated waters in 
 enzymes.  I have several references. The most famous case is Zn 
 metalloenzymes. The pKa for Zn-Water in human carbonic anhydrase II (HCAII) 
 is 7. In alcohol dehydrogenase (ADH) is about 7.6. In SOD the Cu-Water is 
 about 9. The pKa values usually vary depending on active site environments. 
 In xylose isomerase the value is about 7-9 (in this case, the metals are 
 either Mg2+ or Mn2+). There are also other examples such as DNA related 
 enzymes. 

     For ADH, Kvassman, J.; Pettersson, G. Eur. J. Biochem. 1980, 103, 565.
     also, in Zinc Enzymes; Bertini, I. et al. 1986.

     For HCAII, See the above book or Zheng and Merz, JACS 1992, 114, 10498.

     For SOD, I do not have the exact reference, but you could check Joan 
     Valentie papers.  

     For xylose isomerase and DNA related enzymes, there is no exact numbers 
     and most are just guesses. 

=================================
From: teoulf@garm.teokem.lu.se (Ulf Ryde)

For horse liver alcohol dehydrogenase,
G. Pettersson, CRC Crit. Rev. Biochem. 21 (1987)349-389
gives an excellent reviev of pKa values of zinc bound water
(an other ligands) in different complexes.

For carbonic anhydrase, 
Campbell et al., J. Mol. Biol. 90 (1974) 469-489 reports
a pKa between 7 and 8.

For carboxypeptidase the situation is more complicated, but
Auld et al. Biochem. 31 (1992) 3840 gives a pKa of 9.0

Similarily, for thermolysin,
Mock et al., Biochem. J. 302 (1994) 57-68 
provides a recent discussion of pKa values.

Aquist and Warshel, J. Am. Chem. Soc. 112 (1990) 2860-2868
have a more general discussion about pKa values for 
metal bound water molecules in different enzymes.

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