From toukie@zui.unizh.ch  Thu Jan 30 06:19:48 1997
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Date: Thu, 30 Jan 1997 11:25:47 +0100
To: chemistry@www.ccl.net
From: "Hr. Dr. S. Shapiro" <toukie@zui.unizh.ch>
Subject: Cosmo Player version 1.0 beta 3




Dear Colleagues;

        I have just examined the Cosmo Player version 1.0 beta 3 version be-
ing distributed by SGI for Windows 95, and I see that it is set to expire on
1 April 1997.  Does anyone know with what it will be replaced, and will that
replacement be distributed gratis or on a fee-basis only?

        Thanks in advance to all responders.


Sincerely,

S. Shapiro
ZH
toukie@zui.unizh.ch



From toukie@zui.unizh.ch  Thu Jan 30 08:19:59 1997
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Date: Thu, 30 Jan 1997 13:40:21 +0100
To: chemistry@www.ccl.net
From: "Hr. Dr. S. Shapiro" <toukie@zui.unizh.ch>
Subject: Hammett ortho substituent constants?




Dear Colleagues;

        It is my understanding that Hammett sigma constants are restricted
to substituents at meta and para positions because steric influences on the
functionality at C-1 (e.g., COOH, OH) cannot be clearly distinguished from
electronic influences, whereas steric influences on the functionality at C-1
by substituents in the meta or para positions is negligible.

        Has anyone ever undertaken (and pubished) a detailed analysis of the
influence of ortho substituents in an effort to factor the influence of
ortho substituents in to electronic and steric components?  I note that in
the 1982 book "pKa Prediction for Organic Acids and Bases" by D. D. Perrin,
B. Bempsey, and E. P. Serjeant Appendix A.5 is a small list of apparent
sigma ortho values.  Does anyone know of a more recent and/or extensive
lists, particularly ones containing values factored into steric and
electronic components for benzoic acids and phenols?

Thanks in advance to all responders,

S. Shapiro
toukie@zui.unizh.ch



From ccl@www.ccl.net  Thu Jan 30 09:19:51 1997
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Date: Thu, 30 Jan 1997 10:16:02 -0330 (NST)
From: Uli Salzner <uli@smaug.physics.mun.ca>
To: ccl <chemistry@ccl.net>
Subject: dft/user defined methods
Message-ID: <Pine.SGI.3.91.970130092932.24180A@smaug.physics.mun.ca>
MIME-Version: 1.0
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Status: RO
Content-Length: 6644



Hi everybody,
thanks to Doug Fox, AEleen Frisch, Joe Durant, Mikhail Gloukhovtsev, and 
Marta Fores, who answered my questions about how to use user defined DFT 
methods in G94 and how to define a half/half functional. In short there 
is indeed a typo in the Reference Guide (the one with the red spiral). 
This is corrected at the Gaussian web site (address see below). I also 
learned how to set the parameters. The original answers are appended.

One question on the side. When I submit to the list, I simply put in the 
address of the ccl. My mail arrives but the ccl address appears where my 
address should be in the mail header. Obviously I am doing something 
wrong here. Can somebody explain to me, how to submit to the ccl properly?

Thanks again,

Ulrike Salzner
Department of Chemistry
Memorial University of Newfoundland
St. Johns, NF A1B 2N5
Canada

Tel.: (709) 737-2151
Email:uli@smaug.physics.mun.ca


_____________________________________________________________________________
From: Doug Fox


   Dr. Salzner,

    The BHandH/BHandHLYP functionals as implemented in G92/DFT have been
restored due to popular demand starting with G94 Rev. C.3 so you may be 
able to simply use the keywords.  If you have an earlier version the
input to duplicate the G92/DFT functionals would be,

  BHandH:

  # SLYP IOP(5/45=10000500, 5/46=00000500, 5/47=10001000)

  BHandHLYP:

  # BLYP IOP(5/45=10000500, 5/46=05000500, 5/47=10001000)

> 
> To whom it may concern:
> 
> using the DFT user defined methods in G94, user's reference p.61-62, 
> I am trying to construct something like a half/half functional but I 
> have problems to get the order of the coefficinets right. 
> >From the B3LYP description (p.61) I gather the coefficients for B3LYP 
> to be:
> 
> 0.8 for Slater, 0.2 for HF, 0.72 for Becke, 0.19 for VWN, and 0.81 
> for LYP.
> 
> If I transfer this to the formula below I get:
> P1=1.0, P2=0.2, P3=0.72, P4=0.8, P5=0.81, and P6=0.19
> 
> According to the B3LYP example on p. 62 the coefficients should be:
> P1=1.0, P2=0.8, P3=0.2, P4=0.72, P5=0.19, and P6=0.81
> 
> My question is, have I mixed up something or is there a problem with 
> this example? Since it would lead to fatal errors, if I got these 
> coefficients mixed up, I would be very grateful for commends.
> 
____________________________________________________________________________

Received: by m10.lorentzian.com; Mon, 27 Jan 1997 10:03:13 -0500
From: aefrisch@lorentzian.com (AEleen Frisch)
X-Status: 

There was a typo in the first printing of the manual on these pages (with
the red spiral binding). Check our web page (www.gaussian.com/00000432.htm
is the exact document you want)) or the release notes that came with the program
for updates.

Your values for P1 through P5 appear to be correct from my brief glance. However,
be aware that in order to get the local part of LYP, you want P6 to be 1.0 (P5
is just the gradient correction part).

Finally, the BHandH keyword may also provide what you want. Again, see the release
notes or the web site.

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

Message-Id: <199701271601.QAA16643@mephisto.ca.sandia.gov>
To: uli (Uli Salzner)
Date: Mon, 27 Jan 1997 08:01:22 -0800 (PST)
X-Mailer: ELM [version 2.4 PL23]

Hi Uli!

It's been awhile since I dug into the Gaussian manual, so I won't try
that.  However, appended is my explicit route statement for running
Gaussian's implementation of BHandHLYP (which is not Becke's!).

I remember finding multiple errors in the comment cards describing the
route options; wouldn't surprise me that they found their way into the
manual.  My advice is run B3LYP, and then your explicit B3LYP; if you
got it right, then they should be identical.  I read alot of the
source code to figure out what they were actually doing; that is
another option.

Hope this helps.

Joe
-- 

####################################################################
#  Joe Durant                      voice:  (510) 294-3343          #
#  Mail Stop 9057                  FAX:    (510) 294-2276          #
#  Sandia National Laboratories    jdurant@ca.sandia.gov           #
#  Livermore, CA  94551            http://mephisto.ca.sandia.gov   #
####################################################################

# BLYP 6-31G* scf=direct 
iop(5/45=10000500, 5/46=05000500, 5/47=10001000)

BHANDHLYP

0,1
H
H,1,HH
     Variables:

________________________________________________________________________________

Subject: BH&HLYP
Status: RO
Hi, Ulrike:

You can find some info at the Gaussian Web site (www.gaussian.com; FAQ secti=
on).
Please note that the implementation of the BH&HLYP functional in
Gaussian-94 (Rev. D and higher) is as follows: ExcBH&HLYP =3D 0.5 ExLSDA +
0.5 ExHF + 0.5=90EB88 + EcLYP + EcVWN.  Note that this formulation slightly
differs from that proposed by Becke. Furthermore, the answer on BH&HLYP
given in the FAQ also differs
>from the implementation in G-94.

With best wishes,

--------------------------------------------------------
Mikhail Gloukhovtsev
Room 275, Brown Laboratory
Department of Chemistry and Biochemistry
University of Delaware
19716   DE
Phone # 302 831-0887
E-mail mng@UDel.edu
WWW http://udel.edu/~mng/
--------------------------------------------------------

---------------------------------------------------------------------------------
Status: RO
	showed that in the B3LYP example on p. 62 there
	was a mistake. So, in order to get some energy as
	the one provided by the B3LYP default keyword we
	had to use the following parameters:
	P1=1 P2=0.2 P3=0.72 P4=0.8 P5=0.81 P6=1 and not
	P1=1 P2=0.8 P3=0.2 P4=0.72 P5=0.19 P6=0.81 as
	pointed by the set G94 Users reference Manual.

	Hope this helps,


					Marta


 -*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-
 Marta Fores                                _/      _/        _/  _/_/_/_/
 Institut de Quimica Computacional         _/      _/        _/  _/
 Universitat de Girona                    _/      _/  _/ _/ _/  _/  _/_/
 Albereda 3-5                            _/      _/  _/    _/  _/    _/
 17071 Girona, CATALONIA (Spain)          _/_/_/    _/ _/ _/  _/_/_/_/
 Voice +34.72.41.83.57
 FAX   +34.72.41.83.61                                 _/   _/_/_/  _/_/_/
 World Wide Web: http://stark.udg.es/cat/marta.html   _/   _/  _/  _/
 e-mail: marta@stark.udg.es                          _/   _/  _/  _/
                                                    _/   _/_/_/  _/_/_/
                                                           _/
 -*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-





From ccl@www.ccl.net  Thu Jan 30 18:19:54 1997
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Date: Thu, 30 Jan 1997 18:05:56 -0500
To: chemistry@ccl.net
From: bausch@rs6chem.chem.vill.edu (Joseph W. Bausch)
Subject: question about the STABLE keyword in G94




I have read in the "Exploring Chemistry With Electronic Structure Methods"
that  stability of scf solutions on unknown systems should be checked with
the STABLE calculation.  I am wondering about what the implication is if an
optimized geometry then gives an instability in the wavefunction.  With the
Stable=opt keyword the wavefunction is reoptimized to lower energy, but the
book says this is not a geometry optimization.  So, my question is, is this
optimized geometry (that a vibrational analysis has indicated is a mimimum
with no imaginary frequencies) still legitimate?  Or after this new lower
energy wavefunction has been determined with the stable=opt run does
another geometry optimization beginning with this new wavefunction need to
be carried out?

Thanks in advance,
JWB
bausch@rs6chem.vill.edu
-----------------------




From ccl@www.ccl.net  Fri Jan 31 13:29:39 1997
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From: "Wilson, Bruce" <bewilson@eastman.com>
To: "'chemistry@ccl.net'" <chemistry@ccl.net>
Cc: "'bewilson@eastman.com'" <bewilson@eastman.com>
Subject: Summary re term symbols
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Following is the information I received regarding references on
term symbols.  Thanks to Lutfur Khundkar, J. Grant, Ole Swang,
and Richard Bone for their time in responding.  
 
I found both McQuarrie's book and Atkin's book in the library
and have been reading through those.  

----From lkhundkr@neu.edu (Lutfur Khundkar)
Don McQuarrie's "Quantum Chemistry" has an excellent section on naming
and deriving atomic term symbols. The molecular symmetry symbols I
learned from Cotton's book "Chemical Application of Group Theory" as
well as from Herzberg's bible on Molecular spectroscopy. Herzberg's
books are comprehensive, but nowhere as eloquent as McQuarrie's.

-------From hert0531@argon.chem.TU-Berlin.DE (Roland Hertwig)
In principle, Atkins' books suit the purpose. Look for "Physical
Chemistry" 
or even better "Molecular Quantum Mechanics" by P.W. Atkins (OXford
University Press). Also a good book is "Quantum Chemistry" by I.R.A.
Levine.
(Prentice Hall International).

--------From jeg10@po.cwru.edu (J. Grant)
The Text "Spectrophotometric Identification of Organic Compounds"
Fifth Edition, by Silverstein, Bassler and Morrill contains a
through chapter (20 pages) with a bibliography (at chapter's end)
that I have found useful.

-----From Ole.Swang@si.sintef.no (Ole Swang)
The following books all treat group theory for molecules:

F. A. Cotton: "Chemical Application of Group Theory"
P. W. Atkins: "Molecular Quantum Mechanics"
F. L. Pilar: "Elementary Quantum Chemistry"

Cotton's book is the classic. The two others are textbooks on quantum
chemistry, with chapters on molecular symmetry.

-----From rgab@easynet.co.uk (Richard Bone)
I'm not sure if you'll have had a  flood of replies about this yet but
two books I found useful in the education system phase of my life were:

P. W. Atkins,  Molecular Quantum Mechanics (Oxford University Press)
M. Gerloch,  Orbitals, Terms and States.

The first one has useful and accurate discussion in places though is not
very expansive.

The second book is a specialist work devoted to the entire subject in
its
minutiae ...

Otherwise, failing that, I always found solid spectroscopy books, e.g.,
by G. Herzberg, to be valuable in these areas.  I wouldn't settle for
any
undergraduate level spectroscopy text book though as it won't be precise
enough or full enough for your aims.



=================================================================
Bruce E. Wilson (bewilson@eastman.com)
Chemical Information Services, B-150B, Lincoln Street
Eastman Chemical Company
Kingsport, TN  37662-5150
Voice: (423) 229-8886  FAX: (423) 229-6114 

"Opinions are mine, but available free of charge."


From mn1@helix.nih.gov  Fri Jan 31 18:20:07 1997
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Date: Fri, 31 Jan 1997 17:59:33 -0500 (EST)
From: "M. Nicklaus" <mn1@helix.nih.gov>
Message-Id: <199701312259.RAA20320@helix.nih.gov>
To: CHEMISTRY@www.ccl.net
Subject: G94(Sum.+Q): Problem with PES Scan in DFT
Cc: mn1@helix.nih.gov




Dear CCL'ers,

This is the, maybe preliminary, summary of the responses I got 
to my question concerning a problem with PES Scan in DFT in G94.
A few follow-up questions are appended.

@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@

Question:
=========

? I seem to be having a problem with a Potential Energy Surface (PES) scan
? in G94.  I am running a relaxed PES scan on a nucleoside analog, trying
? to rotate the base.  I am running this job at the DFT method/basis set
? B3LYP/6-31G(d).  I'm using cartesian coordinates (a newzmat-generated
? input file with a Z-matrix didn't work previously), pre-optimized at
? the same level of theory from X-ray coordinates.
?
? For the first few conformations, everything seems to have proceeded nicely;
? i.e., the energy started out some 20 kcal/mol or so above the (presumed)
? global energy minimum, and then came down, during the partial optimization,
? to a reasonable value a few kcal/mol above the global min.
? With the current conformation, however, the job seems to be stuck, since
? for nearly 20 steps now, the energy has only been oscillating in a narrow
? band. [rest omitted]

@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@

Responses:
==========

From: Jan Labanowski <jkl@ccl.net>

Try to see, if you have very closely spaced HOMO/LUMO -- usually, due
to Self Interaction problem of DFT, the SCF will oscillate in this case.
I do not know how to fix it in G9X, since I do not use it for DFT, but
other problems have some options, like DMIX (a portion of new density
to be mixed with old density for new SCF iteration), or freezing occupances,
or level shifting technique, or smear approach. If some of those are
available in gaussian, use them. Going on with the run will not help,
it will just keep oscillating. Of course, I may be wrong as to the cause,
since I did not see your MO energies.

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

From: Jennie.Weston@org.chemie.uni-giessen.de (Jennie Weston)

The problem is probably that the optimizer routine is taking too big
steps for your pot E surface. You are apparently in the region of a very
flat minimum (maybe the thing is quite rotationally flexible??). The routine
must step smaller in order to find the stationary point. Kill the job at 
once, further comp time is just wasted. Cut out the geometry corresponding 
to the lowest energy in the many optimization cycles. Use it to make a new
input file (so you don't loose the work already done) (so you don't loose
 the work already been done on the optimization). Include (For Gaussian)
the option opt=tight in the key word line. If this still doesn't work, use
opt=verytight. This decreases the tolerances for the optimization routine
and forces it to step smaller. However, it takes more comp time.

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

From: d3g359@fido.pnl.gov (John Nicholas)

Marc, yes I have seen it often with dft in G94. I do not know the origin
of the problem. I would guess the job may never converge. However,
you should check the forces, if the forces are still high, then maybe
something is wrong other than g94's problem with convergence.

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

From: Samuel_Mikes@hmc.edu

  Is it possible that you entered the step in degrees while the program read
it as radians?  Sometimes the documentation is incomplete or just plain
wrong.

@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@
 

Follow-up questions:
====================

1. Taking up Jennie's suggestion, I realized that this conformation
   may indeed be in a 'difficult' region of the energy surface
   It is quite possible that it is very close to a local maximum
   relative to the scanned torsion, i.e. close to the top of the 
   rotation barrier.  With this---and only this---torsion constrained
   to the presribed value in the scan, I think it is very well possible
   that the energy surface with respect to the remaining coordinates
   is very flat, or otherwise 'weird looking'.  Any thoughts, or
   experiences on this point?

2. Can one restart a PES scan job with tighter convergence for the
   optimization by using Opt=(Restart,Tight,AddRedundant); or will 
   restarting the job from the checkpoint file ignore the new 
   keyword "Tight" and proceed with the same settings as before?

3. How do I extract a specific structure from a PES scan checkpoint
   file; i.e., how do I tell newzmat that I want, say, the (structure
   of the) 17th step in the optimization of the 3rd conformation?


Thanks to all who responded, and thanks in advance to future responders.

Marc

------------------------------------------------------------------------
 Marc C. Nicklaus                        Lab. of Medicinal Chemistry
 e-mail: mn1@helix.nih.gov               National Cancer Institute, NIH
 Phone:  (301) 402-3111                  Bldg 37, Rm 5B29
 Fax:    (301) 496-5839                  BETHESDA, MD 20892-4255    USA
         WWW:  http://www.nci.nih.gov/intra/lmch/MCNBIO.HTM
------------------------------------------------------------------------



From ccl@www.ccl.net  Fri Jan 31 19:20:07 1997
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Date: Fri, 31 Jan 1997 18:22:57 -0500 (EST)
From: Steve Bennett <sbennett@wotan.duch.udel.edu>
To: CCL Users <chemistry@ccl.net>
Subject: Bond order analysis
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	I have recently started using DMol to calculate bond orders 
between transition metals and main group elements.  I am interesting in 
finding references concerning the Mayer implementation as in DMol and how 
it compares to other methodologies, such as NBO and Mulliken analyses.  
Any results will be compiled and summarized to the list.  Thanks in advance



Steven D. Bennett
University of Delaware                  Department of Chemistry
304A Drake Hall                         (302) 831-8720
sbennett@wotan.duch.udel.edu            (302) 737-8485
http://udel.edu/~sbennett/steves.html  

"Although the answer is not unknown, I'm searchin', searchin, and how
I've grown; It's not all right to say goodbye, and the world on a string
doesn't mean a thing"                     Neil Young






From AFED@ichuwr.chem.uni.wroc.pl  Sat Feb  1 07:20:15 1997
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From: "Adam Fedorowicz" <AFED@ichuwr.chem.uni.wroc.pl>
To: poul@ichuwr.chem.uni.wroc.pl
Date:          Sat, 1 Feb 1997 12:54:17 GMT+1
Subject:       Re: CCL:Summary DFT Programs
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Date sent:      Fri, 31 Jan 1997 14:07:06 +0100
From:           Alain Kessi <alain.kessi@psi.ch>
Organization:   Paul Scherrer Institut, Zuerich, Switzerland
To:             Cedric Merlot <cmerlot@cit.enscm.fr>
Copies to:      CCL Computational Chemistry List <chemistry@www.ccl.net>
Subject:        CCL:Summary DFT Programs

Cedric Merlot wrote:
> A week ago I asked for DFT Programs :

In your list of DFT software packages, you're missing Dmol, available
commercially from MSI (http://www.msi.com). The same code can do
molecules/clusters or crystals. It should be among the faster codes,
though I haven't recently done any comparisons.

(Caveat: the writer of the present message has links to the developers
of Dmol)

-- Alain Kessi (alain.kessi@psi.ch), at Paul Scherrer Institut, Zurich
     ++++ stop the execution of Mumia Abu-Jamal ++++
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                        Adam Fedorowicz
                        
              Faculty of Chemistry, Wroclaw University             
                      14, F. Joliot-Curie
                        50-383 Wroclaw
                phone (+48)(71)204308,204200
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               email AFED@ICHUWR.CHEM.UNI.WROC.PL

From COMBA@akcomba.oci.uni-heidelberg.de  Sat Feb  1 07:30:32 1997
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From: "Peter Comba" <COMBA@akcomba.oci.uni-heidelberg.de>
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To: chemistry@www.ccl.net
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Subject: molecular volume
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Dear CCLers

Attached are the very helpful answers for my recent question on
programs for the calculation of molecular volumes from (computed)
coordinates. Thanks for your help.

@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@@
From:          Andrew Rohl <andrew@power.curtin.edu.au>
I have a mac program that calculates molecular volumes very quickly on
a PowerMac.  See JCS Dalton Trans, 1991, 3419 for a description.  I
can send you a copy if you like.  It is written in C if you are
interested in the source.
 Andrew
----------------------------------------------------------------------
 From:          david de corte<David.Decorte@unifr.ch>
Dear Prof. Comba, 
There exists a program which calculates the volume starting from the
coordinates... It is a small FORTRAN-program called SPACEFILL...This
program is included in the MD-package called TINKER which can be
freely downloaded from http://dasher.wustl.edu/tinker/ Other ways to
calculate volumes include Density Funcional programs which calculate
the electron density ..thereafter programs like Cerius2.1 or Molekel
make it possible to calculate the volume of your molecule. I hope this
information will help you further. Kind regards, David
----------------------------------------------------------------------
From:          TOPPER ROBERT<topper@cooper.edu> 
Again, the Molecular Monte Carlo Home Page holds
the answer! If you look at
http://www.cooper.edu/engineering/chemechem/monte.html under "Software
and Numerical Tools for the Discriminating Monte Carlo Practitioner"
you will find a link to STERIC, a program which calulates a number of
steric parameters including molecular volumes. The link takes you to
ftp://hobbes.gh.wits.ac.za/pub/steric/ STERIC was contributed by Brian
Craig Taverner. 
Best, robert
----------------------------------------------------------------------
From:         MARTIN@cmdb.pprd.abbott.com 
SAVOL2 is what you should be using. It is
available from Robert Pearlman. 
pearlman@vax.phr.utexas.edu Yvonne
Martin, Senior Project Leader
----------------------------------------------------------------------
From:    davide@stinch10.csmtbo.mi.cnr.it (Davide Proserpio) 
Dear Peter 
try tolook at this page : 
http://www.gh.wits.ac.za/craig/ and
http://hobbes.gh.wits.ac.za/craig/steric/ you will find information
about STERIC a nice program by Craig Taverner You can also contact 
dodd@roebling.poly.edu (Larry Dodd) about his program :
 "Analytical treatment of the volume and surface area of molecules
 formed by an arbitrary collection of unequal spheres intersected by
 planes" L.R. Dodd and D.N. Theodorou MOLECULAR PHYSICS, Volume 72,
 Number 6, 20 April 1991, 1313-1345.
The program is in Fortran.  A typical input file contains lines of
     2.247950838  -1.236565749   3.658056690    1.931050
     ^^^^^^^^^^^  ^^^^^^^^^^^^   ^^^^^^^^^^^    ^^^^^^^^
     |            |              |              |
     |            |              |              |
     x coord      y coord        z coord        radius
I hope this helps
regards from Milano  (from the same group of Angelo Sironi)
 Davide
----------------------------------------------------------------------
From:          John Waite<chem8@york.ac.uk>
 Dear Peter,
 Ask Larry dodd for a copy of his MOLVOL, fortran code:
    dodd@roebling.poly.edu
 Good luck,
     John
----------------------------------------------------------------------
From:          "P.Bladon"<cbas25@ccsun.strath.ac.uk> 
Yes I have a fortran routine that will do
this. You would probably need to do some work to put it into/link it
another program. Mail be back for more details. 
Peter Bladon


**********************************************************************
Prof Peter Comba
Anorganisch-Chemisches Institut
Universitaet Heidelberg
Im Neuenheimer Feld 270
69120 Heidelberg
Germany

phone    ++49 6221 54 8453
fax      ++49 6221 54 6617
e-mail   comba@akcomba.oci.uni-heidelberg.de

From dsmith@CTCnet.Net  Sat Feb  1 10:20:14 1997
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To: CHEMISTRY@www.ccl.net
From: dsmith@CTCnet.Net (Douglas A. Smith  Ph.D.)
Subject: crystal packing calculations and programs


A very interesting (to me) paper has just appeared in J. Phys. Chem. B,
1997, 101, 798 by Sorescu, Rice and Thompson.  In this paper, they dev3elop
an intermolecular potential for RDX
(hexahydro-1,3,5-trinitro-1,3,5-s-triazine) and perform crystal packing, MC,
and MD studies.

The authors parameterize their  potential based on the known neutron
diffraction structure of RDX.  They also reference several other packages
for performing crystal packing calculations.

What are the options when one does not have the crystal structure available?
Can one reasonably start from a high quality ab initio calculation on a
single molecule (gas phase) and use that structure to pack a crystal?  If
one does, what is the likelihood of getting the crystal structure correct?
Or does one need to perform ab initio calculations in the periodic solid
(e.g., CRYSTAL 95 calculations) before performing crystal packing?

What packages are out there, commercial and "public domain" (free, QCPE,
etc.) that can perform crystal packing calculations?  I would like to
predict space group, density, lattice energy, etc.

Perhaps, since there are pedagogical questions here rather than just a
request for pointers to software, we could keep this discussion public on
the CCL, not just a series of replies directly to me.

Doug
--
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From tratnyek@ese.ogi.edu  Sat Feb  1 12:20:18 1997
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Date: Sat, 1 Feb 1997 08:33:18 -0700
To: chemistry@www.ccl.net
From: "Paul G. Tratnyek" <tratnyek@ese.ogi.edu>
Subject: Re: CCL:Hammett ortho substituent constants?
Cc: toukie@zui.unizh.ch


>Has anyone ever undertaken (and pubished) a detailed analysis of the
>influence of ortho substituents in an effort to factor the influence of
>ortho substituents in to electronic and steric components?

As of when I did the literature search for this (where we found remarkable
little "ortho effect"):

Tratnyek, P. G., and J. Hoign=E9. 1994. Kinetics of reactions of chlorine
dioxide (OClO) in water. II. Quantitative structure-activity relationships
for phenolic compounds. Water Res.  28(1): 57-66.

The best/latest refs on the "ortho effect" were this:

Charton, M. 1971. The nature of the ortho effect. VII. Nuclear magnetic
resonance spectra. J. Org. Chem.  36(2): 266-272.

Charton, M. 1971. The quantitative treatment of the ortho effect. Progr.
Phys. Org. Chem.  8: 235-317.

Charton, M., and B. I. Charton. 1971. The nature of the ortho effect. VI.
Polarographic half-wave potentials. J. Org. Chem.  36(2): 260-265.

=46ujita, T., and T. Nishioka. 1976. The analysis of the ortho effect. Progr=
=2E
Phys. Org. Chem.  12: 49-89.

>sigma ortho values.  Does anyone know of a more recent and/or extensive
>lists, particularly ones containing values factored into steric and
>electronic components for benzoic acids and phenols?

Try the paper by Fujita.

------------------------------------------------------------------
Paul Tratnyek, Department of Environmental Science and Engineering
Oregon Graduate Institute, PO Box 91000, Portland, OR,  97291-1000
http://www.ese.ogi.edu/ese_docs/tratnyek.html  Phone: 503/690-1023
------------------------------------------------------------------



