From chemistry-request@www.ccl.net  Wed Jan  6 03:43:36 1999
Received: from dreamon.oxmol.co.uk (dreamon.oxmol.co.uk [193.132.141.15])
        by www.ccl.net (8.8.3/8.8.6/OSC/CCL 1.0) with ESMTP id DAA16314
        Wed, 6 Jan 1999 03:43:33 -0500 (EST)
Received: from oxmol.co.uk (bludgeon.oxmol.co.uk [193.132.141.84])
	by dreamon.oxmol.co.uk (8.9.0/8.9.0/7) with ESMTP id IAA12964;
	Wed, 6 Jan 1999 08:42:57 GMT
Message-ID: <369320EE.9CD54AAA@oxmol.co.uk>
Date: Wed, 06 Jan 1999 08:38:06 +0000
From: Rob Williams <rwilliams@oxmol.co.uk>
Organization: Oxford Molecular Group
X-Mailer: Mozilla 4.5 [en] (WinNT; I)
X-Accept-Language: en
MIME-Version: 1.0
To: Computational Chemistry List <chemistry@www.ccl.net>
Subject: Re: CCL:QSAR
References: <Pine.A41.4.05.9901051320360.36062-100000@hartree.quantchem.kuleuven.ac.be>
Content-Type: text/plain; charset=us-ascii
Content-Transfer-Encoding: 7bit




> 
> Hi,
> 
> could anyone point me to software packages (both commercial and
> non-commercial) for performing QSAR analysis.
> 
> thank you.
> 
> steven

Hi Steve,

Oxford Molecular have a comprehensive QSAR product called Tsar
(Tools for Structure Activity Relationships). Visit our web site
at http://www.oxmol.co.uk/ if you would like more information.

The Tsar user interface is based around an intuitive spreadsheet 
display that allows you to easily bring together and manipulate both 
structural and property data. As well as the normal spreadsheet 
functionality that you would expect, its range of analysis tools include:

- 2D/3D/4D graph plotting
- Univariate data analysis
- Correlation matrices
- Principal components analysis
- Non-linear mapping
- ReNDeR and forward feed neural networks
- cluster (including Ward) and cluster significance analysis
- discriminant analysis
- multiple regression
- partial least squares
- FIRM (a recursive partitioning algorithm)

In addition, the same spreadsheet environment can be used to 
derive calculated properties of loaded molecules, including:

- Molecular mass, surface area and volume
- R-group analysis with Verloop calculation
- Moments of inertia
- Dipole moments
- logP and molar refractivity
- Rotatable bond count
- Kier and Hall (and similar) indices
- Autocorrelograms
- Atom and ring counting
- Hydrogen bond donor/acceptor counting
- Substructure counting
- Lipinski's rules for screening for "drug-like" compounds

It also has interfaces to other software packages:

- Corina, for fast 1D/2D to 3D structure conversion
- Charge, for fast partial charge derivation
- Cosmic, for fast structure optimisation
- Asp, for shape and electrostatic similarity calculations
- Vamp, fast QM package for optimisation and property calculations
- Topkat, toxicity prediction system
- RS3, our Oracle based informatics framework

Hope this has been of some use,
Rob


From chemistry-request@www.ccl.net  Wed Jan  6 10:46:08 1999
Received: from mail.matav.hu (mail.matav.hu [145.236.224.244])
        by www.ccl.net (8.8.3/8.8.6/OSC/CCL 1.0) with SMTP id KAA17905
        Wed, 6 Jan 1999 10:46:00 -0500 (EST)
Received: (qmail 14138 invoked from network); 6 Jan 1999 16:45:30 +0100
Received: from unknown (HELO inhale) (195.70.54.253)
  by mail.matav.hu with SMTP; 6 Jan 1999 16:45:30 +0100
Message-ID: <369384E9.24EE747D@chemaxon.com>
Date: Wed, 06 Jan 1999 16:44:41 +0100
From: Ferenc Csizmadia <fcsiz@chemaxon.com>
Organization: ChemAxon
X-Mailer: Mozilla 4.01 [en] (WinNT; I)
MIME-Version: 1.0
To: chemistry@www.ccl.net
Subject: New year -> new ideas for chemistry software
X-Priority: 3 (Normal)
Content-Type: text/plain; charset=iso-8859-1
Content-Transfer-Encoding: 8bit



A few weeks ago I posted the following letter to CCL:

=====

I would like to know your opinion about future trends in chemical
software development. What will be the hottest topics in the near
future? What are the areas that need new approaches from program
developers?

=====

Thank you for the contributions. Here are the answers I received so far.

1. =====

I would like to submit an idea which is based on the article of 

Mok, Neumann and Handy, J. Phys. Chem. 1996, 100, 6225-6230.

Precise calculations (approaching FCI-quality) should be quite possible,
at a cost scaling as CASSCF, if one were to include only excitations
corresponding to nondynamical correlation in a CASSCF calculation, and
afterwards using a correlation functional fittet to only dynamical
correlation (He or Ne) in a DFT calculation based on densities from the
CASSCF calculation.

Thomas Bligaard Pedersen
University of Strasbourg and Technical University of Denmark
 <pedersen@quantix.u-strasbg.fr>

2. =====

It seems nearest future trends in chemistry are more or less visible. 

To make it short: Biology, Biochemistry and related topics.

>From the clear domination of physics up to the middle of our century scientific world is moving into "the living cell". You can proof it by analyzing the number of publications, impact-factors of various journals, the number of grants in difference fields of chemistry, and activity of funding organizations in general. Even in this List, proteins and DNA modeling and visualization, docking, MD, structure determination, ..., are the topics discussed quite often. 
Significant contribution and support are coming from the medicine
related applications, i.e., QSAR, screening, drug design, etc.

I am not to say that I like the situation, but one has to accept obvious
things.

Concerning the possible arias of software development, very likely it
could be a structure calculation, refinement, prediction and analyzing
programs for the most important biological molecules like proteins, DNA,
etc. Of course all of the above with up to date Graphics User Interface.

So, if you are going to start new software project, try to collect more
info about structural biochemistry stuff.

Valentin P. Ananikov
NMR Group
ND Zelinsky Institute of Organic Chemistry 
<val@cacr.ioc.ac.ru>

3. =====

It would be nice to have a Windows program that would calculate the
enthalpy of formation at 0K and at 298.15 K, and a program that would
calculate rate constants.  You would take the output file from a
Gaussian 94 or Gaussian 98 calc and drag it into the Chemaxon window,
click Start, and the program would calculate heats of formation or rate.
For heat of formation the Gaussian output might be a G2, G2(MP2) or CBS
job. The algorithm could be bases onA. Nicolaides, A. Rauk, M. N.
Glukhovtsev, L. Radom, JPC, 1996, 100, 17460.  for rate constants,
methods might come from standard books on statistical thermodynamics
(e.g. Steinfeld, Francisco and Hase).

E. Lewars
<elewars@alchemy.chem.utoronto.ca>

4. =====

How to determine crystal structures from powder diffraction data is
still hot topic. The 5 last years have seen the emergence of many ways
of locating optimally a molecular model inside a cell (Monte Carlo,
simulated annealing, genetic algorithm, packing considerations,
optimized grid search,...). It seems that developers believe that
pharmaceutical companies are, or will be interested.
You cannot find any of these new softwares in the public domain, nor in
the commercial one !
        See http://www.cristal.org/iniref.html for more details

Structure/properties prediction is the way to continue to explore, not
really new, but not really successful till now.

Armel Le Bail - Université du Maine, Laboratoire des Fluorures
<alb@cristal.org>

5. =====

In my humble opinion, linear scaling SCF theory will continue to get
hotter, as applications become more wide spread and algorithms get more
robust.

Matt Challacombe
Los Alamos National Laboratory
Theoretical Division
email: mchalla@t12.lanl.gov

6. =====

I think that some of the types of calculations that exist, but are
seldom done, will become more widely used.  Here are some of my picks.

relativistic calculations
solvent effects
band structure calculations
mesoscale calculations
synthesis route prediction
ab initio molecular dynamics

Dave Young
<youngd2@mail.auburn.edu>

7. =====

I am just reading -- again -- a very nice and very general article by
Martin Head-Gordon that appeared in the centennial issue of J. Phys.
Chem. He lists a lot of trends and challenges for electronic structure
theory, and almost all of them are longer term, and still valid today.
The reference is J. Phys. Chem. 1996, 100, 13213. In fact, the entire
issue is worth a look as it contains various general reviews.

Georg Schreckenbach
<schrecke@t12.lanl.gov>

8. =====

I think the new ideas for chemistry software is:
       1. Better organized interface. It is easy to learn.
       2. Moved to cheaper but hign performance PC.

FengLou Mao
Peking University
<mao@csb0.IPC.PKU.EDU.CN>

9. =====

I think that simulation using virtual reality in all branches of
chemistry.

Jorge Arce Molina
Instituto Superior Minero Metalurgico
Las Coloradas s/n.
<Jarce@ismm.edu.cu>

10. =====

I think we dont really need a lot of _new_ programmes; rather, we need
a lot of extant programmes/source codes to be ported into Win95/WinNT
executables.  Now that the price of RAM is so low and we will soon have
PCs with clock speeds exceeding 500 MHz, we should be able to run a lot
of programmes on the PC that heretofore have been restricted to Unix
workstations.

For example, so far as I know, there is no simple, stand-alone programme
for the PC that will calculate the molecular volume or
solvent-accessible surface of a macromolecule (or even of a small
molecule) from its .ent or .mol2 file.  This would be a very useful tool
for the community of PC computational chemists.

Whilst MOPAC and AMPAC have been ported to DOS/Win, I know of no DOS/Win
programme that can perform a conformational search in order to identify
the (most likely) global energy minimum of a molecule _in an aqueous
environment_.  I believe that MacroModel contains a module which does
this, so in principle it is possible to obtain a DOS/Win executable that
can also do this.

So far as I am aware, there are no publically-available DOS/Win
programmes that use genetic algorithms for optimal selection of
variables for linear regression analysis.  Neither, so far as I know,
does there exist a recent version of GOLPE that runs under DOS/Win. 
These would be very valuable chemometric tools for the PC compurtational
chemist.

Around April 1999 the C source code for the programme LigBuilder should
be released.  When it is, it will be a very useful addition to the PC
computational chemistry armamentarium, if only someone would port it to
a DOS/Win executable.

The JPC solvent version was recently described [J. Chem. Phys. 109(1):
260 (98)].  However, there is no DOS/Win-compatible release of this
method; such a release would be a valuable addition to the PC
computational chemists methodological arsenal.

And there are other programmes so far available only for Unix which
ought to be made available to PC users: PARM and GRID are two which
spring to mind at the moment.  And, of course, there remains a need for
new and better ways of quickly calculating log P, log D, pKa, aqueous
solubility, &., &c.

S. Shapiro
<toukie@zui.unizh.ch>

=====

The discussion is still open. If anyone would like to contribute please
send a letter in the subject to me or CCL.

Ferenc

~~~~~~
Ferenc Csizmadia, Ph.D.
ChemAxon Ltd.
Valyog u. 7, H-1032 Budapest, Hungary
http://www.chemaxon.com
T:+3620 9570988
mailto:fcsiz@chemaxon.com


From chemistry-request@www.ccl.net  Thu Jan  7 12:11:19 1999
Received: from ned1.sims.nrc.ca (ned1.sims.nrc.ca [132.246.108.2])
        by www.ccl.net (8.8.3/8.8.6/OSC/CCL 1.0) with ESMTP id MAA00050
        Thu, 7 Jan 1999 12:11:18 -0500 (EST)
Received: (from ramos@localhost)
	by ned1.sims.nrc.ca (8.8.8/8.8.8) id MAA22180;
	Thu, 7 Jan 1999 12:11:18 -0500 (EST)
Date: Thu, 7 Jan 1999 12:11:17 -0500 (EST)
From: Antonio Fernandez-Ramos <ramos@ned1.sims.nrc.ca>
To: CCL <CHEMISTRY@www.ccl.net>
Subject: Onsager model
Message-ID: <Pine.SGI.3.91.990107120904.22116A-100000@ned1.sims.nrc.ca>
MIME-Version: 1.0
Content-Type: TEXT/PLAIN; charset=US-ASCII



Dear netters: 
        I am using the Onsager model to taken into account the solvent
effects.It happens that two structures invert their stabilities when the
polarization energy is included. I know that the polarization is not
included in SCF procedure and the manual looks like that the energy to be
considered is the SCF one. 
My question is: what does it happen
with the polarization energy? 
Should I include that in my final result, or not?

 
My best regards,
Antonio Fernandez-Ramos 
Room 2013; SIMS
National Research Council 
100 Sussex Drive 
Ottawa, ON, K1A-0R6 
FAX :613-947-2838 
Phone: 613-990-0982



From chemistry-request@www.ccl.net  Fri Jan  8 09:08:08 1999
Received: from lrz.uni-muenchen.de (root@dialc099.ppp.lrz-muenchen.de [129.187.26.99])
        by www.ccl.net (8.8.3/8.8.6/OSC/CCL 1.0) with ESMTP id JAA10222
        Fri, 8 Jan 1999 09:08:01 -0500 (EST)
Received: from localhost (root@localhost)
	by lrz.uni-muenchen.de (8.8.8/8.8.8) with SMTP id WAA00844;
	Mon, 4 Jan 1999 22:10:23 +0100
Date: Mon, 4 Jan 1999 22:10:23 +0100 (CET)
From: Eugene Leitl <root@lrz.uni-muenchen.de>
To: Chemistry@www.ccl.net
Subject: Re: CCL:Re: CCL:G:Cerius2/Gaussview
In-Reply-To: <Pine.SOL.3.95.981231100906.9875B-100000@mallard2>
Message-ID: <Pine.LNX.3.96.990104220913.840C-100000@lrz.uni-muenchen.de>
MIME-Version: 1.0
Content-Type: TEXT/PLAIN; charset=US-ASCII




Are there any free tools for GAMESS visualization?

Regards,
Eugene

On Thu, 31 Dec 1998, Ohyun Kwon wrote:
> Dear Dr. Xie;
> I think molden is pretty nice and you don't have to pay. You can download
> it form the following
> website(http://www.caos.kun.nl/~schaft/molden/molden.html) freely.



From chemistry-request@www.ccl.net  Fri Jan  8 09:37:42 1999
Received: from mailrelay.wiley-vch.de ([195.110.5.164])
        by www.ccl.net (8.8.3/8.8.6/OSC/CCL 1.0) with ESMTP id JAA10459
        Fri, 8 Jan 1999 09:37:41 -0500 (EST)
From: niskanen@cc.wiley-vch.de
Received: from wnt009.cc.wiley-vch.de ([195.110.10.199])
          by mailrelay.wiley-vch.de (Post.Office MTA v3.5 release 215
          ID# 0-0U10L2S100) with SMTP id de for <Chemistry@www.ccl.net>;
          Fri, 8 Jan 1999 15:36:24 +0100
Received: by wnt009.cc.wiley-vch.de(Lotus SMTP MTA v4.6.2  (693.3 8-11-1998))  id C12566F3.00503EFC ; Fri, 8 Jan 1999 15:36:30 +0100
X-Lotus-FromDomain: WILEY
To: Chemistry@www.ccl.net
Message-ID: <C12566F3.00503D5C.00@wnt009.cc.wiley-vch.de>
Date: Fri, 8 Jan 1999 15:36:25 +0100
Subject: Chemical Concepts' News
Mime-Version: 1.0
Content-type: text/plain; charset=us-ascii
Content-Disposition: inline







Chemical  Concepts  and  LabControl  are  pleased  to announce that we have
agreed a long-term strategic partnership.

For  Chemical  Conseps'  SpecInfo  customers  we  can  now  offer PC client
Spectacle   XS,   developed   by   LabControl  for  Windows  NT/95/98  with
comprehensive  optical  spectroscopy  tools  including  spectra processing,
quantitative  analysis,  easy  report  generation  and  GLC conformant data
handling.  The  easy-to-handle Web client SpecSurf will be available in the
beginning of this year.

For further information, please, visit our home pages:
http://www.chemicalconcepts.com/
http://www.labcontrol.com/





From chemistry-request@www.ccl.net  Fri Jan  8 11:48:12 1999
Received: from mailhost.lanl.gov (mailhost.lanl.gov [128.165.3.12])
        by www.ccl.net (8.8.3/8.8.6/OSC/CCL 1.0) with ESMTP id LAA11469
        Fri, 8 Jan 1999 11:48:11 -0500 (EST)
Received: from [128.165.22.209] (machgs.lanl.gov [128.165.22.209])
	by mailhost.lanl.gov (8.9.1a/8.9.1/(cic-5, 7/9/98)) with SMTP id JAA22595
	for <CHEMISTRY@www.ccl.net>; Fri, 8 Jan 1999 09:48:09 -0700
X-Sender: schrecke@t12mail.lanl.gov
Message-Id: <v02130519b2bbd32c040e@[128.165.22.209]>
Mime-Version: 1.0
Content-Type: text/plain; charset="iso-8859-1"
Date: Fri, 8 Jan 1999 09:51:11 -0600
To: CHEMISTRY@www.ccl.net (CCL)
From: schrecke@t12.lanl.gov (Georg Schreckenbach)
Subject: Summary: G94/98: How to skip SCF completely?
Content-Transfer-Encoding: 8bit
X-MIME-Autoconverted: from quoted-printable to 8bit by www.ccl.net id LAA11470



Dear CCL,

this is the summary for my earlier query on how to use input ("guess")
 MOs to calculate properties like nmr in G94/98. The essential answer
is, it doesn't work (cf. the comments by Mike Frisch -- and he should
know ...).

   Quite a few people suggested the keywords "Guess=(Read,Only)". It
is possible to calculate population stuff and related properties with this
feature, but it is impossible to go into the CPHF equations (l1002).
   Further, I'd like to single out the response by Rene Fournier: when
posting my question, I was hoping for something along the lines of his
suggestion. In this respect, all I found in the code is the old link 503 that
seems to do the direct minimazation that Rene suggested. However, it
is, apparently, restricted to 256 basis functions (I have a lot more), and
I don't really know how to use it anyways.

   Finally, I wish to pass on the comment by Marta ForÈs i Bocsh
<marta@stark.udg.es>: She had posted -- and summarized -- a related
question some weeks ago. You can search the CCL archives, or get her
summary from me.

Thanx to all who took the time to reply! And, please feel free to comment
on this further.

Best regards, Georg
--
Dr. Georg Schreckenbach           Tel:     (USA)-505-667 7605
Theoretical Chemistry T-12        FAX:     (USA)-505-665 3909
M.S. B268, Los Alamos National      E-mail:  schrecke@t12.lanl.gov
Laboratory, Los Alamos, New Mexico, 87545, USA
Internet:    http://www.t12.lanl.gov/~schrecke/


============================
Here are the detailed answers:
============================

Original question:

Dear CCL,

here is a GAUSSIAN related question: I would like to calculate some
properties (like forces or NMR) based solely on the "input guess". How
~is this best done? (Or is it possible at all in GAUSSIAN?)

More specifically, I imagine to have some input MOs using the
"Guess=Read" command. I would specify a certain DFT method, say,
and then go on to calculate the desired properties.

What I have tried so far is the following.

A) specify a "non-standard route" that resembles a standard route but
contains no 500 links.
   Didn't work because the subsequent links requested some files that
had not been written. Perhaps one can do this in a more clever way?

B) Specify "SCF(MaxCycle=1)" as well as the appropriate flags to
avoid the error termintation due to incomletely converged SCF. These
flags are IOp(8/7=1,5/13=1).
   This procedure comes close to what I want, in particular if I use
SCF=QC. However, the one SCF cycle is still too much because it does
modify the input MOs as is clearly visible from the output. Hence, I would
want to avoid it!

Any comments or suggestions? -- I will summarize as usual.

Thank you very much!

Georg

============================
1) response by Mike Frisch:

From: frisch@lorentzian.com (Mike Frisch)

You could probably hack the program to do this, but all of the properties
in Gaussian are based on derivative expressions which are derived assuming
that the appropriate SCF equations have been solved.  In order to use
orbitals and or a density that comes from somewhere else, the CPHF/CPKS
equations and possibly other terms would need to be modified to reflect
how the density was determined and how it changes in response to the
perturbations of interest.

Mike

============================
2) response by Rene Fournier:

From: Rene Fournier <rene@mountain.chem.yorku.ca>

Hello,

   In most programs the obvious way would be to use
simple mixing convergence procedure with a mixing
parameter equal to zero.  Can you do that in Gaussian?

 --------------------------------------------------------------------
 | Rene Fournier                  | Bureau/Office  303 Petrie       |
 | Chemistry Dpt, York University |      (416) 736 2100 Ext. 30687  |
 | 4700 Keele Street,  Toronto    | FAX: (416) 736-5936             |
 | Ontario, CANADA   M3J 1P3      | e-mail: renef@yorku.ca          |
 --------------------------------------------------------------------

============================
3) One example of a response suggesting Guess=(Read,Only):
(Quite a few people proposed the same thing.)

From: Darko Babic <dbabic@rudjer.irb.hr>

        Dear George,

        This is what I've found in the G98 manual:

"Guess(Only,Read):
May also be used to produce population and other post-calculation analyses
from the data in a checkpoint file. For example, these options alone will
produce a population analysis using the wavefunction in the checkpoint file.
Guess(Only,Read) Prop will cause electrostatic properties to be calculated
using the wavefunction in the checkpoint file."

        I hope this helps.  If it doesn't, I am afraid that there is no simple
way to achieve this.  Please, let me know if this happens.

                                        Sincerely,
                                                                Darko Babic
                                                        Institute "Rudjer
Boskovic"
                                                        HR-10001 Zagreb,
P.O.B. 1016
                                                                  Croatia

============================
4) Response by Neil Henson:

From: Neil Henson <neil.henson@lanl.gov>

What does it do with "SCF(MaxCycle=0)"?

[Comment by G.S.: It goes to the default]

How about setting the SCF convergence criteria to something ridiculous
so that it is already converged before it starts?

[Comments by G.S.: a) there is some maximum possible value for the
convergence criteria, and it is still to low. b) it should do one cycle anyhow]

Neil.

--
* Neil Henson                               Hartlepool Renaissance: a marina, *
* neil.henson@lanl.gov/chimera@hubwest.com  a hung monkey and much much more  *
* http://www.t12.lanl.gov/~njh           Tel: 505-667-7795  Fax: 505-665-3909 *
*  Group T-12, Mail Stop B268, Los Alamos National Laboratory, NM 87545, USA  *





From chemistry-request@www.ccl.net  Fri Jan  8 17:49:55 1999
Received: from achilles.noc.ntua.gr (achilles.noc.ntua.gr [147.102.222.210])
        by www.ccl.net (8.8.3/8.8.6/OSC/CCL 1.0) with ESMTP id RAA16320
        Fri, 8 Jan 1999 17:49:52 -0500 (EST)
Received: from hermes.central.ntua.gr (hermes.central.ntua.gr [147.102.240.3])
	by achilles.noc.ntua.gr (8.8.8/8.8.8) with ESMTP id AAA03485
	for <chemistry@www.ccl.net>; Sat, 9 Jan 1999 00:49:53 +0200 (EET)
Received: by hermes.central.ntua.gr with SMTP
	id AAA19876 ; Sat, 9 Jan 1999 00:45:48 +0200 (EET)
Message-ID: <004601be3b58$dea579e0$1bdf6693@titanfocalpoint>
From: "Nick Fotopoulos" <foton263@central.ntua.gr>
To: "Computational Chemistry List" <chemistry@www.ccl.net>
Subject: Computational solid state graduate exercise theme ...
Date: Sat, 9 Jan 1999 00:47:27 +0200






Dear CCLer's,

I am seting up an exercise for engineering students that will present =
them with the current achievements of computational chemistry =
(especially in the solid state field as many of them follows electrical =
engineering). The final target is to stimulate and prepare them to use =
the readily available s/w tools or at least be able to operate in =
interdisciplinary projects.
The exercise approach is molecule --> supermolecular aggr. --> =
macromolecules ---> solid state
I have already finalized the first 3 phases using freely available s/w =
PCGAMESS-US, Hyperchem 5.0 (almost), and Molden.on WIN95 platform, =
explaining the various uses of CompChem at differenr levels of theory.
I am also aware of BiconEdit program capabilities for DOS and Brillouin =
zones prediction at EHMO level.

Could you suggest me solid state systems and/or other material that =
would be relevant to form a good teaching basis ?
Also, are you aware of software capable for solid state calculations at =
a level of theory greater than EHMO?
I will summarise to the list.

Best regards and wishes for a happy & fruitful new year,



Dr. Nick Fotopoulos
National Technical Univ. of Athens


From chemistry-request@www.ccl.net  Sun Jan 10 10:49:16 1999
Received: from alchemy.chem.utoronto.ca (alchemy.chem.utoronto.ca [142.150.224.224])
        by www.ccl.net (8.8.3/8.8.6/OSC/CCL 1.0) with ESMTP id KAA22607
        Sun, 10 Jan 1999 10:49:15 -0500 (EST)
Received: (from elewars@localhost) by alchemy.chem.utoronto.ca (8.7.4/8.7.3) id KAA14581 for chemistry@www.ccl.net; Sun, 10 Jan 1999 10:49:14 -0500 (EST)
Date: Sun, 10 Jan 1999 10:49:14 -0500 (EST)
From: "E. Lewars" <elewars@alchemy.chem.utoronto.ca>
Message-Id: <199901101549.KAA14581@alchemy.chem.utoronto.ca>
To: chemistry@www.ccl.net
Subject: SUMMARY OF RATE/ACTIVATION ENERGY



FRIDAY  1999  JAN 8

   SUMMARY OF ANSWERS TO ACTIVATION ENERGY/RATE CONSTANT QUESTION

Thanks very much to all who replied to my question.

 Reply #11 is specifically to an earlier question about how to calculate
in a simple way a unimolecular rate constant.

 I now think that the rate constant depends not just on the barrier (TS energy
minus reactant energy), but on the *shape* of the transition-state (activated
complex) region, the saddle-shaped part of the potential energy surface.
 So if you fire reactant molecules toward the saddle in a molecular dynamics
simulation, they pass more easily over a flat saddle than a steep one, even if
the TS's have the same energy. I've never seen it expressed like this, but I
think it gives a good pictorial representation of the situation (one could even
build a mechanical model to illustrate this). (I see how the shape of the PES
can be represented by an analytic function fit to a set of computed (e.g.
ab initio)points, but not how partition functions account for the shape)

   Thanks again to all who helped.   E. Lewars

-----------

        QUESTION
1998 Dec 22, Tuesday

True or false:

Two reactions with exactly the same free energies of activation (delta G of
activation, not Arrhenius activation energy) _must_ have the same rate constants
(at the same temperature).

           E. Lewars
===========================
                   RATE CONSTANT AND BARRIER-QUESTION

#1
(From M. J. Kotelyanskii)
False, 
there is a "fundamental frequency" and "transition factor"
in front of the exponent....

-------------------------------------------------------------------------------
Michael J. Kotelyanskii                      Phone (814) 863 43 81
Polymer Science Program                      FAX   (814) 865 29 17
Department of Materials Science and
Engineering                                  kotelyan@plmsc.psu.edu
Pennsylvania State University                http://www.plmsc.psu.edu/~kotelyan
University Park, PA 16802, USA
--------------------------------------------------------------------------------
 ===========================


#2
(From A. Bagatur'yants)

Certainly false!

BTW, what do you mean under "activation energy", next, what kind of reaction
(mono-, bi-, etc. molecular). The preexponential factor is important anyway.

Best wishes and Happy New Year!

Yours
Prof. Alexander Bagatur'yants
Photochemistry Center, Russian Academy of Sciences
ul. Novatorov 7a, Moscow, 117421 Russia
Phone: (007-095)-936-2588 Fax: (007-095)-936-1255
E-mail: sasha@icp.rssi.ru
Home page: http://www.icp.rssi.ru/eng/bagat/bagat.htm
============

#3
(From J. Villa)

As soon as these two reactions are both unimolecular or both bimolecular this is
true. However, the problem with the molecularity will be only in the units you w
ill
use.
On the other hand your statement is only true if you do not take into account
tunneling corrections or recrossing corrections to the rate constant. This is, t
he
sentence is only completely true if working in the framework of transition state
theory (or variational transition state theory), without any additional correcti
on.

Jordi

Jordi Vill`a
Research Group on Medical Informatics
Carrer del Doctor Aiguader 80
E-08003 Barcelona
Tlf: 34-93-2211009           Fax: 34-93-2213237
jvilla@imim.es         http://www1.imim.es/~jvilla
==============


#4
(From T. Soelling)

Hi,

That has to be true (cf. the transition state theory expressions for the
rate constant).

All the best and happy new year.

   Theis Soelling
**  **  **      **  Mr. Theis Ivan Solling
**  **   ** ** **       Department of Chemistry
******    ******        University of Copenhagen
**  **      **          DK-2100 Copenhagen
**  **      **          Ph. 45-3532-0187/Fax. 45-3532-0212 

 theis@kalium.kiku.dk
=============


#5
>From:  IN%"sichelj@Umoncton.ca"  "J. Sichel"

I can think of two reasons why not.
1. The transition-state-theory expression for k includes a barrier
   transmission coefficent (denoted by kappa) which may vary between
   reactions.
2. Transition-state theory may not be exact for the reactions in question.

     John-M. Sichel
     Dept. de chimie et biochimie
     Universite de Moncton
     Moncton NB, Canada    
================


#6
(From Peter Shenkin)
>From:  IN%"shenkin@still3.chem.columbia.edu"
To:     IN%"elewars@alchemy.chem.utoronto.ca"  "E. Lewars", IN%"sichelj@umoncton
 .ca"  "J. Sichel"

> I can think of two reasons why not.
> 1. The transition-state-theory expression for k includes a barrier
>    transmission coefficent (denoted by kappa) which may vary between
>    reactions.
> 2. Transition-state theory may not be exact for the reactions in question.

It is partly a matter of definition.

If one accepts the definition:

        k_rate = ( k_boltz * T / h_bar ) exp( -DG_act / RT )

then, by definition, k_rate and DG_act are functionally related
and of course any two reactions with the same DG_act must have
the same k_rate.  I think this is the answer most people would
accept.

In this picture, DG_act is the value the activation free energy would
have if the theory were valid.  If the theory is invalid, then the 
underlying physical picture would be misleading.  For instance, if
T-variation studies were performed in which DG_act were
dissected into a DH_act and a DS_act, the DH_act would not
really correspond to the enthalpy difference between reactants
and transition state on some PE surface.

OTOH, if DG_act is computed by some other means, such as by an exact
classical calculation on an exactly correct potential-energy surface,
then in fact the above equation will be correct only to the extent
that transition-state theory (or, ahem, activated-complex theory)
is applicable.  For example, where tunnelling is important, the
k_rate calculated from the computed DG_act would be much smaller than
the experimental k_rate.

       -P.

*** "Freedom's just another word for nothing left to lose." (B. Yeltsin)***
*Peter Shenkin; Chemistry, Columbia U.; shenkin@columbia.edu (212)854-5143*
* MacroModel URL: http://www.cc.columbia.edu/cu/chemistry/mmod/mmod.html  *
============


#7
(From Christopher Cramer)

Depends on whether you consider quantum effects (e.g., tunneling) to be
included in a phenomenological free energy of activation or to be part of
the prefactor kappa. If you are DEFINING a model where the only prefactor
to the exponential of -deltaG(dubdag)/RT is k(B)T/h, then your statement is
true, trivially.

CJC

Christopher J. Cramer
University of Minnesota
Department of Chemistry
207 Pleasant St. SE
Minneapolis, MN 55455-0431
Phone:  (612) 624-0859 || FAX:  (612) 626-2006
cramer@pollux.chem.umn.edu
http://pollux.chem.umn.edu/~cramer
==========


#8
(From Alan Shusterman)
False. The preexponential term is usually written kT/h but I
think the correct term is kT^n/h where "T^n" depends on the kinetic =
line 1 [h for help]order of the reaction. If this is correct, then two reactions could =
have identical delta G* but different rate constants because of =
different kinetic orders.

Alan

(Let me know if I've screwed this up.)

Alan Shusterman
Department of Chemistry
Reed College
Portland, OR
www.reed.edu/~alan
============


#9
(From Alexei Kubasov)
Subject: Re: CCL:RATE CONSTANT AND BARRIER-QUESTION
Date: Wed, 30 Dec 1998 09:31:44 +0300

I think that answer is no.
The full expression for k according the transition-state-theory 
includes coefficient the value of which depends on 
probability of a) non-adiabatic processes and b) tunnel effects. 
Besides this the transition-state-theory can not describe some 
processes (monomolecular ones for example).
Alexei A.Kubasov
Moscow State University
================

#10
(Sorry--lost name)
Subject: Re: CCL:RATE CONSTANT AND BARRIER-QUESTION
Date: Thu, 31 Dec 1998 12:23:31 EST

False.

Sould consider how many molecules are involved in the reactions.
================

#11
Wei-To Chan
chan@ihamilton.wlu.ca
 
Sat Jan  9 18:32:37 EST  04:52:59 -0500 (EST)

   Hi, this is a response to your enquiry about rate constant 
calculation for HNC/HCN isomerisation posted to CCL before 
christmas. It may be kind of late to reply now but
perhaps it is because  HNC/HCN is
a subject (my entire phd thesis is about
this single reaction) that has haunted me to this date 
I can't seem to let go your enquiry.
I must note that I am writing this comment on your
request and others' comments from memory and so
my account may not address the issue precisely.

    The HNC/HCN isomerisation was actually used as
an example to illustrate simple rate constant calculation
in Gilbert and Smith's book "Theory of unimolecular and 
recombination reations" on pg 39-41. I also remembered 
seeing a end-of-the chapter question from Steinfeld, 
Franciso and Hases "chemical reaction and dynamics" on
evaluation of HNC/HCN reaction based on ab initio results. 

 Assuming you have run an ab initio calculation of 
the equilibrium HNC structure and the HNC/HCN isomerisation
transition state you can simply plug several set of 
data from each of the molecules into the transition
state theory formulae.  If you obtained the results 
from say gaussian (or possibly GAMESS) you will obtain
the vibrational, rotational and entropies of the 
structure from a harmonic vibration calculation. 
You then simply substitute the data from gaussian into
the formulae

   K_{uni} = A * exp(-E/kT) 
           = (kT/h)*(Q^(ts)/Q^HNC)*exp(-E/kT)

where K_{uni} is the high pressure 
unimolecular rate constant (low pressure value has
to be evaluated with RRKM master equation method)
k is the boltzman constant, Q^(ts) is
the total entropy of the transition state.
The total entropy is obtained from multiplication
of rotatonal entropy and vibrational entropy.
For unimolecular reaction the translation 
entropy of both the TS and the reactant are identical 
and you can ignore it. The total vibrational 
entropy of the TS must *NOT* include the single imaginary 
frequency corresponding to the motion in the 
direction of the reaction path. With gaussian 9x and possibly
GAMESS exclusion of the imaginary frequency from
the printed values. 

 E is the critical energy (or zero-temperature 
barrier height)
evaluated as the difference 
in the zero-point energies (zpe) of HNC and the TS. 
With gaussian 9x you simply subtract the printed out value 
of the total energy (zpe included) for HNC from that of 
the TS. Note that if your reaction is a bimolecular 
rather than unimolecular
reaction E will have to be evaluated as an enthalpy (H).

     If your ab initio program only evaluate the harmonic
vibrations for you then you have to take the trouble 
of turning to you calculator and evaluate 
the vibrational and rotational entropy from
the computed harmonic vibrations and rotational 
constants. The relevant equations can be found handily
from Gilbert and Smith or from Steinfeld et. al. 
This is not a diffcult task for HNC/HCN. But for
large molecules you may want to use a program like UNIMOL
which is part of Gilbert and Smith's book to avoid
tedious evaluation of vibrational entropy from
tens of harmonic vibrations.

   If you can't even compute the vibrational  
and rotational entropies from molecular orbital calculations
then you have to 'guess' their values. Experimental 
values may be available for the reactant for the TS
you may use methods as described in

"Thermochemical kinetics: methods for the estimation of
thermochemical data and rate parameters"
by Sidney Benson

   I also feel compeled to comment several CCLers' commetns.

  One fellow CCLer urged to compute the barrier height to
the highest degree of accuracy possible. While an accurate
estimate certainly is desirable you must note that 
the energy barrier determined from the transition state formulae

 K_{uni} = A * exp(E/kT) 

is *NOT* the barrier height evaluated from the ab initio method. 
Even precluding the limitation of transition state theory itself
substitution of an EXACT ab initio barrier height 
(and exact entropy values) into the above formulae 
won't get you the exact rate constant. 

  chemical kineticist determine the barrier height 
by fitting the measured rate data into the above equation 
to obtain E. But the equation is to some degree
emperical. A theorist shouldn't equate the experimental 
barrier height with the ab initio value. 

  It is true that the rate constant is so sensitive to 
the barrier height that it is not likely that 
you would be lucky to get an estimate of the rate 
to within a factor of three. But it is quite possible 
to get a reasonably accurate value of the frequency factor
using DFT. For the purpose of kinetic modelling and
evaluation of trend of reactivities across a series of
related molecules tansition state theory could
be a useful tool. 

   Someone recommend you using Don Truhlar's program POLYRATE.
I've never used Truhlar's program but I know it specialize 
in microcanonical variational transition state theory    
and tunneling rate coefficent. Such method is required for
reaction without a sharp barrier  (like some  dissociation reactions) 
or  low-temperature reactions that involve proton transfer.
Such method is terribly time consuming (it requires 
caculation of a reaction pathyway and a number of 
hessian along the pathway) and require quite a bit of expertise.
Truhlar's program is an inappropriate.................
recommendation for evaluation of rate for isomerisation 
and most reactions with a barrier height. 

  Someone also pointed out that it is very unlikely to 
obtain meaningful rate constant from transition state 
theory. You certainly can't expect TST to be 
a quantitative tool like ab initio method. TST 
used as a semi-quantitative is a very valuable tool.
For instance experimentalist can deduce the nature of
the reactant from the value of A (Gilbert and smith pg 7-8).
Drawing from my own recent experience I was led by invoking
TST to understand why is it that
rate of reaction for  certain intramolecular 
nucleophilic addition reaction via formation of
3-membered ring TS actually can be substanitally 
faster than same reaction via formation of less strained
4 and 5-membered ring. It turned out that entropy
of the TS is significantly sensitive to the ring size 
in these reactions.  By using TST to examine
rate of reactions acrossing a series of reaction 
valuable insight can be gained.

Wai-To Chan
Department of Chemistry
York University, Toronto
===================

From chemistry-request@www.ccl.net  Sun Jan 10 14:30:12 1999
Received: from inorg.chem.ethz.ch (elwood.ethz.ch [129.132.65.20])
        by www.ccl.net (8.8.3/8.8.6/OSC/CCL 1.0) with ESMTP id OAA23174
        Sun, 10 Jan 1999 14:30:11 -0500 (EST)
Received: from [192.33.93.28] (dynppp28.dialup.ethz.ch [192.33.93.28])
	by inorg.chem.ethz.ch (8.8.8/8.8.8) with ESMTP id VAA17492
	for <chemistry@www.ccl.net>; Sun, 10 Jan 1999 21:40:00 +0100
X-Sender: senn@elwood.ethz.ch
Message-Id: <v03110700b2beac35af7e@[192.33.93.31]>
Mime-Version: 1.0
Content-Type: text/plain; charset="us-ascii"
Date: Sun, 10 Jan 1999 20:29:57 +0100
To: chemistry@www.ccl.net
From: Hans Martin Senn <senn@inorg.chem.ethz.ch>
Subject: RE:SUMMARY OF RATE/ACTIVATION ENERGY


A very recent paper which is related to this question:

B.K. Carpenter, "Dynamic Behavior of Organic Reactive Intermediates",
Angew. Chem. Int. Ed. 1998, 38, No. 24, 3340-3350.

(Full text available as PDF file at
http://www.Wiley-VCH.de/contents/jc_2002/199824.html; some nice animations
from Carpenters group can be seen at
http://www.chem.cornell.edu/~bkl1/dynamics.html)

It discusses problems and limitations of the commonly used statistical
approaches.

Regards
Hans Martin Senn

 ...........................................................................
Hans Martin Senn
Swiss Federal Institute of Technology (ETH)  Phone  +41 (0)1 632 4460
Laboratory of Inorganic Chemistry            Fax    +41 (0)1 632 1310
ETH Zentrum, CAB C20                         E-Mail senn@inorg.chem.ethz.ch
Universitaetstrasse 6
CH-8092 Zuerich, Switzerland



From chemistry-request@www.ccl.net  Sun Jan 10 22:37:13 1999
Received: from smtp.263.net ([202.96.44.19])
        by www.ccl.net (8.8.3/8.8.6/OSC/CCL 1.0) with SMTP id WAA24571
        Sun, 10 Jan 1999 22:37:07 -0500 (EST)
Message-Id: <199901110337.WAA24571@www.ccl.net>
Received: (fmail 4423 invoked from network); 11 Jan 1999 11:34:17 -0000
Received: from unknown (HELO luoxch) (166.111.11.167)
  by 202.96.44.19 with SMTP; 11 Jan 1999 11:34:17 -0000
Date: Mon, 11 Jan 1999 11:38:3 +0800
From: lvtun <lvtun@263.net>
Reply-To: lvtun@263.net
To: ccl discution <chemistry@www.ccl.net>
Subject: Cacu metal chelating clusters,use what software
X-mailer: FoxMail 2.1 [cn]
Mime-Version: 1.0
Content-Type: text/plain; charset="us-ascii"
Content-Transfer-Encoding: 7bit


Dear CCLs:

 I want to caculat the energy of thiol-metal chelating
cluster.It include six CH3CH2S and two Zn++ or Cd++
formed two metal chelating cluster,I want to caculate
the change of potential of this structure  with regard
to the distance between sulphur atom to the metal ion
and the distance between the two metal ions,can you
suggest me what kinds of method and what software
is most perfect,a shared software is best.
Thank you.
                    sincerely yours
                    LVTUN
                    Dept.Biosci&Biotech
                    Tsinghua University
                    Beijing,10084
                    P.R.China

   


