From nobes@fujitsu.co.uk  Wed Aug  7 03:15:57 1996
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From: nobes@fujitsu.co.uk (Ross Nobes)
Message-Id: <199608070703.IAA27393@kinsei.fujitsu.co.uk>
Subject: Re: CCL:M:Serious errors in MOPAC93 (2)
To: tp@elptrs7.rug.ac.be (Park Tae-Yun)
Date: Wed, 7 Aug 1996 08:03:27 +0100 (BST)
Cc: chemistry@www.ccl.net
In-Reply-To: <Pine.A32.3.91.960806182448.3736B-100000@elptrs7.rug.ac.be> from "Park, Tae-Yun" at Aug 6, 96 06:42:33 pm
X-Mailer: ELM [version 2.4 PL25]
Content-Type: text


Park, Tae-Yun writes:
  > 
  > I found that according to MOPAC93, the following two 
  > alkanes have the Delta_Hf values (by AM1 parameter),
  > 
  > 
  > 
  >      C-C-C-C-C-C-C-C   HEAT OF FORMATION =  -58.62036 KCAL
  > 
  > 
  >        C   C
  >      C-C-C-C-C         HEAT OF FORMATION =  -46.93710 KCAL
  >          C
  > 
  > 
  > which means that normal alkane is more stable than branched 
  > alkane; nonsense!
  > 

Dear Tae-Yun,

It might pay to use PM3 in preference to AM1 in these studies.
For example, according to J.J.P. Stewart (Journal of Computer-
Aided Molecular Design, 4 (1990) 1), AM1 makes n-pentane 2.9
kcal/mol too stable but makes neopentane 7.5 kcal/mol too
UNstable. In comparison, PM3 makes both n-pentane and neopentane
too unstable, by 0.6 and 4.5 kcal/mol respectively. So the error
in the relative energies is reduced from 10.4 to 3.9 kcal/mol
on going from AM1 to PM3.

Best wishes,
Ross Nobes
-- 
+---------------------------------------------------------------------+
| Ross Nobes                                                          |
| Research Fellow                                                     |
| Fujitsu European Centre for Information Technology                  |
| 2 Longwalk Road                         Phone:  +44 181 606 4417    |
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From P.E.Young@dl.ac.uk  Wed Aug  7 07:15:59 1996
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To: chemistry@www.ccl.net
Subject: CCP1 Study Weekend - Final Call


 CCP1 Study Weekend
 
 Topic          Quantum Theory of Large Systems
 
 Date:          Dinner Fri. 20 Sept. to Lunch Sun.  22  Sept. 1996
 
 
 Application and Registration:  
                Deadline 1 Sept 1996
 
 Venue:         Daresbury Laboratory, Daresbury, Warrington UK
 
 Scope of Meeting:
 
 Approximately every two years, the UK CCP1 (Collaborative Computational
 Project 1: Electronic Structure Methods) organises a "Study Weekend". 
 These are very informal meetings (maximum 40 participants) that are
 organised around topics that may form the basis of future collaborative
 work in CCP1.  The previous meeting was organized on Hybrid methods.
 
 The meeting this year at Daresbury is focussed on methods (mainly ab
 initio) for studying large molecules.  Thus the scope of the meeting
 includes  DFT  theory,  the coulomb problem, fast multipole methods,
 distributed multipole methods and related techniques.
 
 Speaker			Topic

 P. Gill			Circumventing the Coulomb Problem
 (Cambridge and 
  Massey University NZ)

 G. Scuseria			Linear Scaling Electronic Structure Methods 
 (Rice Univ. Houston)		for Large Molecules

 T. Ziegler			Beating the Heavy Metal Blues with DFT
 (Calgary)

 N. Burton			Molecular Electronic Structure Calculations
 (Manchester)			Employing a Plane-Wave Basis: A Comparison
				With Gaussian Basis Calculation

 I. Gould			Modelling Chlorophyll in solution: Experiment
 (Imperial College)		and Theory in Unison

 M. Guest			The Treatment of Large Molecular Systems;
 (Daresbury)			NWchem and Fully Distributed Parallel
				Applications

 C. Reynolds			Theoretical and Experimental Studies on
 (Essex)			Cobalt-Based Bioreductive Anti-Cancer Agents
 
 V. Saunders			Hartree-Fock Theory for Crystals of Large
 (Daresbury)			Unit Cell.

 A. Stone			Intermolecular Forces between Large Molecules
 (Cambridge)

 There will also be an "informal" poster session. Please send a title with
 your registration if you wish your poster title to appear in the programme.
 
 Accomdation will be in the Park Royal International Hotel in Stretton near
 Warrington. The hotel is located 12 minutes from Manchester Airport, 1 minute
 from Junction 10 of the M56, 5 minutes from Junction 20 of the M6 and midway
 between the cities of Chester, Liverpool and Manchester.

 The attendance fee is 110 pounds which includes accomodation, meals and
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 Registration enquiries and application forms to be sent to
 
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 e-mail p.e.young@dl.ac.uk
 phone +44-(0)1925-603657   fax +44-(0)1925-603634
 
 
 Informal enquiries to 
 
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From 94970459@tolka.dcu.ie  Wed Aug  7 08:15:58 1996
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	id AA32034; Wed, 7 Aug 1996 13:15:15 +0100
Date: Wed, 7 Aug 1996 13:15:15 +0100 (BST)
From: patrick kane <94970459@tolka.dcu.ie>
To: HChem User <hyperchem@hyper.com>, HChem Supp <support@hyper.com>,
        CCL Every <chemistry@www.ccl.net>
Subject: HyperChem and Schakal
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 Hi,

 I would be much obliged if anyone tell me if there is a file format 
which is compatible with both HyperChem and Schakal.

 Thank you in anticipation for your help.

 Regards,
 Paddy.

 Paddy Kane
 Dublin City University
 94970459@tolka.dcu.ie


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


From katrien@uia.ua.ac.be  Wed Aug  7 11:15:59 1996
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From: "Katrien.Franckaerts" <katrien@uia.ua.ac.be>
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To: CHEMISTRY@www.ccl.net
Subject: electron density in MP2
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Hi,

I am searching for the explicit formula representing the Moller Plesset 
second order electron density correction (for closed shell systems)???
Where can I find good information about this subject???

Katrien 

Email: katrien@uia.ua.ac.be
Adress: Franckaerts Katrien
        University of Antwerp (UIA)
        Universiteitsplein 1
        2610 Wilrijk
        Belgium
        

From Matthew.Harbowy@unilever.com  Wed Aug  7 12:16:04 1996
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Date: 07 Aug 1996 16:54:45 +0100
From: "Matthew Harbowy" <Matthew.Harbowy@unilever.com>
To: "chemistry@www.ccl.net" <chemistry@www.ccl.net> (Return requested) (Receipt notification requested)
Cc: "hyperchem@hyper.com" <hyperchem@hyper.com> (Return requested)
Return-Receipt-To: "Matthew Harbowy" <Matthew.Harbowy@unilever.com>
Subject: Branched vs straight chain alkanes
Mime-Version: 1.0



     In the Handbook of Chem and Physics, it reports
     
     octane:               -49.82
     2,2,3,3,TMB:          -53.99
     
     
     My results for AM1 and MM+ show (Hyperchem 3.0 calculations)
     
                         am1                mm+               exp
     
     octane             -58.628            (6.448 s.e.)       -49.82
     
     2,2,3,3,TMB        -40.155            (12.36 s.e.)       -53.99
     
     -------------     ----------        --------------      ------------
     
     oct - tmb          -18.473            -5.912              4.17
     
     
     So, yes, it would seem that both semi-empirical systems *and* 
     molecular mechanics (which should work great) fail to reproduce the 
     experimental figures.
     
     Or, I've made a mistake.
     
     
     -matt

From owner-chemistry@ccl.net  Wed Aug  7 13:16:00 1996
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From: jle@world.std.com (Joe M Leonard)
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To: chemistry@ccl.net
Subject: Looking for pointers for analytical derivs in torsional space


Folks,

	Does anybody have information/pointers, etc. on work involving
analytical expressions for molecular mechanics functions in terms of
torsional space?  Things like VdW and Charge derivatives/gradients
vs. rotation about the torsional angle...

	I'll summarize if there's sufficient interest!

THanks in advance,

Joe Leonard
jle@world.std.com

From takeuchi@ibc.wustl.edu  Wed Aug  7 13:24:56 1996
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Date: Wed, 7 Aug 1996 11:45:11 -0500 (CDT)
From: Yasuo Takeuchi <takeuchi@ibc.wustl.edu>
To: CCL <chemistry@www.ccl.net>
cc: Felice Chu <felice@bioorganic.mechanisms.ucsb.edu>,
        Franca FRATERNALI <franca@crypt.u-strasbg.fr>
Subject: Summary of Fe(III) parameters
Message-ID: <Pine.SOL.3.91.960807111123.28006B-100000@ibc>
MIME-Version: 1.0
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Dear Netters,

I posted the following question:

> Dear CCL'ers:
>
> I would like to calculate the compound which have Fe(III) by MM3 or
> AMBER.  Does anybody know Fe(III) parameters or literatures?  The
> compound is;
>
>         O----------
>         |         Ar
>  ---O----------O---
> Ar  |  Fe(III) |
>  ---O----------O---
>         |         Ar
>         O----------
>
> Any suggestions are welcomed.  Thanks in advance.


Hereby, I summerized the answers from many CCLers, which gave me a great 
help.  I got three following literatures about Fe(III) parameters:

1. Lin, W. et al.  Inorg. Chem. 1994, 33, 884.
2. Bernhardt, P. V. et al.  Inorg. Chem. 1992, 31, 2638.
3. Bouraoui, A. et al.  J. Chem. Soc., Perkin Trans. 1990, 2, 1211.

Thanks a lot to every one.

Sincerely,
Yasuo Takeuchi
----------------------------------------------------------------
Yasuo Takeuchi, Ph.D.                 
Institute for Biomedical Computing      takeuchi@ibc.wustl.edu
Washington University, Box 8036         FAX   314-362-0234
700 South Euclid Avenue                 PHONE 314-362-2273
St. Louis, MO 63110-1012
U.S.A.

******************************************************************
Date: Thu, 01 Aug 1996 16:42:13 -0700 (PDT)
From: Wayne Steinmetz <WSTEINMETZ@POMONA.EDU>
To: takeuchi@ibc.wustl.edu
Subject: calculations on your iron(III) complex

You suggested molecular mechanics as your method of choice.  Have you
considered semi empirical molecular orbital methods?  Warren Hehre of
Wavefunction, Inc. has done an excellent job of parameterizing transition 
metal
elements.  His flagship product Spartan is easy to use.

*******************
Date: Fri, 2 Aug 1996 09:52:01 GMT+1
From: "Dr. Uwe Schmitz" <uwe@docadchem.com>
To: Yasuo Takeuchi <takeuchi@ibc.wustl.edu>
Subject: Re: CCL:Fe(III) parameters

Dear Yasuo Takeuchi:

This is probably of interest for you.



What is MOMEC?

MOMEC is a molecular mechanics system that has been developed for strain 
energy minimisation of metal complexes and operates in a Microsoft
Windows environment. It has a number of features that facilitate its 
application to a wide variety of problems and

features that are not available in most molecular mechanics programs. It 
is designed to be used in conjugation with HyperChem.


MOMEC 1.0 offers:

-       Graphical input and output through HyperChem.
-       A choice of either conjugate gradients or full matrix Newton
        Raphson refinement or a combination of the two methods.
-       True constraints of internal coordinates.
        Raphson refinement or a combination of the two methods.
-       True constraints of internal coordinates.
-       Selective inclusion of 1,3-interactions.
-       Modeling of coordination geometries by either intraligand
        repulsion, electrostatic interactions, ligand field based
        electronic functions or a combination of various methods.
-       An existing extensive force field for metal complexes.
-       An editor for force field parameters and data files.
-       Ready extension to new systems.
-       Run of batch jobs.
-       Additional modules are available for applications in
        conjunction with MOMEC and/or HyperChem include Jahn-Teller,
        Energy and Conversion.
-       Implemented parameter sets: Ti, Cr, Fe, Co, Ni, Cu, Zn, Rh, Pt
        Additional parameters are under development.


What is Provided?

MOMEC is an Microsoft Windows program. It is designed to accept input 
>from HyperChem and produce output readable by HyperChem. MOMEC has a
Windows surface that can be used to set up and modify the MOMEC control 
file, to modify force field parameters, coo
r
dinates and atom types, to run MOMEC either interactively or as a batch 
job, to look at a summary of any MOMEC run and examine errors that
occurred during the strain energy minimisation, to run various other 
modules that are available for the use in conj
u
nction with MOMEC, and to launch HyperChem with or without the most 
recently minimised structure in the workspace.


Additional modules available for applications in conjunction with MOMEC 
and/or HyperChem include Jahn-Teller (structural optimisation of
Jahn-Teller distorted hexacoordinate compounds), Energy (computation of 
energy as a function of constrained internal
c
oordinates) and Conversion (input and output of structure files in 
various formats such as cartesian coordinates SCHAKAL, SHELX, CSD,
ORTEP, MacroModel etc.). Additional modules are under development.

See also: Peter Comba, Trevor W. Hambley; Molecular Modeling of Inorganic 
Compounds (1995), VCH Publishers (Weinheim); ISBN 3-527-29076-1


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------------------------------------------------------------------
Dr. Uwe Schmitz                 Email:  schmitz@docadchem.com
                                Mobile: +49 (171) 3116631
ALTENHOFF+SCHMITZ
Westfalendamm 35                Tel:    +49 (231) 421575
D-44141 Dortmund                FAX:    +49 (231) 414963
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                                        http://www.asw.topnet.de/
------------------------------------------------------------------
Have a look at our restyled WEB pages URL http://www.docadchem.com
                         1. August 1996
***********************
Date: Fri, 02 Aug 1996 10:16:50 -0500
From: Lipkowitz <lipkowitz@chem.iupui.edu>
To: Yasuo Takeuchi <takeuchi@ibc.wustl.edu>
Subject: RE: CCL:Fe(III) parameters

I compiled a list of published MM parameters. Maybe what you're looking 
for is
in that list. See Reviews in Computational Chemistry, Volume 6, 1995, VCH
Publishing Co.
***********************





From sichelj@Umoncton.CA  Wed Aug  7 14:16:01 1996
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Date: Wed, 7 Aug 1996 14:34:45 -0300 (ADT)
From: "John-M. Sichel" <sichelj@Umoncton.CA>
Subject: Re: CCL:electron density in MP2
To: "Katrien.Franckaerts" <katrien@uia.ua.ac.be>
Cc: CHEMISTRY@www.ccl.net
In-Reply-To: <Pine.SOL.3.91.960807164627.7836A-100000@inch.uia.ac.be>
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See I.N.Levine, Quantum Chemistry, 4th edn (1991), p.511-5

                 (2)                 (0)           2
The formula is: E   =   Sum     |<psi   |H'|phi  >|
                 0    s not 0        s         0
                                --------------------
                                   (0)    (0)
                                  E    - E
                                   0      s
with symbols as defined in Levine.

On Wed, 7 Aug 1996, Katrien.Franckaerts wrote:

> Hi,
> 
> I am searching for the explicit formula representing the Moller Plesset 
> second order electron density correction (for closed shell systems)???
> Where can I find good information about this subject???
> 
> Katrien 
> 
> Email: katrien@uia.ua.ac.be
> Adress: Franckaerts Katrien
>         University of Antwerp (UIA)
>         Universiteitsplein 1
>         2610 Wilrijk
>         Belgium
>         
> 
> -------This is added Automatically by the Software--------
> -- Original Sender Envelope Address: katrien@uia.ua.ac.be
> -- Original Sender From: Address: katrien@uia.ua.ac.be
> CHEMISTRY@www.ccl.net: Everybody | CHEMISTRY-REQUEST@www.ccl.net: Coordinator
> MAILSERV@www.ccl.net: HELP CHEMISTRY or HELP SEARCH | Gopher: www.ccl.net 73
> Anon. ftp: www.ccl.net   | CHEMISTRY-SEARCH@www.ccl.net -- archive search
>              Web: http://www.ccl.net/chemistry.html 
> 
> 

     John-M. Sichel
     Dept. de chimie et biochimie
     Universite de Moncton
     Moncton NB, Canada    
     E1A 3E9

     Tel: (506-)858-4313       E-mail: SICHELJ@UMONCTON.CA

I know you believe you understand what you think I said, but I am not sure
you realize that what you heard is not what I meant. (Gaussian92)


From peon@medchem.dfh.dk  Wed Aug  7 14:22:08 1996
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Date: Wed, 7 Aug 1996 19:21:02 +0200
To: chemistry@www.ccl.net
From: peon@medchem.dfh.dk (Per-Ola Norrby)
Subject: Re: CCL:Branched vs straight chain alkanes


Matthew Harbowy wrote:

>     My results for AM1 and MM+ show (Hyperchem 3.0 calculations)
>
>                         am1                mm+               exp
>
>     octane             -58.628            (6.448 s.e.)       -49.82
>
>     2,2,3,3,TMB        -40.155            (12.36 s.e.)       -53.99
>
>     -------------     ----------        --------------      ------------
>
>     oct - tmb          -18.473            -5.912              4.17
>
>
>     So, yes, it would seem that both semi-empirical systems *and*
>     molecular mechanics (which should work great) fail to reproduce the
>     experimental figures.

        The semi-empirical results are one thing, the molecular mechanics
something completely different.  You *CANNOT* use molecular mechanics
steric energies as heats of formation.  In fact, you can only compare
molecular mechanics steric energies when you have identical connectivities.
Naturally the steric energy of tmb is higher than oct, it is much more
congested.

        Of the molecular mechanics programs I'm aware of, only the true MM2
and MM3 from Allinger are able to estimate heats of formation.  (I don't
think any of the various MM2-copies out there includes this feature).  Even
in the Allinger programs, this feature is limited to a small number of
structural features for which corrections have been included.  However, the
alkanes are there.  The MM2(91) values for octane and tmb are given below
(in kcal/mol)

                            steric energy          heat of formation

    octane (all trans)          4.7433                  -53.59

          tmb                  11.7932                  -54.00


        As you can see, the trend is right.  I believe the value for octane
will get closer to the experimental value if you include the contributions
>from other conformations.

        As for the AM1 values, energy errors average 1-2 kcal/mol even when
you compare conformations (Gundertofte et al, J.Comp.Chem. 12, 200, 1991),
so isomeric energies should have larger errors.  I'm a bit surprised by an
error of over 20 kcal/mol though, I had expected better.

        Per-Ola Norrby


^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^^
 *  Per-Ola Norrby
 *  The Royal Danish School of Pharmacy, Dept. of Med. Chem.
 *  Universitetsparken 2, DK 2100 Copenhagen, Denmark
 *  tel. +45-35376777-506, +45-35370850    fax +45-35372209
 *  Internet: peon@medchem.dfh.dk, http://compchem.dfh.dk/



From Alan.Shusterman@directory.Reed.EDU  Wed Aug  7 14:27:21 1996
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Date: 07 Aug 96 11:10:52 PDT
From: Alan.Shusterman@directory.Reed.EDU (Alan Shusterman)
Subject: CCL: Branched vs straight chain alkanes
To: chemistry@www.ccl.net


--- Matthew Harbowy wrote:
So, yes, it would seem that both semi-empirical systems *and* molecular
mechanics (which should work great) fail to reproduce the experimental figures.
     
Or, I've made a mistake.
--- end of quote ---

A number of comments (such as the one above) regarding AM1 and MM+, and their
apparent inability to reproduce the effect of branching on experimental heats
of formation are misplaced.

First, molecular mechanics strain energies (MM+) should never, by themselves,
be used to compare heats of formation of geometric isomers, such as octane and
2,2,3,3-tetramethylbutane.  Different parameters are used to calculate the
strain energies of geometric isomers.  Therefore, even if both isomers were
calculated to have identical energies they might still have different heats of
formation.  Strain energy comparisons are only useful for stereoisomers,
conformational isomers, and other molecules whose energies are calculated using
identical parameters.

Second, as has already been remarked by others, AM1 (and PM3) heats of
formation do not reproduce experimental heats of formation with arbitrary
precision.  This was never claimed by the inventors of these methods, and
thousands of calculations have borne this out.  "Typical" errors for these
methods are in the range of 5-10 kcal/mol, but much larger errors are
frequently encountered.

Third, it is important before complaining about poor computational results to
analyze the results correctly.  This means taking a good look at the structure
of the calculated molecule.  Many of the molecular formulas that have recently
been attributed to various hydrocarbons and carbocations have been incorrect
(note: it is much easier to identify the correct formula when a graphical model
is used than when a Z matrix is used, but one must still be careful).

Fourth, 2,2,3,3-tetramethylbutane is hardly a typical "branched" hydrocarbon. 
Although it is highly branched and should, therefore, have a "low" heat of
formation, it is also very crowded, and this should raise its heat of
formation, i.e., its heat of formation results from compensating factors.  This
is borne out by the following series of C8 experimental heats of formation:
octane (-49.8), 4-methylheptane (-50.7), 2,2-dimethylhexane (-53.7),
2,5-dimethylhexane (-53.2), 2,2,3,3-tetramethylbutane (-54.0).

By the way, AM1 provides reasonable estimates of these heats of formation for
all but two molecules: octane (-58.5), 4-methylheptane (-54.9),
2,2-dimethylhexane (-51.2), 2,5-dimethylhexane (-53.3),
2,2,3,3-tetramethylbutane (-40.0).  Three of the errors are less than 5
kcal/mol, and only one is greater than 10 kcal/mol.  Not bad, but not useful
for comparing the effects of branching.  Unfortunately, while one might have
guessed that the most crowded molecule, 2,2,3,3-tetramethylbutane, would be the
most difficult to model correctly, one would not have guessed that the most
"normal" molecule, octane, would be the next worse in this series.

Modeling is not for the careless.

Alan Shusterman
Department of Chemistry
Reed College
Portland, OR  97202 

From gabriel@jg1.bchem.temple.edu  Wed Aug  7 15:16:02 1996
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The Department of Biochemistry at Temple University School of Medicine

is proud to announce a new web site containing easy access to

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entitled "Protein and Nucleic acid Resource Manager" or PNaRM is 

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We hope that you find this site useful for your work.    


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From topper@cooper.edu  Wed Aug  7 15:20:27 1996
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Subject: CCL:Branched vs straight chain alkanes
To: chemistry@www.ccl.net
Date: Wed, 7 Aug 1996 15:10:10 -0400 (EDT)
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On this topic, several articles by DeTar are enlightening,
in which he discusses how one can estimate heats of
formation from steric energies. See

D.F. DeTar, J.Org.Chem.56, p.1463 (1991) 

and articles thereafter in that volume.

Other useful/relevant references are:

K.B. Wiberg and J.J. Wendoloski, JACS 104, p.5679 (1982);
Wiberg, J.Comput. Chem. 5, p.197 (1984);
ibid., J.Org. Chem. 50, p.5285 (1985).

and

N.L. Allinger,L.R. Schmitz, I. Motoc, C. Bender and
J.K. Labanowski, J. Phys. Org. Chem. 3, p.732 (1990).

Hope this helps
rqt

************************************************************************
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Asst. Prof. of Chemistry               phone:   (212) 353-4378
The Cooper Union                       FAX:     (212) 353-4341 
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From kotelyan@che.udel.edu  Wed Aug  7 15:24:01 1996
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From: Michael Kotelyanskii <kotelyan@che.udel.edu>
Subject: Re: CCL:Branched vs straight chain alkanes
To: Matthew Harbowy <Matthew.Harbowy@unilever.com>
Cc: "chemistry@www.ccl.net" <chemistry@www.ccl.net>,
        "hyperchem@hyper.com" <hyperchem@hyper.com>
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Just a silly comment:

Are you sure, that the energy is calculated in the LOWEST
conformation? 
I mean global, vs. just a local minimum?

Michael Kotelyanskii PhD
Department of Chemical Engineering
University of Delaware                          kotelyan@che.udel.edu
Newark DE 19716                                    


On 7 Aug 1996, Matthew Harbowy wrote:

> 
>      In the Handbook of Chem and Physics, it reports
>      
>      octane:               -49.82
>      2,2,3,3,TMB:          -53.99
>      
>      
>      My results for AM1 and MM+ show (Hyperchem 3.0 calculations)
>      
>                          am1                mm+               exp
>      
>      octane             -58.628            (6.448 s.e.)       -49.82
>      
>      2,2,3,3,TMB        -40.155            (12.36 s.e.)       -53.99
>      
>      -------------     ----------        --------------      ------------
>      
>      oct - tmb          -18.473            -5.912              4.17
>      
>      
>      So, yes, it would seem that both semi-empirical systems *and* 
>      molecular mechanics (which should work great) fail to reproduce the 
>      experimental figures.
>      
>      Or, I've made a mistake.
>      
>      
>      -matt
> 
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> 



From rpgrasso@ssnet.com  Wed Aug  7 17:16:03 1996
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Greetings all,

I'm looking for the coordinates for beta cyclodextrin.  Can anyone help?

Thanks,
Bob


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From Matthew.Harbowy@unilever.com  Wed Aug  7 17:26:26 1996
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The modelling results, although they were minima indeed, were intended as a 
'careless once-off' in continuations of Tae-Yung Park's ongoing discussion. I 
wasn't attempting to publish hard numbers, just to back his observation that AM1
did not reproduce reality. I expected better results, to be honest, and so I 
decided to post them after I calculated them. I fully *expected* my am1 results 
to mirror the experimental results.

As people have suggested, I should not have mentioned the strain energy results 
in the same breath, and probably should have taken my own advice when I was 
composing the post and left it out.

Indeed, as most have suggested, modelling is not for the careless. Neither is 
thermodynamics, I might add, since one can couch any variation plus or minus as 
a combination of conjugation, strain, hyperconjugation, etc., ad-nauseam. To 
make an argument that I would expect Dewar himself to resound, it isn't the 
numbers, or how you get them, but what they tell you about the experiments.

There's been a lot of noise about the 'accuracy' of the numbers, and getting 
gradients below 0.01 etc, but not a lot of talk about what the point of doing 
something like that is. I'm not really sure, other than perhaps eating up 
computer time, why someone would *want* a gradient to drop from 0.1 to 0.01 or 
less. What could be so accurate that the inherent error of modelling doesn't 
swamp?

matt

______________________________ Reply Separator _________________________________
Subject: CCL:Branched vs straight chain alkanes
Author:  chemistry-request@www.ccl.net at INTERNET
Date:    8/7/96 3:32 PM


Just a silly comment:
     
Are you sure, that the energy is calculated in the LOWEST 
conformation?
I mean global, vs. just a local minimum?
     
Michael Kotelyanskii PhD
Department of Chemical Engineering
University of Delaware                          kotelyan@che.udel.edu 
Newark DE 19716
     
     
On 7 Aug 1996, Matthew Harbowy wrote:
     
>
>      In the Handbook of Chem and Physics, it reports 
>
>      octane:               -49.82
>      2,2,3,3,TMB:          -53.99
>
>
>      My results for AM1 and MM+ show (Hyperchem 3.0 calculations) 
>
>                          am1                mm+               exp 
>
>      octane             -58.628            (6.448 s.e.)       -49.82 
>
>      2,2,3,3,TMB        -40.155            (12.36 s.e.)       -53.99 
>
>      -------------     ----------        --------------      ------------ 
>
>      oct - tmb          -18.473            -5.912              4.17 
>
>
>      So, yes, it would seem that both semi-empirical systems *and*
>      molecular mechanics (which should work great) fail to reproduce the 
>      experimental figures.
>
>      Or, I've made a mistake.
>
>
>      -matt
>
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From chpajt@bath.ac.uk  Wed Aug  7 19:16:04 1996
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Date: Wed, 7 Aug 1996 23:19:10 +0100 (BST)
From: A J Turner <chpajt@bath.ac.uk>
To: Matthew Harbowy <Matthew.Harbowy@unilever.com>
cc: "chemistry@www.ccl.net" <chemistry@www.ccl.net>
Subject: Re: CCL:Branched vs straight chain alkanes
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Hi!

To answer the point on gradient.  You need the gradient at least as low as
0.01 to properly acquire vibrational frequencies.  A gradient of
0.1Kcal/angs.mol will give a hessian asymetery of around 0.1% and a
gradient of 0.01 will give a asymetry of about 0.01% (easy to remeber) for
central finit difference (like that in MOPAC).

A gradient of 1.0 will often give incorrect low frequencies - or spurious
negative frequencies.

My point my be that accuracy and self consistency are not the same thing.

Best wishes

Alex 

 -------------------------------------------------------------------
|Alexander J Turner         |A.J.Turner@bath.ac.uk                  |
|Post Graduate              |http://www.bath.ac.uk/~chpajt/home.html|
|School of Chemistry        |+144 1225 8262826 ext 5137             |
|University of Bath         |                                       |
|Bath, Avon, U.K.           |Field: QM/MM modeling                  |
 ------------------------------------------------------------------- 



From usdcc2p5@ibmmail.com  Wed Aug  7 19:56:31 1996
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Matthew Harbowy wrote:                                                     
                                                                            
 >     My results for AM1 and MM+ show (Hyperchem 3.0 calculations)         
 >                                                                          
 >                         am1                mm+               exp         
 >                                                                          
 >     octane             -58.628            (6.448 s.e.)       -49.82      
 >                                                                          
 >     2,2,3,3,TMB        -40.155            (12.36 s.e.)       -53.99      
 >                                                                          
 >     -------------     ----------        --------------      ------------ 
 >                                                                          
 >     oct - tmb          -18.473            -5.912              4.17       
 >                                                                          

To this I should like to add the pm3 results (as suggested earlier) (MOPAC 6):

octane:  	-50.75
2,2,3,3, TMB:  	-49.96

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

oct - tmb:        -.79

Thus the better (but still not quite good enough) accuracy of pm3 for this type of
system over that of am1 is easily demonstrated.  The error relative to experimental
for octane is less than 1 kcal, that for TMB just 4 kcal, much better in each case
than the am1 values.  It has been said elsewhere (check the CCL archive) that when
one has a system with "lots of protons", pm3 should be used over am1.  I think this 
is a good example.

-- 
J. Patrick Cannady
Dow Corning Corporation
jpcannady@dcrn.e-mail.com

All opinions expressed are those of the author and not
necessarily those of Dow Corning Corporation.

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Date: Wed, 7 Aug 1996 16:53:11 -0700
From: dzirl@nyknicks.asd.sgi.com (David Zirl)
Message-Id: <9608071653.ZM8749@nyknicks.asd.sgi.com>
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To: chemistry@www.ccl.net
Subject: Molecular Inventor Workshop at ACS Exposition
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Mark Benzel, the author of Molecular Inventor at Silicon Graphics, will be
presenting a workshop at the American Chemical Society Exposition entitled

	"Programming and Using Molecular Inventor"

on Wednesday, August 28, 1996 at 9am in room 221E.  If you are
attending the exposition, you are encouraged to register and attend.  To
pre-register please send e-mail with your name, address, e-mail, phone, fax and
the name and number of the workshop (#14) to K_poole@acs.org

For more information on Molecular Inventor see:

	http://www.sgi.com/ChemBio/MolecularInventor

or send e-mail to chembio@sgi.comm

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Workshop # 14:

Programming and Using Molecular Inventor(TM).  Sponsor:  Silicon Graphics,
booths 300-302.  Instructor:  Mark Benzel. August 28, 9am-noon. Room 221E in
the Orange County Convention Center, Orlando, Florida.

Molecular Inventor is a set of extensions to Open Inventor which simplifies the
development of molecular graphics applications. In addition, it specifies
extentions to the Open Inventor file format which allow the transfer of
chemical data between applications and the display of the data even in
applications which have no knowledge of chemical systems. The features of
Molecular Inventor include optimized rendering of molecular structures,
advanced selection and highlighting mechanisms and generation of isosurfaces
and 3D contours.

This session will discuss the basic architecture of Molecular
Inventor and how to use it to create applications. Use of Molecular Inventor
with Silicon Graphics collaborative tools will also be presented.


