From elazhary@theochem.uni-stuttgart.de  Thu Aug 28 05:20:34 1997
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From: "Dr. Adel El-Azhary" <elazhary@theochem.uni-stuttgart.de>
Subject: Experimental geometry
To: chemistry@www.ccl.net
Date: Thu, 28 Aug 97 11:01:44 METDST
Mailer: Elm [revision: 70.85]


Dear CCL members:

I sent an e-mail to ccl yesterday but it looks like that it was not received.
So my apologies if you receive it twice. My question is that I am doing some 
calculation on some small molecules for which effective, substituted, average 
or equilibrium experimental geometries are available. So which of these is the
best to be comapred to the calculated geometry.

Best regards,

Adel El-Azhary

From s9610264@cougar.vut.edu.au  Thu Aug 28 06:20:34 1997
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Date: Thu, 28 Aug 1997 20:12:56 +1000 (EST)
From: Adnan Hazar <s9610264@cougar.vut.edu.au>
To: CCL <chemistry@www.ccl.net>
Subject: Re: Problem with HyperNMR
Message-ID: <Pine.GSO.3.96.970828201013.17917D-100000@cougar.vut.edu.au>
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Sometime ago I presented a problem I had with HyperNMR.  It just was not
able to deal with "large" no of protons. Including from HyperChem I have
received the following messages:
-----------------------------------------------------------------------

From: Wayne Steinmetz <WSTEINMETZ@POMONA.EDU> 

One eventually runs out of memory and then has to be sly and crafty.
I face the problem with erythromycin.  Fortunately, more of the spins are
weakly coupled to one another.  In order to handle the portion of the
spectrum due to the strongly coupled spins, I consider a subspectrum.
For example, in the desosamine ring attached to the macrolide ring of
erythromycin, the 2' and 3' protons are nearly degenerate so strong
coupling is assured.  The 2' proton is coupled to the 3' and also a 1'.
The 3' is coupled to the 2' and also to the 4'axial and 4'equatorial.
The network goes on but
to handle the portion of the spectrum due to the 2' and 3' and perform a
simulation involving the 1', 2', 3', 4'equatorial, and 4'axial protons.
Normally the total spin system of a molecule can be broken down to
subsystems, manageable islands of spins.   

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

From: Serge Pachkovsky <ps@ocisgi7.unizh.ch>

This looks very much like an excuse by a sub-standard support droid.
There indeed are quite a few spin states in this system. (Not 2^37,
however. More like 2^37 * 2^17 * 6^3 * 3^7, if you assume the molecule
to consist entirely of H-1, C-13, O-17, and N-14) The nice part, though,
is what THIS IS ABSOLUTELY IRRELEVANT.

Depending on gory implementation details, a strightforward realization
of GIAO-SCF shielding tensors at the INDO level (which, I believe, is
the level employed by HyperNMR) may require from about 12*Norb^2 (if
the developer in question feels generous) to (9*Natom + 3)*Norb^2 (if
he insists on been wasteful) words of memory. In fact, it is possible
to go by with much less than this. Coupling constants are a bit more
difficult, with something between (3*Natom + 9)*Norb^2 to 12*Natom*Norb^2
for a naive implementation. I do not know enough about HyperNMR to be
able to guess how sofisticated its memory handling is.  

In your particular case, there are 64 atoms and 145 orbitals, so the
shilding tensor calculation should need from 2Mb (for a "generous"
implementation) to 93Mb (for a "wasteful" one). Coupling constants
might need from 32Mb to 132Mb, possibly in addition to the shielding
tensor requirements. Keep in mind what these are back-of-the-envelope
estimations, actual requirements may differ by a factor of 2 or four
in either direction, depending on the actual implementations' quality.
Your support contact should be able to provide you with a tighter
estimate.

In any event, you should be able to compute shielding tensors for a
molecule of this size with 64Mb of real memory, provided that the
program and operating system you are using do not impose some arbitrary
limit on the resources which can be used. Coupling constants may be a
bit more problematic, though, both in terms of memory use and calculation
time.

Regards,            

/Serge.P   
-----------------------------------------------------------------------

From: Joel Polowin <joelp@agiss.com>

Hardware level: nothing you can do; that kind of memory simply
can't be packed into a PC.

Software level: You may be able to reduce the number of spin
states by marking some protons as rotationally equivalent, such
as the three protons on a methyl group.  (Use with caution: for
example, the six protons on two different methyl groups are not
necessarily all equivalent to each other!)  Apart from that, your
best bet is probably to calculate the spectrum for only part of
the system at a time and then take the total spectrum as being the
sum of the spectra of the parts.

Joel Polowin
joelp@agiss.com       
-----------------------------------------------------------------------

**********************
Adnan Hazar
Chemical Sciences
Victoria University
Australia
**********************


From buyong@ibmnla.chem.uga.edu  Thu Aug 28 10:20:44 1997
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To: chemistry@www.ccl.net
Subject: comparison betweem EXP and Compuation
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On Thu, 28 Aug 1997, Dr. Adel El-Azhary wrote:

> Dear CCL members:
>
> I sent an e-mail to ccl yesterday but it looks like that it was not
received.
> So my apologies if you receive it twice. My question is that I am doing
some
> calculation on some small molecules for which effective, substituted,
average
> or equilibrium experimental geometries are available. So which of these
is the
> best to be comapred to the calculated geometry.

This is a good question. Too often, we compare computed molecular
structure with experimental value without concerning whether they are
comparable.
        First of all, WHAT IS A MOLECULE? (see, Gribov, L. A.
J. Mol. Struc. 1993,300,415). There is one quite accuarte definition:
it is the smallest particle of the substance made up of eletrons and
nuclei of a definit mass. This definition can be expressed mathematically
by the schrodinger equation. However, we must reduce to classical
expresions if we want to compare calculated structure with a real
experiment. We have to use classic models, different models for
different experiments.
        Let us start from several experimental procedures obtaining
the information of molecular structure. Two kinds of operational bond
lengths R(0) and R(s) may be derived directly from rotational and
rotation-vibrational spectroscopy. The R(0) structure is derived from
the ground state rotational constants B(0) directly, or more usually with
assumptions about some of the structural parameters. When the rotational
constants for various isotopic species are observed, the substituted
structure R(s) can be determined by Kraitchman method. When vibrational
(both harmonic and anharmonic) properties are recorded, one may obtained
equilibrium structure R(e) with some approximation. Only is the R(e)
really comparable with the value from quantum mechanical calculations,
which give the distance between equilibrium nuclear position R(e).
  X-ray or neutron diffraction experiments give the average nuclear
positions at thermal equilibrium, and from which the average nuclear
position
the internuclear distance R(alpha) is defined. When we refer to the
structure at 0 K, we get R(z) structure, which may derived from
rotational and rotation-vibrational spectroscopy.
        Gas phase electron diffraction experiments give the thermal
average value of internuclear distance: R(g) structure.
        The relationship and interconversion of those strcutures may be
formulated by classical approximation (see reference cited in the end
of this message). MM3(96) version will print out all those structures.
If you are using molecular mechanical method, MM3(96) is a good option.
you can compare your calculated results with  comparable experimental
data. Other molecular mechanical packages, as I know, do not realized
the difference. If you are talking about QM calculation, of course,
experimental equilibrium structure is first choice. However, if it is
not available, R(s) structure is close to R(e). I have derived a formula
R(s) =[R(z) + R(e)]/2 . R(z) comes third, then R(alpha), and finally
R(g). Note that QM results are base sets and correlation dependent, and
convergence should be considered in the comparison.

Refernce:
a) Kuchitus, K. in Accurated Molecular Structures, Ed Domenicano, A et al.
Oxford Science Publication, 1992.
b) Ma, B.; et al. J. Physical chem. 1996, 100, 8763.
                 J. Am. Chem. Soc. 1997, 119, 2570.
                 J. Mol. Struc. In press ( the issure dedicated to Dr.
Kuchitsu).




=================================================================
Dr. Buyong Ma             buyong@ibmnla.chem.uga.edu
Computational Center for Molecular Structure and Design
Department of Chemistry
University of Georgia
Athens, Georgia 30602 USA            Voice (706) 542-2044
=================================================================




From ccl@www.ccl.net  Wed Aug 27 08:28:57 1997
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Gregor Fels wrote:

> Dear CCL readers,
> we are looking for a way to export Spartan output data to VRML
> format, more precise we would like convert data like the color coding
> of an electrostatic potential or the result of a HOMO- or
> LUMO-presentation to VRML (rather than merely the
> coordinates).
>
> Any suggestion?
>
> Gregor
>
> Dr. Gregor Fels
> Universitaet-GH-Paderborn
> FB 13-Org. Chemie
> Warburgerstr. 100
> D-33098 Paderborn, Germany
>
> Tel. 0049-5251-602181/Fax -603245
> EMail GF@chemie.uni-paderborn.de
>
> ---
> Administrivia: This message is automatically appended by the mail
> exploder:
> 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

Hi,

   I would also like to be able to ddo this with Spartan or Hyperchem.
Please e-mail me any responses you obtain.



Sincerely,

Ken Fountain

> ---



--------------0B4E6F0EA14736EF7800DF09
Content-Type: text/html; charset=us-ascii
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<HTML>
Gregor Fels wrote:
<BLOCKQUOTE TYPE=CITE>Dear CCL readers,
<BR>we are looking for a way to export Spartan output data to VRML
<BR>format, more precise we would like convert data like the color coding
<BR>of an electrostatic potential or the result of a HOMO- or
<BR>LUMO-presentation to VRML (rather than merely the
<BR>coordinates).

<P>Any suggestion?

<P>Gregor

<P>Dr. Gregor Fels
<BR>Universitaet-GH-Paderborn
<BR>FB 13-Org. Chemie
<BR>Warburgerstr. 100
<BR>D-33098 Paderborn, Germany

<P>Tel. 0049-5251-602181/Fax -603245
<BR>EMail GF@chemie.uni-paderborn.de

<P>---
<BR>Administrivia: This message is automatically appended by the mail exploder:
<BR>CHEMISTRY@www.ccl.net: Everybody | CHEMISTRY-REQUEST@www.ccl.net: Coordinator
<BR>MAILSERV@www.ccl.net: HELP CHEMISTRY or HELP SEARCH | Gopher: www.ccl.net
73
<BR>Anon. ftp: www.ccl.net&nbsp;&nbsp; | CHEMISTRY-SEARCH@www.ccl.net --
archive search
<BR>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;
Web: <A HREF="http://www.ccl.net/chemistry.html">http://www.ccl.net/chemistry.html</A></BLOCKQUOTE>
Hi,

<P>&nbsp;&nbsp; I would also like to be able to ddo this with Spartan or
Hyperchem.&nbsp; Please e-mail me any responses you obtain.
<BR>&nbsp;
<BR>&nbsp;

<P>Sincerely,

<P>Ken Fountain
<BLOCKQUOTE TYPE=CITE><A HREF="http://www.ccl.net/chemistry.html"></A>

<P>---</BLOCKQUOTE>
&nbsp;&nbsp;</HTML>

--------------0B4E6F0EA14736EF7800DF09--



From robert@pauli.utmb.edu  Wed Aug 27 14:20:26 1997
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From: "Robert Fraczkiewicz" <robert@pauli.utmb.edu>
Message-Id: <9708271252.ZM15750@pauli.utmb.edu>
Date: Wed, 27 Aug 1997 12:52:42 -0500
In-Reply-To: "Gerrit-Jan's Geocities mail" <gjlinker@geocities.com>
        "CCL:Standard Color codes for atoms" (Aug 27,  1:06pm)
References: <199708271208.FAA15265@geocities.com>
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To: "Gerrit-Jan's Geocities mail" <gjlinker@geocities.com>,
        <CHEMISTRY@www.ccl.net>
Subject: Re: CCL:Standard Color codes for atoms
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On Aug 27,  1:06pm, Gerrit-Jan's Geocities mail wrote:
> Subject: CCL:Standard Color codes for atoms
> Hello all,
>
> I am looking for the standard color codes for atoms. As far as I can
> remember the standard color for Carbon is black, the one for Oxigen is
> blue, Nitrogen is Green. But I am not sure, I am just guessing.
>

I thought that the standard color coding was like this:

  C   black
  O   red
  N   blue
  S   yellow
  H   white

Robert Fraczkiewicz
University of Texas Medical Branch
Galveston, TX 77555


From d3e102@ames2.pnl.gov  Wed Aug 27 14:20:33 1997
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Date: Wed, 27 Aug 1997 10:29:56 -0700
From: d3e102@emsl.pnl.gov
Subject: Updated Ab Initio Benchmarks
To: chemistry@www.ccl.net
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The third version of the EMSL Ab Initio Benchmark Report is
available at http://www.emsl.pnl.gov:2080/docs/tms/abinitio/cover.html.

This version includes information on 40 different hardware platforms
and 11 different software packages.  Compared to the two previous
versions our access to some of the "latest and greatest" processors was
more restricted.  Most significant was the lack of availability of
a highspeed Pention II machine, but that defficiency should be rememdied
shortly.

Please address any comments regarding what you like or don't like to me.


-- 

David Feller                                |
Environmental Molecular Sciences Laboratory | 
Battelle Pacific Northwest National Lab     |
Mail Stop K1-90                             | e-mail:d3e102@emsl.pnl.gov
906 Battelle Blvd                           | Fax: (509)-375-6631
Richland, WA 99352                          |


From jkl@ccl.net  Thu Aug 28 17:20:41 1997
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From: Jan Labanowski <jkl@ccl.net>
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Date: Thu, 28 Aug 1997 17:10:49 -0400 (EDT)
Message-Id: <199708282110.RAA03720@krakow.ccl.net>
To: chemistry@www.ccl.net
Subject: Molecular Weight Calculator for Windows95 (v4.0) available in 
	CCL archives
Cc: jkl@ccl.net


Version 4.0 of Molecular Weight Calculator for Windows 95 now available
in CCL archives:

   ftp://www.ccl.net/pub/chemistry/software/MS-WINDOWS95/Molecular_Weight

Enjoy and thank Matthew Monroe (Monroem@UNC.Edu)

Jan Labanowski
jkl@ccl.net


