From rc_davis@srs.gov  Mon May  3 05:37:16 1993
From: rc_davis@srs.gov (Ricardo  C.  Davis)
Message-Id: <9305030937.ZM20814@cmas3.srs.gov>
Date: Mon, 3 May 1993 09:37:16 -0400
Organization: Westinghouse Savannah River Company
To: chemistry@ccl.net
Subject: ACS E-mail Addresses?


Do the American Chemical Society's offices in Washington, D.C. have
 Internet/BITnet addresses?  It sure would be nice...If so, please post to the
list.

RCD

-- 

    Ricardo C. Davis                    Internet: rc_davis@srs.gov
     Building 773-42A, SCS-SRTC, Westinghouse Savannah River Co.
           P.O. Box 616, Aiken, SC  29802  (803)725-5172


From jtgolab@amoco.com  Mon May  3 04:39:49 1993
Date: Mon, 3 May 1993 09:39:49 -0500
From: jtgolab@amoco.com
Message-Id: <9305031439.AA16253@vacc47.nap.amoco.com>
To: CHEMISTRY@ccl.net
Subject: Re: gammes



>In-Reply-To: flicker@engin.umich.edu

I think that you mean "GAMESS" (=General and Atomic Molecular Electronic
Structure Systems).  Mike Schmidt is the caretaker/improver/guru of the
program and I quote him here from the GAMESS manual:

  "This version of GAMESS is described in the Quantum Chemistry Program
  Exchange newsletter: M.W.Schmidt, K.K.Baldridge, J.A.Boatz, J.H.Jensen,
  S.Koseki, M.S.Gordon, K.A.Nguyen, T.L.Windus, S.T.Elbert QCPE Bulletin,
  10, 52-54 (1990).  Questions about GAMESS may be addressed to: Mike
  Schmidt = mike@si.fi.ameslab.gov ."

Among some of the delightful features of GAMESS are the following...
it runs on almost every (modern) machine known to peoplekind; it comes
complete with scripts to compile it, scripts to run it, (very) good
documentation, and all the source code (if you like to make modifications);
and finally, help and support is very easy to obtain thru Email.

:Joe
 jtgolab@amoco.com

From sliu@mastermodel.ps.uci.edu  Mon May  3 00:03:28 1993
Message-Id: <9305031503.AA10292@mastermodel.ps.uci.edu>
To: chemistry@ccl.net
Subject: GROMOS
Date: Mon, 03 May 93 08:03:28 -0800
From: Song Liu <sliu@mastermodel.ps.uci.edu>


Dear everyone:

Can someone tell me where to find the source code and user manual for GROMOS?

Thanks

Song Liu
Chemistry,
UC. Irvine


From feng@lisboa.ks.uiuc.edu  Mon May  3 08:47:57 1993
From: Zhou Feng <feng@lisboa.ks.uiuc.edu>
Message-Id: <9305031848.AA20390@lisboa.ks.uiuc.edu>
Date: Mon, 3 May 93 13:47:57 -0500
To: chemistry@ccl.net
Subject: attending ACS?



Does anybody how could I attend the American Chemical Society?

---
		Feng Zhou

+--------------------------------------------------------------------
|Theoretical Biophysics 		feng@lisboa.ks.uiuc.edu
|University of Illinois			Tel: (217)-244-1612
|3121 Beckman Institute			Fax: (217)-244-6078
|405 N Mathews, Urbana, IL61801		NeXTmail Ok
+--------------------------------------------------------------------

From jle@world.std.com  Mon May  3 12:02:14 1993
Date: Mon, 3 May 1993 16:02:14 -0400
From: jle@world.std.com (Joe M Leonard)
Message-Id: <199305032002.AA11033@world.std.com>
To: chemistry@ccl.net
Subject: Electrostatic potential questions


Folks...

	I've seen several articles over the last few years, most recently
Alkorta, Villar and Arteca, J Comp Chem 14,530(1993), demonstrating
that electrostatic potentials calculated with the MNDO wavefunction were
more similar to high-level ab initio results that those obtained from
AM1 or PM3.  Does anybody have an idea as to why this is the case
(or what references I've missed that discuss such reasons)?

	Along these lines, what is the accepted wisdom when fitting
charges to electrostatic potentials - how close to the VdW surface
should points used in the fit be?

Joe Leonard
jle@world.std.com


From kmoore@ncsc.org  Mon May  3 12:17:39 1993
Date: Mon, 3 May 93 16:17:39 EDT
From: Kevin Moore <kmoore@ncsc.org>
Message-Id: <9305032017.AA23964@duck.ncsc.org>
To: chemistry@ccl.net
Subject: hydrogen bonding...


Hello-
     I am doing some ab initio calculations on a couple of molecules to
determine the chemical shifts of a few protons. The results for one molecule
are not coming as close to experiment as I had expected. In response to
this, I was hoping to strategically position one or two waters in a manner
that would satisfy the H-bonding that the system is probably doing in
solution. I know that some work has been done on looking at water x-mers
and related, but was wondering if there has been any work looking at
secondary amines? On a more fundamental level, how would one approach the
problem of best orienting one or two waters in relation to a molecule
such as pyrrolidine. I have received suggestions of sticking it in
a water box, minimize and then do dynamics and look at which h2o seem to
stick closest to the molecule in the dynamics. Any other ideas? Is this a
reasonable way to get started? I am trying to minimize the CPU time involved
with generating the HF minimized structure for this type of system (the
actual molecule is larger than pyrrolidine).

++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
||  Kevin Moore                      North Carolina Supercomputing Center   ||
||  Scientific Support Analyst       3021 Cornwallis Rd.                    ||
||  (919) 248-1179                   Research Triangle Park, NC 27709       ||
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++

From mmcallis@alchemy.chem.utoronto.ca  Mon May  3 14:19:57 1993
Date: Mon, 3 May 93 18:19:57 -0400
From: mmcallis@alchemy.chem.utoronto.ca (Mike McAllister)
Message-Id: <9305032219.AA18915@alchemy.chem.utoronto.ca>
To: chemistry@ccl.net
Subject: MP2 freqs



Hey Netters,  I hope someone can answer a fairly easy question for me:
   Is it customary to 'scale' MP2 frequencies and ZPVE values the same
   way one typically does with HF values???   If yes, what factor is 
   normally used?? Also,  a GAUSSIAN output calculates infrared intensities
   and reports them in units of 'KM/MOLE', anybody now what the heck KM/MOLE
   is????? How reliable is the calculation of intensities??

Thanks for any help in advance.

Mike McAllister
University of Toronto


From DSMITH@uoft02.utoledo.edu  Mon May  3 18:06:41 1993
Date: Mon, 03 May 1993 23:06:41 -0500 (EST)
From: "DR. DOUGLAS A. SMITH, UNIVERSITY OF TOLEDO" <DSMITH@uoft02.utoledo.edu>
Subject: Re: hydrogen bonding...
To: kmoore@ncsc.org
Message-Id: <01GXR7G52F8800663R@UOFT02.UTOLEDO.EDU>


Kevin Moore writes:

>     I am doing some ab initio calculations on a couple of molecules to
>determine the chemical shifts of a few protons. The results for one molecule
>are not coming as close to experiment as I had expected. In response to
>this, I was hoping to strategically position one or two waters in a manner
>that would satisfy the H-bonding that the system is probably doing in
>solution. I know that some work has been done on looking at water x-mers
>and related, but was wondering if there has been any work looking at
>secondary amines? On a more fundamental level, how would one approach the
>problem of best orienting one or two waters in relation to a molecule
>such as pyrrolidine. I have received suggestions of sticking it in
>a water box, minimize and then do dynamics and look at which h2o seem to
>stick closest to the molecule in the dynamics. Any other ideas? Is this a
>reasonable way to get started? I am trying to minimize the CPU time involved
>with generating the HF minimized structure for this type of system (the
>actual molecule is larger than pyrrolidine).

We recently published a paper (JACS 1993, 115, 2912) entitled "Theoretical
Studies on Hydration of Pyrrole, Imidazole, and Protonated Imidazole in the
Gas Phase and Aqueous Solution".  While these compounds are not secondary
amines but rather aromatic, the general approach is, I think, what you 
are after.  We looked at these molecules at the HF/6-31G* and MP2/6-31G*
levels for total geometry optimization both in gas phase and hydrated
(one molecule of water per solute, position optimized either in the plane
or above the plane of the solute; two molecules of water as well for 
imidazole).  Single point calculations were carried out at the MP2/6-311++G**
//MP2/6-31G* level and combined with frequency analyses and BSSE corrections
at the MP2/6-31G* level to calculate the free energies of hydration.

In addition, we carried out Monte Carlo simulations using Jorgensen's Boss
3.1 program for dilute aqueous solutions in order to determine the hydrogen
bonding geometries and free energies.  The MC results were also analyzed
using radial distribution functions.

To answer your question as to how to best orient one or two water molecules
around such molecules, the best answer is 1) look at what is already in the
literature, such as our paper or others with more relevant systems to your
own, and start from the reported optimized positions; 2) take your best 
guess based on solid chemical intuition, then optimize both in plane and
out of plane; 3) triple check everything.  For instance, we tried to look
at imidazole with one water in the plane making a sigma hydrogen bond and
a second water in the pi region.  However, all attempts led to a structure
in which one water formed a sigma hydrogen bond while the second water
formed a hydrogen bond to the first water.

We are now writing up our results of similar studies on histamine.

Last piece of advice - these are big, _expensive_ calculations if done right,
which includes perturbation or correlation during the optimization, and
at a basis set level sufficient to describe hydrogen bonding, i.e. at least
6-31G* or DZP, with at least one set of diffuse functions.  The latter
are extremely important, as shown by our results and those of others,
such as Janet Del Bene.

On another note, let me plug the symposium on Modeling the Hydrogen Bond, 
which I am chairing at the Chicago ACS meeting in August.  It will run
two full days, Sunday and Monday, and will include a number of big names
and forefront research in this area.

Doug

Douglas A. Smith
Assistant Professor of Chemistry
The University of Toledo
Toledo, OH  43606-3390

voice    419-537-2116
fax      419-537-4033
email    dsmith@uoft02.utoledo.edu

P.S.  reprints of our article are available by request - email or US mail.

From imtvi06@cc.csic.es Mon May  3 23:29:48 1993
Date: Tue,  4 May 1993  5:28:05 UTC+0100
From: Luis Montero <imtvi06@cc.csic.es>
Subject: Electrostatic potential questions
To: chemistry-request@ccl.net (confirm)
Message-Id: <326*/S=imtvi06/OU=cc/O=csic/PRMD=iris/ADMD=mensatex/C=es/@MHS>

Dear netters:

The interesting finding of Arteca's paper is, from my point of view a casual
quality of MNDO. Let us take into account that this method took a consistent
approximate hamiltonian (Pople's NDDO, 1965-67) and parametrized it to give
fair results for a fixed set of molecules which experimental geometries and
heats of atomization were accurately determined. This work have been done
for each element. It gave no meaning to different terms in hamiltonians, if
you take them separately, but a certainly confident result for tarjet proper-
ties (geometries and heats of formation, known the experimental heats of
formation of gaseous elements) of the molecules. Electrostatic fields depend
on molecular eigenfunctions, and they could be good from these grounds.

AM1 and PM3 (truly AM1, beacuse PM3 is a reparameterization) introduced some
terms in the distance matrix dependent term after the SCF procedure. It was,
in the pure molecular SCF, the core-core interaction term of the Born Oppen-
heimer approximation. Many theoreticians of semiempirical methods attribute
to this term some of the frequent wrong results. In fact, this distance matrix
dependent term is theoreticaly consistent, but it is used for introducing
corrections to the approximate SCF results when geometrical quantities are
calculated. AM1 used a variable set of "forza bruta" (Dewar's words) gaussian
terms in this part of the calculation to improve results for certain non pure-
ly bonding cases as hydrogen bridges and cyclic CH structures. It, consequen-
tly, afected parameters in the SCF hamiltonian. Probably, these extrange
inclusion in the full SCF procedure affected more the quality of molecular
eigenfunctions than the former parameterization of MNDO.

I have some non published results where it is clearly seen the lowest quality
of molecular wave functions by PM3, being molecular geometries OK.

Best regards,

Luis Montero
Universidad de La Habana (silicon%ceniai.cu@igc.apc.org)
CSIC, Madrid (imtvi06@cc.csic.es)

From imtvi06@cc.csic.es Mon May  3 23:29:48 1993
Date: Tue,  4 May 1993  5:28:05 UTC+0100
From: Luis Montero <imtvi06@cc.csic.es>
Subject: Electrostatic potential questions
To: chemistry-request@ccl.net (confirm)
Message-Id: <326*/S=imtvi06/OU=cc/O=csic/PRMD=iris/ADMD=mensatex/C=es/@MHS>

Dear netters:

The interesting finding of Arteca's paper is, from my point of view a casual
quality of MNDO. Let us take into account that this method took a consistent
approximate hamiltonian (Pople's NDDO, 1965-67) and parametrized it to give
fair results for a fixed set of molecules which experimental geometries and
heats of atomization were accurately determined. This work have been done
for each element. It gave no meaning to different terms in hamiltonians, if
you take them separately, but a certainly confident result for tarjet proper-
ties (geometries and heats of formation, known the experimental heats of
formation of gaseous elements) of the molecules. Electrostatic fields depend
on molecular eigenfunctions, and they could be good from these grounds.

AM1 and PM3 (truly AM1, beacuse PM3 is a reparameterization) introduced some
terms in the distance matrix dependent term after the SCF procedure. It was,
in the pure molecular SCF, the core-core interaction term of the Born Oppen-
heimer approximation. Many theoreticians of semiempirical methods attribute
to this term some of the frequent wrong results. In fact, this distance matrix
dependent term is theoreticaly consistent, but it is used for introducing
corrections to the approximate SCF results when geometrical quantities are
calculated. AM1 used a variable set of "forza bruta" (Dewar's words) gaussian
terms in this part of the calculation to improve results for certain non pure-
ly bonding cases as hydrogen bridges and cyclic CH structures. It, consequen-
tly, afected parameters in the SCF hamiltonian. Probably, these extrange
inclusion in the full SCF procedure affected more the quality of molecular
eigenfunctions than the former parameterization of MNDO.

I have some non published results where it is clearly seen the lowest quality
of molecular wave functions by PM3, being molecular geometries OK.

Best regards,

Luis Montero
Universidad de La Habana (silicon%ceniai.cu@igc.apc.org)
CSIC, Madrid (imtvi06@cc.csic.es)

