From wall@phys.chem.ethz.ch  Fri Jun 14 05:54:04 1996
Received: from bernina.ethz.ch  for wall@phys.chem.ethz.ch
	by www.ccl.net (8.7.5/950822.1) id FAA07839; Fri, 14 Jun 1996 05:35:59 -0400 (EDT)
Received: from helios (actually helios-chem.ethz.ch) by bernina.ethz.ch 
          with SMTP inbound; Fri, 14 Jun 1996 11:35:39 +0200
Received: from jetson.ppc-sun by helios.ethz.ch id AA26531;
          Fri, 14 Jun 1996 11:35:38 +0200
Received: by jetson.ppc-sun (5.x/SMI-SVR4) id AA07451;
          Fri, 14 Jun 1996 11:35:37 +0200
Date: Fri, 14 Jun 1996 11:35:37 +0200
From: wall@phys.chem.ethz.ch (Ernst U. Wallenborn)
Message-Id: <9606140935.AA07451@jetson.ppc-sun>
To: chemistry@www.ccl.net
Subject: [R] G94 Excited States
X-Sun-Charset: US-ASCII



Hi there,

A while ago (May 20th) i posted a question concerning the 
ab-initio calculation of electronic spectra. I got a couple
of answers and posted a summary of these (May 29th).

I tested the methods recommended to me on a toy problem
(formaldehyde) and thought it might be an idea to make the
data available to you, in case someone is interested to see them.

Just have a look at http://www.chem.ethz.ch/~wall/form.html
where a link to a Postscript document containing the details
of the calculation is also available.




Thanks again for helping me with that.

--
Ernst-Udo Wallenborn
Laboratorium fuer Physikalische Chemie
ETH Zentrum
CH-8092 Zuerich


 

From toukie@zui.unizh.ch  Fri Jun 14 06:21:01 1996
Received: from rzusuntk.unizh.ch  for toukie@zui.unizh.ch
	by www.ccl.net (8.7.5/950822.1) id FAA07823; Fri, 14 Jun 1996 05:33:52 -0400 (EDT)
Received: by rzusuntk.unizh.ch (4.1/SMI-4.1.9)
	id AA13809; Fri, 14 Jun 96 11:33:48 +0200
X-Nupop-Charset: Swiss
Date: Fri, 14 Jun 1996 11:34:45 +0100 (MET)
From: "Hr Dr. S. Shapiro" <toukie@zui.unizh.ch>
Sender: toukie@zui.unizh.ch
Reply-To: toukie@zui.unizh.ch
Message-Id: <41685.toukie@zui.unizh.ch>
To: chemistry@www.ccl.net
Subject: Seeking references ...


Dear Colleagues;

     I am seeking published references giving neutron diffraction-derived
structural details for phenolic compounds containing an oxygen or sulphur
atom ortho the the -OH group; or a carbonyl moiety (C=O), nitro moiety (NO2),
amino moiety (NH2, RHR), or amido moiety (NHCOR) ortho to the -OH group.  So
far the _only_ reference I have come across is Bacon & Jude, Z. Kristallogr.
Kristallgeom. Kristallphys. Kristallchem. 138: 19-40 (1973), which is for
salicylic acid.

     If anyone can recommend additional references, I would be very grateful
to hear from you.

     Thanks in advance to all responders.


Sincerely,

(Dr.) S. Shapiro
Inst. f. orale Mikrobiol. u. allg. Immunol.
Zent. f. Zahn-, Mund- u. Kieferheilkd. der Univ. ZH
Plattenstr. 11
Postfach
CH-8028 ZH 7

Internet: toukie@zui.unizh.ch
FAX-nr: ( ... + 1) 261'56'83

From Jeffrey.Gosper@brunel.ac.uk  Fri Jun 14 06:43:14 1996
Received: from etamin.brunel.ac.uk  for Jeffrey.Gosper@brunel.ac.uk
	by www.ccl.net (8.7.5/950822.1) id FAA07661; Fri, 14 Jun 1996 05:01:04 -0400 (EDT)
Received: from chem-pc-18 (actually chem-pc-18.brunel.ac.uk) 
          by etamin.brunel.ac.uk with SMTP (PP);
          Fri, 14 Jun 1996 10:00:56 +0100
Date: Fri, 14 Jun 1996 10:00:53 BST
From: Jeffrey J Gosper <Jeffrey.Gosper@brunel.ac.uk>
Reply-To: Jeffrey.Gosper@brunel.ac.uk
Subject: Summary: IUPAC colors for atoms
To: chemistry@www.ccl.net
Message-ID: <ECS9606141053A@brunel.ac.uk>
Priority: Normal
MIME-Version: 1.0
Content-Type: TEXT/PLAIN; CHARSET=US-ASCII


Original Message: 
'I was told the other day that the color used to represent atoms have been  
defined by IUPAC. Does anyone know a source of information on this topic?' 
  
There question seemed to generate quite a bit of interest and I had a number of 
 
requests to forward any information I received on the topic. 

The explicit answer was provided by Jeff Williams (Information Officer, IUPAC) 
              
how stated the following as a response: 
              
'No, IUPAC has not made recommendations about the colours used to  
represent different atoms.' 
              
              
As IUPAC has not provided standards what are people actual using in this  
respect? Also given that we all have an interest in computational chemistry,  
which largely depends on the visualization of molecules, maybe there should be
a standard setup by the IUPAC. Just a thought. 
              

/\/\/\/\/\/\/\/\/\/\/\/\/\/\/\/\/\/\/\/\/\/\/\/\/\/\/\/\/\
 Dr. Jeff Gosper                                         
 Dept. of Chemistry		                        
 BRUNEL University                                     
 Uxbridge Middx UB8 3PH, UK                            
 voice:  01895 274000 x2187                            
 facsim: 01895 256844                                  
 internet/email/work:   Jeffrey.Gosper@brunel.ac.uk     
 internet/WWW: http://http1.brunel.ac.uk:8080/~castjjg 
Re_View's Home page (A molecular display/animation/analysis program):
   http://http1.brunel.ac.uk:8080/depts/chem/ch241s/re_view/re_view.htm
\/\/\/\/\/\/\/\/\/\/\/\/\/\/\/\/\/\/\/\/\/\/\/\/\/\/\/\/\/



From smillefiori@dipchi.unict.it  Fri Jun 14 07:54:07 1996
Received: from ns.dipchi.unict.it  for smillefiori@dipchi.unict.it
	by www.ccl.net (8.7.5/950822.1) id HAA08293; Fri, 14 Jun 1996 07:07:14 -0400 (EDT)
Received: from millefiori.dipchi.unict.it ([151.97.236.168])
          by ns.dipchi.unict.it (post.office MTA v1.9.3 ID# 0-11335)
          with SMTP id AAA184 for <chemistry@www.ccl.net>;
          Fri, 14 Jun 1996 13:06:11 +0100
X-Sender: smillefiori@dipchi.unict.it
X-Mailer: Windows Eudora Version 1.4.4
Mime-Version: 1.0
Content-Type: text/plain; charset="iso-8859-1"
Content-Transfer-Encoding: quoted-printable
To: chemistry@www.ccl.net
From: "Millefiori Salvatore" <smillefiori@dipchi.unict.it>
Subject: software for PED
Date: Fri, 14 Jun 1996 13:06:11 +0100
Message-ID: <19960614120611337.AAA184@millefiori.dipchi.unict.it>


Hi,

I am looking for free PC-software to get the Potential Energy Distribution
(PED) for description of vibrations which involve mixtures of internal
coordinates of molecules.

Thanks,
                 Andrea Alparone.=20
=20
__________________________________________________________________________
=20
Dr. Andrea Giovanni Alparone               ________       ___
(c/o Prof. Salvatore Millefiori)           \___    \_____/  /
Dottorato di Ricerca Scienze Chimiche,         \          _/
Universit=E0 di Catania.                          \______ CT\
Address: Dipartimento Scienze Chimiche,                \___\
Viale A. Doria,6- 95125 Catania, ITALY.
Phone: 39-95-330319 (334)
E-mail: smillefiori@dipchi.unict.it
__________________________________________________________________________


From gever@ruca.ua.ac.be  Fri Jun 14 09:54:05 1996
Received: from maze.ruca.ua.ac.be  for gever@ruca.ua.ac.be
	by www.ccl.net (8.7.5/950822.1) id JAA08797; Fri, 14 Jun 1996 09:06:22 -0400 (EDT)
Received: by maze.ruca.ua.ac.be
	(1.37.109.4/16.2) id AA00937; Fri, 14 Jun 96 15:04:16 +0200
Date: Fri, 14 Jun 1996 15:04:16 +0200 (METDST)
From: Gert Everaert <gever@ruca.ua.ac.be>
Sender: Gert Everaert <gever@ruca.ua.ac.be>
Reply-To: Gert Everaert <gever@ruca.ua.ac.be>
Subject: Re: CCL:software for PED
To: Millefiori Salvatore <smillefiori@dipchi.unict.it>
Cc: chemistry@www.ccl.net
In-Reply-To: <19960614120611337.AAA184@millefiori.dipchi.unict.it>
Message-Id: <Pine.3.88.9606141442.B618-0100000@maze.ruca.ua.ac.be>
Mime-Version: 1.0
Content-Type: TEXT/PLAIN; CHARSET=US-ASCII


This may be of interest :

gar2ped is a utility program for post-processing the archive records of 
GAUSSIAN 94 frequency calculations. Features include isotopic shifts, 
potential energy distribution, APT population analysis, and vibrational 
mode animation. It was written by C. Van Alsenoy and J.M.L. Martin and is 
available by anonymous ftp from the Computational Chemistry Archives at 
ftp://ftp.ccl.net/pub/chemistry

Sincerely,

Gert

_______________________________________________________________________________

Gert Everaert
RUCA, Department of Chemistry             Tel:     + 32 3 218 03 63        
Groenenborgerlaan 171                     Fax:     + 32 3 218 02 33
B 2020  Antwerpen                         E-mail   gever@ruca.ua.ac.be	 
Belgium
_______________________________________________________________________________





From owner-chemistry@ccl.net  Fri Jun 14 10:54:06 1996
Received: from bedrock.ccl.net  for owner-chemistry@ccl.net
	by www.ccl.net (8.7.5/950822.1) id KAA09142; Fri, 14 Jun 1996 10:27:16 -0400 (EDT)
Received: from phy.mtu.edu  for kxiang@mtu.edu
	by bedrock.ccl.net (8.7.5/950822.1) id KAA12497; Fri, 14 Jun 1996 10:27:15 -0400 (EDT)
Received: from phyfac1.phy.mtu.edu (phyfac1.phy.mtu.edu [141.219.151.67]) by phy.mtu.edu (8.6.10/8.6.9) with SMTP id KAA17434 for <chemistry@ccl.net>; Fri, 14 Jun 1996 10:27:15 -0400
From: Kai-hua Xiang <kxiang@mtu.edu>
Received: (from kxiang@localhost) by phyfac1.phy.mtu.edu (8.6.10/MTU-1.2) id KAA02844 for chemistry@ccl.net; Fri, 14 Jun 1996 10:28:43 -0400
Message-Id: <199606141428.KAA02844@phyfac1.phy.mtu.edu>
Subject: molecules absorbed on porous activated carbon
To: chemistry@ccl.net
Date: Fri, 14 Jun 1996 10:28:42 -0400 (EDT)
X-Mailer: ELM [version 2.4 PL24]
Content-Type: text


Dear Friends,

     Are there any softwares that can quantitatively compare the interactions
of different molecules, such as mercury,nitrogen, alcohol, etc. with the porous
activated carbon?

     Any suggestions are welcome.

     Thanks in advance!

Kai-hua Xiang
kxiang@mtu.edu

From dsmith@debye.dasgroup.com  Fri Jun 14 11:54:09 1996
Received: from cool95.third-wave.com  for dsmith@debye.dasgroup.com
	by www.ccl.net (8.7.5/950822.1) id LAA09513; Fri, 14 Jun 1996 11:08:39 -0400 (EDT)
Received: from dirac ([206.31.47.72]) by cool95.third-wave.com
          (Netscape Mail Server v1.1) with SMTP id AAA104
          for <CHEMISTRY@www.ccl.net>; Fri, 14 Jun 1996 11:08:29 +0000
X-Sender: dsmith@pop.dasgroup.com
X-Mailer: Windows Eudora Version 1.4.4
Mime-Version: 1.0
Content-Type: text/plain; charset="us-ascii"
X-Priority: 1 (Highest)
To: CHEMISTRY@www.ccl.net
From: dsmith@dasgroup.com (Douglas A. Smith  Ph.D.)
Subject: need dielectric constant for THF
Date: Fri, 14 Jun 1996 11:08:29 +0000
Message-ID: <19960614110828955.AAA104@dirac>


We are doing some MOPAC 93/COSMO calculations and need the following
information, if anyone has it.

(1) Dielectric constant for THF (tetrahydrofuran)
(2) Solvent radius for THF (the value used for RSOLV)

Thanks in advance.

Doug
--
Dr. Douglas A. Smith, President and CEO     |  voice: (814) 262-9091
The DASGroup, Inc.                          |    fax: (814) 262-9337
P.O. Box 5428                               |  email: dsmith@dasgroup.com
Johnstown, PA 15904-5428                    |     

Contract R&D specialists in computational chemistry, process modeling,
synthesis and design of novel compounds for chemistry, materials science,
and biotechnology.


From owner-chemistry@ccl.net  Fri Jun 14 13:54:08 1996
Received: from bedrock.ccl.net  for owner-chemistry@ccl.net
	by www.ccl.net (8.7.5/950822.1) id NAA10390; Fri, 14 Jun 1996 13:11:51 -0400 (EDT)
Received: from bioc1.msi.com  for marvin@bioc1.msi.com
	by bedrock.ccl.net (8.7.5/950822.1) id NAA20987; Fri, 14 Jun 1996 13:11:48 -0400 (EDT)
Received: from iris147.biosym.com by bioc1.msi.com (5.64/0.0)
	id AA20986; Fri, 14 Jun 96 10:10:35 -0700
Received: by iris147.msi.com (940816.SGI.8.6.9/930416.SGI)
	for chemistry@ccl.net id KAA09077; Fri, 14 Jun 1996 10:11:10 -0700
Date: Fri, 14 Jun 1996 10:11:10 -0700
From: marvin@msi.com (Marvin Waldman)
Message-Id: <199606141711.KAA09077@iris147.msi.com>
To: chemistry@ccl.net
Subject: SMALLEST BOUNDING BOX - THE PROBLEM THAT WOULD NOT DIE


Before some clever computational geometrist(?) flames me, I thought
I would flame myself.  My previous "analytical" solution does not
even work for the simple case of a tetrahedron!

Cory C. Pye wrote:
>the likelihood that any two faces opposite to each other would be parallel is 
>small, and given any face A, B, C, and the point P farthest from the plane 
>containing it, a slight rotation of the normal of the plane toward 
>avg(A,B,C)-P would shorten the distance from the plane to P, and thus the 
>most likely scenario would entail a vertex pair as being on the two planes.

This appears to be correct for the case of a tetrahedron.  If one
constructs a tetrahedron of edge length 1, then I calculate its height to be
sqrt(2/3).  So, constructing a plane containing one face and another
plane parallel and intersecting the opposite point has the two planes
a distance of sqrt(2/3) apart.  Projecting the 4 points onto one of the
planes produces a triangle with a base of 1 and a height of sqrt(3)/2.
The fourth point (from the opposite plane) is inside the triangle.
The minimum bounding rectangle for this triangle is then adjacent to one
edge and intersects the opposite point.  So, the bounding box for the
construction I originally proposed has a volume of:

   sqrt(2/3) * 1 * sqrt(3)/2 = 1/sqrt(2)

Now, consider the following construction.  Construct a plane intersecting
one edge of the tetrahedron and parallel to the opposite (non-adjacent)
edge.  Construct a plane for the opposite edge parallel to the first
plane.  The two planes are a distance 1/sqrt(2) apart (proof is left to
the reader - have fun).  Projecting the four points onto one of these
planes produces a square with diagonals equal to 1 and edges equal to
1/sqrt(2).  So the bounding box for this construction has a volume of:

    1/sqrt(2) * 1/sqrt(2) * 1/sqrt(2) = 1/( 2*sqrt(2) )

which is clearly smaller than the original "solution".

The paper of Martin and Stephenson that I referred to in my earlier
posting mentions that the bounding rectangle of minimum area (and I
think minimum perimeter) must be adjacent to one of the edges of the
2D convex hull.  I had incorrectly assumed that this property could
be extended to 3 dimensions and would work for any metric!  The extension
to any metric was clearly a case of faulty (stupid!) reasoning on my
part.  However, it was somewhat surprising that the metrics that do
work for 2 dimensions using the convex hull approach (rectangle adjacent
to one of the edges works for minimum area and maybe perimeter) don't
work analogously in 3 dimensions (box adjacent to one of the faces doesn't
work for minimum volume or area).  It was only after reading Cory Pye's
posting that I began to think harder about the problem, and discovered
the alternate solution for the tetrahedron.

With all this in mind, I would now like to propose an addendum to my
original solution.  I will not claim it works all the time, as I don't
have a proof, and I would be interested if anyone can find a counter-example.
Consider all the bounding boxes formed from planes adjacent to one face
of the 3D convex hull as before.  In addition, consider the following
set of bounding boxes.  For each pair of non-adjacent edges of the
3D convex hull, form the pair of planes going through one edge and parallel
to the other edge.  If either of these planes penetrates the convex
hull, reject this pair.  Otherwise, project all the points onto one of
the planes and form the 2D bounding rectangle for these points using
the 2D convex hull as before.  Consider all the bounding boxes formed
>from this approach (planes coincident with pairs of edges) and the bounding
boxes from the original approach (planes coincident with a face and its
furthest point) and select the box of minimum volume (or maybe area).
Once again, many improvements may be envisioned to the above algorithm
to improve its efficiency.  A solution for the VDW surface of the molecule
may be similarly constructed (I think) by constructing the convex hull
of the VDW surface by generating planes which are tangent to triplets
of the VDW spheres and for which all the remaining spheres lie on one
side of the plane.  The intersections of these planes defining the convex
hull for the VDW surface define a new set of points, faces, and edges 
to which we can apply the above algorithm.  

Two more special cases need to be considered.  For a planar molecule such as 
benzene, we need to construct additional planes to define the VDW convex hull 
by constructing pairs of planes tangent to 2 of the spheres and which are 
perpendicular to the parallel bounding planes above and below the plane 
of the atoms.  For a linear molecule, the problem has the trivial solution
of 2 planes tangent to the 2 spheres at the ends of the molecule
and perpendicular to the line going through the atoms.  The 4 remaining
planes are chosen to be tangent to the largest VDW sphere of the atoms,
perpendicular to the first 2 planes, and perpendicular to each other.

Regards,

Marvin Waldman, Ph.D.
Director, Rational Drug Design
Molecular Simulations Inc.
e-mail: marvin@msi.com
Web:    http://www.msi.com

