From rozas@pinar1.csic.es  Wed Nov 26 04:37:26 1997
Received: from pinar.csic.es  for rozas@pinar1.csic.es
	by www.ccl.net (8.8.3/950822.1) id DAA15919; Wed, 26 Nov 1997 03:56:55 -0500 (EST)
Received: from pinar.csic.es by pinarvms.csic.es (PMDF V5.1-4 #13290)
 id <01IQGMJHD0QO001VWQ@pinarvms.csic.es> for CHEMISTRY@www.ccl.net;
 Wed, 26 Nov 1997 09:57:40 CE
X400-Received: by /PRMD=iris/ADMD=mensatex/C=es/; Relayed; Wed,
 26 Nov 1997 09:55:43 +0000
Date: Wed, 26 Nov 1997 09:55:43 +0000
From: Isabel Rozas <rozas@pinar1.csic.es>
Subject: SUMMARY of Sn basis sets
To: CHEMISTRY@www.ccl.net
Message-id: <925*rozas@pinar1.csic.es>
Content-identifier: 925
MIME-version: 1.0 (Generated by Ean X.400 to MIME gateway)
X400-Content-type: P2-1984 (2)
X400-MTS-identifier: [/PRMD=iris/ADMD=mensatex/C=es/;971126095543]
X400-Originator: rozas@pinar1.csic.es
X400-Recipients: non-disclosure:;



Thanks to everybody for your answers and advices about basis 
sets for Sn.

In my question message I forgot to mention that I had checked 
the web place: http://www.emsl.pnl.gov:2080/forms/basisform.html 
but, in any case thanks to: Michael Hartmann, Stephan P.A. Sauer, 
Ole Swang, Reinaldo Pis Diez, and Pablo Vitoria Garcia, for 
suggesting it.

Thanks also to Alexander Hofmann, Han Zuilhof, Carles Bo, 
Antonio Fernandez Ramos, and Jose Ignacio Garcia-Laureiro 
for suggesting:
http://wserv1.dl.ac.uk:800/emsl_pnl/basisform.html

And to Alexander Hofmann for suggesting:
http://www.theochem.uni-stuttgart.de
 
to Pablo Vitoria Garcia for suggesting:
ftp://ftp.caos.kun.nl/pub/misc/deft/dgauss_bases
ftp://ftp.caos.kun.nl/pub/misc/deft/deft_bases
and http://tcpc.bham.ac.uk/molpro/basispe.html

to John Waite for providing a whole contracted GTO basis 
set for Sn 

and spetial thanks to Michael Hartmann, Han Zuilhof, Christoph 
Widauer, Ole Swang, Pablo Vitoria Garcia, and Antonio M. Marquez, 
for their nice commentaries, explanations and advices and also 
for providing the following references:
S. Huzinaga, J. Andzelm, M. Klobukowski, E. Radzio-Andzelm, Y. Sakai, 
H. Tatewaki, Gaussian Basis Sets for Molecular Calculations, Elsevier, 
Amsterdam, 1984. (Huzinaga basis sets).
Str?mberg, A; Gropen, O; Wahlgren, U.: J. Comput. Chem. 4 (1983) 
181 (VDZ basis sets).

-----------------------------------------------------------------------
   Isabel Rozas                                 ROZAS@PINAR1.CSIC.ES
   Instituto de Quimica Medica (C.S.I.C.)       Phone: 34-1-562 2900
   c/ Juan de la Cierva 3                       Fax: 34-1-564 4853
   28003-Madrid (Spain)
-----------------------------------------------------------------------


From simek@rudjer.irb.hr  Wed Nov 26 06:37:26 1997
Received: from rudjer.irb.hr  for simek@rudjer.irb.hr
	by www.ccl.net (8.8.3/950822.1) id FAA16268; Wed, 26 Nov 1997 05:48:02 -0500 (EST)
Received: from tom (tom.irb.hr [161.53.129.102])
	by rudjer.irb.hr (8.8.7/8.8.7) with SMTP id LAA30680;
	Wed, 26 Nov 1997 11:48:14 +0100 (MET)
Message-ID: <347C8BDB.1E20@rudjer.irb.hr>
Date: Wed, 26 Nov 1997 12:51:39 -0800
From: Visnja Simek <simek@rudjer.irb.hr>
Reply-To: simek@rudjer.irb.hr
Organization: Rudjer Boskovic Institute
X-Mailer: Mozilla 3.01 (Win16; I)
MIME-Version: 1.0
To: chemistry@www.ccl.net
Subject: Literature about excited electronic states
Content-Type: text/plain; charset=us-ascii
Content-Transfer-Encoding: 7bit


Hello!
  
  I would appreciate if somebody point me to books, reviews or other
sources dealing with the electronic excited states from theoretical(!)
and experimental point of view.
 I would collect the answers and send them to the list.
 Thank you in advance,
                              Visnja

~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ 
Visnja Simek                        
         Rudjer Boskovic Institute  
HR-10001 Zagreb, CROATIA           
         phone:(385-1) 456 11 46   
fax:(385-1) 27 26 48                
         e-mail:simek@rudjer.irb.hr;
simek@faust.irb.hr
~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~

From doublet@gauss.lsd.univ-montp2.fr  Wed Nov 26 08:37:37 1997
Received: from gauss.lsd.univ-montp2.fr  for doublet@gauss.lsd.univ-montp2.fr
	by www.ccl.net (8.8.3/950822.1) id IAA16639; Wed, 26 Nov 1997 08:26:26 -0500 (EST)
Received: (from doublet@localhost)
	by gauss.lsd.univ-montp2.fr (8.8.5/8.8.5) id OAA77380
	for chemistry@www.ccl.net; Wed, 26 Nov 1997 14:27:02 +0100
Date: Wed, 26 Nov 1997 14:27:02 +0100
From: Marie-Liesse Doublet <doublet@lsd.univ-montp2.fr>
Message-Id: <199711261327.OAA77380@gauss.lsd.univ-montp2.fr>
To: chemistry@www.ccl.net
Subject: Bmtrx version2 Program



Hi,

I would like to know if someone knows something about
the Bmtrx program from Komornicki (Palo Alto) that convert
(apparently) the cartesian Hessian matrix in internal coordinates.
Where can I find it ? Does it bring something more than Gamess
for the transformation Cart. --> internal ?

Thanks.
(Could you please send the answers to pasfav@crit.univ-montp2.fr ?)


        Frederic



************************************************************************
          Dr. Frederic Favier

            -----------
             LAMMI
  (Laboratoire des Agregats Moleculaires
       et Materiaux Inorganiques)
      Universite des Sciences
    et Techniques du Languedoc
      Place Eugene Bataillon            
    34 095 Montpellier Cedex 05      e-mail : pasfav@crit.univ-montp2.fr

*************************************************************************

From mckelvey@kodakr.kodak.com  Wed Nov 26 08:43:22 1997
Received: from kodakr.kodak.com  for mckelvey@kodakr.kodak.com
	by www.ccl.net (8.8.3/950822.1) id IAA16570; Wed, 26 Nov 1997 08:07:35 -0500 (EST)
Received: from mail.rl.kodak.com by kodakr.kodak.com with SMTP id AA14166
  (5.67b/IDA-1.5 for <CHEMISTRY@www.ccl.net>); Wed, 26 Nov 1997 08:04:55 -0500
Received: from mozart.rl.kodak.com by mail.rl.kodak.com (8.8.3/1.1.10.5/17Jan97-0515PM)
	id IAA12324; Wed, 26 Nov 1997 08:20:11 -0500 (EST)
Received: from kodak.com (stomper.rl.kodak.com [150.220.76.39]) by mozart.rl.kodak.com (950413.SGI.8.6.12/950213.SGI.AUTOCF) via ESMTP id IAA25013; Wed, 26 Nov 1997 08:08:18 -0500
Message-Id: <347B2FAA.9D9FA718@kodak.com>
Date: Tue, 25 Nov 1997 20:06:02 +0000
From: John McKelvey <mckelvey@kodakr.kodak.com>
Reply-To: mckelvey@kodakr.kodak.com
Organization: Eastman Kodak Company
X-Mailer: Mozilla 4.02 [en] (WinNT; I)
Mime-Version: 1.0
To: hou@agouron.com
Cc: CHEMISTRY@www.ccl.net
Subject: Re: CCL:LoBoS, a Beowulf cluster at NIH
References: <199711252018.MAA11911@horton.agouron.com>
Content-Type: text/plain; charset=us-ascii
Content-Transfer-Encoding: 7bit


Comment:

While the price of the more expensive 200Mhz PPRO chip may not get a lot cheaper,
I would note that the price of the (only) 10% slower 180Mhz/256Kcache chip is
available for ~40% of that of its faster brother/sister.  They can be had for as
little as $175.

John

Xinjun Hou wrote:

> On Mon, 24 Nov 1997, Chris Harwell wrote:
> >...
> >3. Don't be taken in by the Intel Bunny people and automatically buy a
> >PentiumII.  The PentiumII is a PentiumPro with MMX (useless for
> >floating point ops) and faster memory access.  Unfortunately, the
> >advantages are offset by an off-chip cache that runs at half the speed
> >of the PentiumPro.  Our benchmarks showed that the PentiumII performance
> >improvements barely scale up with the faster clock rates.
>
> Another issue is the cost of processor in the future: PPro's architecture
> (on-chip cache) makes it very costly in production. This is another reason
> Intel came up with PentiumII with off-chip cache. The off-chip cache structure
> is also cheaper to expand, both in terms of size and clock speed.
>
> So bottom line is that PPro with on-chip cache has a better architecture
> than Pentium II for computional extensive work, but Intel might not lower
> the price further or devepop it more (high clock speed or more cache).  The
> cost/performance ration of two CPU would change in the future.
>
> Xinjun
>
> C     Xinjun J. Hou (hou@agouron.com)      Agouron Pharmaceuticals, Inc.
> C10110000110100101101110011010100111010101101110010010000110111101110101
>
> -------This is added Automatically by the Software--------
> -- Original Sender Envelope Address: hou@Agouron.COM
> -- Original Sender From: Address: hou@Agouron.COM
> 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 McKelvey                    *
* Computational Science Laboratory *
* Imaging Research and Development *
* Building 83                      *
* Research Laboratories            *
* Eastman Kodak Company            *
* Rochester, NY 14650-2216         *
* (V)716-477-3335                  *
* (F)716-722-2327                  *
* (E)McKelvey@Kodak.COM            *
************************************



From kharroub@cit.enscm.fr  Wed Nov 26 10:37:28 1997
Received: from cit.enscm.fr  for kharroub@cit.enscm.fr
	by www.ccl.net (8.8.3/950822.1) id KAA17202; Wed, 26 Nov 1997 10:21:02 -0500 (EST)
Received: from [193.52.205.156] by cit.enscm.fr (AIX 4.1/UCB 5.64/4.03)
          id AA18628; Wed, 26 Nov 1997 16:09:17 +0100
Message-Id: <3.0.2.32.19971126161844.00908d60@cit.enscm.fr>
X-Sender: kharroub@cit.enscm.fr
X-Mailer: QUALCOMM Windows Eudora Light Version 3.0.2 (32)
Date: Wed, 26 Nov 1997 16:18:44 +0100
To: CHEMISTRY@www.ccl.net
From: Kharroubi Mohamed <kharroub@cit.enscm.fr>
Subject: Bond Dissociation Energies
Cc: CHEMISTRY@www.ccl.net
Mime-Version: 1.0
Content-Type: text/plain; charset="us-ascii"


Hello!
  
  I would appreciate if somebody point me to books, reviews or other
sources dealing with the calculation of bond dissociation energies (BDE)
from theoretical (semi-empirical, ab initio or DFT) and experimental point
of view.
 Thank you in advance.


===================================
Mohamed KHARROUBI
LCA  UPRSA-5076
ENSCM
8, rue de l'Ecole Normale
F-34296 MONTPELLIER CEDEX 5
FRANCE
tel:    04.67.14.72.06
fax:    04.67.14.72.20
e-mail: kharroub@cit.enscm.fr
====================================

From glossman@overnet.com.ar  Wed Nov 26 10:42:24 1997
Received: from carpincho.overnet.com.ar  for glossman@overnet.com.ar
	by www.ccl.net (8.8.3/950822.1) id KAA17331; Wed, 26 Nov 1997 10:34:35 -0500 (EST)
Received: from nppp157.overnet.com.ar (nppp157.overnet.com.ar [200.16.163.165])
	by carpincho.overnet.com.ar (8.8.8/8.8.5) with SMTP id MAA19736
	for <chemistry@www.ccl.net>; Wed, 26 Nov 1997 12:35:03 -0300
Message-Id: <3.0.1.16.19971126122833.1a3f56e4@pop.overnet.com.ar>
X-Sender: dfa953uo@pop.overnet.com.ar
X-Mailer: Windows Eudora Light Version 3.0.1 (16)
Date: Wed, 26 Nov 1997 12:28:33
To: chemistry@www.ccl.net
From: "Dr. M. Daniel Glossman" <glossman@overnet.com.ar>
Subject: programs for plotting densities
Mime-Version: 1.0
Content-Type: text/plain; charset="us-ascii"


 Dear netters:

  I would like to receive information about any software (commercial or not)
  for the Windows NT environment that could be useful for plotting two and
  three dimensional electon densities and electrostatic potentials starting
  from Gaussian 94 computed wavefunctions ( .out and .chk files).

  I thank you in advance for your answers.



						Daniel Glossman

******************************************************************************
Dr. M. Daniel Glossman
Universidad Nacional de Lujan		e-mail: glossman@overnet.com.ar
Departamento de Ciencias Basicas	Phone: (+54) 323 23171
Casilla de Correo 221			FAX: (+54) 323 25795
(6700) Lujan
Republica Argentina

From widauer@inorg.chem.ethz.ch  Wed Nov 26 12:37:31 1997
Received: from inorg.chem.ethz.ch  for widauer@inorg.chem.ethz.ch
	by www.ccl.net (8.8.3/950822.1) id MAA17974; Wed, 26 Nov 1997 12:00:37 -0500 (EST)
Received: from rosmarin (rosmarin.ethz.ch [129.132.65.132])
	by inorg.chem.ethz.ch (8.8.8/8.8.8) with SMTP id SAA18970
	for <CHEMISTRY@www.ccl.net>; Wed, 26 Nov 1997 18:00:11 +0100
Message-Id: <3.0.32.19971126175958.00912100@elwood.ethz.ch>
X-Sender: widauer@elwood.ethz.ch
X-Mailer: Windows Eudora Pro Version 3.0 (32)
Date: Wed, 26 Nov 1997 18:00:22 +0100
To: CHEMISTRY@www.ccl.net
From: Christoph Widauer <widauer@inorg.chem.ethz.ch>
Subject: SUMMARY of As and Sb basis sets
Mime-Version: 1.0
Content-Type: text/plain; charset="iso-8859-1"
Content-Transfer-Encoding: quoted-printable


dear netters

Sorry that I summarize late. Here are the answers and advices for my
question about all electron basis sets for As and Sb. Thanks a lot for all
answers and advices. Special Thanks to Kerwin Dobbs and Cory.=20

Here is a list of the answers:

1.) Nathalie Goldbout wrote:

 I have optimized basis sets for these atoms.=20
PNL distributes them (http://www.emsl.pnl.gov:2080/forms/basisform.html).
As you will find them, they are DZVP but you can make them=20
TZVP.=20

Nathalie

2.)Kerwin Dobbs suggests:

They are not very large basis sets, but you could use my=20
3-21G* basis sets for these elements. They will get you=20
decent geometries (and frequencies) to be used in calculations
with larger basis sets. If you have access to Gaussian 94,
they are already in there.=20

-As 0
     S 3 1.00
0.540761380E+04    0.626011000E-01
0.818174360E+03    0.372779000E+00
0.179265690E+03    0.685184200E+00
    SP 3 1.00
0.237778288E+03    -.112838429E+00    0.149679775E+00
0.542566227E+02    0.872274379E-01    0.562322265E+00
0.163280291E+02    0.968188275E+00    0.459323497E+00
    SP 3 1.00
0.171018532E+02    -.291453678E+00    0.256855918E-01
0.580514411E+01    0.296961892E+00    0.483396807E+00
0.190208419E+01    0.886579104E+00    0.588785396E+00
     D 3 1.00
0.274372090E+02    0.154495200E+00=20
0.708404400E+01    0.511431800E+00=20
0.185582260E+01    0.582193500E+00=20
    SP 2 1.00
0.167540361E+01    -.505760964E+00    0.252824660E-01
0.341655706E+00    0.125176452E+01    0.987432836E+00
    SP 1 1.00
0.113630312E+00    0.100000000E+01    0.100000000E+01
     D 1 1.00
0.293000000E+00    0.100000000E+01=20
****
-Sb 0
     S 3 1.00
0.132893830E+05    0.609843000E-01  =20
0.201052180E+04    0.366848700E+00  =20
0.441698150E+03    0.691050100E+00
    SP 3 1.00
0.598889050E+03    -.112720134E+00    0.153067117E+00
0.130038601E+03    0.826443261E-01    0.613597248E+00
0.421328602E+02    0.970257861E+00    0.391699015E+00
    SP 3 1.00
0.515133288E+02    -.277043338E+00    -.137869858E+00
0.244359459E+02    0.575032340E-01    0.536354977E+00
0.742093080E+01    0.108470283E+01    0.650867638E+00
     D 3 1.00
0.115809550E+03    0.116627900E+00=20
0.323058350E+02    0.483436300E+00=20
0.102503280E+02    0.590139500E+00=20
    SP 3 1.00
0.731423541E+01    0.440381164E+00    0.153051809E-01
0.284405286E+01    -.473734095E+00    0.516083219E+00
0.110585467E+01    -.822134968E+00    0.538757047E+00
     D 3 1.00
0.548621020E+01    0.248365600E+00=20
0.192161960E+01    0.574315400E+00=20
0.666062650E+00    0.364304400E+00=20
    SP 2 1.00
0.127863729E+01    0.601695106E+00    -.222527566E-01
0.241232097E+00    -.125869202E+01    -.989643364E+00
    SP 1 1.00
0.866296732E-01    0.100000000E+01    0.100000000E+01
     D 1 1.00
0.211000000E+00    0.100000000E+01=20
****

3.)Cory from University of calcgary wrote:

The reference is:
S. Huzinaga, J. Andzelm, M. Klobukowski, E. Radzio-Andzelm, Y. Sakai, H.=20
Tatewaki, Gaussian Basis Sets for Molecular Calculations, Elsevier,=
 Amsterdam,
1984.=20
These are all minimal basis sets. What we did was split the outermost shell
and add a d-polarization function accordind to Huzinaga's suggestions.

For example, the arsenic minimal basis set is (4333/433/4). We split the=
 outer
most s and p shell (since the d shell is not participating in the bonding,
we left it as a single-zeta), and added a d-polarization function to obtain
(43321/4321/41*) - note that the 1* at the end stands for a polarization fn,=
=20
some authors just use the *, so be careful.

The resulting basis set (in MUNGAUSS/MONSTERGAUSS format) is:
     1S     1.000000
        15860.364           0.0171048
        2391.2232           0.1200249
        542.23120           0.4378747
        146.00269           0.5576566
     2S     1.000000
        219.08007           -.1096535
        24.437631           0.6475717
        10.206970           0.4248194
     3S     1.000000
        18.744848           -.2334702
        3.1047892           0.7294911
        1.2970598           0.4044278
     4S     1.000000
        1.8301844           -.1924620
        0.28147770          0.6866084
     5S     1.000000
        0.10437810          1.000000
     2P     1.000000
        670.45052           0.000000        0.0275156
        157.17065           0.000000        0.1794001
        48.639537           0.000000        0.5052466
        16.532308           0.000000        0.4576592
     3P     1.000000
        7.4556466           0.000000        0.3248901
        2.9185276           0.000000        0.5568808
        1.1701325           0.000000        0.2280292
     4P     1.000000
        0.17189969          0.000000        0.5495546
        0.44648872          0.000000        0.3297273
     5P     1.000000
        0.06621832          0.000000        1.000000
     3D     1.000000
        49.802186           0.0618851
        13.722924           0.2858504
        4.3622725           0.5264330
        1.3044304           0.4103582
     4D     1.000000
        0.2930000           1.000000
****

For antimony, the minimal basis set is (43333/4333/43), this becomes
(433321/43321/431*) , giving
     1S     1.000000
        39022.365           0.0166099
        5882.7978           0.1168445
        1336.0527           0.4316276
        360.85938           0.5658267
     2S     1.000000
        537.93220           -.1140683
        62.500390           0.6463407
        27.197858           0.4259875
     3S     1.000000
        50.167831           -.2738817
        9.1496108           0.8622209
        4.1385594           0.2916257
     4S     1.000000
        7.9705964           0.3451482
        1.8315322           -.8192352
        .83166100           -.3885285
     5S     1.000000
        1.2644570           0.2282069
        .20413637           -.7343321
        .07938248           -.4004066
     2P     1.000000
        1824.8261           0.000000        0.0243008
        429.63172           0.000000        0.1658149
        134.35726           0.000000        0.4934148
        47.067397           0.000000        0.4764640
     3P     1.000000
        146.26897           0.000000        -.0249529
        19.176344           0.000000        0.4788591
        7.5448193           0.000000        0.5894057
     4P     1.000000
        3.1351377           0.000000        0.4330085
        1.3685954           0.000000        0.5296693
        .59068398           0.000000        0.1168509
     5P     1.000000
        .30628842           0.000000        -.3619153
        .12718587           0.000000        -.5374627
        .05241622           0.000000        -.2013450
     3D     1.000000
        213.55477           0.0392992
        62.116599           0.2241339
        21.914940           0.5229188
        7.9902814           0.4250002
     4D     1.000000
        5.0718312           0.2751370
        1.8456173           0.5677492
        .64518169           0.3414352
     5D     1.000000
        .21100000           1.0000000
****


Note that the format is the same for both P shells above and for SP shells.
(exponent s-contraction p-contraction). This explains the 0.0000 in the=20
P shells in the s-contraction coefficient column. Gaussian XX wouldn't have
this.


-COry

4.)  Doug Fox  wrote:

For As the 6-311G basis set is defined and is roughly triple zeta
in quality. Also we have adopted Curtiss's 6-41G basis set for As=20
as a double zeta quality basis which you can select as 6-31G.  There
are no comparable basis sets built in for Sb nor do I have a suggestion
that I could support for such a basis.

Again, thanks to all who answered. The next time I will summrize earlier
for sure.

christoph
----
Christoph Widauer
Laboratorium f. Anorganische Chemie
ETH-Zentrum CAB C8
Universit=E4tsstrasse 6
CH-8092 Zuerich=20

Phone (Zurich): +41 (1) 632 61 19
Fax (Zurich): +41 (1) 632 10 90
e-mail: widauer@inorg.chem.ethz.ch




From ryszard@lisa.moldyn.com  Mon Nov 24 13:35:14 1997
Received: from worf.moldyn.com  for ryszard@lisa.moldyn.com
	by www.ccl.net (8.8.3/950822.1) id MAA05974; Mon, 24 Nov 1997 12:55:13 -0500 (EST)
Received: from lisa.moldyn.com by worf.moldyn.com via ESMTP (950413.SGI.8.6.12/950213.SGI.AUTOCF)
	for <@worf.moldyn.com:CHEMISTRY@www.ccl.net> id MAA12997; Mon, 24 Nov 1997 12:55:01 -0500
Received: by lisa.moldyn.com (951211.SGI.8.6.12.PATCH1502/940406.SGI.AUTO)
	 id MAA26328; Mon, 24 Nov 1997 12:54:59 -0500
Date: Mon, 24 Nov 1997 12:54:57 -0500 (EST)
From: Ryszard Czerminski <ryszard@worf.moldyn.com>
To: CHEMISTRY@www.ccl.net
Subject: tRNA modelling: summary
Message-ID: <Pine.SGI.3.91.971124125150.24179E-100000@lisa.moldyn.com>
MIME-Version: 1.0
Content-Type: TEXT/PLAIN; charset=US-ASCII




---- Original question:

Dear All,

I am looking for information about tRNA modelling.
In particular for MD simulations
and parametrization of rare nucleotides (pseudo-uracil
etc...)

Ryszard Czerminski         phone : (617)354-3124 x 13
Moldyn, Inc.               fax   : (617)491-4522
955 Massachusetts Avenue   e-mail: ryszard@moldyn.com
Cambridge MA, 02139-3180   or      ryszard@photon.com

SUMMARY:

If anybody has information about charges (preferably published)
used for rare nucleotides either with amber or charmm ff
I would appreciate to hear from you...

RC.

---- Thank you to all who responded (in chronological order)

Darrell R. Davis
Christoph Schneider
Thomas Hermann
John E. Reissner
Kevin J. Mcconnell
Pascal Auffinger

---- useful RNA links

http://www.imb-jena.de/RNA.html
http://www.ibc.wustl.edu/~zucker/ma       (does not work ?)
http://algodones.unm.edu/~phraber/ma.html (does not work ?)

---- and recent references
---- (biased by my interests and by no means complete)

%
% tRNA structure and dynamics
%
@INCOLLECTION{Auffinger98,
   AUTHOR = "Pascal Auffinger and Eric Westhof",
   BOOKTITLE  = "Modification and Editing of RNA: The alternation of
                 RNA Structure and Function",
   chapter = 6,
   title = "Effects of Pseudouridylation on tRNA Hydration and Dynamics:
            A Theoretical Approach",
   PUBLISHER = {Americal Society for Microbiology},
   ADDRESS = {Washington, DC 20005},
   YEAR = 1998 }

@INCOLLECTION{Auffinger97a,
   AUTHOR = "Pascal Auffinger and Eric Westhof",
   BOOKTITLE  = "Enclyclopedia of computational chemistry",
   title = "Molecular Dynamics Simulations of Nucleic Acids",
   PUBLISHER = {Wiley \& Sons},
   ADDRESS = {NY},
   YEAR = 1997 }

@ARTICLE{Hermann97,
   author = "Thomas Hermann and Pascal Auffinger and William G. Scott
             and Eric Westhof",
   title = {Evidence for a hydroxide ion bridging two magnesium ions at the
            active site of the hammerhead ribozyme},
   journal = {Nucl. Acid Res.},
   year = 1997,
   volume = 25,
   number 17,
   pages = {3421-3427},
   abstract = {In the presence of magnesium ions cleavage by the hammerhead ribozyme
      RNA at a specific residue leads to 2'3'-cyclic phosphate and 5'-OH
      extremities. In the cleavage reaction an activated ribose 2'-hydroxyl
      group attacks its attached 3'-phosphate. Molecular dynamics simulations
      of the crystal structure of the hammerhead ribozyme, obtained after flash-
      freezing of crystals under conditions where the ribozyme is active,
      provide evidence that a $\mu$-bridging OH$^-$ ion is located between
      the two Mg$^{+2}$ ions close to the cleavable phosphate. Constrained
      simulations show further that a flip from the C3'-endo to the C2'-endo
      conformation of the ribose at the cleavable phosphate brings the
      2'-hydroxyl in proximity to both the attacked phosphorus atom and the
      $\mu$-bridging OH$^-$ ion. Thus, the simulations lead to a detailed
      new insight into the mechanism of hammerhead ribozyme cleavage where
      a $\mu$-hydroxo bridged magnesium cluster, located on the deep groove
      side, provides an OH$^-$ ion that is able to activate the 2'-hydroxyl
      nucleophile after a minor conformational change in the RNA.}}

@ARTICLE{Auffinger97b,
   author = "Pascal Auffinger and Eric Westhof",
   title = {{RNA} Hydration: Three nanoseconds of multiple molecular dynamics
            simulations of the solvated {tRNA$^{Asp}$} anticodon hairpin.},
   journal = {J. Mol. Biol.},
   year = 1997,
   volume = 269,
   pages = "326-341",
   abstract = {The hydration of the tRNA$^{Asp}$ anticodon hairpin was
      investigated through the analysis of six 500 ps multiple molecular
      dynamics (MMD) trajectories generated by using the PME method for the
      treatment of the long-range electrostatic interactions. Although similar
      in their dynamical characteristics, these six trajectories display
      different local hydration patterns reflecting the landscape of the
      ``theoretical'' conformational space being explored. The statistical
      view gained through the MMD strategy allowed us to characterize the
      hydration patterns around important RNA structural motifs such as G-U base
      pair, the anticodon U-turn, and two modified bases: pseudouridine
      and 1-methylguanine [...] No long-lived hydrogen bond between water and
      a 2'-hydroxyl has been observed. Water molecules with long-residence
      times are found bridging adjacent pro-R$_P$ phosphate atoms. The conformation
      of the pseudouridine is stiffened by a water-mediated base-backbone interaction
      and the 1-methylguanine is additionally stabilized by long-lived hydration
      patterns. Such long-lived hydration patterns are essential to ensure
      the structural integrity of this hairpin motif. Consequently, our simulations
      confirm the conclusions reached from an analysis of X-ray crystal structures
      according to which water molecules form an integral part of nucleic acid
      structure. The fact that the same conclusion is reached from a static and a
      dynamic point of view suggest that RNA and water together constitute the
      biologically relevant functional entity}}

@ARTICLE{Auffinger97c,
   AUTHOR = {Pascal Auffinger and Shirley Louise-May and Eric Westhof},
   TITLE = {Hydration of C-H groups in tRNA},
   JOURNAL = {Faraday Discuss.},
   YEAR = 1997,
   VOLUME = 103,
   PAGES = {151-174},
   abstract = {MD simulations of the anticodon hairpin of tRNA$^Asp$ and
     of full tRNA, both in a solvent bath with neutralizing NH$_4^+$
     counter ions, have been produced with the particle mesh ewald (PME)
     method and multiple molecular dynamics (MMD) strategy [...]}}

@ARTICLE{Auffinger97d,
   author = "Pascal Auffinger and Eric Westhof",
   title = {{RNA} Hydration: Three nanoseconds of multiple molecular dynamics
            simulations of the solvated {tRNA$^{Asp}$} anticodon hairpin.},
   journal = {J. Mol. Biol.},
   year = 1997,
   volume = 274,
   pages = "54-63",
   abstract = {MD simulations reveal that, in C$_{3'}$-endo sugar puckers,
     only three orientations are accessible to the 2'-hydroxyl groups distinctive
     of RNA molecules: towards (i) the O$_{3'}$, (ii) the O$_{4'}$ of the
     same sugar, and (iii) the shallow groove base atoms. In the rarer
     C$_{2'}$-endo sugar puckers, orientations towards the O$_{3'}$ atom of
     the same sugar are strongly favoured. Surprisingly, in helical regions, the
     frequently suggested intra-strand O$_{2'}$ - H(n)...O$_{2'}$(n+1) interaction
     is not found. This observation led to the detection of an axial C-H...O
     interaction between the C$_{2'}H(n) group and the O$_{4'}$(n+1) atom
     contributing to the stabilization of RNA helical regions. Subsequent analysis
     of crystallographic structures of both RNA and A-DNA helices fully supports
     this finding. Specific hydration patterns are also thought to play
     a significant role in the stabilization of RNA structures. In the shallow
     groove of RNA, known as a favorable RNA or protein binding region, three
     well defined hydration sites are located around the O$_{2'}$ atoms. These
     hydration sites, occupied by water molecules exchanging with a bulk,
     constitute after dehydration, anchor points for specific interactions between
     RNA and nucleic acids, proteins or drugs. Therefore, the fact that the
     2'-hydroxyl group is not monopolised by axial stabilization, together with
     its water like behavior, facilitates complex formation involving RNA
     helical regions.}}

@ARTICLE{Jia97,
   author = {Yiwei Jia, Alexander Sytnik, Liangquan Li, Serguei Vladimirov,
             Barry S. Cooperman, and Robin M. Hochstrasser},
   title = {Nonexponential kinetics of a single {tRNA$^{Phe}$} molecule
            under physiological conditions},
   journal = {Proc. Natl. Acad. Sci. USA, Biophysics},
   year = 1997,
   volume = 94,
   pages = "7932-7936",
   abstract = {The fluorescence decay functions of individual, specifically
     labeled tRNAPhe molecules exhibit nonexponential character as a result
     of conformational dynamics occurring during the measurement on a single
     molecule. tRNAPhe conformational states that interchange much more slowly
     are evidenced by the distribution of lifetimes observed for many individual
     molecules. A structural model for the nonexponential decay indicates that
     the tRNAPhe-probe adduct fluctuates between two states, one of which provides
     conditions that quench the probe fluorescence.} }

@MISC{Lahiri97,
   author = "Ansuman Lahiri and Lennart Nilsson",
   title = {Molecular dynamics study of the anticodon loop of Yeast tRNAphe},
   howpublished = "http://hackberry.chem.niu.edu/ECCC4/articles/article41"
   year = 1997,
   month = November,
   abstract = {Molecular dynamics simulations of the aqueous solution of Yeast
     tRNAphe anticodon loop with counterions were carried out. We looked at the
     stability of the system and the simulation protocol by a long simulation
     (over 1 ns)  and a set of shorter simulations (duration 300 ps each)
     which differed only in the initial velocity assignments. In all the cases,
     the structure remains close to the starting crystal structure with
     a 3'-stacked conformation nicely maintained. We have also investigated
     the dynamics of the anticodon loop interacting with UUU and UUC
     ribotrinucleotide diphosphates, codons for the amino acid phenylalanine.},
   note = {CHARMM22 all atom parameter set + modified parameters for rare
           nucleotides}}

@ARTICLE{Auffinger96a,
   author = {P. Auffinger and E. Westhof},
   title = {H-bond stability in the {tRNA$^{Asp}$} anticodon hairpin: 3 ns of
            multiple molecular dynamics simulation},
   journal = "Biophys. J.",
   year = 1996,
   volume = 71,
   pages = "940-954",
   abstract = { Multiple MD trajectories of the solvated and neutralized
     17-residue tRNS$^{Asp}$ anticodon hairpin were generated for a total of
     3 ns. Explicit treatment of all long-ranged electrostatic interactions
     by the particle mesh Ewald algorithm, as implemented in the AMBER MD
     software package, effected a degree of structural stabilization not
     previously achieved by use of a long 16A solvent interaction truncation
     scheme. The increased stability of this multiple molecular dynamics set
     was appropriate for an in-depth analysis of the six 500-ps-long
     trajectories and allowed the characterization of a number of key
     structural interactions. The dynamical behavior of the standard 
     Watson-Crick base-pairs, the noncanonical G30-U40 ``wobble'' base
     pair, and the $\Psi$32-C38 pseudo-baise pair is presented as well as
     that of two C-H...O hydrogen bonds found to contribute to array
     of tertiary interactions that stabilize the seven-nucleotide native
     loop conformation. The least mobile residue in the loop is U33,
     which forms the U-turn motif and which participates in several
     hydrogen-bonding interactions, whereas the most mobile residue is the
     apical residue G34 at the wobble position, a factor undoubtedly important
     in its biologocal function. The set of multiple molecular dynamics
     trajectories does not converge on a 500-ps time scale to a unique
     dynamical model but instead describes an ensemble of structural
     microstates accessible to the system under the present simulation
     protocol, which is the result of local structural heterogeneity
     rather than of global conformational changes.}}

@ARTICLE{Auffinger96b,
   author = "P. Auffinger and E. Westhof",
   title = {Molecular dynamics simulations of the anticodon
            hairpin of tRNA$^{Asp}$: Structuring effects of C-H...O hydrogen
            bonds and of long-range hydration forces},
   journal = JACS,
   year = 1996,
   volume = 118,
   pages = "1181-1189",
   abstract = {The inclusion of long-range sovent interactions out to 16A
     in a molecular dynamics study of the anticodon loop of tRNA$^{Asp}$ led
     to an overall structural stabilization of the RNA hairpin tertiary interactions
     in a set of six independent fully solvated and neutralized 100ps MD trajectories
     as compared to a shorter-ranged solvent interaction electrostatic model (8A).
     The increased structural stabilization allowed for the emegence of non-classical
     C-H...O hydrogen bonds in the MD trajectories. The presence of the C-H...O
     hydrogen bonds in the crystal structure was subsequently verified and
     dynamically characterized and their contribution to the preservation
     of the tertiary native conformation was assessed [...]} }

@ARTICLE{Louise96,
   AUTHOR = {Shirley Louise-May and Pascal Auffinger and Eric Westhof},
   TITLE = {Calculations of nucleic acid conformations},
   JOURNAL = {Curr. Opin. Struct. Biol.},
   YEAR = 1996,
   VOLUME = 6,
   PAGES = {289-298},
   abstract = {The present computational power and sophistication
     of theoretical approaches to nucleic acid structural investigation
     are sufficient for the realization of static and dynamic models
     that correlate accurately with current crystallographic, NMR and
     solution-probing structural data, and consequently are able to
     provide valuable insights and predictions for a variety of nucleic
     acid conformational families. In molecular dynamics simulations,
     the year 1995 was marked by the foray of fast Ewald methods, an
     accomplishment resulting from several years' work in the search
     for an adequate treatment of the electrostatic long-range forces
     so primordial in nucleis acids behavior. In very large systems, and 
     particularly in the RNA-folding field, techniques originating from
     artificial intelligence research, like constraint satisfaction
     programming or genetic algorithms, have established their utility
     and potential.}}

@ARTICLE{Westhof96a,
   author = "E. Westhof et al.",
   title = {},
   journal = Science,
   year = 1996,
   volume = 272,
   pages = "1343",
   abstract = {} }

@ARTICLE{Auffinger95,
   AUTHOR = {P. Auffinger; S. Louise-May; E. Westhof},
   TITLE = {Multiple molecular dynamics simulations of the
            anticodon loop of tRNA$^Asp$ in aqueous solution with counterions},
   JOURNAL = JACS,
   YEAR = 1995,
   VOLUME = 117,
   PAGES = {6720-6726},
   abstract = {In a systematic search for a stable protocol with which to extend
     our dynamical investigations, a nanosecond of MD simulations of the solvated
     anticodon loop of tRNA$^Asp$ consisting of ten unique trajectories was obtained
     by slight modifications to the starting conditions. These changes produced
     divergent trajectories which varied widely in structural and dynamical
     characteristics. However, the properties of these trajectories could not
     be directly correlated to the slight modifications introduced in the system,
     and thus, questions were raised regarding the probity of the standard
     protocol we utilized. Instead of a detailed analysis of the results, the
     multiple molecular dynamics approach was used as a diagnostic for estimating
     the reliability of the set of trajectories generated and the extent
     of relevant biochemical information which cen be extracted from it. We address
     here issues concerning critical evaluation of molecular dynamics methodology
     and detection of protocol instabilities. We infer that an ensemble of
     initial uncorrelated trajectories should be generated in order to investigate
     the constancy of structural and dynamical properties of the system under study}}

@ARTICLE{Nakamura94,
   author = {Shugo Nakamura and Junta Doi},
   title = {Dynamics of transfer RNAs analyzed by normal mode calculation},
   journal = {Nucl. Acids Res.},
   year = 1994,
   volume = 22,
   number = 3,
   pages = {514-521},
   abstract = {Normal mode calculation is applied to tRNA$^{Phe}$ and
      tRNA$^{Asp}$, and their structural and vibrational aspects are
      analyzed. Dihedral angles along the phosphate-riboze backbone
      ($\alpha, \beta, \gamma, \epsilon, \ksi$) and dihedral angles of
      glycosyl bonds ($\chi$) are selected as movable parameters.
      The calculated displacement of each atom agrees with experimental data
      In modes with frequencies higher then 130cm$^{-1}$, the motions are
      localized around each stem and the elbow region of the L-shape.
      On the other hand, collective motions such as bending and twisting
      of arms are seen in modes with lower frequencies. Hinge axes and
      bend angles are calculated without prior knowledge. Movements in modes
      with very low frequencies are combinations of hinge bending motions
      with various hinge axes and and bend angles. The thermal fluctuations
      of dihedral angles well reflect the structural changes of transfer RNAs.
      There are some dihedral angles of nucleotides located around the elbow
      region of L-shape, which fluctuate about five to six time more than
      the average value. Nucleotides in the position seem to be influential
      in the dynamics of the entire structure. The normal mode calculation
      seems to provide much information for the study of conformational
      changes of transfer RNAs induced by aminoacyl-tRNA synthetase or
      codon during molecular recognition}}
      
@ARTICLE{Nardi94,
   author = {F. Nardi and W. Doster and B. Tidor and M. Karplus and
             S. Cusack and J. C. Smith},
   title = {Dynamics of tRNA: Experimental Neutron Spectra Compared with Normal
            Mode Analysis},
   journal = {Israel J. Chem.},
   year = 1994,
   volume = 34,
   pages = {233-238},
   abstract = {A comparison is made of experimental inelastic neutron scattering
     spectra from tRNA with spectra calculated from a normal mode analysis.
     The experimental data indicate that a dynamic transition occurs with
     temperature, as is seen in proteins. At low temperatures a broad peak
     is seen in the dynamic structure factor, due to the lowest frequency
     collective modes. This peak is centered at ~40cm$^{-1}$, somewhat higher
     than that observed in small globular proteins. The vibrational frequency
     distribution calculated from the normal mode analysis rises to a broad
     maximum at ~50cm$^{-1}$, in general accord with the experiment. However
     the lowest frequency vibrations in the harmonic model (<40cm$^{-1}$)
     are nor present in experimental sample. Possible reasons for this are
     discussed.},
   note = {in calculations tRNA-Phe was used}}

@ARTICLE{Harvey93,
   author = "Harvey, S. C.;  Gabb, H. A.",
   title = {Conformational transitions using molecular dynamics with minimum
            biasing},
   journal = Biopolymers,
   year = 1993,
   volume = 33,
   pages = "1167-1172",
   abstract = {The molecular dynamics algorithm (MD), which simulates intramolecular
    motions on the subnanosecond timescale, has been modified to allow the
    investigation of slow conformational transitions that do not
    necessarily occur spontaneously in MD simulations. The method is
    designated CONTRA MD (CONformational TRAnsitions by Molecular
    Dynamics with minimum biasing). The method requires the prior
    definition of a single conformational variable that is required to vary
    monotonically from an initial conformation to a final target
    conformation. The simulation is broken up into a series of short free
    MD segments, and we determine, after each segment of MD, whether or not
    the system has evolved toward the final conformation. Those segments
    that do not move the system in that direction are deleted. Those that
    do move it toward the final conformation are patched together
    sequentially to generate a single representative trajectory along the
    transition pathway. The CONTRA MD method is demonstrated first by
    application to the simultaneous C2'-endo to C3'-endo repucker and anti
    to syn N-glycosidic torsion transitions in 2'-deoxyadenosine and then to
    the large-scale bending in phenylalanine transfer RNA.}}



From glossman@overnet.com.ar  Mon Nov 24 16:37:08 1997
Received: from carpincho.overnet.com.ar  for glossman@overnet.com.ar
	by www.ccl.net (8.8.3/950822.1) id QAA07435; Mon, 24 Nov 1997 16:09:03 -0500 (EST)
Received: from nppp239.overnet.com.ar (nppp239.overnet.com.ar [200.16.164.252])
	by carpincho.overnet.com.ar (8.8.8/8.8.5) with SMTP id SAA04163
	for <chemistry@www.ccl.net>; Mon, 24 Nov 1997 18:10:11 -0300
Message-Id: <3.0.1.16.19971124180255.1c8f8ee6@pop.overnet.com.ar>
X-Sender: dfa953uo@pop.overnet.com.ar (Unverified)
X-Mailer: Windows Eudora Light Version 3.0.1 (16)
Date: Mon, 24 Nov 1997 18:02:55
To: chemistry@www.ccl.net
From: "Dr. M. Daniel Glossman" <glossman@overnet.com.ar>
Subject: using Molden with NT
Mime-Version: 1.0
Content-Type: text/plain; charset="us-ascii"



 Dear netters:

 I am looking for somebody in the net who has been succesfull in using
 the Molden program in a Windows NT environment. I need some advice.

 Thanks in advance


					Daniel Glossman


***************************************************************************
Dr. M. Daniel Glossman
Universidad Nacional de Lujan              e-mail: glossman@overnet.com.ar
Departamento de Ciencias Basicas           Phone: (+54) 323 - 23171
Casilla de Correo 221                      Fax: (+54) 323 - 25795
6700 - Lujan
Republica Argentina

****************************************************************************


From kristyan@euch4e.chem.emory.edu  Mon Nov 24 16:55:23 1997
Received: from euch4e.chem.emory.edu  for kristyan@euch4e.chem.emory.edu
	by www.ccl.net (8.8.3/950822.1) id PAA07314; Mon, 24 Nov 1997 15:45:31 -0500 (EST)
From: <kristyan@euch4e.chem.emory.edu>
Received: by euch4e.chem.emory.edu (AIX 3.2/UCB 5.64/4.03)
          id AA29755; Mon, 24 Nov 1997 15:45:32 -0500
Date: Mon, 24 Nov 1997 15:45:32 -0500
Message-Id: <9711242045.AA29755@euch4e.chem.emory.edu>
To: chemistry@www.ccl.net
MIME-Version: 1.0
Content-Type: text/plain; charset=unknown-8bit
Content-Transfer-Encoding: 8bit



 Dear Collagues
 Dear Isabel Rozas & Han Zuilhof

>A more substantial double zeta DFT basis set is available for Sn on the
>EMSL website, from which it can be downloaded.
>http://wserv1.dl.ac.uk:800/emsl_pnl/basisform.html

    I did not have too much time to check, but after a few tries a gave up
 on this web site. (But there may be some, and this www is definitely useful.)
 I have one on file, available below.  See the definition of this rep. of
 basis (very simple) in 

    Sandor  Kristyan.: Note on the choice of basis set in density functional
  theory calculations for electronic structure of molecules (test on the
  atoms from the first three rows of the periodic table (2 ² N ² Z ² 18),
  water, ammonia and pyrrole)
    Chemical Physics Letters, 256, 1996, 229-240
  (This article has no info about Sn.)

 kristyan@euch4e.chem.emory.edu
 Sandor Kristyan
 November 21, 1997

FOR       SN
S   1     12741.6740  0.061135
    2     1928.46920  0.367293
    3     423.807970  0.690545
S   4     564.682200 -0.109749
    5      55.241831  0.718112
    6      23.121421  0.349097
P   7     816.773230            0.082073
    8     191.127720            0.426433
    9      56.771595            0.635902
S  10      48.493098 -0.270898
   11       8.770315  0.840906
   12       4.037810  0.310103
P  13     121.244870           -0.031564
   14      19.577904            0.415167
   15       7.571713            0.654993
D  16     108.056300  0.119824
   17      30.131576  0.487591
   18       9.530036  0.584987
S  19       7.615495 -0.347566
   20       1.729893  0.793758
   21       0.771888  0.413201
P  22       3.047403            0.398267
   23       1.302218            0.555779
   24       0.544629            0.130139
D  25       4.962610  0.252949
   26       1.712083  0.572761
   27       0.577195  0.369039
S  28       1.197655 -0.238559
   29       0.173037  0.705986
P  30       0.267529            0.321091
   31       0.104183            0.565904
S  32       0.066960  0.423612
P  33       0.041626  0.221811
******


From arthur@csb0.IPC.PKU.EDU.CN  Mon Nov 24 21:37:08 1997
Received: from csb0.IPC.PKU.EDU.CN  for arthur@csb0.IPC.PKU.EDU.CN
	by www.ccl.net (8.8.3/950822.1) id UAA08924; Mon, 24 Nov 1997 20:53:57 -0500 (EST)
Received: by csb0.IPC.PKU.EDU.CN (920330.SGI/940406.SGI.AUTO)
	for chemistry@www.ccl.net id AA04702; Tue, 25 Nov 97 09:53:53 -0800
Date: Tue, 25 Nov 1997 09:53:53 -0800 (PST)
From: Arthur Wang <arthur@csb0.IPC.PKU.EDU.CN>
To: CCL mailing list <chemistry@www.ccl.net>
Subject: Summary: logP for amino acids
Message-Id: <Pine.SGI.3.91.971125095000.4697A-100000@csb0.IPC.PKU.EDU.CN>
Mime-Version: 1.0
Content-Type: TEXT/PLAIN; charset=US-ASCII




Dear CCLers,

Two weeks ago, I posted such a question:

"We are currently on a project of de novo protein design. A set of scales
which describe the hydrophobicities of the natural amino acids is what we
badly need. So, would you please kindly provide any clue for the following
issues:  (1) Any paper describing such a set of scales (2) LogP values for
the 20 natural amino acids and oligopeptides (up to buta- or
pentapeptides).  (3) Solubilities for these amino acids and
oligopeptides."

And the answers I have received are:


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

From: Thomas Scior <thomas.scior@uni-tuebingen.de>

NI HOW Arthur ! 
Please, do apologize I do not speak Chinese ! 
But conerning your question : 
there is a book called 
Introduciiton to  LIPOPHILICITY 
from 
VCH Verlagsgesellschaft Weinheim Germany 
maybe there is a home page http://vch.de   or   .com 

If you can not find this book , please mail me in December 
again, then I can give you the exact reference.
Also, I am doeing the same kind of  project  
with small molecules 

see
http://link.springer.de/link/service/journals/00894/bibs/7003008/70030332.htm

Best wishes 

Tom Scior, 
Pharmacy 
Molecular Modeling
germany

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

From: Wayne Steinmetz <WSTEINMETZ@POMONA.EDU>

You will probably find the data and discussion in the following paper useful:
W. E. Steinmetz, "A CoMFA Analysis of Selected Physical Properties of 
Amino Acids in Water", Quant. Struct.-Act. Relat., 14, 19-23 (1995).
There is a medicinal chemistry institute headed by Professor Ren Li in Beijing.
Thje institute should have a subscription to this journal.

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

From: Richard Gillilan <richard@TC.Cornell.EDU>

Andrew Karplus' latest paper on that subject is well 
worth looking at:

 "Hydrophobicity regained" P.A. Karplus
  Protein Science (1997) 6:1-6

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

From: <Steve.Bowlus@sandoz.com>

A literature search concerning Z-scales and Svante Wold (spelling?) should
provide some leading references for (1), and probably references relating to
(2), since the scales include that information, if I recall correctly.

Several years ago (1991-1994?), Tripos did an application note on this topic.
You might try contacting them.  The presentation was given by Wally Reiher (are
you out there, Wally?).

sb

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

From: victoria@acdlabs.com (Victoria Barclay)

Advanced Chemistry Development has software to calculate LogP
(and as of this fall, LogD and Solubility) for peptides (and oligopeptides)
in zwitterionic form.  Literature values for 3600 structures
with known LogP and the conditions of determination can also be
automatically looked up.  Our algorithm is based on well-characterized 
logP contributions of separate atoms, structural fragments, 
and intramolecular interactions between different fragments. 
If you would like to receive a copy of our demo CD,
which contains a demo version of the software and more detailed
product information, please let me know.

Best regards,
Victoria
-------------------
Victoria Barclay, Ph.D.
Manager, Scientific Support
Advanced Chemistry Development, Inc.  
Suite 605, 133 Richmond St. W., Toronto, Canada M5H 2L3
Voice: (416) 368-3435  Fax: (416) 368-5596  Toll-free: 800-304-3988
e-mail:  victoria@acdlabs.com    web: http://www.acdlabs.com

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

From: Willie Cui <info@microsimulations.com>

Authur,

For the hydro. scale, try HINT by Kelloge of Virgina Common Wealth Univ.
I do not quite remember the web address. If you have difficulty locate
it,let me know I will find it out for you.

-- 
Willie Cui			voice: 201-512-0486
MicroSimulations		fax:   201-512-0489
478 Green Mountain Road		email: info@microsimulations.com
Mahwah, NJ 07430		URL:   http://www.microsimulations.com

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

From: Kapi Rosenfeld <kapi@engpub1.bu.edu>

a good paper to look at (although a little bit old) is the analysis
performed by J. Cornette et al published in the late 80's or
early 90's in the Journal of Molecular Biology.  These authors
analyze about 40 different hydrophobicity scales.  (if i remember
correctly the last author on this paper is C. DeLisi.

R. Rosenfeld

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

From: shaun@uthct.edu (Shaun D. Black)

Dear Arthur,

      I have developed and published parameters for about 60 amino acid
side chains (native, post-translational, co-translational, and artificial).
You can check them out at:

http://pegasus.uthct.edu/ResUTHCT/Investigators/SBlack/aagrease.html
 (parameters for native 20 amino acids, molecular weights, refs., etc.)

http://pegasus.uthct.edu/ResUTHCT/Investigators/SBlack/aamodgre.html
 (parameters etc. for many modified amino acids)

I hope this helps!

Best regards,

Shaun Black


  =-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=
  = Shaun D. Black, PhD   | Internet e-mail address:   shaun@uthct.edu  =
  = Dept. of Biochemistry | University of Texas Health Center at Tyler  =
  = Tyler, TX  75710      | World Wide Web:       http://www.uthct.edu  =
  =-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=

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

From: Tomoko Niwa <t.niwa@nippon-shinyaku.co.jp>

Please check the following papers: 

Tomoko Sotomatsu-Niwa, Akio Ogino, Evaluation of the hydrophobic
parameters of the amino acid side chains of peptides and their 
application in QSAR and conformational studies, THEOCHEM (1997), 
392, 43-54.
 
We statistically analyzed the experimentally determined 1-octanol/water
partition coefficient, log P, of a wide variety of N-acetyl-di- and tripeptide
amides and unblocked di- and tripeptides to evaluated the hydrophobic
parameters of the amino acid side chains of peptides.  For blocked peptides,
hydrophobic parameters were defined for amino acids having un-ionizable and
ionizable side chains.  For unblocked peptides, hydrophobic parameters were
evaluated for 12 amino acids with un-ionizable side chains.  In order to
estimate the hydrophobic parameters for unnatural and ionizable amino acids, a
procedure was developed based on the relationship between our hydrophobic
parameters and the log P values of model amino acids calculated by the fragment
constant method.  Use of the hydrophobic parameters in quantitative
structure-activity relationship (QSAR) studies of bioactive peptides and
conformational studies of proteins have also been presented.
(Our method is valid for the log P values for buta- or pentapeptides. ) 


Table 4  Hydrophobic parameters for the amino acid side
chains of unblocked peptides

amino acid   pa(N)      pa(MC)       pa(N) a                pa(MC) a
CLOGP-R

 A   Ala     0.24     0.12      0.19         0.24         2.680
 G   Gly     0.00     0.00      0.00         0.00         2.281
 I   Ile     0.99     1.10      0.72         1.17         4.137
 L   Leu     1.03     1.24      0.92         1.28         4.137
 M   Met     0.64     0.89      0.67         0.93         2.828
 F   Phe     1.36     1.55      1.35         1.57         4.248
 P   Pro     0.19       b         c           c           3.314
 S   Ser     0.02    -0.20     -0.08         0.04         0.693
 T   Thr     0.47     0.06      0.07         0.25         1.002
 W   Trp     1.76     1.78      1.72         1.93         4.248
 Y   Tyr     0.94     0.90      0.78         1.01         3.581
 V   Val     0.42     0.68      0.49         0.82         3.608


a  Taken from Ref. 10.
b  pa(M): 0.64, pa(C): 0.92
c  pa(location, number of residues); pa(N,2): 0.35, pa(MC,2): 1.16, pa(N,3):
0.00, pa(MC,3): 0.81, pa(N,4): -0.34, pa(MC,4): 0.46.


Abraham, Donald J.; Leo, Albert J., Extension of the fragment method to
calculate amino acid zwitterion and side chain partition coefficients,
Proteins:  Struct., Funct., Genet. (1987), 2(2), 130-52

Leo, A. J., Computer calculation of peptide hydrophobicity, Pharmacochem. Libr.
(1991), 16(QSAR:  Ration. Approaches Des. Bioact. Compd.), 349-52

Fauchere, Jean Luc; Charton, Marvin; Kier, Lemont B.; Verloop, Arie; Pliska,
Vladimir, Amino acid side chain parameters for correlation studies in biology
and pharmacology, Int. J. Pept. Protein Res.  DATE: 1988  VOLUME: 32  NUMBER: 4
PAGES: 269-78  

Akamatsu, Miki; Fujita, Toshio, Quantitative analyses of hydrophobicity of di-
to pentapeptides having unionizable side chains with substituent and structural
parameters, J. Pharm. Sci. (1992), 81(2), 164-74
   
Akamatsu, Miki; Okutani, Shinichi; Nakao, Kazuya; Hong, Nam Joo; Fujita,
Toshio, Hydrophobicity of N-acetyl-di- and tripeptide amides having unionizable
side chains and correlation with substituent and structural parameters, Quant.
Struct.-Act. Relat.  DATE: 1990  VOLUME: 9  NUMBER: 

Akamatsu, Miki; Yoshida, Yohji; Nakamura, Hideaki; Asao, Masaaki; Iwamura,
Hajime; Fujita, Toshio, Hydrophobicity of di- and tripeptides having
unionizable side chains and correlation with substituent and structural
parameters, Quant. Struct.-Act. Relat.  DATE: 1989  VOLUME: 8  NUMBER: 3

[8] R.-S. Tsai, B. Testa, N. El Tayar, P.-A. Carrupt, 
J. Chem. Soc. Parkin Trans. 2, (1991), 1797.
[9] P. Vallat, P. Gaillard, P.-A. Carrupt, R.-S. Tsai, 
B. Testa, Helv. Chim. Acta, 78 (1995), 471.
[11] W. E. Steinmetz, Quant. Struct.-Act. Relat., 14 (1995), 19.
[12] N. El Tayar, H. Karajiannis, H. van de Waterbeemd, 
Amino Acids, 8 (1995), 125.

Best Regards

=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=
Tomoko Sotomatsu Niwa, Ph.D. 
Research Lab. Nippon Shinyaku Co., Ltd.
Nishiohji Hachijo Minami-ku Kyoto, 601 Japan
tel 075-321-9047, fax 075-321-9038
t.niwa@nippon-shinyaku.co.jp
=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=

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


God bless all of you!

Arthur

_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/
_/   Arthur Wang                     Doctoral Candidate     _/
_/   Molecular Design Lab                                   _/
_/   Institute of Physical Chemistry, Peking University     _/
_/   Beijing 100871, P.R.China                              _/
_/                                                          _/ 
_/   E-mail: arthur@ipc.pku.edu.cn                          _/
_/   Tel: 86-10-62751490    Fax: 86-10-62751725             _/
_/   WWW: http://www.ipc.pku.edu.cn/moldes/arthur/home.html _/
_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/

 




From tgakrh@sg10.chem.tue.nl  Tue Nov 25 04:37:14 1997
Received: from mailhost.tue.nl  for tgakrh@sg10.chem.tue.nl
	by www.ccl.net (8.8.3/950822.1) id EAA10313; Tue, 25 Nov 1997 04:05:53 -0500 (EST)
Received: from sg10.chem.tue.nl [131.155.80.53] by mailhost.tue.nl (8.8.5)
	  for <chemistry@www.ccl.net>
	  id KAA03511 (ESMTP). Tue, 25 Nov 1997 10:05:47 +0100 (MET)
Received: from tgakrh@localhost by sg10.chem.tue.nl (8.8.5) 
	  for chemistry@www.ccl.net
	  id KAA16031. Tue, 25 Nov 1997 10:05:45 +0100 (MET)
From: Roelant Harmsen <tgakrh@sg10.chem.tue.nl>
Message-Id: <199711250905.KAA16031@sg10.chem.tue.nl>
Subject: Basis Set for Pd
To: chemistry@www.ccl.net (Computational Chemistry List)
Date: Tue, 25 Nov 1997 10:05:45 +0100 (MET)
X-Mailer: ELM [version 2.4 PL23]
Content-Type: text



Hi Everyone,

Does anyone know of a good gaussian type basis set for palladium
optimised for DFT?

Thanks,
Roelant

**********************************************************************
Roelant Harmsen                      |tel: ++31 40 2473575/5032
University of Technology Eindhoven   |fax: ++31 40 2455054
Laboratory of Inorganic              |e-mail : tgakrh@chem.tue.nl
Chemistry and Catalysis (TAK)        |www: http://www.tak.chem.tue.nl/
P.O. box 513                         |personal/rharmsen
5600 MB Eindhoven                    |
The Netherlands                      |AD&D: Xahnar (Wild Mage)
**********************************************************************


From yubofan@guomai.sh.cn  Tue Nov 25 06:37:14 1997
Received: from guomai.sh.cn  for yubofan@guomai.sh.cn
	by www.ccl.net (8.8.3/950822.1) id GAA11108; Tue, 25 Nov 1997 06:28:35 -0500 (EST)
Received: from default (Email-39 [210.0.0.7])
	by guomai.sh.cn (8.8.7/8.8.7) with ESMTP id TAA08613
	for <CHEMISTRY@www.ccl.net>; Tue, 25 Nov 1997 19:25:58 +0800 (CST)
Message-Id: <199711251125.TAA08613@guomai.sh.cn>
From: "Yubo Fan" <yubofan@guomai.sh.cn>
To: <CHEMISTRY@www.ccl.net>
Subject: Need some reference about molecular geometry optimization.
Date: Tue, 25 Nov 1997 19:28:39 +0800
X-MSMail-Priority: Normal
X-Priority: 3
X-Mailer: Microsoft Internet Mail 4.70.1157
MIME-Version: 1.0
Content-Type: text/plain; charset=HZ-GB-2312
Content-Transfer-Encoding: 7bit



Hi,

I am doing geometry optimization of a big molecule. I think it is
impossible for me to do these jobs for the whole molecule which contains
over 40 C atoms, so I want to split it into several parts and calculate
each of them respectively. Then I will put them together. Is this thought
possible? If possible, could you please give me some advice or reference
with the same kind of work.

With best regards

Y. Fan
=============================================================
Yubo Fan                         Email: yubofan@guomai.sh.cn
Organic Synthesis Lab                   yubofan@fudan.edu.cn
The Department of Chemistry
Fudan University                 Phone: 8621-65648139
No. 220 Handan Road              Fax:   8621-65641470
Shanghai, 200433
P. R. China
=============================================================


From metz@phindigo.oci.uni-heidelberg.de  Tue Nov 25 11:37:16 1997
Received: from phindigo.oci.uni-heidelberg.de  for metz@phindigo.oci.uni-heidelberg.de
	by www.ccl.net (8.8.3/950822.1) id LAA12811; Tue, 25 Nov 1997 11:34:26 -0500 (EST)
Received: by phindigo.oci.uni-heidelberg.de (940816.SGI.8.6.9/940406.SGI.AUTO)
	 id RAA20001; Tue, 25 Nov 1997 17:35:49 -0100
From: "Markus Metz" <metz@phindigo.oci.uni-heidelberg.de>
Message-Id: <9711251735.ZM19999@phindigo.oci.uni-heidelberg.de>
Date: Tue, 25 Nov 1997 17:35:34 +0000
In-Reply-To: Steven Creve <Steven.Creve@chem.kuleuven.ac.be>
        "Re: CCL:G:atom in molecules" (Nov 24, 10:05am)
References: <Pine.A32.3.96.971124100344.36460A-100000@hartree.quantchem.kuleuven.ac.be>
X-Mailer: Z-Mail (3.2.0 26oct94 MediaMail)
To: Steven Creve <Steven.Creve@chem.kuleuven.ac.be>
Subject: Summary AIM-Visualization Programs
Cc: chemistry@www.ccl.net
Mime-Version: 1.0
Content-Type: text/plain; charset=us-ascii



Summary of the responses to visualize Atom in Molecules.

On the following mail ...

>
> I am using GAUSSIAN 94 to calculate the properties of atoms in molecules (1)
> using the SCF density.(keywords: AIM=ALL, DENSITY=LAPLACIAN)
> For example the attractors, critical points on attractor interaction lines,
> zero flux surfaces, bond paths and the second derivative of the electron
> density of cyclopropane were calculated.
> What I am interested in are the bent bonds in this molecule.
> Does anybody know, how to visualize this data?

> (1) R. F. W. Bader, Atoms in Molecules: a quantum theory, Clarendon Press,
>     Oxford, 1990.

 ... I got the responses:

------------------------------------------------------------
Keith E. Laidig <laidig@u.washington.edu> wrote:
	You can get all of Bader's code directly from him.  There are
postscript generating routine within the package (I think).  Anyway, you
can build easily upon these programs to produce pictures in most graphic
environments.  Bader's email address is:

	bader@mcmail.cis.mcmaster.ca

and his WWW page is:

	http://www.chemistry.mcmaster.ca/faculty/bader/bader.html.


--------------------------------------------------------------------------------
<Leonardo.Demaria@trieste.infn.it>
Hi, there are some persons here working on that. They are using a sofware
called AVS (Advanced Visual System) to visualize all the needed quantities.
AVS however is expensive but as far as they told me it is very good.
You can find more info about it on:

	http://www.avs.com

Good luck,
	Leonardo
--------------------------------------------------------------------------------

Dr. Paul L. A. Popelier hat ein Programm namens MORPHY, welches er gern
zur Verfuegung stellt (zusammen mit einigen seiner Artikel). MORPHY
erlaubt es, die vollstaendige AIM Analyse durchzufuehren, wenn man ein
Gaussian-94 WFN File bereitstellt. Das Programm erzeugt
Postscript-Output. Ich habe es im Rahmen meiner Dissertation verwendet
und bin sehr zufrieden mit der Darstellung. Dr Popeliers Email ist:
pla@umist.ac.uk.

Eine weitere Visualisierung ist in Chem. Eur. J. 1997, 3, No. 8, 1244ff.
zu finden. Die Autoren (R. Glaser und D. Farmer) benutzen ein eigenes
Programm namens CCGVF. Ich weiss leider nicht, ob sie es herausgeben.

Vielleicht hilft dies ein bisschen weiter,

Magnus
--
========================================================================
Magnus Kessler                  kessler@mpi-muelheim.mpg.de
PhD Student
MPI fuer Kohlenforschung        Lembkestrasse 5
Strukturchemie                  D-45470 Muelheim / Germany
========================================================================

--------------------------------------------------------------------------------
I wrote Dr. Propelier and he sent me the program.

Best regards,
							Markus.

-- 
--------------------------------------------------------------------------------
Markus Metz
Universitaet Heidelberg					Tel.: 06221-54-6066
Organ.-Chem. Institut Lehrstuhl III			Fax: 06221-54-4885
Im Neuenheimer Feld 270
69120 Heidelberg
--------------------------------------------------------------------------------


From hp003@THEORY.dra.hmg.gb  Tue Nov 25 12:37:23 1997
Received: from relay.mod.uk  for hp003@THEORY.dra.hmg.gb
	by www.ccl.net (8.8.3/950822.1) id MAA12935; Tue, 25 Nov 1997 12:13:33 -0500 (EST)
Received: from hermes.dra.hmg.gb by relay.mod.uk with local SMTP id <g.14876-0@relay.mod.uk>; Tue, 25 Nov 1997 17:13:26 +0000
Received: from THEORY.dra.hmg.gb by hermes.dra.hmg.gb (MX V4.2 VAX) with SMTP;
          Tue, 25 Nov 1997 17:13:20 GMT
Received: (from hp003@localhost) by THEORY.dra.hmg.gb (8.7.6/8.7.3) id RAA18114
          for CHEMISTRY@www.ccl.net; Tue, 25 Nov 1997 17:13:01 GMT
From: Mike Fearn <hp003@dra.hmg.gb>
Message-ID: <199711251713.RAA18114@THEORY.dra.hmg.gb>
Subject: Two centre coulomb integral evaluation.
To: CHEMISTRY@www.ccl.net
Date: Tue, 25 Nov 1997 17:13:00 GMT
X-Mailer: Elm [revision: 212.4]




Dear all,

 As part of the development of a new semi-empirical method, I'd be
most grateful if anyone can  point me to (ideally freely available)
code which can evaluate two-center two-electron integrals 
using slater orbitals (s,p type) for a given nuclear separation.

Many thanks in advance.

Mike Fearn.
hp003@dra.hmg.gb




From yu@infiniti.wavefun.com  Tue Nov 25 14:37:18 1997
Received: from volvo.wavefun.com  for yu@infiniti.wavefun.com
	by www.ccl.net (8.8.3/950822.1) id OAA13629; Tue, 25 Nov 1997 14:03:22 -0500 (EST)
Received: by volvo.wavefun.com (931110.SGI/930416.SGI)
	for CHEMISTRY@www.ccl.net id AA04909; Tue, 25 Nov 97 11:06:18 -0800
Received: from infiniti.wavefun.com(198.147.95.4) by volvo.wavefun.com via smap (V1.3)
	id sma004905; Tue Nov 25 11:05:24 1997
Received: from ) by infiniti.wavefun.com (931110.SGI/950213.SGI.AUTOCF) id AA15843 for @volvo.wavefun.com:CHEMISTRY@www.ccl.net; Tue, 25 Nov 97 11:01:28 -0800
From: "Jianguo Yu" <yu@infiniti.wavefun.com>
Message-Id: <9711251101.ZM15841@infiniti.wavefun.com>
Date: Tue, 25 Nov 1997 11:01:27 -0800
Reply-To: yu@wavefun.com
X-Mailer: Z-Mail (3.2.3 08feb96 MediaMail)
To: CHEMISTRY@www.ccl.net
Subject: Spring-1998 Computational Chemistry Workshops
Mime-Version: 1.0
Content-Type: text/plain; charset=us-ascii



Dear colleagues,

A brief note to announce the upcoming Spring 1998 Computational Chemistry
workshops schedule held in Wavefunction, Inc., Irvine, California:

_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/
_/ Format:      3-day intensive workshop on electronic structure  _/
_/              methods and applications, and hands-on molecular  _/
_/              modeling laboratory on individual workstations.   _/
_/                                                                _/
_/ Schedule:    January 14-16, March 18-20, May 13-15, 1998       _/
_/                                                                _/
_/ Instructors: Warren Hehre  &  Wayne Huang                      _/
_/                                                                _/
_/ Textbooks:   o "Chemistry with Computation", Warren Hehre &    _/
_/                Wayne Huang, 1995.                              _/
_/              o "A Laboratory Book of Computational Organic     _/
_/                Chemistry", Warren Hehre, Alan Shusterman &     _/
_/                Wayne Huang, 1996.                              _/
_/              o "A Short Course in Modern Electronic Structure  _/
_/                Methods", Warren Hehre, 1993-1997.              _/
_/                                                                _/
_/ For complete brochure, drop me a note to workshop@wavefun.com  _/
_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/_/

--
+---------------------------------------------------------------+
|  Wayne Huang, Ph.D.           |  18401 Von Karman, Suite 370  |
|  Computational Chemistry      |  Irvine, California 92612     |
|  Wavefunction, Inc.           |  714-955-2120 <> 955-2118(fax)|
|  huang@wavefun.com            |  Web: http://www.wavefun.com  |
+---------------------------------------------------------------+





From iguana@one.net  Wed Nov 26 21:37:36 1997
Received: from mail.one.net  for iguana@one.net
	by www.ccl.net (8.8.3/950822.1) id UAA20873; Wed, 26 Nov 1997 20:50:14 -0500 (EST)
Received: from port-38-31.access.one.net ([209.50.100.93] HELO default ident: IDENT-NOT-QUERIED [port 12292]) by mail.one.net with SMTP id <16797-11506>; Wed, 26 Nov 1997 20:48:37 -0500
Message-Id: <3.0.5.32.19971126205536.007a5650@mail.one.net>
X-Sender: iguana@mail.one.net
X-Mailer: QUALCOMM Windows Eudora Light Version 3.0.5 (32)
Date: 	Wed, 26 Nov 1997 20:55:36 +0000
To: CHEMISTRY@www.ccl.net
From: Ray Crawford <iguana@one.net>
Subject: CCL:cyclodextrin inclusion complexes
Mime-Version: 1.0
Content-Type: text/plain; charset="us-ascii"


Dear All,

Could someone give me any references or suggestions of the most
appropriate force field for calculations of cyclodextrin inclusion
complexes ?  

 Thank you very much in advance!

-- 
***********************************************************************
                  Universidade Federal de Pernambuco

                Centro de Ciencias Exatas e da Natureza

                  Departamento de Quimica Fundamental

                        http://www.dqf.ufpe.br

                         Recife - PE - Brazil                
                    

	Gerd Bruno da Rocha               E-Mail : gbr@npd.ufpe.br          
                                                 : gerd@dqf.ufpe.br

                  MSc Student in Computational Chemistry

***********************************************************************

-------This is added Automatically by the Software--------
-- Original Sender Envelope Address: gbr@NPD.UFPE.BR
-- Original Sender From: Address: gbr@NPD.UFPE.BR
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 




