From glee@calstatela.edu  Tue Nov 28 00:08:33 1995
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Date: Mon, 27 Nov 1995 20:58:54 -0800
From: Ging Lee <glee@calstatela.edu>
Message-Id: <199511280458.UAA01020@mars.calstatela.edu>
To: CHEMISTRY@www.ccl.net
Subject: hydrogel materials
Content-Length: 376



Hello people,

I would like to know if anyone out there who can give me a pointer to find
information about a class of material call "hydrogel".  They can come from
either theory or synthese work.  I have looked in out library and not even
one book was on this subject, so that's why I need your help.


Thank you very much in advance.

Ging Lee
glee@chem0sun.calstatela.edu

From ipcakc@ipc.iisc.ernet.in Mon Nov 27 03:23:20 1995
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Date: Mon, 27 Nov 1995 13:52:59 +0500
From: ipcakc@ipc.iisc.ernet.in (Dr.A.K.Chandra)
Message-Id: <199511270852.NAA10226@postoffice.iisc.ernet.in>
To: CHEMISTRY@www.ccl.net
Subject: INTRAMOLECULAR H-ABSTRACTION IN ENES
Status: RO


dear netters,
Are there any reports on INTRA-MOLECULAR (NOT INTERMOLECULAR) H-ABSTRACTION
IN EXCITED STATES (LIKE LOWEST TRIPLET STATES) OF OLEFINIC COMPOUNDS? I HAVE
FOUND ONLY INTER-MOLECULAR REACTIONS (LIKE RADICAL ADDITIONS TO OLEFINS IN
GROUND STATES.)  EVEN IN GROUND STATE (I.E. LOWEST SINGLET STATE) REACTIONS
ARE ALSO WELCOMED. 
Thanks in advance.
Sridhar
E-mail : ipcakc@postoffice.iisc.ernet.in (or)
         akc@hamsadvani.serc.iisc.ernet.in


From owner-chemistry@ccl.net Mon Nov 27 19:56:03 1995
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Date: Mon, 27 Nov 95 21:56:25 WDT
From: rvgloss@criba.edu.ar (Daniel Glossman)
Message-Id: <9511280056.AA09564@criba.edu.ar>
To: chemistry@ccl.net
Subject: reduction potentials and energy differences
Status: RO


Dear netters:

Is it possible to establish any relationship between the differences 
in energy of the anion and the neutral molecule and the experimental
reduction potential for organic molecules?

Thank in advance

							Daniel Glossman

**************************************************************************
Dr. Daniel Glossman

Programa QUINOR - CONICET                 Universidad Nacional de Lujan      
Departamento de Quimica                   Departamento de Ciencias Basicas
Universidad Nacional de La Plata          Division Quimica
Casilla de Correo 962                     Casilla de Correo 221
(1900) La Plata                           (6700) Lujan
Republica Argentina                       Republica Argentina
Phone/FAX: (54 21) 259485                 FAX: (54 323) 25795
E-mail: rvgloss@criba.edu.ar              E-mail: glossman@unlu01.edu.ar
***************************************************************************
							
							


From smori@chem.s.u-tokyo.ac.jp Mon Nov 27 23:29:41 1995
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	id AA02822; Tue, 28 Nov 95 13:29:07 JST
Message-Id: <9511280429.AA02822@utsc.s.u-tokyo.ac.jp>
Date: Tue, 28 Nov 1995 13:33:48 +0900
To: chemistry@www.ccl.net
From: smori@chem.s.u-tokyo.ac.jp (Mori Seiji)
X-Sender: smori@chem.s.u-tokyo.ac.jp (Unverified)
Subject: NMR calculation-ISOTROPIC and ANITROSOPY
Cc: smori@utsc.s.u-tokyo.ac.jp, help@gaussian.com
Mime-Version: 1.0
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Status: RO


  Dear Sirs,

 I posted to CCL about the methods of NMR calculation a fey days ago , and
had an other question.
In G94, I tried to calculate the chemical shifts , there are magnetic
shieldings 
in the output, however, no chemical shift but isotropic  and anitrosopy. 
I examine meaning of these terms in the user's manual of Gaussian 94 and 
several original papers,for example,
M. Schindler, et al. JCP, 1982, 76, 1919
and Pulay et al. JACS, 1990, 112, 8251, and so on which there is replies 
of my previous questions
, but I only know that isotropic terms is "likely" to be 
corresponding to the chemical shifts which was experimentally observed. 
I had had experiments in organic chemistry, and I am now carrying out the 
ab initio calculations but I amn't much familiar to know the theory 
of NMR spectroscopy. 
Would you please tell me the physical meaning of isotropic  and anitrosopy, 
and which is an equivalent of the experimental chemical shift? It is better
that 
you show the references. 

    Sincerely yours,
    Seiji Mori
####################################################

  Seiji Mori
  Graduate student in Nakamura Laboratory
  Department of Chemistry
  The University of Tokyo
  Hongo 7-3-1, Bunkyou-ku, Tokyo 113, JAPAN.
  email:smori@chem.s.u-tokyo.ac.jp

####################################################



From owner-chemistry@ccl.net  Tue Nov 28 05:38:40 1995
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Date: Tue, 28 Nov 95 10:24:46 GMT
Message-Id: <7673.9511281024@rahman.earth.ox.ac.uk>
From: Keith Refson <Keith.Refson@earth.ox.ac.uk>
Subject: Re: CCL:statistical error in simulations
To: chemistry@ccl.net
Organisation: Earth Sciences Department, Oxford University.


Dear Rafael,

> I'm looking for references about calculation of errors in quantities 
> like RDF, running integration numbers,... obtained by means of MD/MC
> simulations. 

Take a look at Allen and Tildesley, p191 onwards.  Also worth a look
is

@Article{schiferl:85,
  author = 	 {S. K. Schiferl and D. C. Wallace},
  title = 	 {Statistical Errors in Molecular Dynamics Averages},
  journal = 	 jcp,
  year = 	 1985,
  volume =	 83,
  number =	 10,
  pages =	 {5203-5209}
}

Keith Refson
------------------------------------------------------------------------------
| Email   : keith@earth.ox.ac.uk    | Dr Keith Refson, Dept of Earth Sciences|
| TEL(FAX): +44 1865 272026 (272072)| Parks Road, Oxford OX1 3PR, UK         |
------------------------------------------------------------------------------

From separk@cs.usc.edu  Tue Nov 28 07:38:45 1995
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Date: Tue, 28 Nov 95 4:37:27 PST
From: "S. Park" <separk@cs.usc.edu>
To: CHEMISTRY@www.ccl.net
Cc: separk@pollux.usc.edu
Subject: Questions about the docking problem
Message-ID: <CMM.0.90.2.817562247.separk@pollux.usc.edu>


Hello,

I have been studying the rigid molecular docking problem and have several
questions about the assumptions typically made.  Since my major is computer
science, I lack lots of basic knowledge on the subject and I wonder if 
anyone could kindly tell me about your opinion and give me any references
that I could use for the study.  I would really appreciate it !

Here are my questions:

It seems to me that there are three assumptions for the molecular docking 
problem:

1. Rigidity
2. Availability of the atomic coordinates
3. Solvent effects related assumption

First of all, I would like to know how "accurate" the results we have with
the assumptions above.  For example, I understand that the answers are
"approximate" solutions for the real answer.  But how reliable (or,
exact, valid ?) are they ?  Can we quantify this ?

Secondly, it seems to me that most of the automated docking procedures
make use of the atomic coordinates of the molecules.  But what if we don't
have their crystal structures ?  How could we find the mode of binding in
these cases ?

Thirdly, I wonder how much information could we glean from the geometric
complementarity based approach.  I understand that this is a sort of
"screening" process for later "energy minimization".  It seems to me that
geometric complementarity serves as a necessary condition for the real
answer.  But what if we miss the real "answer" in this "screening" step ?

Finally, I wonder how reliable the result that comes from without considering
the surrounding solvent is.  It seems to me that one of the reasons that we
don't consider the solvent effect is due to the expensive computational cost.
But then how "accurate" is the result ?

Thank you very much for your time !

Regards,
Seongbin Park (separk@pollux.usc.edu)

From owner-chemistry@ccl.net  Tue Nov 28 07:42:41 1995
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Message-Id: <20944.9511281205@loki.brunel.ac.uk>
Subject: Early termination of IRC calculations
To: chemistry@ccl.net
Date: Tue, 28 Nov 1995 12:05:26 +0000 (GMT)
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Dear compuational colleagues,

I have been performing a number of IRC calculations using Mopac 6 on 
an VAXstation 3520 and I have had a problem with the early termination of 
the IRC calculation, which was due to MOPAC running out of time. However I have 
provided enough time for the calculation to run to completeion and placed 
it on a parasitic queue that has an infinite time allowance. (See below) 

Also in DIMSIZES.DAT I have given the following
MAXTIM=1000000, MAXDMP=21000


Also I have failed to RESTART any of these IRC calculations.

If anyone has a solution please advise me ASAP.

Thanks in advance

Jeff Gosper


*******************************************************************************
** FRANK J. SEILER RES. LAB., U.S. AIR FORCE ACADEMY, COLO. SPGS., CO. 80840 **
*******************************************************************************
 AM1 CALCULATION RESULTS
*******************************************************************************
*          MOPAC:  VERSION  6.00               CALC'D. 27-NOV-95               
*  LARGE    - EXPANDED OUTPUT TO BE PRINTED
*  X-PRIOR  - GEOMETRY CHANGES TAKE PRIORITY IN DRC
*  RESTART  - CALCULATION RESTARTED
*  IRC=N    - INTRINSIC REACTION COORDINATE  1 DEFINED
*   T=      - A TIME OF  0.100E+07 SECONDS REQUESTED
*  DUMP=N   - RESTART FILE WRITTEN EVERY 25000.0 SECONDS
*  AM1      - THE AM1 HAMILTONIAN TO BE USED
*  PRECISE  - CRITERIA TO BE INCREASED BY 100 TIMES
*  ISOTOPE  - FORCE MATRIX WRITTEN TO DISK (CHAN. 9 )
 ***********************************************************************043BY043
AM1 PRECISE ISOTOPE T=1000000 IRC=1 LARGE X-PRIO RESTART
TS optimized
FINAL HEAT OF FORMATION =       -57.83639 KCAL

 ......Z-matrix cut from here


 ......output for numerous cycles appears then 
 
RUNNING OUT OF TIME, RESTART FILE WRITTEN
GEOMETRY AND VELOCITY ARE IN RESTART FILE IN ASCII
	    
	     
	      
TOTAL CPU TIME:         75008.92 SECONDS
     
 == MOPAC DONE ==

From andreas@majestix.msp.univie.ac.at  Tue Nov 28 08:38:41 1995
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	 id OAA11413; Tue, 28 Nov 1995 14:26:40 +0100
From: "Andreas Parusel" <andreas@majestix.msp.univie.ac.at>
Message-Id: <9511281426.ZM11411@majestix.msp.univie.ac.at>
Date: Tue, 28 Nov 1995 14:26:36 +0100
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To: chemistry@www.ccl.net, pm@katz.cc.univie.ac.at
Subject: Excited States with GAUSSIAN
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 Dear Sirs!

 I am posting here just for an information. If anybody is working with
 the GAUSSIAN94 programm and its use for calculation of excited states and/or
    the fluorescence, i'd be glad if he  could contact me for some questions!

 Thanks a lot for everybody in advance!

 Andreas Parusel, Vienna

-- 
=======================================================================
   _/_/  _/_/                    andreas@majestix.msp.univie.ac.at    =
  _/  _/_/  _/                   andreas@phys-chemie.uni-wuerzburg.de =
  _/  _/_/  _/                   parusel@aries.scs.uiuc.edu           =
   _/_/  _/_/                                                         =
                                                                      =
  Andreas Parusel                Institut fuer Theoretische Chemie    =
  Drorygasse 15/27               Althanstr. 14                        =
  A-1030 Wien                    A-1030 Wien                          =
  +43 1 7519244                  Tel +43 1 31336 1572                 =
=======================================================================

From bernhard@quant1.chemie.uni-leipzig.de  Tue Nov 28 08:53:42 1995
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          id AA15346; Tue, 28 Nov 1995 13:20:51 +0100
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To: Uli Salzner <uli@smaug.physics.mun.ca>
Cc: ccl <chemistry@www.ccl.net>, bernhard@quant1.chemie.uni-leipzig.de
Subject: Re:DFT/spurious integrated densities 
In-Reply-To: (Your message of Fri, 24 Nov 95 13:22:28 -0330.)
             <Pine.3.05.9511241328.A24103-9100000@smaug.physics.mun.ca> 
Date: Tue, 28 Nov 95 13:20:51 +0100



Hi,

few weeks ago i struggle over the same problem. 
I got the tip to add the keywords

SCF=NoVarACC INT=FineGrid

which work in ca. 90% of all cases (using B3LYP). 
The first is not fully known to me (didn't find the keyword in the
g92 manual), but i think it enhance the accuracy of the integrals
or is related to this point, the second point results in better
numerics while integration. Don't take it for good, i'm just a
starter...
If this doesn't work, then a slight alteration of the geometry helps 
sometime (nearly in all remaining cases).

Bernhard Eck

From moshe_o@VNET.IBM.COM  Tue Nov 28 10:08:42 1995
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   Tue, 28 Nov 95 09:55:42 EST
Date: Tue, 28 Nov 95 16:36:37 IST
From: "Moshe Olshansky" <moshe_o@VNET.IBM.COM>
To: chemistry@www.ccl.net
Subject: combining different basis sets - an addition


Dear netters!
After posting the summary of the responses I got an additional
note which may be of interest to some of you.  Here it is:

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

Date: Mon, 27 Nov 1995 16:23:15 -0330 (NST)
From: Uli Salzner <uli@smaug.physics.mun.ca>
Subject: basis set mixing

Dear Moshe,
I just read read the answers you received according basis set mixing and I think
one important point was not addressed. It is definetly important that a basis
set has to be balanced but that does not mean that you have to use the same
basis set for each atom. In fact, to use the "same" basis set for different
atoms may be the perfect way to get an unbalanced basis set.

For example:
consider the calculation of an ionic compound such as LiF. If you use 6-31G* on
both atoms, you have a very good basis set for Li. Since Li looses about 90% of
its 2s electron (maybe even more) when bound to F, it has almost no electrons in
the 2s and 2p. For such a cation a valence double zeta basis set is very good. On
the other hand fluorine is an anion with a diffuse charge distribution. For an
anion the 6-31G* basis set quite bad. What you get is spurious charge transfer
>from  F to Li.

Thus, one uses different basis sets for different atoms all the time even if they
have the same name. What you have to figure out is how to combine different
basis sets in the right way. For the above example it would be a improvement to
use 6-31+G* on F. This gives a better balanced basis set than 6-31G* on both
atoms. Similar arguments hold for polarization functions. You have to decide
which atoms need them and which don't. For instance for third row systems you
definetely need d-functions. But there is no problem to combine a sulfer basis
set with d-functions with hydrogen basis set that contains only s-functions
because hydrogen d-orbitals are so high in energy that the effect would be
negligible.

Bets wishes,
Uli Salzner

uli@smaug.physics.mun.ca

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

P.S. and now I have an additional question:
     I am a mathematician,  not a chemist,  so let me look at the
     basis sets purely mathematically.  If one has a complete (and
     hence necessarily infinite) basis set,  he/she gets a limit
     of Hartree-Fock model.  Otherwise (with limited basis set) one
     gets some approximation to this limit and the more complete the
     basis set is the better is the approximation.  Now assume one
     uses a certain "standard" basis set and gets some result (from
     Hartree-Fock model).  And now we add ANY additional function to
     this basis set.  This does not make the basis set less complete
     and so it should lead to at least as good (or even better) an
     approximation as the original basis did (it is also possible
     to get the original solution by taking that additional function
     with zero coefficient for every electron).
     Is there anything wrong with this statement?

Moshe Olshansky
IBM Israel Science & Technology
<moshe_o@vnet.ibm.com>

From WILLSD@conrad.appstate.edu  Tue Nov 28 11:08:42 1995
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 28 Nov 1995 10:51:16 -0400 (EDT)
Date: 	Tue, 28 Nov 1995 10:51:13 -0400 (EDT)
From: willsd@conrad.appstate.edu
Subject: Re: CCL:NMR calculation-ISOTROPIC and ANITROSOPY
In-reply-to: <9511280429.AA02822@utsc.s.u-tokyo.ac.jp>
Sender: WILLSD@conrad.appstate.edu
To: Mori Seiji <smori@chem.s.u-tokyo.ac.jp>
Cc: chemistry@www.ccl.net, smori@utsc.s.u-tokyo.ac.jp,
        help@gaussian.com
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On Tue, 28 Nov 1995, Mori Seiji wrote:

>   Dear Sirs,
> 
>  I posted to CCL about the methods of NMR calculation a fey days ago , and
> had an other question.
> In G94, I tried to calculate the chemical shifts , there are magnetic
> shieldings
snip... 
> Would you please tell me the physical meaning of isotropic  and anitrosopy, 
> and which is an equivalent of the experimental chemical shift? It is better
> that 
> you show the references. 
> 
>     Sincerely yours,
>     Seiji Mori
> ####################################################
> 
snip...
>   email:smori@chem.s.u-tokyo.ac.jp

Seiji:
I ran into this proble recently and have a suggestion:
1) You need the isotropic part of the shielding tensor.
2) Chemical shifts can be calculated from this isotropic part using some 
simple theory:  I recommend the information in chapter 2 of :
Multinuclear NMR, J. Mason Ed., Plenum Press, New York, 1987.
You will also need the isotropic shielding for the chemical shift 
standard for your nucleus. (In my case it was (EtO)2.BF3 for 11B NMR).

Steve Williams
Chemistry
Appalachian State University
Boone, NC 28608
willsd@appstate.edu


From Yue@biotech.lan.nrc.ca  Tue Nov 28 11:53:57 1995
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From: "Yue, Shi-Yi (*ASTRA)" <SHI-YI.YUE@NRC.CA>
To: ccl <chemistry@www.ccl.net>
Subject: MD trajectory presentation on Mac
Date: Tue, 28 Nov 95 11:51:00 EST
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Encoding: 14 TEXT
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Hello everybody,

   I am looking a software on Mac which can be used to
present trajectory files of molecular dynamics simulation
>from Unix systems.
Any comments and suggestions are welcome.

Thank you in advance!

shiyi yue
yue@biotech.lan.nrc.ca




