From denis@messiaen.scf.fundp.ac.be  Tue Nov  8 03:24:43 1994
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From: denis@messiaen.scf.fundp.ac.be (Jean-Pierre Denis)
Message-Id: <9411080800.AA31535@messiaen.scf.fundp.ac.be>
To: "Stavrev Krassimir" <krasimir@qtp.ufl.edu>
Cc: chemistry@ccl.net, denis@messiaen.scf.fundp.ac.be
Subject: Re: CCL:Mac software inquiry 
In-Reply-To: (Your message of Mon, 07 Nov 94 09:15:41 EST.)
             <9411071415.AA21456@crunch> 
Date: Tue, 08 Nov 94 09:00:37 +0100


Dear Netter,

	What you can do is to place your binary file in a
Compact Pro document, after saving it you can segment this
archive on your own, e.a. segment it for D.D., H.D.
diskettes or other blok size.

	Grettings.

	Jean-Pierre DENIS

	denis@scf.fundp.ac.be

From toukie@zui.unizh.ch  Tue Nov  8 04:24:43 1994
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	id AA04509; Tue, 8 Nov 94 09:36:51 +0100
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Date: Tue, 8 Nov 1994 09:31:05 +0100 (MET)
From: "Hr Dr. S. Shapiro" <toukie@zui.unizh.ch>
Sender: toukie@zui.unizh.ch
Reply-To: toukie@zui.unizh.ch
Message-Id: <34266.toukie@zui.unizh.ch>
To: chemistry@ccl.net
Subject: Oxidisability of phenolics


Dear Colleagues;

     For a study in progress I need to have quantitative data about the
"oxidisability" of various mono- and disubstituted phenolic compounds, pre-
ferably at room or physiological temperature and at ca. physiological pH
(i.e., ca. pH 7).  Can anyone recommend a compendium or source of such data?

     I found a 1982 book called "The Encyclopaedia of Chemical Electrode Po-
tentials" (authors: Antelman & Harris) listing EMF values for some monobasic
phenols.  According to this book, "The OH- reactions are considered to be at
a pH of 11, other reactions in the absence of the H ion are considered to
have a pH of 7, and those involving the H ion a pH of 11.  Those involving
both H+ and OH- can be construed to occur at a pH of 7."  Considering the
above, can anyone recommend a way of converting the values on pp. 244-245 of
this book to EMF values for pH 7 and 37oC?

     Finally, some of the phenolics in which we are interested are not listed
in "The Encyclopaedia of Chemical Electrode Potentials".  Is there a way of
theoretically calculating them?  I have at my disposal the semi-empirical QM
programme "MOPAC 6.0".

     I thank all responders in advance for generously sharing their thoughts
and ideas with me.


Yours sincerely,

(Dr.) S. Shapiro
Institut fuer orale Mikrobiologie und allgemeine Immunologie
Zentrum fuer Zahn-, Mund-, und Kieferheilkunde der Universitaet Zuerich
Plattenstrasse 11
Postfach
CH-8028 Zuerich, Switzerland

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

From ARILAHTI@finabo.abo.fi  Tue Nov  8 08:24:45 1994
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	by www.ccl.net (8.6.9/930601.1506) id HAA06620; Tue, 8 Nov 1994 07:28:39 -0500
From: <ARILAHTI@finabo.abo.fi>
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 id <01HJ8N8DHA80CCK77N@finabo.abo.fi>; Tue, 8 Nov 1994 14:28:15 EET
Date: Tue, 08 Nov 1994 14:28:15 +0200 (EET)
Subject: Summary on multiple MOPAC runs
To: chemistry@ccl.net
Message-id: <01HJ8N8DKRLUCCK77N@finabo.abo.fi>
X-VMS-To: IN%"chemistry@ccl.net"
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Content-transfer-encoding: 7BIT


For some time ago, I asked for help in how to make only one 
MOPAC run at a time in a sequence of MOPAC runs. Here comes 
the summary. Thanks to everybody who responded.

        regards
	--ari

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

Ari Lahti, M.D., M.Sc.
Dept. Phys. Chem.
Abo Akademi University
Porthansg. 4-6
FIN-20500 Abo
Finland
tel.: 358-21-654617
fax:* 358-21-654706
e-mail: arilahti@abo.fi

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

From: aiba@volta.vmsmail.ethz.ch (Aiaz Bakassov, Phys. Chem., ETH Zurich)

&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&
..the best solution turned to be what I really disliked:
to call operating system from FORTRAN program.
This allows you to NOT care about any queues,
for FORTRAN proceeds operator by operator.

For UNIX the tool is UNIX FORTRAN function
"system". The lines in the FORTRAN program look
like:
        
      INTEGER ISTAT
      CHARACTER COMMAND*(80)
      ....
      COMMAND='here is an appropriate UNIX command'
      ISTAT=SYSTEM(COMMAND)

and you can put as many UNIX commands as you want
just call SYSTEM(..) again and again
with new commands inside. 
&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&&
So, the overall FORTRAN program goes
ONCE into a normal batch queue. Important is this:
the calls for your MOPAC runs are successive
because FORTRAN waits till the previous operator
has been completed. So, you would have only
one MOPAC at time! Is this what you needed ?
Best regards and wish you success! 

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

From: soperpd@nylon.es.dupont.com (Paul D. Soper)

Ari,

    I have one solution for this problem.  I generate the .csh
file for the job by simply telling MOPAC not to start running
immediately.  Each of these .csh files is copied to a directory
used only for job control.

    A file named job_list is created which has one .csh file name
per line.  A script called run_next then...

    1)  Takes the first line (file name) from job_list
    2)	Adds some lines to the end of the file so it
 	  will execute run_next when it is done
    3)  Submits the modifed .csh file to the batch processing
	  system 

This is run_next:

#!/bin/csh

set home_dir = `pwd`

while (1 == 1)

  if (! -e job_list) then
    echo "job_list not found on" `date +"%D at %T"` >> job_history.txt
    break
  endif

  if (-z job_list) then
    echo "job_list empty on" `date +"%D at %T"` >> job_history.txt
    break
  endif

  set job = `head -1 job_list`
  tail +2 job_list > list.tmp
  mv list.tmp job_list

  if (! -e $job) then
    echo "$job not found on" `date +" %D at %T"` >> job_history.txt
  else if (-z $job) then
    echo "$job empty on" `date +" %D at %T"` >> job_history.txt
  else

    echo "## The rest of this deck was added by the user"                  	      >> $job
    echo ""							       	       	      >> $job
    echo "cd $home_dir"					       	       	              >> $job
    echo 'echo '"$job"' `date +" ended on %D at %T"` >> job_history.txt'              >> $job 
    echo "run_next"                                                	       	      >> $job
    echo ""                                                        	       	      >> $job

    echo "$job" `date +" begun on %D at %T "` `bsub -q parallel $job` >> job_history.txt

    break
  endif

end

exit

    I hope this gives you some ideas.

Good luck,
Paul

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

From: jxh@biosym.com (Joerg Hill)

If I need to wait for a job to complete I use the following script:

----------------------------- waitforjob ------------------------------
# procedure which waits for termination of process with process id $1

if [ "$1" != "" ]
then
  jobid=$1
else
# no jobid means big sleep
  jobid=1
fi

echo waiting for process $jobid

while [ `ps -p $jobid | wc -l` -gt 1 ]
do
  sleep 120
done
--------------------------------- EOF ----------------------------------

Use it with the process ID of the job you are waiting for as parameter.

Joerg-R. Hill

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

From: "Dr. Daniel L. Severance" <dan@sage.Syntex.Com>


  Hi,
     I'm not sure what's in the MOPAC batch script, but you could modify
it to submit the job using the UNIX batch command.  The file
/usr/lib/cron/queuedefs contains a line like:
b.2j2n90w

   which tells the UNIX batch command to only allow 2jobs to run at a time
(2j) and give them a nice value of 2 (2n) and wait 90 seconds between
checking to see if one of the running jobs is finished before submitting
another (90w).  Every 90secs it checks to see if a slot is open, then
goes back to sleep for another 90 secs. until it finds that one job has
finished.

   To use batch in your script just put the string:
/bin/batch <<!

   before the commands which submit the job, and the string:
!

   At the end of script before the exit (if you have one).  Then you can
go ahead and submit them all at once, but they will only run in pairs (in
this example).

   Good luck!
      Dan

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

From: btluke@VNET.IBM.COM

Ari,

When I ported MOPAC7 to the RS/6000, I modified the program so
that it simply reads a file called MOPNAMES.  This file is a
list of input file names and the program then runs each job in
order and builds the names of the output files from the input
file names.

This program is available from the Quantum Chemistry Program
Exchange (QCPE) in either an RS/6000 version or in a distributed
version.  This latter version uses PVM (a free message passing
protocol) to sequentially run each job on a netwrok of workstations
or on an SP1/SP2 scallable-parallel machine.  This means that
each machine/node is given an input file and the "master" process
waits until a node is finished before a new one is sent to it.

Brian

Brian T. Luke, Ph.D.
IBM Corporation
btluke@vnet.ibm.com

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

From: Richard Bone <rgab@trpntech.com>

        Reply to:   RE>CCL:MOPAC necessarily batch?
Hi, I saw your message.  Appended is some notes I made for myself
when I set up MOPAC93 at my former place of work.  I think they 
confirm your conclusion:

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

   4.  To use the submit-command

To stack mopac93 jobs up - just type 

submit <dataset root-name> 

and the file will be added to a .qjob file in $mopacdir.


*************************** SOME THINGS TO NOTE  ************
*************

i) Do not run the mopac shell-script as a background process (&)

ii) If you run mopac93 from a script file you will have to put the line

   'source $mopacdir/mopac93.csh' 

   at the top.

iii) DO NOT stagger jobs in  a script file; they will all run concurrently.

iv) To stagger jobs use the "submit" command.

v) Peculiarity of data-set names:  NO "."  - Your dataset root names may
   not contain a period (.) - use underscore (_) or hyphen (-) instead.


Richard Bone


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




From jkl@ccl.net  Tue Nov  8 09:24:58 1994
Received:  for jkl@ccl.net
	by www.ccl.net (8.6.9/930601.1506) id JAA07954; Tue, 8 Nov 1994 09:19:08 -0500
Date: Tue, 8 Nov 1994 09:19:08 -0500
From: Jan Labanowski <jkl@ccl.net>
Message-Id: <199411081419.JAA07954@www.ccl.net>
To: chemistry@ccl.net
Subject: ACES II Workshop at OSC
Cc: jkl@ccl.net


Dear Netters,

There is still place for 3 more participants to the ACES II (Advanced
Concepts in Electronic Structure) Hands-On Workshop organized jointly by
Quantum Theory Project at University of Floryda and Ohio Supercomputer Center.
Date: Dec. 9-10, 1994, Place: Columbus, Ohio.
The deadline for registrations is Nov. 15th. You can register by e-mail.

More information about the workshop can be retrieved via e-mail by sending
  select chemistry
  get info/aces2.workshop
  quit
to MAILSERV@ccl.net. By gopher (gopher www.ccl.net 73): info,
aces2.workshop, and via WWW: http://www.ccl.net/aces2-workshop.html
Hurry, since such intensive workshops are not organized frequently.

Jan Labanowski
jkl@ccl.net

-- 

Dr. Jan K. Labanowski, Senior Research/Supercomputer Scientist/Specialist, etc.
Ohio Supercomputer Center, 1224 Kinnear Rd, Columbus, OH 43212-1163
ph:(614)-292-9279,  FAX:(614)-292-7168,  E-mail: jkl@ccl.net  JKL@OHSTPY.BITNET


From ANWAR@vms.huji.ac.il  Tue Nov  8 10:24:50 1994
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From: <ANWAR@vms.huji.ac.il>
To: CHEMISTRY@ccl.net
MIME-version:  1.0
Content-type:  Text/plain; charset=US-ASCII
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Subject:  ENZYMATIC REACTION


Dear Netters,

I would like to know if somebody encountered this kink of situation:
activation energy in an enzymatic hydrolysis reaction whichmwas over
25 Kcal/mol (Experimental measurement).

Thanks to all in advance.

Anwar Rayan

E-mail: anwar@vms.huji.ac.il

From peeter@chem.ut.ee  Tue Nov  8 10:32:16 1994
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From: peeter@chem.ut.ee (Peeter Burk)
Subject: Cadpack: where and how?
To: chemistry@ccl.net
Date: Tue, 8 Nov 1994 16:57:32 +0200 (EET)
X-Mailer: ELM [version 2.4 PL23]
Content-Type: text
Content-Length: 525       


Dear all,
I am interested in program package CADPACK. How can one
obtain a copy of it? How much does it cost? How can I contact
people, who maintain/sell/distribute it?
Please replay directly to me and I will summarise for net.
Best regards,
		Peeter
-- 
Peeter Burk, Ph.D.                      Jakobi 2, EE2400 Tartu, Estonia
Institute of Chemical Physics           Phone (372-7) 441-453   	
Tartu University                        Fax   (372-7) 441-453   	
Estonia                                 E-mail peeter@chem.ut.ee


From noy@tci005.uibk.ac.at  Tue Nov  8 11:25:22 1994
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From: noy@tci005.uibk.ac.at (Noy)
Message-Id: <9411081621.AA21676@tci005.uibk.ac.at>
Subject: MD or MC
To: chemistry@ccl.net
Date: Tue, 8 Nov 1994 17:21:40 +0100 (NFT)
X-Mailer: ELM [version 2.4 PL23]
Content-Type: text
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Dear CCL readers,
	I still remember the earlier time when I just started coming
into the computer simulation field, observing colleagues running
molecular dynamics and Monte Carlo program. I was so surprised that
MD could collect many picoseconds in a day (some finished in an hour
on IBM RS6000) while another mate stopped his MC in a week. 
	Unfortunately, more CPU time doesn't mean more results and
the dynamic properties owe its availability to MD. 
	Which one, MD or MC, you will select if CPU time-constraint
is imposed ? Both methods explore the phase space but MD seems to
go ahead much faster. If the efficiency is one thing to think about
MD is preferred since it never rejects the configuration. What is
the advantage of MC and this should explain its survival through the
year 2000.
						take care,
						Teerakiat
---------------------------------------------------------------------------
Teerakiat Kerdcharoen (NOY)

Institute of General and Inorganic and Theoretical Chemistry
Innrain 52a, A-6020 Innsbruck AUSTRIA
e-mail:  noy@tci2.uibk.ac.at, noy@tci5.uibk.ac.at
      :  noy@atc.atccu.chula.ac.th, noy@atc2.atccu.chula.ac.th ( Bangkok )
Research :  Molecular Dynamics simulations
         :  Computer Aided Molecular/Material Designs
---------------------------------------------------------------------------
***  I still remember that night in Bangkok.


From ANWAR@vms.huji.ac.il  Tue Nov  8 12:25:07 1994
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Date:     Tue,  8 Nov 94 15:30 +0200
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From: <ANWAR@vms.huji.ac.il>
To: CHEMISTRY@ccl.net
MIME-version:  1.0
Content-type:  Text/plain; charset=US-ASCII
Content-Transfer-Encoding: 7BIT
Subject:  ENZYMATIC REACTION


Dear Netters,

I would like to know if somebody encountered this kink of situation:
activation energy in an enzymatic hydrolysis reaction whichmwas over
25 Kcal/mol (Experimental measurement).

Thanks to all in advance.

Anwar Rayan

E-mail: anwar@vms.huji.ac.il

From jig@qorg.unizar.es  Tue Nov  8 12:34:23 1994
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	by www.ccl.net (8.6.9/930601.1506) id MAA11643; Tue, 8 Nov 1994 12:22:32 -0500
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	(1.37.109.4/16.2) id AA27225; Tue, 8 Nov 94 18:21:12 GMT
From: Jose Ignacio Garcia <jig@qorg.unizar.es>
Subject: DeFT: Basis sets for Sulfur
To: chemistry@ccl.net
Date: Tue, 8 Nov 94 18:21:09 MET
Mailer: Elm [revision: 70.85]


Dear netters,

I am using the StAmant's DeFT program to calculate some heterocyclic molecules.
This program contains DFT optimized basis sets only for first-row atoms. Now I
intend to calculate some sulfur-containing heterocycles, and I am seeking for
suitable basis sets to be used with this software.
I know that conventional ab initio basis sets, such as the popular Pople ones,
can be also used with DeFT in lieu of the built-in orbital basis sets, but I
do not know how the necessary auxiliary basis set have to be constructed.
Can anyone to point me to a reference, ftp-site, etc. where find suitable
basis sets for Sulfur to be used in DFT calculations? Otherwise, how could I
to construct the auxiliary basis sets for this atom?

Cheers,

Jose Ignacio

From hinsenk@ERE.UMontreal.CA  Tue Nov  8 12:39:47 1994
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Date: Tue, 8 Nov 94 11:57:20 -0500
From: hinsenk@ERE.UMontreal.CA (Hinsen Konrad)
Message-Id: <9411081657.AA08549@cyclone.ERE.UMontreal.CA>
To: noy@tci005.uibk.ac.at
Cc: chemistry@ccl.net
In-Reply-To: <9411081621.AA21676@tci005.uibk.ac.at> (noy@tci005.uibk.ac.at)
Subject: Re: CCL:MD or MC


Teerakiat Kerdcharoen wrote:

	   Which one, MD or MC, you will select if CPU time-constraint
   is imposed ? Both methods explore the phase space but MD seems to
   go ahead much faster. If the efficiency is one thing to think about
   MD is preferred since it never rejects the configuration. What is
   the advantage of MC and this should explain its survival through the
   year 2000.

The choice between MD and MC depends not on your CPU time allocation,
but on the problem you want to solve. Sometimes you don't have a
choice; e.g. if your system doesn't observe Newtonian mechanics,
you have to use MC (or some other appropriate technique, depending
on the problem). Sometimes MD is inefficient, e.g. because it samples
too small a region of phase space (which, by the way, has nothing
to do with rejecting configurations or not). You might also choose
MC because a special efficient MC technique is available for your
problem.

I'd recommend to read some books on MC techniques; they will show
you what MC is good for.

-------------------------------------------------------------------------------
Konrad Hinsen                     | E-Mail: hinsenk@ere.umontreal.ca
Departement de Chimie             | Tel.: +1-514-343-6111 ext. 3953
Universite de Montreal            | Fax:  +1-514-343-7586
C.P. 6128, succ. A                | Deutsch/Esperanto/English/Nederlands/
Montreal (QC) H3C 3J7             | Francais (phase experimentale)
-------------------------------------------------------------------------------



From ANWAR@vms.huji.ac.il  Tue Nov  8 13:26:12 1994
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Date:     Tue,  8 Nov 94 15:30 +0200
Message-id: <08110094153035@HUJIVMS>
From: <ANWAR@vms.huji.ac.il>
To: CHEMISTRY@ccl.net
MIME-version:  1.0
Content-type:  Text/plain; charset=US-ASCII
Content-Transfer-Encoding: 7BIT
Subject:  ENZYMATIC REACTION


Dear Netters,

I would like to know if somebody encountered this kink of situation:
activation energy in an enzymatic hydrolysis reaction whichmwas over
25 Kcal/mol (Experimental measurement).

Thanks to all in advance.

Anwar Rayan

E-mail: anwar@vms.huji.ac.il

From mensa@med.unc.edu  Tue Nov  8 14:24:58 1994
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	by www.ccl.net (8.6.9/930601.1506) id NAA13547; Tue, 8 Nov 1994 13:51:48 -0500
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	id AA03031; Tue, 8 Nov 94 13:51:43 EST
Date: Tue, 8 Nov 94 13:51:43 EST
From: mensa@med.unc.edu (Adriana C. Vidal)
Message-Id: <9411081851.AA03031@naples.med.unc.edu>
To: chemistry@ccl.net
Subject: Sybyl Biopolymer Loop Search users



 When I run Sybyl (version 6.0) Biopolymer Loop Search for
 a given sequence gap, I obtain -as expected- a set of loops
 ranking from lowest to highest RMS values. The manual suggests
 to choose the loop #1, i.e. lower RMS value.
 But in some cases, loops #1 have negative homology values.
 Does anyone know which homology matrix is the program using,
 besides the pmutation one?
 And, is one suppose to pick loop #1 regardless the negative
 homology value?

 I will much appreciate your help,

 Adriana C. Vidal
 mensa@med.unc.edu

From h.rzepa@ic.ac.uk  Tue Nov  8 15:24:56 1994
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On behalf of Roger Sayle, the availability of RasMol
for X-Window, MS Window and Macintosh platforms is
announced. It is available by anon ftp from
ftp.dcs.ed.ac.uk in pub/rasmol

If you dont know it already, this is VERY fast pdb, xyz, and other
format molecular renderer. It has a sophisticated selection
and attribute syntax, and can produce ribbon displays etc.

It can be compiled as 8-bit or 32-bit, for those machines that
support 24-bit graphics.

Dr Henry Rzepa, Department of Chemistry, Imperial College, LONDON SW7 2AY;
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From ZUILHOF@CHEM.CHEM.ROCHESTER.EDU  Tue Nov  8 15:29:43 1994
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Date: Tue, 08 Nov 1994 15:56:15 -0400 (EDT)
Subject: Summary: UHF vs ROHF in semiempirical calc's of radical cations
To: chemistry@ccl.net
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Dear CCl'ers,
As promised I hereby send you the summary of all responses I received on my 
questions about the use of ROHF versus UHF in semiempirical calculations of
radical cations. This summary starts with the original posting, followed by the
responses.
A big THANKS to all those who responded!

                                              Han Zuilhof

##############################################################################
Original posting:

Subj:	ROHF versus UHF in semiempirical calc.'s of radical cations

Dear CCl'ers,

Semiempirical programs such as MOPAC allow the properties of radicals
and radical ions to be calculated with both the Restricted Open-shell
Hartree-Fock method (ROHF) and the Unrestricted Hartree-Fock (UHF) methods.
I want to calculate reactionpaths for nucleophilic attack on a series of
radical cations.

Does anyone know of 
1) any apriori reasons why one method might be preferred over the other in 
such calculations?
2) literature data in which the performance of the ROHF and UHF methods 
for the study of radical cations is compared directly?

Please report directly to me, and I'll summarize to the net.
Thanks in advance,
                    Han Zuilhof


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

A very informative answer, dealing with many issues came from 
prof. Thomas Bally:

From:	IN%"BALLY%CFRUNI52.BITNET@CEARN.cern.ch"  2-NOV-1994 08:02:49.67
To:	IN%"ZUILHOF@CHEM.CHEM.ROCHESTER.EDU"
CC:	
Subj:	RHF vs. UHF

Dear Mr. Zuilhof,

You were asking on CCL about using UHF vs.RHF for calculating the attack of
nucleophiles on radical cations.

The question of UHF vs. RHF is a thorny one and it becomes thornier when
you go to semiempirical methods, even if you disregard for the moment the
problems posed by spin contamination which I will address below.

By allowing alpha and beta-electrons to occupy different spatial MO's (which is
the essence of the UHF model) you take into account a special form of electron
correlation called "spin polarization" which expresses itself experimentally in
negative hyperfine coupling constants in ESR spectra and is hence a physical
phenomenon. However, the UHF model has a tendency to overestimate the extent of
spin polarization which results in an overestimation of the stability of
systems where spin polarization is important (for example systems containing
allylic radical moieties such as they occur quite often in radical ions) if
compared to systems where this effect is less important.

In semiempirical methods, electron correlation effects are already "absorbed"
somehow in the parameters and therefore, in systems with high spin polariza-
tion, you count some of these twice in semiempirical UHF calculations. As a
consequence, the stability of systems where spin polarization is important (see
above) is often *absurdly* overestimated by semiempirical methods.

On the other hand, if you do RHF (I suppose you are referring to the "half-
electron" method which is used rather than the "real" Roothaan ROHF method in
Dewar's modelsbut this makes no difference), you artificially suppress spin
polarization entirely (it cannot occur if alpha and bete-electrons are
constrained to occupy pairwise the same spatial MO's). Hence the stability of
systems where this is important (see above) is *underestimated* with this
model.

To this you have to add the problem of "high-spin contamination" in UHF
wavefunctions which are not eigenfunctions of the S**2 operator and hence
cannot be classified as singlets, doublets, triplets. Most decent programs will
tell you about the *expectation value* of a UHF wavefunction with regard to
S**2 (usually called <S**2>) and the deviation of this expectation value from
the value for a pure singlet(=0), doublet (=0.75), triplet (=2.75) etc. tells
you how far you have gone astray from pure spin states in your calculation. As
a rule of thumb, a UHF wavefunction is acceptable if <S**2> deviates less than
0.1 from the "correct" value. You will find that this deviation is often
exceeded, especially in systems with high spin polarization.

So what can you do? Unfortunately I cannot give you a good answer. Due to the
above-mentioned problems and some other shortcomings of semiempirical methods
(problems with small rings) I have personally all but given up semiempirical
calculations on radical ions and switched to ab-initio based methods which have
become quite affordable with the advent of modern workstations. On the other
hand you may get away with semiempirical methods for large systems if

  (a)  You do have cases where spin polarization is unimportant
       (i.e. if the difference between UHF and RHF heats of formation
       is, say, less than 5 kcal/mol)

  (b)  If the <S**2> values for doublets are <0.85.

The grist of the matter is, that you should always do *both* RHF and UHF
calculations. If the results do not differ substantially, both with regard to
geometries and relative energies, you are probably safe (unless you have small
rings, but that's another can of worms).

Don't hesitate to get back to me if you have follow-up questions or if you need
guidance for getting started with ab-initio calculations (of such calculations
are feasible for your systems)..

  thomas bally

P.S. please don't reply to the address from where you got this message (I use
     it exlusively for CCL) but to the one indicated below:

------------------------------------------------------------------------------
|  Prof. Thomas Bally                    |  E-mail:  Thomas.Bally@unifr.ch   |
|  Institute for Physical Chemistry      |                                   |
|  University of Fribourg                |  Tel:     011-41-37 826 489       |
|  Perolles                              |  FAX:     011-41-37 826 488       |
|  CH-1700 FRIBOURG                      |                                   |
|  Switzerland                           |                                   |
------------------------------------------------------------------------------

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

Both Serge Pachkovsky and John McKelvey commented that MOPAC/AMPAC etc do not
implement the REAL/CORRECT ROHF method, but rather Dewar's half-electron method:

From:	IN%"ps@ocisgi7.unizh.ch"  2-NOV-1994 03:58:29.52
To:	IN%"ZUILHOF@CHEM.CHEM.ROCHESTER.EDU"
CC:	
Subj:	RE: CCL:ROHF versus UHF in semiempirical calc.'s of radical cations

Dear Han,

In your message to the CCL you write:
> Semiempirical programs such as MOPAC allow the properties of radicals
> and radical ions to be calculated with both the Restricted Open-shell
> Hartree-Fock method (ROHF) and the Unrestricted Hartree-Fock (UHF) methods.
                       ^^^^

This is not exactly true. Semiempirical programs usually implement half-electron
method (and Mopac is not an exception), not ROHF, which is notorious for the
poor SCF convergence properties. Although half-electron method often gives
results one would expect from the exact ROHF treatment (and in some cases is
exactly equivalent to it), there is one important distinction: electronic
energy computed within the half-electron approximation is not variational.

With my best regards,

Serge Pachkovsky.

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

Careful...NONE of the semi-empirical methods derived from MOPAC or AMPAC does 
the CORRECT ROHF. They all use a half-electron method of Dewar followed by a 
small C.I. for clean up. Gaussian and GAMESS will do the ROHF for the 
semiempirical methods correctly, I believe.

-- 

John M. McKelvey			email: mckelvey@Kodak.COM
Computational Science Laboratory	phone: (716) 477-3335
2nd Floor, Bldg 83, RL
Eastman Kodak Company			
Rochester, NY 14650-2216

---------------------------------------------------------------------------
the matter of spin contamination occurring in UHF calculations was adressed
by several people:
Dave Ewing writes:

From:	IN%"EWING@jcvaxa.jcu.edu"  "DAVID W. EWING (216) 397-4742"
To:	IN%"ZUILHOF@CHEM.CHEM.ROCHESTER.EDU"
CC:	
Subj:	RE: CCL:ROHF versus UHF in semiempirical calc.'s of radical cations


With ROHF you don't have to worry about spin contamination.

Dave Ewing
John Carroll University
ewing@jcvaxa.jcu.edu
----------------------------------------------------------------------------

and Irene Newhouse wrote:

From:	IN%"newhoir@mail.auburn.edu"  3-NOV-1994 12:35:15.41
To:	IN%"ZUILHOF@CHEM.CHEM.ROCHESTER.EDU"
CC:	
Subj:	RE: CCL:ROHF versus UHF in semiempirical calc.'s of radical cations

There are people who are VERY suspicious of ROHF -- people like Andy Holder,
one of the authors of AMPAC v4.  On the other hand, UHF can, especially very
close to the transition state, suffer from 'spin contamination', that is,
states with the wrong spin mix in.  At very stage, SZ**2 is plotted, so that
you can TELL if it's happening.  Which way you do it, depends on if you're
trying to qualitatively describe experiments, or do a thorough theoretical`
investigation.  If the former, I'd try it both ways & be happy if the results
are about the same.  If the latter, all either method is good for is a guess
to plug into ab initio computations!

Good luck!`
Irene Newhouse 
###############################################################################
###############################################################################

******************************************************************************
**   Dr. Han Zuilhof           **  e-mail: ZUILHOF@chem.chem.rochester.edu  **
**   Department of Chemistry   **  (optional: ZUILHOF@rulgca.leidenuniv.nl) **
**   University of Rochester   **                                           **
**   Rochester, NY, 14627      **  Fax:   (716) 473-6889                    **
**   USA                       **  Voice: (716) 275-2219                    **
******************************************************************************
**                                                                          **
**                        "Excite a photochemist!"                          **
**                                                                          **
******************************************************************************



From WANG@IRBM.IT  Tue Nov  8 16:24:52 1994
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From: <WANG@IRBM.IT>
Date: Tue, 8 Nov 1994 21:58:11 +0100 (WET)
To: chemistry@ccl.net
CC: WANG@IRBM.IT
Message-Id: <941108215811.68e1@IRBM.IT>
Subject: Macromodel_Amber charges


Dear all,

AMBER force field in Macromodel 4.5 gives guanine (also C, T and U) a 
net charge of -0.236.  Does anyone have the same experience with other 
molecules ?

Thanks,

Bingze Wang

From PHYSPLMP@MIZZOU1.missouri.edu  Tue Nov  8 16:27:49 1994
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Date: Tue, 08 Nov 94 14:21:50 CST
To: jig@qorg.unizar.es
cc: chemistry@ccl.net
Subject: Re: CCL:DeFT: Basis sets for Sulfur
In-Reply-To:  jig@qorg.unizar.es -- Tue, 8 Nov 94 18:21:09 MET


I have an interest in sulfur also but have not started DFT calculations yet.
I'd appreciate learning any pointers you receive from the net.  Thanks in
advance.  Pat Plummer, Univ. of MO-Columbia

From ashy@rose.chem.wesleyan.edu  Tue Nov  8 17:26:10 1994
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From: Ashwin Dinakar<ashy@rose.chem.wesleyan.edu>
To: chemistry@ccl.net
Subject: CCL:Coordinates for Water-Dimer



Hello Netters,
              Iam looking for some references(experimental) on the
coordinates for water-dimer. I would appreciate it if your replies are sent
directly to me and I will summarize all the responses.
           Thanks in advance,
           Ashwin Dinakar,
           Wesleyan University.

From helden@gaucho.ucsb.edu  Tue Nov  8 17:31:29 1994
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From: helden@gaucho.ucsb.edu (Gert von Helden)
Message-Id: <9411082210.AA16903@gaucho.ucsb.edu>
Subject: AMBER parameters for non prot. arginine ?
To: chemistry@ccl.net
Date: Tue, 8 Nov 1994 14:10:16 +22305458 (PST)
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Hi everybody
We are doing gas phase conformational studies on small protonated peptides. The
peptide we started with is Bradykinin. Unfortunately, this peptide has two
Argininegroups in it. Since we deal with only singly protonated species,
only one arg sidechain is protonated. I looked into amber and there are no
parameters for argenine with a non protonated sidechain (which makes sense,
since they will be always protonated in solution). So my questions are:
a) Did anybody calculated parameters for non protonated arg.
b) Are there any standard AMBER atomtypes that could be used for the

    -C=N-H
     |
     NH2
   
   end of the sidechain, so that the only thing to do would be to 
   calulate charges?

Thanks for any help,  Gert

  
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
+ Gert von Helden, Dept. of Chemistry, UCSB, Santa Barbara, CA 93106 +
+ Tel   : 805-893-2673, Fax   : 805-893-8703                         +
+ E-mail: helden@gaucho.ucsb.edu                                     +
++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++


From cooksj@ttown.apci.com  Tue Nov  8 17:36:21 1994
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	id AA21479; Tue, 8 Nov 94 17:11:11 -0500
Date: Tue, 8 Nov 94 17:11:11 -0500
From: cooksj@ttown.apci.com (Stephen J. Cook)
Message-Id: <9411082211.AA21479@ttown.apci.com>
To: chemistry@ccl.net
Subject: Re: CCL:DeFT: Basis sets for Sulfur
X-Attribution: sjc
Reply-To: cooksj@ttown.apci.com


>>>>> "Jose" == Jose Ignacio Garcia <jig@qorg.unizar.es> writes:

    Jose> Can anyone to point me to a reference, ftp-site, etc. where find
    Jose> suitable basis sets for Sulfur to be used in DFT calculations?
    Jose> Otherwise, how could I to construct the auxiliary basis sets for
    Jose> this atom?

	The DGauss basis sets have been made available on the
	new UniChem web page at
	http://www.cray.com/apps/UNICHEM/Mainpage.html

	The basis sets are described in the reference:

	N. Godbout, D. R. Salahub, J. Andzelm, and E. Wimmer,
	Can. J. Chem. 70, 560 (1992).

-- 
*********************************************************************
* Steve Cook                                cooksj@ttown.apci.com   *
* Air Products and Chemicals, Inc.          Tel. (610) 481-2135     *
* 7201 Hamilton Blvd.                       FAX  (610) 481-2446     *
* Allentown, PA 18195                                               *
* USA                                                               *
*********************************************************************
*             Emacs - the choice of a GNU generation                *
*********************************************************************
* Disclaimer: The opinions expressed here are those of the author.  *
*             Any resemblance between my opinions and those of Air  *
*             Products is purely coincidental...                    *
*********************************************************************

From steve@carbo.cc.binghamton.edu  Tue Nov  8 19:24:54 1994
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Date: Tue, 8 Nov 1994 18:56:21 -0500 (EST)
From: Steven Schafer <steve@carbo.cc.binghamton.edu>
Subject: Q: Molecular Dynamics Animations
To: chemistry@ccl.net
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	Are there any public domain programs for Silicon Graphics systems 
that can take a dynamics run from SYBYL and create a movie from it?  
Also, what visualization programs support input from GAMESS?

	Thanks in advance, 

	Steven Schafer
	S.U.N.Y. Binghamton Chemistry Department
	Binghamton, New York




From ungsik@radon.sait.samsung.co.kr  Tue Nov  8 19:29:59 1994
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Date: Wed, 9 Nov 94 09:14:09 +0900
From: ungsik@radon.sait.samsung.co.kr (Ungsik Yu)
Message-Id: <9411090014.AA03296@radon.sait.samsung.co.kr>
To: CHEMISTRY@ccl.net
Subject: metallocene parameters


Hi,

Does anyone have force field parameters for the Ti and Zr atmos
which will be used for the modeling of metallocene catalysts?

Also does anyone have geometric parameters for the common metallocene
catalysts such as cyclopentadienyl or indenyl zirconium dichloride?

I plan to use Biosym/DISCOVER for classical calculations and Cray/UNICHEM
(DGauss and MNDO 93) and Gaussian 92 for quantum chemical calculations.

Any help is appreciated.

Thanks, Ungsik
----------------------------------------------------------------
Ungsik Yu, Ph.D.             ungsik@radon.sait.samsung.co.kr
Samsung Adv. Inst. Tech.     P.O. Box 111, Suwon, 440-600, KOREA
Tel: 82-331-280-9169         Fax: 82-331-280-9158
----------------------------------------------------------------


