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Date: Mon, 30 Aug 93 21:15:12 -0700
From: mxm@biosym.com (Max Muir )
Message-Id: <9308310415.AA03140@iris80.biosym.com>
To: CHEMISTRY@ccl.net
Subject: Responses to 'finding transition states with MOPAC6.0'



Dear CyberChemists,

thanks for your help.

 >using MOPAC6.0 I have been attempting to correlate calculated
 >heats of formation of some transition states with experimental
 >activation energies for the following reaction
 >
 >              H       R1                            R1
 >     .         \     /                            ./
 >  tBu     +     C = C      ------->   tBu - CH2 - C
 >               /     \                             \
 >              H       R2                            R2
 >
 > I am getting some credible looking structures for the transition
 > states.  However, I cannot seem to get close to the saddle point, 
 > where the gradient normal is zero.  I set SCFCRT=10^-12 and
 > GNORM=0.0001, and the calculation exits normally thus-
 >
 > CYCLE:   9 TIME: 195.67 TIME LEFT: 356495.2 GRAD.:     0.000 HEAT: 4.288334
 >
 > But when I do a FORCE calcn to verify the single -ve ROOT, MOPAC reports that
 > GRADIENT NORM = 0.12229, which is not really good enough for publication is 
 > it?  I have one and one only negative root.  What's the problem?  What's the

 (Hysterical questions deleted).


 I fixed up WRITE.f to write out gradient norm as the calculation finishes
 (like AMPAC).  Thus . . 

 CYCLE:   6 TIME: 240.34 TIME LEFT: 357099.6 GRAD.:     0.000 HEAT: 4.288334    
          HESSIAN CALCULATED NUMERICALLY
 CYCLE:   7 TIME: 240.05 TIME LEFT: 356618.8 GRAD.:     0.000 HEAT: 4.288334    

 -------------------------------------------------------------------------------
 GRAPH UHF AM1 NODIIS ITRY=500 MMOK DMAX=0.20 TS SCFCRT=0.000000000001 +
 GNORM=0.0002 LET NOINTER RECALC=1
 INSIGHT generated AMPAC/MOPAC input file
 DATE: Tue Aug 24 18:44:09 1993


     GEOMETRY OPTIMISED USING EIGENVECTOR FOLLOWING (EF).     
     SCF FIELD WAS ACHIEVED                                   


                                AM1    CALCULATION
                                                       VERSION  6.00
                                                       30-Aug-93               




          FINAL HEAT OF FORMATION =          4.28833 KCAL


          TOTAL ENERGY            =      -1257.77074 EV
          ELECTRONIC ENERGY       =      -6795.64588 EV
          CORE-CORE REPULSION     =       5537.87514 EV

          mxm GRADIENT NORM           =        0.0001815  <-------<<  Yippee!!
          IONIZATION POTENTIAL    =          7.96377
          NO. OF ALPHA ELECTRONS  =         25
          NO. OF BETA  ELECTRONS  =         24
          MOLECULAR WEIGHT        =    113.222


          SCF CALCULATIONS  =              491
          COMPUTATION TIME = 28 MINUTES AND  15.740 SECONDS


 However, it looks like there is no easy way to get the refined structure
 into MOPAC for the force calcn without altering the file readers/writers.

 And in any case it does not seem to matter.  

 I here append the responses.

_______________________________________________________________________

Date: 30 Aug 93  8:08 +0200
From: Frank Jensen <frj@dou.dk>
Subject: mopac ts's

	Max,
	Your "problem" is simply that the geometry as printed in the
output or achieve file only contain some 5-6 digits. In the optimization
the full accuracy of the geometry is produced and you may obtain very
small gnorm's, but the final geometry is only printed with an accuracy
that gives you the gnorm of ~0.1 in the force calculation. A force
calculation with a gnorm < 1.0 is fine. If you realy need the full accuracy
you would have to change the format statement in the code to print out
more digits.
	Frank
_______________________________________________________________________

From: jas@medinah.atc.ucarb.com (Jack Smith)
Subject: Re: finding transition states using MOPAC6.0

Max:

   If you're using SADDLE to locate the transition state, then follow it
with a gradient minimization (I usually use EF) before doing the FORCE
calculation.  SADDLE does not appear to refine its final geometry.  I'd
save the trial saddle point before doing the gradient minimizatin, though -
I have had many "SADDLE" points just fall off to one side of the saddle
point and have to start all over.  I'd also follow the FORCE calculation
with IRC calculations along both directions of the negative root to confirm
that the transition state indeed connects the desired reactants to desired
products.

   According to the MOPAC documentation, the PRECISE keyword should
generate publication quality results (as far as SCF convergence and
Gradient Norms are concerned).
 
_______________________________________________________________________

From: NEELY@DUCVAX.AUBURN.EDU
Subject: Re: finding transition states using MOPAC6.0

I've had problems with a second step in MOPAC 6 'claiming' a larger
gradient norm than the previous step did.  I've not gotten a satis-
factory answer to this question.  In your case, you need to re-
member that nothing is really 0 with floating point arithmetic on
a computer--it's all roundoff error.   I'd be quite satisfied with
a gradient norm of about 0.1 for publication, & I suspect most 
people would, especially for a transition state..
Irene Newhouse
_______________________________________________________________________


From vkitzing@sunny.mpimf-heidelberg.mpg.de  Tue Aug 31 11:26:17 1993
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From: vkitzing@sunny.mpimf-heidelberg.mpg.de (Eberhard von Kitzing)
Message-Id: <9308310726.AA06801@sunny.mpimf-Heidelberg.mpg.de>
Subject: Re: query regarding AMBER energy minimization
To: mbu!neel@vigyan.ernet.in, CHEMISTRY@ccl.net (Computational Chemistry List)
Date: Tue, 31 Aug 1993 09:26:17 +0200 (MET DST)
In-Reply-To: <9308302202.AA11960@iisc.ernet.in> from "neel@vigyan.ernet.in" at Aug 30, 93 05:02:57 pm
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> 
> Hello everybody, when i do energy minimization using AMBER forcefield
> i frequently get "linmin failure'. Can anybody tell me what is this
> linmin & how to avoid it and what it is? Where from i can get to 
> know minimization algorithms used in AMBER ?Thank you , Neel
> 
Most optimization procedures work in two step. First they try to
estimate a good direction in which the energy is expected to lower
considerably and second it follows this direction and tries to find
the minimum of the energy function along this line (terminus
technicus: line search). Subroutines doing this task are traditionally
called "linmin". 

If you use the single precision version of AMBER, you can probably
avoid this problems by using the double precision version. If not, you
may have located a difficult area with a low gradient.  In this
situation truncation errors start to become a severe problem. If this
is a low energy area you may have found your goal. In the other case
you may use a short dynamics run to leave this area.

For more detail please see my articles:
E. v.Kitzing, Meth. Enzym. (1992) 211, 449-466
E. v.Kitzing, Prog. Nucl. Acid Res. Mol. Biol. (1992) 43, 89-110

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

Eberhard von Kitzing
Max-Planck-Institut fuer Medizische Forschung
Jahnstr. 29, D69120 Heidelberg, FRG

FAX : +49-6221-486 459  (work)
Tel.: +49-6221-486 467  (work)
Tel.: +49-6221-385 129  (home)

internet: vkitzing@sunny.mpimf-heidelberg.mpg.de


From jas@medinah.atc.ucarb.com  Tue Aug 31 04:43:52 1993
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Date: Tue, 31 Aug 1993 09:43:52 -0500
To: chemistry@ccl.net
From: jas@medinah.atc.ucarb.com (Jack Smith)
Subject: 4-coord angles


   Given five of the six central angles in a general four-coordinate
arrangment (2 special cases, of course, being a tetrahedron and a square
plane), what is the forumula for the sixth (and redundant) angle in terms
of the other five?  Is there a simple invariant (sum rule?) for this system
that I'm missing?  I thought I'd see if anyone already knew the answer
before I went through the trig myself. 

-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=
  JACK A. SMITH                 ||
  Union Carbide Corp.           ||  Phone:    (304) 747-5797
  Catalyst Skill Center         ||  FAX:      (304) 747-5571
  P.O. Box 8361                 ||
  S. Charleston, WV  25303      ||  Internet: jas@medinah.atc.ucarb.com
-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=


From mercie@cumc.cornell.edu  Tue Aug 31 09:27:40 1993
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Date: Tue, 31 Aug 1993 13:27:40 -0400 (EDT)
From: Gustavo Mercier <mercie@med.cornell.edu>
Subject: Re: Theoretical Calculations of Lanthanide Organic Complexes
To: Nivan Bezerra <21NBCJ@npd1.ufpe.br>
Cc: chemistry@ccl.net
In-Reply-To: <01H2D2JRF26U8Y503Q@NPD1.UFPE.BR>
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On 30 Aug 1993, Nivan Bezerra wrote:

> Dear Netters,
> 
> 	I am interested in theoretical methods for the calculations of
> organic complexes of lanthanides, especially Eu(III).
> 	Does anyone know any packages for this type of calculation using
> MO, extended Huckel, Xalpha, Density Functional Theory, INDO, AMPAC,
> MOPAC, etc?
> 	Thank you very much.

You may try several things:

	1) Standard packages like G92, Hondo, GAMESS etc using effective
core potentials that include relativistic effects in an "average" fashion.
See below for references regarding ecp's for lanthanides and other atoms.

	2) You may try DFT computations. A package like ADF from Baerends
group includes a "basis set" for Eu and you can include relativistic effects.
You may contact them to obtain the program (1500 DG fro academic users)-
adf@chem.vu.nl or tevelde@chem.vu.nl

Regarding semiempirical methods I am unfamiliar with programs that have
parameterized the Lanthanides. Anybody aware of such program?

Good Luck!

Gus Mercier
mercie@cumc.cornell.edu

*** cut here*



The following references should provide you with very recent ECP's for
most of the periodic table. The comments I have heard from those who
have used them are rather favorable (comments limited to energetics and
geometries):

	Stevens et. al. J. Chem.Phys. 81 (12), Pt. II, 1984
	First and Second Row atoms

	Stevens et. al. Can. J. Chem. 70, 612, (1992)
	Third through Fifth row atoms. Some typos are known:

	Table 2: In RECP for second Vp-f component:
			-129.87594 should read -129.78594
	Table 4: Basis for Fe
			Cp term for 1sp should be -0.007940, not -0.07940
			asp term for 4sp should be 0.0410, not 0.410
	Table 7: Result for Be
			Eval with core a should read -1.01214, not -0.01214

	Cundari and Stevens J. Chem. Phys. 98 (7) 1993
	Lanthanides

I hope this is useful. These papers also discuss the variety of methods
available to generate ECP's, relativistic effects and references to ECP's
for DFT computations.

Good Luck
gus mercier
mercie@cumc.cornell.edu





From pathology@a1.mscf.upenn.edu  Tue Aug 31 16:44:01 1993
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Date: Tue, 31 Aug 93 20:44:01 -0400
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From: "PATHOLOGY & LAB. MEDICINE" <pathology@a1.mscf.upenn.edu>
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To: "stephen urquhart" <urquhart@mcmail.cis.mcmaster.ca>, chemistry@ccl.net
Subject: RE: Educational PC based kinetics programs search.
Msg-Class: !AS


Stephen, take a look at the program produced by the lab of Carl Frieden at 
the Department of Biochemistry and Molecular Biophysics at Washington 
University School of Medicine.  The main program is KINSIM and is described 
in good detail in C Frieden, "Numerical intergration of rate equations by 
computer," Trends in Biochemical Science, 18:58-60 (1993).  The program 
runs on VAX, Mac and PC and is available by ftp.  It is oriented towards 
enzyme kinetics, but you may find it useful for other situations, too.

Gregg Wells
Department of Pathology
University of Pennsylvania
Philadelphia, PA  19104-4283
email:  pathology@a1.mscf.upenn.edu



From merkle@parc.xerox.com  Tue Aug 31 06:27:28 1993
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From: Ralph Merkle <merkle@parc.xerox.com>
To: chemistry@ccl.net, nanotech@cs.rutgers.edu
Subject: Molecular Manufacturing and Chemical Design Automation News
Message-Id: <93Aug31.132735pdt.12171@manarken.parc.xerox.com>
Date: 	Tue, 31 Aug 1993 13:27:28 -0700


Chemical Design Automation News permanently ceased publication
with the August 1993 issue.

Unfortunately, I had an invited article on "Molecular Manufacturing:
Adding Positional Control to Chemical Synthesis" scheduled for the
*September* issue....  C'est la vie.

The article is now available in postscript format by anonymous FTP
>from "parcftp" in file "/pub/nano/MolecularManufacturing.ps".

Ralph C. Merkle
Xerox PARC
3333 Coyote Hill Road
Palo Alto, CA 94304
merkle@xerox.com

From hogue@canada.den.mmc.com Mon Aug 30 19:30:57 1993
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To: chemistry@ccl.net
Subject: Uranium
Status: RO

Does anyone out there have working parameters for uranium?  Pat Hogue

From NETNEWS@UICVM.CC.UIC.EDU  Tue Aug 31 09:36:53 1993
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Date: Tue, 31 Aug 1993 14:36:53 -0500 (CDT)
From: Prasad Ravi <U21709@uicvm.uic.edu>
Subject: Parallel & cluster versions of CHARMm, GAMESS, Discover, MOPAC
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Hello Folks,
 
I am wondering if there exist parallel and/or cluster versions of the
above packages - I am especially interested in versions that use PVM
for message passing.
 
Thanks for any information.
 
Prasad Ravi.
pravi@ncsa.uiuc.edu

From jas@medinah.atc.ucarb.com  Tue Aug 31 12:26:59 1993
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Date: Tue, 31 Aug 1993 17:26:59 -0500
To: chemistry@ccl.net
From: jas@medinah.atc.ucarb.com (Jack Smith)
Subject: Re: 4-coord angles (answer)



The original question:

>   Given five of the six central angles in a general four-coordinate
>arrangment (2 special cases, of course, being a tetrahedron and a square
>plane), what is the forumula for the sixth (and redundant) angle in terms
>of the other five?  Is there a simple invariant (sum rule?) for this system
>that I'm missing?  I thought I'd see if anyone already knew the answer
>before I went through the trig myself. 

   The answer appears to be that the sum of the cosines = -2.  Try it.  

Thanks, Christoph, Peter and Phil.

-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=
  JACK A. SMITH                 ||
  Union Carbide Corp.           ||  Phone:    (304) 747-5797
  Catalyst Skill Center         ||  FAX:      (304) 747-5571
  P.O. Box 8361                 ||
  S. Charleston, WV  25303      ||  Internet: jas@medinah.atc.ucarb.com
-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=-=


From caldwell@utdallas.edu  Tue Aug 31 12:46:18 1993
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From: "Richard A. Caldwell" <caldwell@utdallas.edu>
To: chemistry@ccl.net
Subject: HUckel for Macs
Cc: caldwell@utdallas.edu
Message-Id: <93Aug31.174632cdt.74201@utdallas.edu>
Date: Tue, 31 Aug 1993 17:46:18 -0500



Does anyone have a good public domain Hueckel MO program for Macintoshes?
I'd like to make it generally available to our students.

Thanks,

Dick Caldwell

From CUNDARIT@MSUVX1.MEMST.EDU  Tue Aug 31 12:50:46 1993
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Date: Tue, 31 Aug 1993 18:50:46 -0600 (CST)
From: CUNDARIT@memstvx1.memst.edu
Subject: lanthanide chemistry
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Hi,

	The latest version of GAMESS from Mark Gordon and the Iowa State
group has the lanthanide ECPs and valence basis sets developed by myself
and Walt Stevens (JCP 1993, 98, 5555) built in.  For now, they are limited to
single-point energy runs, but work with any wavefunction. 
	Our initial results at Memphis State for predicting the structure of 
the simplest lanthanide trihalides are excellent (i.e., reproduction of
bond lengths to within 1-3%).  We run into the usual problem for d- and
f-block chemistry with regards to energetics, i.e. there is a limited
exptl. data base to compare with, so the jury must remain out on that one
for now.
	It is my understanding that the Ross-Pitzer-Ermler team is in the
last phases of developing and testing ECPs and valence basis sets for 
the lanthanides.  Dolg, Preuss and Stoll have developed lanthanide 
effective core potentials with a variety of core sizes.  So there are
a few options on the ab-initio side.
	As far as semi-empirical approaches, the only one I am aware of
is the INDO appraoch derived by Mike Zerner, Notker Rosch and co.   
	One application of computational methods to lanthanides that we are
very excited about is the use of molecular mechanics.  I commend to the
attention of anyone interested in such an approach to lanthanide chemistry
the paper by Ben Hay (IC, 1991, 30, 2876).  We have implemented Ben's
paramters into Chem3D+ on a Quadra 800 and in the space of an hour we can
optimize the structure of a good sized lanthanide complex, include a dozen or 
so simulated annealing cycles.  The coupling of the Chem 3D+ GUI with the 
MM2 force field eases the analysis and treatment of high coordination number 
lanthanide complexes.

				Tom Cundari
				Assistant Professor
				Department of Chemistry
				Memphis State University
				Memphis, TN 38152
				phone: 901-678-2629
				fax: 901-678-3447

