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From: dlim@minerva.cis.yale.edu (Dongchul Lim)
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Subject: calculation of atomic charges (summary)
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<SUMMARY of Quick Calculation of Atomic Charges>
I'd like to thank all who responded.
Here is a summary (rather severe chop-off of all signatures was made...)
-D.LIM (dlim@minerva.ycc.yale.edu)

------------------------------
>From connectivity information:
------------------------------
Johannes Gasteiger et al, 1993 or 1994 in J. Comp. Chem. or J. Chem. Inf. Comput. Sci. 
Steven Dixon and Peter Jurs J. Comp Chem, 1993 or 1994.
	Dave Elrod dwelrod@upj.com   

The Gasteiger-Marsili method (along with its variants) is the most popular 
The original reference is J. Gasteiger and M. Marsili, Tetrahedron, 3
6, 3219 - 3288 (1980), although there have been enhancements since.
	Tom Slee slee@hyper.com

Skorczyk(Acta Cryst., A32, 447 (1976)) or Gasteiger and Marsili(Tetrahedron
36, 3219(1980)).  Both methods are available in commercial software packages
such as CHEM-X.  Also most molecular modeling programs have some way of
getting partial atomic charges from a look up table or computing them from
dipole moment values.
	Jerry Perlstein lsaw00@risque.chem.rochester.edu

-------------------------------------
>From electronegativity equilibration:
-------------------------------------
Shen, Subramaniam, Wong, McCammon "Superoxide Dismutase:
Fluctuations in the Structure and Solvation of the Active Site Channel
Studied by Molecular Dynamics Simulation"
Biopolymers 1989, 28, 2085-2096 - take a look at reference 19: Sanderson,
R. T. "Polar Covalence", 1983, Academic Press, Orlando, FL.).
	Jim Briggs

charge distribution in molecules; the Electronegativity Equalization Method.
Huheey, J.E.; "Inorganic Chemistry: Principles of Structure and Reactivity",
3rd ed., Harper & Row, New York, 1983, 159.
	Mick Kappler

A.K. Rappe and W.A. Goddard III, J. Phys. Chem. 95, 3358-3363 (1991)
	-Jim



From srheller@asrr.arsusda.gov  Tue May  3 10:22:15 1994
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Date: 3 May 94 09:44:00 EDT
From: "STEPHEN R. HELLER" <srheller@asrr.arsusda.gov>
Subject: One software package for review
To: "chemed-l" <chemed-l@uwf.cc.uwf.edu>
cc: "chminf-l" <chminf-l@iubvm.ucs.indiana.edu>,
        "chemistry" <chemistry@ccl.net>,
        "orgchem" <orgchem@extreme.chem.rpi.edu>


3 May, 1994


Subject:  Computer Software for Review



     As the Software Review Editor for the ACS Journal of
Chemical Information and Computer Science (JCICS) I often get
software for review in the journal.  I now have one package in
hand (see below) and I am looking for someone who is willing to
review the software.  In return for the review you get to keep
the software.  The review should be completed in 1-2 months.  The
length of the review is 4-10 double spaced typed pages.  Sample
reviews can be found in most of the recent issues of JCICS.

     Please try to give me some (short) reason to choose you over
another person. DO NOT SAY YOU WILL REVIEW ANYTHING I HAVE
AVAILABLE. Messages with such replies are trashed!

     I have tried this approach for about the past three years
and it is working reasonably well. (REMINDER: For those who
haven't finished your reviews of software sent months and months
ago, this last sentence does not apply to you!)  As a result, I
am continuing this new method to find reviewers using this e-
mail/user group system.  I reserve the right to abandon this if
it is a problem, or inappropriate.  I will not notify people if I
have found a reviewer.  If you don't hear from me within a few
days I have chosen someone else to review the particular package.

     As I get many, many, (too many) replies to this message,
please do not respond after 4 May, 1994 (Wednesday), as I am sure
the software will be gone by then.


     I can be reached on Internet (SRHELLER@ASRR.ARSUSDA.GOV).

 
     PLEASE BE SURE TO INCLUDE AN STREET ADDRESS, PHONE, and FAX
NUMBER!!!  (I send the software by Federal Express.)  Without
this information I WILL NOT consider your request.


     Steve Heller


The package I now have is:

1. SigmaStat for Windows from Jandel Scientific. This is a
statistical package for the PC.




From raeker@tc6.fi.ameslab.gov  Tue May  3 12:23:33 1994
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From: raeker@tc6.fi.ameslab.gov (Todd J. Raeker)
Message-Id: <9405031535.AA26688@tc6.fi.ameslab.gov>
Subject: Bulk electronic densities needed
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  I have a need for atomic electron densities of 3d,4d,5d
transition metals derived from DFT bulk calculations. I would
prefer parameters for a Gaussian expansion.  Does anyone
know of a reference or, better yet, a program I could get and
run myself?  Any pointers would be greatly appreciated.


Thanks in advance.
Todd.
--


Dr. Todd J. Raeker         |  307B Wilhelm Hall      |  Money Talks !!
raeker@tc4.fi.ameslab.gov  |  Iowa State University  |  Mine keeps
Phone (515)-294-9927       |  Ames Laboratory, USDOE |  saying goodbye.
FAX   (515)-294-5204       |  Ames, Iowa 50011       |


From hwang@iris100.biosym.com  Tue May  3 12:35:42 1994
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Date: Tue, 3 May 94 08:42:58 -0700
From: hwang@biosym.com (Ming-Jing Hwang)
Message-Id: <9405031542.AA23753@iris100.biosym.com>
To: chemistry@ccl.net
Subject: Re:  CCL:Development of new Force Fields



Frank Jensen wrote:

>...Why not simply select say, a Morse potential
>instead? The Taylor expression contains four parameter 
>(r0 and a,b,c), the Morse only three. ...

One reason, a practical one, to use power series instead of Morse function 
is to make parameterization easier when using quantum mechanical energy data.  
With a power series the entire energy function (i.e. force field) becomes 
linear with respect to the force field parameters (force constants) which 
are being sought, when reference values (bond and angle references) and 
nonbond parameters are held fixed.  The parameters (k1, k2, k3, etc.) can 
then be solved analytically with one matrix operation.  New bond and angle 
references can be projected from the linear force constants (k1) just solved, 
and optimal references (the so called "natural" bond lengths and bond 
angles of the hypothetical "unperturbed" state on the hypersurface of the 
training set molecules) can be obtained within a few iterations (when all 
the linear force constants vanish or are essentially zero).  This advantage of 
using the linear-least-squares fitting is lost if a Morse potential
is used.  Note also there is no structure minimization during the 
paramterization since the data fitted are direct energy surface properties 
(configurational energy differences, and energy 1st and 2nd derivatives, 
etc. from ab initio calculations) and not the geometric parameters 
(equilibrium bonds, angles, and torsions) or vibrational frequencies 
commonly used in the traditional methods.  This facilitates automation 
of many parts of the parameterization procedures in the derivation 
of CFF93 force field.  Efficient fitting procedures make it
possible to use large amount of quantum mechanical data to fit detailed
(Class II) force fields and obtain reliable results.


Ming-Jing Hwang
hwang@biosym.com


From R1JJH@VM1.CC.UAKRON.EDU  Tue May  3 15:22:19 1994
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Date: Tue, 03 May 1994 14:27:26 -0400 (EDT)
From: Jack Houser <R1JJH%AKRONVM.BITNET@phem3.acs.ohio-state.edu>
Subject: Gaussian 90 on Tungsten
To: Supercomputer bulletin board <chemistry@ccl.net>
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Dear Netters:
 
I, a humble organic chemist, have been asked by a colleague to run an
ab initio calculation on W(CO)6 and its radical cation.  Never having run
a calculation on an inorganic compound before, I looked in the Gaussian 90
manual and found that there were two basis sets, LANLIMB and LANL1DZ which
were usable for H through Bi.  Does anybody know whether one of these is
better than the other for my purposes, and is there anything else I should
add to the route card?  Thanks for the help.
 
Jack Houser
Department of Chemistry
The University of Akron
Akron Ohio 44325-3601

From LONCHARICH_RICHARD_J@Lilly.com  Tue May  3 17:23:28 1994
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Date: Tue, 03 May 1994 15:26:44 -0500 (EST)
From: Rick Loncharich <LONCHARICH_RICHARD_J@Lilly.com>
Subject: mixed parameters in semiempirical methods
To: chemistry@ccl.net
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SUBJ:  mixed parameters in semiempirical methods

Douglas Smith and co-workers published a structural study of some
aromatic amines in which they document the hazards of using mixed
AM1-MNDO parameters.  (J. Comp. Chem.  1992, 13(5), 640-650.)

Has anyone else published on the hazards of using mixed parameters
in semi-empirical calculations?  I would appreciate any additional 
references that document the hazards of doing this.

Thanks

Rick Loncharich
internet:   rjl@lilly.com


From: LONCHARICH RICHARD J          (MCVAX0::RX82788)

To:   FOREIGN TRANSPORT ADDRESSEE   (MCDEV1::IN%"chemistry@ccl.net")

From longshot@chem.duke.edu  Tue May  3 20:22:22 1994
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From: longshot@chem.duke.edu (Brad Isbister)
Message-Id: <9405032326.AA05648@canada.chem.duke.edu>
To: chemistry@ccl.net
Subject: AMBER 4.0 help


I'm going through the process of learning AMBER and I'm stuck at the minimization routine.  I have created a record for MeOH and gotten through the prep, link, edit, and parm modules.  I took the starting coordinates from a drawing out of SYBYL.  I've put the molecule in a box of TIP3P water and would like to minimize for a couple hundred steps (but even one will do!).

When I run the minimization, all of the support files get read in, the starting coords are written to output, and then it dies, apparently before any energy calculations.  The error message says COORDINATE RESETTING CANNOT BE ACCOMPLISHED, DEVIATION IS TOO LARGE.  What kinds of things might cause this problem?  I've appended the relevant section of the .out file to to this message.

I've varied several of the input settings, but in a random way since I don't understand the source of the problem.  Any suggestions?

Thanks,

-Brad
---------------------------------Clip N Save------------------------------------
Brad Isbister					Duke University
longshot@chem.duke.edu				Department of Chemistry
Computational/Biophysical chemistry		E.J. Toone group


Now, the .out file:


   3.  ATOMIC COORDINATES AND VELOCITIES

     Methanol                                                                   
 begin time read from input coords =     0.000 ps


     COORDINATE RESETTING CANNOT BE ACCOMPLISHED,
     DEVIATION IS TOO LARGE
     NITER, NIT, LL, I AND J ARE :    0    2    1    1    2


                    FINAL RESULTS

   NSTEP       ENERGY          RMS            GMAX      NAME    NUMBER
      1           0.000         0.000       154.738     H1A       1

 BOND    =          0.0000  ANGLE   =          0.0000  DIHED =          0.0000
 VDWAALS =          0.0000  ELECT   =          0.0000  HBOND =          0.0000
 1-4 NB  =          0.0000  1-4 ELEC=          0.0000  CONST =          0.0000

 %MINMD-F-ERSTOP, fatal error

     Routine      Sec       %
     --------------------------
     Pairlist      0.00    0.00
     Nonbond       0.00    0.00
     Bond          0.00    0.00
     Angle         0.00    0.00
     Dihedral      0.00    0.00
     Shake         0.18    1.57
     Pol. der      0.00    0.00
     Efielde       0.00    0.00
     Indip         0.00    0.00
     Matmul        0.00    0.00
     Other        11.48   98.43
     --------------------------
     Total        11.67    0.00 Hours

From news@nntp-server.caltech.edu  Tue May  3 22:22:23 1994
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From: hpritcha@cco.caltech.edu
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Subject: GAMESS on a PARAGON
Date: 4 May 1994 01:41:20 GMT
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Hello mlist.chemistry world,

Has anybody out in the mlist chemistry world built
an executable of the GAMESS electronic structure
program for an Intel Paragon running OSF which
actually works?  I would appreciate hearing from
any such persons, as I cannot get beyond building
an exec which immediately gives a Segmentation fault
when started in a compute partition.  Not even
a core file to help diagnose!

Thanks in advance.

Howard Pritchard                
818-395-6537                    
hpritcha@ccosun.caltech.edu     

