From gostowskir@apsu01.apsu.edu  Sun Mar 22 11:19:29 1998
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 chemistry@www.ccl.net; Sun, 22 Mar 1998 09:39:31 CST
Date: Sun, 22 Mar 1998 09:44:59 -0600
From: Rudy Gostowski <gostowskir@apsu01.apsu.edu>
Subject: running GAMESS on a Pentium166MMX
To: CCL group <chemistry@www.ccl.net>
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This may be a redundant question but I have a Gateway 166MMX with 16Mb RAM
and a 2.1Gb harddrive.  Is this system adequate to do ab initio
calculations on molecules with 22 carbons and 17 hydrogens ?
If not what upgrades would you suggest ?
I have determined that the memory can go to 128 with two 64Mb DIMMs.
The processor can be moved up to a 200Mhz only.
In addition does anyone have experience with the Evergreen 200Mhz chip (has
64k on board rather than the Intel 32k)
Finally is the current harddrive adequate or should it be replaced with a
SCSI unit ?

Your replys will be greatly appreciated.

Rudy Gostowski
Department of Chemistry
Austin Peay State University
Box 4547
Clarksville, TN  37044
931-648-7624
FAX 931-648-5996
gostowskir@apsu01.apsu.edu

From aranyos@MIT.EDU  Sun Mar 22 12:19:28 1998
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Date: Sun, 22 Mar 1998 11:59:50 -0500
To: chemistry@www.ccl.net
From: Attila Aranyos <aranyos@MIT.EDU>
Subject: Top PC vs. Unix


Hi,

Does anyone know how fast (or slow :)) is a top PC with all you can get now
(P-II 333 MhZ (may be dual) and tip-top HD contorller ) compared with a
Unix workstation?

thanks:

attila



From milan@par16.mgsl.dcrt.nih.gov  Sun Mar 22 14:19:28 1998
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From: Milan Hodoscek <milan@par10.mgsl.dcrt.nih.gov>
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Subject: CCL:Top PC vs. Unix
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Reply-To: milan@par10.mgsl.dcrt.nih.gov


>>>>> "Attila" == Attila Aranyos <aranyos@MIT.EDU> writes:

    Attila> Hi, Does anyone know how fast (or slow :)) is a top PC
    Attila> with all you can get now (P-II 333 MhZ (may be dual) and
    Attila> tip-top HD contorller ) compared with a Unix workstation?

I put some new results which answer your question on my standard
benchmark table for a molecular dynamics program CHARMM. Please, see

http://kihp6.cmm.ki.si/parallel/summary.html 

Milan Hodoscek (http://kihp6.ki.si/)


From elewars@alchemy.chem.utoronto.ca  Sun Mar 22 15:19:32 1998
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Date: Sun, 22 Mar 1998 14:30:48 -0500 (EST)
From: "E. Lewars" <elewars@alchemy.chem.utoronto.ca>
Message-Id: <199803221930.OAA05752@alchemy.chem.utoronto.ca>
To: chemistry@www.ccl.net
Subject: RESPONSE TO EHM REF REQUEST


1998 March 22

 Regarding the request for a review of the extended Hueckel method:
 This is a brief summary of its features; ref 2 is a review.

    SUMMARY OF FEATURES OF EHM    ca. Jan 1998
---------------

Strengths and weaknesses of the EHM

STRENGTHS
  One big advantage of the EHM over more elaborate semiempirical methods and
ab initio and DFT is that the EHM can be applied to large systems containing
almost any element.  The EHM can treat esentially all elements, since the only
element-specific parameter needed is the (valence-state) ionization potential
[1], which is generally available.  In contrast, more elaborate semiempirical
methods have not been parameterized for many elements (altho' recent parameteri-
zations of PM3 and MNDO for transition metals make these much more generally
useful than hitherto).  For ab initio and DFT methods, basis sets may not be
available for elements of interest, and besides ab initio and even DFT are
hundreds of times slower than the EHM and are limited to much smaller systems.
The applicability of the EHM to large systems and to a variety of elements is
one reason why it has been extensively applied to polymeric and solid-state
structures [2].  the EHM is faster than more elaborate semiempirical methods,
partly because the Fock matrix needs to be diagonalized only once to yield the
eigenvalues and eigenvectors (the eigenvectors must be transformed back to those
of the original nonorthogonalized matrix).  In contrast, methods like AM1 and
PM3 (as well as ab initio calculations) require repeated matrix diagonalization
because the Fock matrix must be iteratively refined in the SCF procedure.

  The spartan reliance of the EHM on a paucity of empirical parameters makes it
relatively easy (in the right hands) to interpret its results, which depend, in
the last analysis, only on geometry (which affects overlap integrals) and
ionization potentials.  With a strong dose of chemical intuition this has
enabled the method to yield powerful insights [3].

  The applicability to large systems, including polymers and solids, containing
almost any kind of atom, and the relative transparency of the physical basis
of the results, are the main advantages of the EHM.

  Surprisingly for such a conceptually simple approach, the EHM has a
theoretically-based advantage over otherwise more elaborate semiempirical
methods, in that it treats orbital overlap properly: AM1 and PM3, for example,
use the _neglect of differential overlap_ (NDO) approximation, meaning that they
take S_ij = delta_ij, as in the simple Hueckel method.  The EHM can thus give
superior results [4].
  The EHM is a very valuable teaching tool because it follows straightforwardly
from the simple Hueckel method yet uses overlap integrals and matrix
orhtogonalization in the same fashion as the mathematically more elaborate
ab initio procedure.

  Finally, the EHM, albeit more elaborately parameterized than in its original
incarnation, has recently been shown to be a serious competitor to the very
useful and popular semiempirical AM1 method for calculating molecular geometries
[5].

WEAKNESSES
  The weaknesses of the standard EHM probably arise at least in part from the
fact that it does not (contrast the ab initio method) take into account
electron spin or electron-electron repulsion, ignores the fact that molecular
geometry is partly determined by internuclear repulsions, and makes no attempt
to overcome these defects by parameterization.

  The standard EHM gives, by and large, poor geometries and energies.  Although
it predicts a CH bond length of ca. 1.0 A, it yields CC bond lengths of 1.92,
1.47 and 0.85 for ethane, ethene and ethyne, respectively, cf the actual values
of 1.53, 1.33 and 1.21 A, and although the favored conformation of an alkane is
usually correctly identified, the energy barriers and differences are only in
modest agreement with experiment [6].  Because of this inability to reliably
calculate geometries, EHM calculations are usually not used for geometry
optimizations, but rather utilize experimental bond lengths and angles.

[1]  J. Hinze, H H. Jaffe, J Am Chem Soc 84 (1962) 540; A Stockis, R. Hoffmann
     102 (1980) 2952
[2]  R. Hoffmann, "Solids and Surfaces: A Chemist's View of Bonding in Extended
     Structures", VCH publishers, 1988.
[3]  (a) The Woodward-Hoffman rules: R. B. Woodward, R. Hoffmann, "The
     Conservation of Orbital Symmetry", Academic Press, 1970.
     (b) Counterintuitive orbital mixing: J. H. Ammeter, H.-B. Buergi, J. C.
     Thibeault, R Hoffmann, J Am Chem Soc 100 (1978) 3686.
[4]  Rationalizing nonplanar CC double bonds: J. Spanget-Larsen, R Gleiter,
     Tetrahedron, 39 (1983) 3345.

[5]  S. L. Dixon, P C Jurs, J Comp Chem 15 (1994) 733.

[6]  R. Hoffmann, J Chem Phys 39 (1963) 1397.
=====================

From lmoskal@emory.edu  Thu Mar 19 21:18:57 1998
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	for <chemistry@www.ccl.net>; Thu, 19 Mar 1998 20:27:33 -0500 (EST)
Date: Thu, 19 Mar 1998 20:27:32 -0500 (EST)
From: Lyudmila V Moskaleva <lmoskal@emory.edu>
X-Sender: lmoskal@curly.cc.emory.edu
Reply-To: Lyudmila V Moskaleva <lmoskal@emory.edu>
To: chemistry@www.ccl.net
Subject: Summary: B3LYP Raman Activities
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Dear All:
A few days ago I posted a question concerning calculation of Raman
Activities in Gaussian94.
I wish to thank everyone who responded!
The answer on my question is that Raman scattering Activities and Raman
depolarization Ratios require calculation of third
derivatives which is only available at HF level in Gaussian.

Cheol Ho Choi mentioned that it is possible to calculate them numerically
by introducing an external electric field, but very painful.

Regards,
Lyudmila

>Dear Subscribers:
>Can anyone,
>please, advise me on the following
>subject. I am doing frequencies calculations at B3LYP level in
>Gaussian94.
>For some reason, in the output I get all zeros in the place of Raman
>scattering Activities and Raman depolarization Ratios:
>
>                     1                      2                      3
>                    ?A                     ?A                     ?A
> Frequencies --  -549.0164                33.2578               119.9049
> Red. masses --     7.8867                 2.2972                 3.9523
> Frc consts  --     1.4006                 0.0015                 0.0335
> IR Inten    --     0.0177                 0.0940                 0.0677
> Raman Activ --     0.0000                 0.0000                 0.0000
> Depolar     --     0.0000                 0.0000                 0.0000
>
>Is there any keyword or "IOP" that would force the program to calculate
>these parameters or does this feature only function for HF calculations?
>
>Thank you in advance for any response.
>
>Sincerely,
>Lyudmila Moskaleva
>
>e-mail: lmoskal@emory.edu 



















From mao@csb0.IPC.PKU.EDU.CN  Fri Mar 20 03:19:01 1998
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	for CHEMISTRY@www.ccl.net id AA19586; Fri, 20 Mar 98 15:53:57 -0800
Date: Fri, 20 Mar 1998 15:53:45 -0800 (PST)
From: Fenglou Mao <mao@csb0.IPC.PKU.EDU.CN>
To: "CHEMISTRY@www.ccl.net" <CHEMISTRY@www.ccl.net>
Subject: summary:Molecular Modeling C++ class library
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Dear cclers,
    Several days ago, I sent a message for Molecular Modeling C++ 
class library. Many people e-mailed me to summary I recieved.
I am very sorry to tell all of you that it was no Molecular Modeling 
C++  class library available now. About three months ago, I had begun to
write a Molecular Modeling C++ class library, but one month ago I had 
an urgent affair to do, I will resume it about three month later. 
Any suggestion about the class library structure will be welcome.

    Best wishs!

Sincerely Yours,

FengLou Mao
*******************************
ADD:Mr. FengLou Mao
    Peking University
    BeiJing
    P.R.China
Tel:86-10-62751490
Fax:86-10-62751725




From d.w.price@reading.ac.uk  Fri Mar 20 12:19:04 1998
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From: Dave Price <d.w.price@reading.ac.uk>
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Subject: Pair Potentials from ab initio/DFT calcs?
Content-Type: multipart/alternative; boundary="------------50672FD6FE5014644E576A50"



--------------50672FD6FE5014644E576A50
Content-Type: text/plain; charset="us-ascii"

Dear All,
                I have been trying to derive a set of pair potentails
for some small diatomic molecules
and atoms in a metal oxide lattice using DFT calculations.  The lattice
ion in each case was surrounded
by point charges to represent counter ions and the atom or molecule
placed at distances between
1 and 10 Ang from the ion and the energy of the systems were
calculated.  This has been of questionable
success.  (I know that DFT doesn't describe vdW forces very well, if at
all).

Question 1:  Has anyone else had success with these sort of
calculations?

Question 2: How does one overcome the convergence problems of
intrinsically unstable geometries?

Question 3: Can the problems of the lowering of symmetry by placing say
an atom 10 Ang away from
a ion with cubically arranged point charges cause convergence problems
and be overcome?

Any help would be appreciated.
                    Cheers,
                                    Dave


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

Dr. David W. Price,       Tel: +44 (0)118 9875123  extn 7415
Department of Chemistry,  Fax: +44 (0)118 9316331
University of Reading,    mailto:d.w.price@reading.ac.uk
Whiteknights,
READING                http://www.chem.rdg.ac.uk/g50/mmrg/dave/dave.html
RG6 6AD
U.K.

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



--------------50672FD6FE5014644E576A50
Content-Type: text/html; charset="us-ascii"

<HTML>
Dear All,
<BR>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;
I have been trying to derive a set of pair potentails for some small diatomic
molecules
<BR>and atoms in a metal oxide lattice using DFT calculations.&nbsp; The
lattice ion in each case was surrounded
<BR>by point charges to represent counter ions and the atom or molecule
placed at distances between
<BR>1 and 10 Ang from the ion and the energy of the systems were calculated.&nbsp;
This has been of questionable
<BR>success.&nbsp; (I know that DFT doesn't describe vdW forces very well,
if at all).

<P>Question 1:&nbsp; Has anyone else had success with these sort of calculations?

<P>Question 2: How does one overcome the convergence problems of intrinsically
unstable geometries?

<P>Question 3: Can the problems of the lowering of symmetry by placing
say an atom 10 Ang away from
<BR>a ion with cubically arranged point charges cause convergence problems
and be overcome?

<P>Any help would be appreciated.
<BR>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;
Cheers,
<BR>&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;
Dave
<PRE>&nbsp;
------------------------------------------------------------------------

Dr. David W. Price,&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; Tel: +44 (0)118 9875123&nbsp; extn 7415
Department of Chemistry,&nbsp; Fax: +44 (0)118 9316331
University of Reading,&nbsp;&nbsp;&nbsp; <A HREF="mailto:d.w.price@reading.ac.uk">mailto:d.w.price@reading.ac.uk</A>
Whiteknights,&nbsp;
READING&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp; <A HREF="http://www.chem.rdg.ac.uk/g50/mmrg/dave/dave.html">http://www.chem.rdg.ac.uk/g50/mmrg/dave/dave.html</A>
RG6 6AD&nbsp;
U.K.

------------------------------------------------------------------------</PRE>
&nbsp;</HTML>

--------------50672FD6FE5014644E576A50--


From ccl@www.ccl.net  Fri Mar 20 15:19:05 1998
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Date: Fri, 20 Mar 1998 14:48:14 -0500 (EST)
From: "Stephen R. Heller" <srheller@gig.usda.gov>
X-Sender: srheller@origin
To: jcicshelp <chemistry@ccl.net>, chemweb@ic.ac.uk,
        chminf-l@listserv.indiana.edu, orgchem@extreme.chem.rpi.edu
Subject: Software to review
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March 20, 1998

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 have one (1) new software product 
for review. I am looking for people who are willing to
review this software product.  In return for the
review which is published in JCICS you get to keep the software
or database.  The review should be completed in 1-3 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 six 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 23 March 1998 (Monday), as I am
sure the software will be gone by then.

     I can be reached on Internet (SRHELLER@GIG.US.GOV).

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


     Steve Heller


The package I now have is:

gNMR from Cherwell Scientific.  gNMR is a program for simulating 
1-D NMR spectra for any NMR active nucleus - in a single molecule or in 
a mixture.




Steve Heller, NIST 820 Diamond Avenue, Room 101
Gaithersburg, MD 20899 USA
Phone: 301-975-3338    FAX: 301-926-0416
E-mail:  srheller@gig.usda.gov
WWW:     www.hellers.com/~steve



From root@liposome.genebee.msu.su  Sat Mar 21 11:19:17 1998
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Date: Sat, 21 Mar 1998 19:13:26 +0300 (MSK)
From: root <root@liposome.genebee.msu.su>
To: chemistry@www.ccl.net
Subject: SUMMARY: nonmales in chemistry 
Message-ID: <Pine.LNX.3.95.980321190749.18325A-100000@liposome.genebee.msu.su>
MIME-Version: 1.0
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I thank to all who replied. Sorry for waiting so long: but at least I'm
sure to have catched all the replies. 

Regards,
Eugene Leitl, MSU, Polymer Sci. Dept.

P.S. Replies edited.

-------------------------------------------------------------------------
"Susan R. Atlas" <susie@sapphire.phys.unm.edu>:
Count me in on your 'woman computational chemist survey'.  I would
identify most strongly as a theoretical chemical physicist, but I do my
share of first-principles calculations. 
-------------------------------------------------------------------------
Anonymous (male): 
we recently solicited resumes for a computational chemistry position. 5 of
the 80 resumes received were from persons highly likely to be female.  Two
were ones where no reasonable conclusions could be drawn, and the
remainder were ones highly likely to be male.  One can rarely, however, be
certain from a resume as to a person's gender (and since that's an illegal
basis for selection, it is simply something we make a guess at in order to
satisfy some Department of Labor reporting requirements).
-------------------------------------------------------------------------
"Cicariello-Cook, Janet" <janetc@idt.net>:
On the CCL you suggested an informal poll to find out an approximate
percentage of non-males in the comp chem field. I can think of 20 women
(including myself) off the top of my head. Given some time to think
about it, and go through old conference lists, etc, I'm sure I can
increase this number. And this would just be people I've actually met.
-------------------------------------------------------------------------
"Abby L. Parrill" <parrill@argus.cem.msu.edu>:
I am one of the comp chem women on the list.  I am not offended at all by
addresses such as 'Dear Sirs', however. 
-------------------------------------------------------------------------
Don Gregory <dgregory@msi.com>:
I just did a rudimentary check down through our corp. phone list, and
there are some people I'm not familiar with, so this would be an
underestimate.  The ratio of male to female 'scientists' at MSI is roughly
16% non-male.  "MSI" today is approx. 300 people, approx.40-50% of which
are scientific in nature, so you can come up with whatever raw numbers
seem reasonable. 
-------------------------------------------------------------------------
"Lisa M. Balbes, Ph.D." <balbes@inlink.com>:
At the 1997 Gordon Conference on QSAR, there were 10-20% women.  At the
charleston conference I just left, there were closer to 30% women. 
-------------------------------------------------------------------------
Terri Soar <9610538n@Lv.Levels.Unisa.Edu.Au>:

I'm just replying to add my name to the "female CCL participant" tally as
(and am proud to admit) a female! 

My supervisor is also female and is a member of the CCL community,
(although I know that she won't bother replying to your email for the poll
as she tends to just look at the message subject headings and ditch the
ones that appear irrelevant to her work!). 

I tend not to get offended by the odd email that address it to Sirs as
these authors are most likely from countries/cultures that just haven't
caught up with equal opportunity and equal talents amongst the genders. 
-------------------------------------------------------------------------

In this context the following recent bit of information may also be of
interest: 

(from) SCIENCE-WEEK - Part 1/3

A Free Weekly Digest of the News of Science

March 20, 1998

4. WOMEN NOW SUBSTANTIAL PORTION OF ALL NEW US CHEMISTS
The latest survey of the American Chemical Society, covering
chemists and chemical engineers who graduated between July 1996
and June 1997, shows the following statistics for new women
graduates (percentage of total graduates who are women):
Chemistry Bachelor's Degree: 48.2%
Chemistry Master's Degree: 46.2%
Chemistry PhD Degree: 31.6
Chemical Engineering Bachelor's Degree: 35.4%
Chemical Engineering Master's Degree: 29.3%
Chemical Engineering PhD Degree: 22.9%
QY: Michael Heylin
mailto://edit.cen@acs.org
(Chem. & Eng. News 9 Mar 98)




From bausch@chem.vill.edu  Sat Mar 21 13:19:17 1998
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To: CHEMISTRY@www.ccl.net
From: "Joseph W. Bausch" <bausch@chem.vill.edu>
Subject: transition state problem (?)




To the CCL community:

	I am interested in locating a transition state and determining the
energetics of a degenerate process which I'll represent as A --> TS --> A'.
Using G94, I employed a QST2 calc at HF/STO-3G using A and A' HF/STO-3G
geometries (with atoms ordered properly) as input.  The method appeared to
work fine as the transition state it found looked like what I "expected",
and the relative energy is about 7 kcal/mol higher than A.  I then took
this geometry and did an OPT=TS calc at HF/3-21G and this job ran
successfully, with the relative energy being about 5 kcal higher than A.
To confirm that this transition state connected A and A', I ran an IRC calc
at 321g, and this worked.
	So, desiring to have higher level of theory data, I then did an
OPT=TS calc at HF/6-31G*, which ran successfully, this time the TS being ~4
kcal/mol higher in energy than A.  The results of the calculations I'll
describe next have me a bit confused.
	I have run OPT=TS calculations at B3LYP/6-311G* and also at
MP2/6-31G*,  and both of these calculations ran to completion.  However,
the energy of TS at B3LYP/6-311G* is ~2 kcal/mol MORE stable than A, and at
MP2/6-31G* TS is MORE stable than A by ~11 kcal/mol!  Has anybody out there
had a similar situation to this?  Can I assume that DFT and MP2 levels just
aren't very good for the energetics of transition states, or are these
results perhaps peculiar to the specific molecule I am investigating?  If
my DFT and MP2 levels of theory aren't good for this type of problem, what
level of theory is considered reliable for this type of calculation?

Cheers and TIA,
Joe
---




From lavelle@mbi.ucla.edu  Sat Mar 21 23:19:21 1998
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Date: Sat, 21 Mar 1998 20:00:22 -0800
To: chemistry@www.ccl.net, pc-help@gaussian.com
From: Laurence Lavelle <lavelle@mbi.ucla.edu>
Subject: G94W  and  2e- integral storage
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Hi,


I have some questions on integral storage, and performance benchmarks in
general. I know it is often said that answers to "benchmark" questions
are "system dependent" and the only way to make comparisons are real
tests. This however means that one has to buy the hardware and then see
"how things turn out". 

Quantitative answers or "real comparisons" will be much appreciated.


1) Does the latest version of G94W allow for more than one path for 2 e-
integral storage. That is, can they be stored on more than one hard
drive?


2) Is there a quantitative way of estimating direct SCF speed, versus
integral storage on hard drive(s)?  

That is,  knowing CPU specs like CINT95, CFP95 

(e.g., SPECint95 = 7.12, SPECfp95 = 5.21); 

and hard drive specs (e.g., two HD each with their own SCSI controller,
that have sustained data transfer of 10 MB/s) can one estimate the
relative speeds of direct SCF vs conventional? 


Bottom line: The above two HD can store 20 MB of 2e- integrals per sec
(up to a max of 2 x 9000 MB = 18000 MB). <bold>Which CPU's can
recalculate more than 20 MB of 2 e- integrals per sec to make direct SCF
faster than conventional? 

</bold>


About benchmarks in general:

1) How does one know if a software package or modules within a package
are  more dependent on integer performance or floating point performance? 

 

2) How does one compare performance numbers stated as CINT95(intensive
integer performance), CFP95 (intensive floating point performance) or
MIPS (10^6 instructions per sec)?


Much appreciated.


Laurence

<center>


""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""

Laurence Lavelle, Ph.D.

University of California Los Angeles

Molecular Biology Institute, and Department of Chemistry & Biochemistry

Laboratory of Structural Biology & Molecular Medicine

Los Angeles, CA 90095-1570, USA

 

Email:LAVELLE@MBI.UCLA.EDU

Phone (Lab): (310) 206-8270

Phone (Office): (310) 825-2083

Fax: (310) 267-1957

http://www.doe-mbi.ucla.edu/people/lavelle/lavelle.html

""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""


It will be a great day when schools have all the money they need,

and the military has bake day sales.




In nature's infinite book of secrecy

A little I can read.


</center>


From jkl@ccl.net  Sun Mar 22 22:19:33 1998
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From: Jan Labanowski <jkl@ccl.net>
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Date: Sun, 22 Mar 1998 22:09:44 -0500 (EST)
Message-Id: <199803230309.WAA25932@krakow.ccl.net>
To: chemistry@www.ccl.net
Subject: coupling vibrational relaxation to fluid flow
Cc: jkl@ccl.net


Dear Gurus,

I need help... One of our customers needs a piece of software.
The problem involves coupling vibrational relaxation effects to
fluid flow of a gas (say oxygen). Is there a piece of software which
would perform vibrational kinetics using SSH theory (or whatever which
works well enough), so it is possible to solve conservation equation for
oxygen along with the equation of motion. The conservation equation for
oxygen will have source term made up of v-t and v-v energy transfers.
They would like to model these energy transfers using the latest
modeling approaches in this field. 

If you have any pointers, I will die (hopefully not before I can relay
this information) indebted.

Your,

Jan Labanowski
jkl@ccl.net



