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Date: Sat, 22 Feb 2003 01:18:27 -0500 (EST)
From: Eric Yan <ericyan@brillouin.ccqc.uga.edu>
To: Alexandrova <Alexandrova@cc.usu.edu>
cc: chemistry@ccl.net
Subject: Re: CCL:Gaussian->MOLPRO basis transfer
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What basis sets are you looking for?
Have you tried the online basis set form from PNL?
Take a look at this site:
http://www.emsl.pnl.gov:2080/forms/basisform.html
It automatically generates basis sets for different QC packages.
Hope it helps.

 --------------------------------------------------------------------
  Eric   Yan                   | phone: 706 542-7447
  Ctr. for Comp. Quantum Chem. | fax:   706 542-0406
  University of Georgia        | e-mail: ericyan@ccqc.uga.edu
  Athens, GA  30602-2556       | http://zopyros.ccqc.uga.edu
 --------------------------------------------------------------------

On Fri, 21 Feb 2003, Alexandrova wrote:

> Hello, everybody!
> Couldn't you help me with basis sets in MOLPRO. Some basis sets for some 
> elements are missing there. Is there a posibility to take (transfer, input 
> manually?) basis set from Gaussian into the MOLPRO file? May be to make MOLPRO 
> to grab basis set from Gaussian? Do you know how to do it?
> Thank you very much in advance.
> Anastassia Alexandrova
> PhD student
> Dr. Boldyrev research group
> Dept. of Chemistry
> Utah State University
> 
> 
> 
> -= This is automatically added to each message by mailing script =-
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> 
> 
> 
> 
> 
> 


From chemistry-request@server.ccl.net Sat Feb 22 07:55:11 2003
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From: "fuyao" <fuyao@mail.ustc.edu.cn>
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Subject: Solvation energy of H2O in water in PCM model
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Hello, everybody!

I want to know what is the solvation energy of H2O in water according to PCM model in Gaussian software.Does the solvation energy equal to the vaporization energy(H2O (liquid, 298K, 1atm) ¨¤ H2O (gas,1 atm, 298K))?What is the reaction equation for the solvation energy of water (the state of every species in the equation?) which difine in Gaussian PCM model?


Thank you very much in advance.

*******************************************
Dr.Yao Fu
Department of Chemistry
University of Science & Technology of China
Hefei, Anhui 230026P. R. China
Tel:86-551-3640051(House)
86-551-3606640(Office)
Mobile:86-13855190155
Fax:86-551-3606689
E-mail: fuyao@mail.ustc.edu.cn
*******************************************



From chemistry-request@server.ccl.net Sat Feb 22 02:49:02 2003
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Date: Fri, 21 Feb 2003 23:48:43 -0800
From: "David A.  Case" <case@scripps.edu>
To: M Brunsteiner <m.brunsteiner@ucl.ac.uk>
Cc: chemistry@ccl.net
Subject: Re: CCL:system size and pressure correlations in MD
Message-ID: <20030222074843.GA2404@scripps.edu>
References: <Pine.GSO.4.05.10302191702090.17557-100000@ultra.chem.ucsb.edu> <3E54C35F.1F4D8F22@ucl.ac.uk>
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On Thu, Feb 20, 2003, M Brunsteiner wrote:
> 
> I am looking for information on pressure 
> correlations in liquds. If I did a molecular 
> dynamics simulation, how would the size of the 
> pressure fluctuations depend on the system size
> (the box-size in an MD simulation) 

The simplest place I know to look for information on this is section 114
of "Statistical Physics", by Landau and Lifshitz.  With some (seemingly
reasonable) approximations, the mean square fluctuations in pressure
are given by kT/(V*beta), where beta is the compressibility.  Hence,
roughly, the pressure fluctuations should scale as the inverse square
root of the volume.  Many moons ago, I ran some water simulations on various
box sizes, that seemed to bear this out, but you should probably check things
yourself.

..hope this helps...dac

-- 

==================================================================
David A. Case                     |  e-mail:      case@scripps.edu
Dept. of Molecular Biology, TPC15 |  fax:          +1-858-784-8896
The Scripps Research Institute    |  phone:        +1-858-784-9768
10550 N. Torrey Pines Rd.         |  home page:                   
La Jolla CA 92037  USA            |    http://www.scripps.edu/case
==================================================================



From chemistry-request@server.ccl.net Sat Feb 22 08:12:53 2003
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Hi all,

I used delphi for electrostatic calculations on my protein in vacuum 
with grid resolution 1.5 Angstrom/grid point and zero ionic strength. 
However, it always end up not finishing the job (core dumped). THis 
doesn't happen when i change the solvent dielectric to 80. Could anybody 
please suggest what can be done about it? I know a finer grid resolution 
will produce more accurate results but how fine should the grid 
resolution be? With the crashes, I had to run mine with 2.5 
Angstrom/grid point for both vacuum and water.

Any help would be much appreciated.

Thank you.

Rowyna Kueh
Postgraduate student
Universiti Malaya



From chemistry-request@server.ccl.net Sat Feb 22 04:42:17 2003
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Subject: Summer School in Density Functional Theory
From: Jussi Eloranta <eloranta@jyu.fi>
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Dear ccl-net members,

The 13th Jyv=C3=A4skyl=C3=A4 Summer School (August 11th - 29th 2003) has =
one week
(Aug 11 thru 15) dedicated for density functional theory. The general=20
course
outline is as follows (PDF file as attachment):

Density Functional Theory (CH1)

Time: 30 hours during 11 - 15 Aug 2003
Location: University of Jyv=C3=A4skyl=C3=A4, Jyv=C3=A4skyl=C3=A4, =
Finland.
Lecturers: Prof. Jesus Navarro (CSIC - University of Valencia, Spain)
                  Prof. John Perdew (Tulane University, New Orleans, =
USA)
Course content: Density functional theory of quantum liquids and=20
electronic systems
Course credits: ECTS 10 cr (equivalent to 5 study weeks in Finland)
Registration: http://www.jyu.fi/summerschool
Contacts: Jussi Eloranta (eloranta@jyu.fi) and Juha Ruuska=20
(jss@cc.jyu.fi)

Abstract

Electronic systems (about 15 hours including discussion and=20
demonstrations):

1. Introduction to density functional theory
2. Wavefunction theory
3. Definitions of density functionals
4. Formal properties of functionals
5. Uniform electron gas
6. Local and semi-local approximations
7. Hybrid functionals and hyper-GGA=D0=A5s
8. Optimized effective potential
9. Test and applications of functionals

Quantum liquids (about 15 hours including discussion and=20
demonstrations):

1. The physics of liquid helium
2. Density functional theory and strongly interacting systems
3. Density functional theory for bosons: 4He systems
4. Density functional theory for fermions: 3He systems
5. Mixed statistics 4He - 3He systems

Additional homework and related reading will be distributed during the=20=

lectures.


Jussi Eloranta

Jussi Eloranta (eloranta@jyu.fi)
Professor of Chemistry
University of Jyv=C3=A4skyl=C3=A4




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Dear ccl-net members,


The 13th Jyv=C3=A4skyl=C3=A4 Summer School (August 11th - 29th 2003) has =
one week

(Aug 11 thru 15) dedicated for density functional theory. The general
course

outline is as follows (PDF file as attachment):


<fontfamily><param>Times</param>Density Functional Theory (CH1)


Time: 30 hours during 11
</fontfamily><fontfamily><param>Lucida =
Grande</param>-</fontfamily><fontfamily><param>Times</param>
15 Aug 2003

Location: University of Jyv=C3=A4skyl=C3=A4, Jyv=C3=A4skyl=C3=A4, =
Finland.

Lecturers: Prof. Jesus Navarro (CSIC - University of Valencia, Spain)

                 Prof. John Perdew (Tulane University, New Orleans,
USA)

Course content: Density functional theory of quantum liquids and
electronic systems

Course credits: ECTS 10 cr (equivalent to 5 study weeks in Finland)

Registration:
=
<underline><color><param>1998,1998,FFFE</param>http://www.jyu.fi/summersch=
ool</color></underline><color><param>0000,0000,FFFD</param>

</color>Contacts: Jussi Eloranta
=
(<underline><color><param>1998,1998,FFFE</param>eloranta@jyu.fi</color></u=
nderline>)
and Juha Ruuska
=
(<underline><color><param>1998,1998,FFFE</param>jss@cc.jyu.fi</color></und=
erline>)


Abstract


Electronic systems (about 15 hours including discussion and
demonstrations):


1. Introduction to density functional theory

2. Wavefunction theory

3. Definitions of density functionals

4. Formal properties of functionals

5. Uniform electron gas

6. Local and semi-local approximations

7. Hybrid functionals and
hyper-GGA</fontfamily><fontfamily><param>Lucida =
Grande</param>=D0=A5</fontfamily><fontfamily><param>Times</param>s

8. Optimized effective potential

9. Test and applications of functionals


Quantum liquids (about 15 hours including discussion and
demonstrations):


1. The physics of liquid helium

2. Density functional theory and strongly interacting systems

3. Density functional theory for bosons: 4He systems

4. Density functional theory for fermions: 3He systems

5. Mixed statistics 4He
</fontfamily><fontfamily><param>Lucida =
Grande</param>-</fontfamily><fontfamily><param>Times</param>
3He systems


Additional homework and related reading will be distributed during the
lectures.</fontfamily>



Jussi Eloranta


Jussi Eloranta
=
(<underline><color><param>1998,1998,FFFE</param>eloranta@jyu.fi</color></u=
nderline>)

Professor of Chemistry

University of Jyv=C3=A4skyl=C3=A4





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From jkl@ccl.net Sat Feb 22 14:09:13 2003 -0500
Return-Path: <orlov_yury@yahoo.com>
Message-ID: <20030222190911.2645.qmail@web13208.mail.yahoo.com>
Received: from [129.70.136.201] by web13208.mail.yahoo.com via HTTP; Sat, 22 Feb 2003 11:09:11 PST
Date: Sat, 22 Feb 2003 11:09:11 -0800 (PST)
From: Orlov Yury <orlov_yury@yahoo.com>
Subject: 03.08.04 Symp. Integrative Bioinformatics - 2003, Bielefeld, Germany 
To: chemistry@ccl.net

Symposium
Integrative Bioinformatics 

Bielefeld, Germany, August 4th - 5th, 2003   

http://cweb.uni-bielefeld.de/agbi/home/index.html?id=142

Molecular biology produces huge amounts of data in the
post-genomic era. Among them, there is data describing
metabolic mechanisms and pathways, structural genomic
organization, patterns of regulatory regions;
proteomics, transcriptomics, and metabolomics data. On
one hand, analysis of these data is determined
essentially by the methods and concepts of computer
science; on the other hand, it depends on a range of
biological tasks solved by researchers. Currently,
there are about 400 database informational systems and
various analytical tools available via the Internet
and directed at solving various biological tasks. The
challenge we have is to integrate these list-parts
> from genomics and proteomics at novel levels of
understanding. Integrative Bioinformatics would be
this new area of research using the tools of computer
science and electronic infrastructure applied to
Biotechnology. These tools will also represent the
backbone of the concept of virtual cell. 
This symposium addresses primarily the scientists
working in this emerging field of Integrative
Bioinformatics and, hence, would discuss the
corresponding problems and present concepts. Besides
invited talks, we would like to invite all researchers
interested in these problems and active participation
in this symposium. The number of participants will be
restricted. 

Topics 
·	Molecular Databases/ Information Systems 
·	Database Integration 
·	Metabolic Network Control 
·	Metabolic Engineering 
·	Metabolic and Regulatory Networks 
·	Metabolic and Regulatory Network Modeling 

Deadlines 
Extended Abstracts - April 15th 
Notification of authors - June 1st 
Registration - June 15th

Organization Committee
R. Hofestaedt (University Bielefeld)
N. Kolchanov (Russian Academy of Science, Novosibirsk)
T. Dandekar (University Wuerzburg)  

Contact
Prof. Dr. Ralf Hofestaedt 
Bielefeld University 
Bioinformatics Department
Universitätsstrasse 25
D-33615 Bielefeld
E-Mail: bio-workshop@techfak.uni-bielefeld.de 

Organization

Bielefeld University,
IMBIO e.V. and
DFG-Schwerpunkt Informatikmethoden
zur Analyse und Interpretation grosser
genomischer Datenmengen

http://cweb.uni-bielefeld.de/agbi/home/index.html?id=142



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