From chemistry-request@server.ccl.net Tue Oct  9 00:33:03 2001
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To: CHEMISTRY@ccl.net
Subject: CCL: ADSORPTIVE INTERACTION
Date: Tue, 9 Oct 2001 06:45:10 +0200 
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Dear CCLers:
I am writing this mail on behalf of my collegue. She needs to perform
calculations on 
ADSORPTIVE INTERACTIONS by Frontier Orbital Theory. She needs to perform
HOMO and LUMO
energy and orbital coefficients. Using MOPAC interfaced in InsightII, she
gets the HOMO
and LUMO energies but not the orbital coefficients. Could you please tell us
how to get the
orbital coefficients in the calculation. Thanks in advance.
	-parthi

From chemistry-request@server.ccl.net Tue Oct  9 08:26:10 2001
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From: "TELKUNI" <telkuni@venus.dti.ne.jp>
To: <chemistry@ccl.net>
Subject: PW91 calculation trouble of Gaussian98W
Date: Tue, 9 Oct 2001 21:18:47 +0900
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Hello! CCLers,

I'm trying to do DFT calculation with Gaussian98W (Version-5.2, Rev-A.7).
I have serious problems.

My purpose is to optimize the SiH4 structure (It is similar to methane.) with 
PW91 (Pardew and Wang 91) using my PC (Memory=256MB, OS=Win98SE,
CPU=Celeron 400MHz). 

When I set the Job File as follows ( "***... " means the input form):

   --- ---  Job File --- ---   

    % " %chk=SiH4.chk "

    Route " # PW91PW91/6-31G Opt "

    Title Section " SiH4 "

    Charge , " 0 1 "

    - Molecule (Structure) -
    Si  
    H     1   r21        
    H     1   r31           2   a312       
    H     1   r41           2   a412          3   d4123         0
    H     1   r51           2   a512          3   d5123         0
 
     r21            1.460856
     r31            1.460848
     r41            1.460839
     r51            1.460818
     a312         109.476160
     a412         109.474287
     a512         109.469184
    d4123       -120.012518
    d5123        119.993483
  ---   ---   ---   ---   ---   ---   ---   

 I always get following message:

     Run Progress: Link died!
 
    "Severe Error Message # 2070   
     The processing of the last link ended abnormally. 
     All processing has been aborted."


  And it always ends with:

    Default route:  MaxDisk=2000MB
    ------------------------------------
    #T SVWN/6-31G(d) Test SCF=(Tight,QC)
    ------------------------------------


I can't understand what the message means and don't know the clue of 
the solution. If anyone know the reason or solution, please teach me.

All responses, I will appreciate. And I will summarize them for novice Gaussian98 
user, just like me!


  Thanks in advance,


----------------------------------------------
               Telkuni Tsuru     

  Kyushyu Electronic Technology and Research

          telkuni@venus.dti.ne.jp
----------------------------------------------



From chemistry-request@server.ccl.net Mon Oct  8 21:40:16 2001
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Date: Tue, 9 Oct 2001 9:41:49 +0800
From: Denny <dilys98@mails.tsinghua.edu.cn>
To: Zhenhua Li <lbbg123@etang.com>
CC: "chemistry@ccl.net" <chemistry@ccl.net>
Subject: Re: CCL:exact energy of atoms or small poly-atoms
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aug-cc-pv6z

****************************
* Denny Chen		   *
* Center for Astrophysics  *
* Tsinghua University	   *
* Beijing, P.R.China       *
* 8610-62792126(phone)     *
* 8610-62792125(fax)       *
****************************
Email:dilys98@mails.tsinghua.edu.cn

********You wrote*********
>Dear listers,
>Have you any idea how to find energies of exact or close to 
exact (either
>SCF or correlation level) one-particle basis set limit for 
atoms or small
>poly-atoms?
>Are there any exact energies of atoms or small poly-atoms 
(exact solution of
>Schrodinger equation)?
>
>Li Zhenhua
>
>
>
>
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Jan: jkl@ccl.net



From chemistry-request@server.ccl.net Tue Oct  9 06:02:14 2001
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From: VITORGE Pierre 094605 <vitorge@azurite.cea.fr>
To: "'elewars'" <elewars@trentu.ca>, chemistry@ccl.net
Subject: RE: charges on sphere, summary
Date: Tue, 9 Oct 2001 11:46:51 +0200 
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I am only a chemist; but most of the answers do not convince me from a
mathematical point of view: show the answer to math specialists before
writting on the list!
I am not convince when you (explicitly or implicitly) add the last charge to
the n-1 previous ones, just because geometries can be very different in the
n and n-1 cases.
It is neither a simple mathematical problem to put small spheres on a big
one.

Pierre Vitorge
CEA Saclay
DEN/DPC/SCPA/LCRE Bat.450 pce 157D
UMR 8587 (Universite d'Evry-CNRS-CEA)
91191 Gif sur Yvette cedex
France
pierre.vitorge@cea.fr
phone +33 169-08-32-65,
secretary: +33 169-08-32-50, 
fax: +33 169-08-32-42
http://perso.club-internet.fr/vitorgen/pierre/pierre.html
pierre.vitorge@laposte.net


-----Message d'origine-----
De: elewars [mailto:elewars@trentu.ca]
Date: lundi 8 octobre 2001 16:06
À: chemistry@ccl.net
Objet: CCL:charges on sphere, summary


2001 Oct 8

Hello,

Here is the summary of replies I got to the question about the energy of

a set of charges confined on/in a sphere.
I thank all who responded, and hope I have not overlooked any reply. All

the answers were intereresting and helpful.

E. Lewars
===
The question:

2001 Oct 3

Hello,

A colleague posed this question.
Suppose you have two like point charges (e.g. two protons, considered
dimensionless), which must be on or inside a sphere. The minimum energy
geometry (MEG) is that they be on the surface, at the ends of a diameter

of the sphere. For three charges, the MEG is on the surface, at the
corners of an equilateral triangle. And so on for 4, 5, ...? charges,
the MEG having all of them on the surface.
Question: is there a number or numbers _n_ of charges for which
migration of one or more charges _into_ the sphere would lower the
energy? Is there some theorem in math or physics that deals with this?

Thanks

E. Lewars
=============
#1
Prof. Lewars,

I enjoy this type of problem.  I know it is a theorem that there
is no arrangement of (pos and neg) charges in space that is
a local minimum.  I suspect that the same is true of charges
in an environment where there are some fixed charges about,
which would mean that the charges in the interior can always
move in some direction so as to lower the total energy.
Then the MEG would have to have all charges on the surface.

David Anick MD PhD
David.Anick@gte.net

Dear Prof. Lewars,

Ignore previous response.   The proof is easy.
Suppose you have n point charges in fixed positions
and you want to add the (n+1)st.  Let F be
the electric field generated by the original n.
Then div(F) = 0 (Gauss's law).  The divergence
theorem says that the surface integral of F<dot>n^
over a small bubble enclosing the new charge,
equals the volume integral of div(F), which we
know is zero.  Make the bubble very small.
F<dot>n^ is positive in some direction(s) and
negative in others. If the position of the new charge
were a local min, F would point inward everywhere on
the bubble, i.e. F<dot>n^ would be negative on
the entire bubble surface.  This contradiction shows
that there cannot be any local min for the energy
as a function of the position of the new charge (with
the other n positions fixed), except on the boundary.
Once that charge moves to the boundary, the others
may lower the energy further by moving around on
the boundary, but that's not your question.
NOTE: there can be saddle points for the potential
energy in the interior, i.e. an interior charge might
experience a force of zero, but they would be
unstable stationary points.  In the limit where there
are thousands of charges spread out on the surface
in a uniform distribution, as you know, the potential
inside becomes constant.

David Anick MD PhD
David.Anick@gte,net
==============
#2
Use the variational procedure to maximize the
distance between points with the constraint that they lie on a
sphere of radius R.  The constraint is a lagrange multiplier
and you simply work though the Ritz variational method.

Alternatively, argue from simple geometry. In two dimensions, if you
have a n-point polygon with all points on a circle of radius R, then the

configuration which maximizes the distance (and hence minimizes the
energy or cost function)  between all points is a regular polygon.  So,
again,
it's a result of the  variational theorem.

ERB

--
Prof. Eric R. Bittner
Department of Chemistry
Univ. of Houston
ph:  713-743-2775    fax: 713-743-2709
bittner@uh.edu
http://k2.chem.uh.edu/bittner/


Actually, I didn't read your question carefully enough, but you could
still use the variational method
followed by classical perturbation theory to check this.
But, geometry seems to argue that if you have  n points distributed
evenly over a sphere
at the vertices of a regular polyhedron, the lowest energy
configuration for the addition of one charge *inside* the sphere is at
the center.
The issue of whether perturbing one vertex of the polyhedron keeping the

rest fixed
is simple as well.  From the point of view of the one charge being
deflected, moving closer to
any of the (n-1) charges must increase its potential energy. So the
minimal energy configuration
for the deflected charge is at r-> + infinity. This must be true for all

n> 1.


--
Prof. Eric R. Bittner
Department of Chemistry
Univ. of Houston
ph:  713-743-2775    fax: 713-743-2709
bittner@uh.edu
http://k2.chem.uh.edu/bittner/
----------------------------------------------------------------------------
---------------

The sun, with all those planets revolving around it and dependent upon
it,
can still ripen a bunch of grapes as if it had nothing else in the
universe
to do. -Galileo Galilei, physicist and astronomer (1564-1642)
=================
#3
Dear Prof. Lewars,

I can't cite any theorems with respect to your
colleague's question. However, since same-charge
repulsion diminishes with the square of the distance,
a good rule of thumb would be to make the smallest
distance between charges as large as possible.
This is related to the question of how many spheres
of a given radius can be fitted into a sphere of unit-
radius. The topic of densest packing might be a
good starting point for searching the mathematical
literature. Borane or metal clusters might also provide
examples. Since the boundary conditions are different
(no penetration of packed spheres vs. minimum
repulsive energy), the packing problem is probably
not the definitive answer but still a good starting point.

>From a more practical point of view, I think that
charges inside the sphere become competitive when
the smallest distance d between charges on the surface
of the sphere is smaller than the radius of the sphere.
In a regular octahedron, d=sqrt(2)*r. In a cube,
d=2r/sqrt(3). In a 4-sided antiprism the ratio d/r would
be somewhat smaller (but still larger than 1, I believe).
Therefore my guess is that with 8 charges one should
be inside the sphere. The other 7 charges might be
in an arrangement derived from a capped octahedron.

Yours,
     Stefan Fau
______________________________________________________________________
Dr. Stefan Fau                    |      fau@qtp.ufl.edu
Quantum Theory Project     |     (352) 392-6714
University of Florida
Gainesville, FL 32611-8435
===============
#4

 Just a quick comment which I think shows that at some
point you will want to put charge inside the sphere:
if you consider a uniform charge density smeared over
the sphere surface (approximating the situation where
there are already many protons), the energy to add
a new charge q on the surface comes out (in my hands)
as 8 pi q sigma while the energy to put it at the
center of the sphere is 4 pi q sigma, ie it is smaller.

If you find a sophisticated exact result I'd be interested
to hear about it...

Cheers,simonson@schlitz.u-strasbg.fr
 Organization: CNRS

Tom Simonson
==========
#5
Dear Dr. Lewars !

If the charges are mobile within the sphere they will always accumulate
on the
surface - that's just Faraday's principle. If you have a charged piece
of metal
(i.e. "real life" equivalent of a system in which charges are freely
mobile
within a certain volume) any addiditonal charges will always accumulate
on the
surface (that's actually independent of the shape of the piece of metal.

regards,

egbert

Egbert Zojer <egbert.zojer@tugraz.at>

===================
=============





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From chemistry-request@server.ccl.net Tue Oct  9 10:14:48 2001
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  Tue, 9 Oct 2001 16:14:46 +0200
Subject: TDDFT - MO's
To: CHEMISTRY@ccl.net
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Dear CCLers,

TDDFT (at least Gaussian outputs) give information on transition energy,
oscillator strengths, and the
MO's envolved in the respective transition.

  Excitation energies and oscillator strengths:

  Excited State   1:   Singlet-B1     8.0068 eV  154.85 nm  f=0.0142
       3 -> 14        -0.01126
       5 ->  6         0.69120
       5 -> 11         0.01351

with the coefficients defining only the alpha electron. The question now is:

There is a lot of discussion if the basis set (which even in HF theory is only a
model for the real AO's), which
represents the real electron density of the whole state, can be used for
interpretation as MO's. It seems to be
accepted, that these auxiliary functions usually are able to represent the
frontier orbitals reasonably well. But
can we then really interpret these orbitals as the ones from and to which
electrons are excited? Is this model
stable and can it be interpreted photochemically?
I am not aware of any publication dealing with this.

Best regards

Andreas Goeller

P.S.: I will summarize the results.



From chemistry-request@server.ccl.net Tue Oct  9 11:48:01 2001
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Date: Tue, 09 Oct 2001 11:48:03 -0400
From: David Smith <Hunter3@mindless.com>
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Hello all,

I have recently compiled Autodock under redhat6.0 and the compilation
went well except for a few warnings which didn't seem to be to bad.  I
followed the instruction according to an online instruction document on
compiling this software on redhat and everything went good, and most of
the programs work in the suit.

However, the primary program autodock3 when run, after 5-10 seconds I
get back an error:

"Segmentation fault (core dump)"

with no output or further error messages.  So I don't even know were to
start with this problem.  I've repeated the process with the software
included examples and I get the same error, so I believe this may be do
to a faulty compilation.

Has anyone out there experience this kind of problem (under linux 2) or
does any one have any info that might be helpful to solving this
problem?

Thanks for everyone's comments.

David Smith

From chemistry-request@server.ccl.net Tue Oct  9 11:25:25 2001
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External fields are introduced into the Hamiltonian by the substitutions

	p -->  p-qA  ;  H -> H +q(phi)

This is referred to as minimal coupling or, more formally, as the
principle
of minimal electromagnetic coupling and ensures gauge invariance of the 
resulting Hamiltonian. My questions is: Who introduced this principle ?
I have been looking in a number of standard books ranging from 
classical electromagnetic theory to QED without finding such historical
references and a general discussion of the principle.
   All the best,
      Trond Saue
-- 
Trond SAUE                                (DIRAC:
http://dirac.chem.sdu.dk/)
Laboratoire de Chimie Quantique et Modélisation Moléculaire
Université Louis Pasteur ; 4, rue Blaise Pascal ; F-67000 STRASBOURG
tél: 03 90 24 13 01   fax: 03 90 24 15 89   email:
saue@quantix.u-strasbg.fr


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SimBioSys Inc. is pleased to announce CLiDE and CLiDE Lite v 2.0

CLiDE, an acronym for Chemical Literature Data Extraction, is a document image
processing software, which extracts content of printed chemistry documents. The
aim of CLiDE is to process whole pages from scanned chemical documents and to
extract the maximum amount of information from both the text and the graphic regions.

CLiDE is a chemistry intelligent equivalent of an OCR software. Just as an OCR can
recognize characters from a scanned images of a printed text, CLiDE can recognize
structures, reactions and text from scanned images of printed chemistry literature.

FEATURES & BENEFITS
-    Extracts chemical structure and text information from printed/scanned pages and
stores the information in various forms (e.g. MOL file, ChemDraw).
-    CLiDE also extracts reaction information.  Reaction information can be entered into
databases automatically. Saves hours of redrawing.
-    Extracts generic structure information from graphics and text.  CLiDE will expand
condensed generic structures so they can be entered into your DB either  expanded or
condensed.
-    CLiDE recognizes and extracts page layout information.  Bibliographical information
(e.g. title, author etc.) is conveniently extracted automatically thus  saving time cataloging
and organizing your DB.

AVAILABILITY
CLiDE v2.0 is primarily available on MS Windows 2000/NT 4.0/Me/98/95 platforms.
CLiDE Lite is also available from: SciStore: http://chemstore.cambridgesoft.com/software/product.cfm?pid=269

Further information regarding CLiDE and CLiDE Lite can be found at http://www.simbiosys.ca/
--
Aniko Simon Ph.D.
aniko@simbiosys.ca



From chemistry-request@server.ccl.net Tue Oct  9 10:07:38 2001
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From: "tianxiao young" <txyoung@hotmail.com>
To: chemistry@ccl.net
Cc: chemistry-request@server.ccl.net
Subject: potential developement
Date: Tue, 09 Oct 2001 14:07:32 +0000
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Hello,

I am using AMBER to calculate the hydration of thorium. Firstly I calculate 
the potential of Th(IV)-H2O using quantum mechanical method. My question is 
how to use this potential line to get the force field of AMBER, such as the 
bond constant, the angle constant and the dihedral angle constant? I can not 
find my answer in the AMBER manaul. I am new to AMBER, would you please help 
me out? Do you know any good references on force field developement? Your 
kind help is most appreciated.

Best wishes,

young

_________________________________________________________________
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From chemistry-request@server.ccl.net Tue Oct  9 12:36:58 2001
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From: Szilveszter Juhos <szilva@ribotargets.com>
To: David Smith <Hunter3@mindless.com>
cc: CCL <chemistry@ccl.net>
Subject: Re: CCL:Running Autodock3 under linux2
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On Tue, 9 Oct 2001, David Smith wrote:
> "Segmentation fault (core dump)"

You can find strace/ltrace useful or if you have a debugger like gdb (that
is always comes with Linux) you can try:

gdb <program_that_generated_the_core> core 
[ ..lot of info written... ]

(gdb) where
[ ..this will give you a backtrace.. ]

If you are lucky that can give a clue what went wrong.
In the strace output you can check for permission/open errors first.

Szilva


From chemistry-request@server.ccl.net Tue Oct  9 12:57:27 2001
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To: David Smith <Hunter3@mindless.com>
Cc: CHEMISTRY@ccl.net
From: ranjan@iitk.ac.in
Subject: Re: CCL:Running Autodock3 under linux2
Date: Tue, 9 Oct 2001 16:32:26 GMT
X-Mailer: Endymion MailMan Standard Edition v3.0.35


Hi David,
It seems to be a general problem for linux users.
Actually the problem is with smaller stack size in linux.So set the stack size 
to a larger size.
type in the shell:
ulimit -s 66666
the value is essentially any thing you like ( i.e of the order of 60 MB here)
Thr default for linux is 8MB. Keep increasing the stack size till it does not 
give core dump.
It should help..

Chinmoy Ranjan,
I.I.T Kanpur
India.

 Hello all,
> 
> I have recently compiled Autodock under redhat6.0 and the compilation
> went well except for a few warnings which didn't seem to be to bad.  I
> followed the instruction according to an online instruction document on
> compiling this software on redhat and everything went good, and most of
> the programs work in the suit.
> 
> However, the primary program autodock3 when run, after 5-10 seconds I
> get back an error:
> 
> "Segmentation fault (core dump)"
> 
> with no output or further error messages.  So I don't even know were to
> start with this problem.  I've repeated the process with the software
> included examples and I get the same error, so I believe this may be do
> to a faulty compilation.
> 
> Has anyone out there experience this kind of problem (under linux 2) or
> does any one have any info that might be helpful to solving this
> problem?
> 
> Thanks for everyone's comments.
> 
> David Smith
> 
> -= This is automatically added to each message by mailing script =-
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> 
> 
> 
> 




From chemistry-request@server.ccl.net Tue Oct  9 13:49:56 2001
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Date: Tue, 09 Oct 2001 19:44:53 +0200
To: David Smith <Hunter3@mindless.com>
From: Xiao-Ping Zhang <zhang@dbb.su.se>
Subject: Re: CCL:Running Autodock3 under linux2
Cc: chemistry@ccl.net
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Hi, David,

You may check the stack size of your machine. Try to set it as unlimited.

Good luck!

Xiao-Ping Zhang

At 11:48 AM 10/9/01 -0400, you wrote:
>Hello all,
>
>I have recently compiled Autodock under redhat6.0 and the compilation
>went well except for a few warnings which didn't seem to be to bad.  I
>followed the instruction according to an online instruction document on
>compiling this software on redhat and everything went good, and most of
>the programs work in the suit.
>
>However, the primary program autodock3 when run, after 5-10 seconds I
>get back an error:
>
>"Segmentation fault (core dump)"
>
>with no output or further error messages.  So I don't even know were to
>start with this problem.  I've repeated the process with the software
>included examples and I get the same error, so I believe this may be do
>to a faulty compilation.
>
>Has anyone out there experience this kind of problem (under linux 2) or
>does any one have any info that might be helpful to solving this
>problem?
>
>Thanks for everyone's comments.
>
>David Smith
>
>-= This is automatically added to each message by mailing script =-
>CHEMISTRY@ccl.net -- To Everybody  | CHEMISTRY-REQUEST@ccl.net -- To Admins
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>Ftp: ftp.ccl.net  |  WWW: http://www.ccl.net/chemistry/   | Jan: jkl@ccl.net

------------------------------------------------
Xiao-Ping Zhang
Department of Biochemistry and Biophysics
Arrhenius Laboratories of Natural Sciences
Stockholm University
106 91 Stockholm
Sweden

Phone: +46-(0)8-162472 (O); +46-(0)8-6121936 (H)
Fax:     46-08-153679
e-mail: zhang@dbb.su.se




From chemistry-request@server.ccl.net Tue Oct  9 16:05:38 2001
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Date: Tue, 9 Oct 2001 22:05:37 +0200 (CEST)
From: =?iso-8859-1?q?y=20tantirungrotechai?= <yt203y@yahoo.de>
Subject: Visualize NMR tensors with gaussview?
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Dear All, 

I have tried to repeat the calculation given at the 
http://www.gaussian.com/show/nmrvisgv001.htm but not
succeeded. Basically it's a gaussian run with nmr
keyword on ethane, ethylene and ethyne. Everything
runs smoothly (I have accessed to Gaussian 98 Rev.A7)
until I tried to format the checkpoint. In contrast to
the example file given at the URL address, there is no
information on the current density in my formatted
checkpoint. So I wonder how one could view NMR tensors
according to that webpage?  Or is it just happen that
there's something wrong in that part of Rev A7 (the
example output file is produced by the development
version)?

Any suggestions would be appreciated. 

Best regards,
Yuthana Tantirungrotechai







__________________________________________________________________

Es ist soweit: das Nokia Game beginnt. Sei bereit für das multimediale Abenteuer. Melde dich bis zum 3. November bei http://de.promotions.yahoo.com/info/nokiagame an!


From chemistry-request@server.ccl.net Tue Oct  9 20:48:02 2001
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Date: Tue, 09 Oct 2001 17:51:07 -0700
To: CCL <chemistry@ccl.net>
From: Laurence Lavelle <lavelle@mbi.ucla.edu>
Subject: Summary: Average DNA-Protein binding (free) energy
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Here is the summary. Two responses.


>Sender: chandra@ysbl.york.ac.uk
>Date: Thu, 04 Oct 2001 09:58:13 +0100
>From: Chandra Verma <chandra@ysbl.york.ac.uk>
>Organization: York Structural Biology Laboratory
>X-Mailer: Mozilla 4.7C-SGI [en] (X11; I; IRIX 6.5 IP22)
>X-Accept-Language: en
>To: Laurence Lavelle <lavelle@mbi.ucla.edu>
>Subject: Re: CCL:Average DNA-Protein binding (free) energy
>
>Hi
>
>Look up the work of L. Nilsson



>Date: Tue, 9 Oct 2001 13:07:53 -0400 (EDT)
>From: Nai-Yuan Chang <nch@MIT.EDU>
>To: <lavelle@mbi.ucla.edu>
>Subject: Re: Average DNA-Protein binding (free) energy
>
>
>Hi,
>
>   You may find these 2 references helpful:
>1. Acc. Chem. Res. 2000, 33, 889-897
>2. Curr. Opin. in Struct. Bio. 2000, 10, 311-317
>
>Regards,
>Nai-yuan
>
>=========================================================================
>Date: Wed, 03 Oct 2001 15:40:34 -0700
>To: CCL <chemistry@ccl.net>
>From: Laurence Lavelle <lavelle@mbi.ucla.edu>
>Subject: Average DNA-Protein binding (free) energy
>Mime-Version: 1.0
>Content-Type: text/plain; charset="us-ascii"; format=flowed
>
>I am looking for a (review ?) paper discussing DNA-protein binding
>energies.
>
>That is, experimental and calculated average delta G values (per DNA base
>pair) for:
>
>   DNA  +   Protein   <----->   DNA-Protein
>
>
>Comments and/or literature pointers. Appreciated.
>
>Laurence Lavelle


From chemistry-request@server.ccl.net Tue Oct  9 22:51:27 2001
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Date: Tue, 09 Oct 2001 22:50:15 -0400
From: David Smith <Hunter3@mindless.com>
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To: ranjan@iitk.ac.in
CC: CHEMISTRY@ccl.net
Subject: Re: CCL:Running Autodock3 under linux2
References: <200110091643.WAA12474@qasid.cc.iitk.ac.in>
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Hey there,

Thanks for your suggestion,  setting my stack size to unlimited got me
past the segmentation fault problem but I ended up with another.  Now
I'm getting another error:

"Floating Point exception (core dumped)"

Any Ideas???

Thanks to all,

David Smith

ranjan@iitk.ac.in wrote:
> 
> Hi David,
> It seems to be a general problem for linux users.
> Actually the problem is with smaller stack size in linux.So set the stack size
> to a larger size.
> type in the shell:
> ulimit -s 66666
> the value is essentially any thing you like ( i.e of the order of 60 MB here)
> Thr default for linux is 8MB. Keep increasing the stack size till it does not
> give core dump.
> It should help..
> 
> Chinmoy Ranjan,
> I.I.T Kanpur
> India.
> 
>  Hello all,
> >
> > I have recently compiled Autodock under redhat6.0 and the compilation
> > went well except for a few warnings which didn't seem to be to bad.  I
> > followed the instruction according to an online instruction document on
> > compiling this software on redhat and everything went good, and most of
> > the programs work in the suit.
> >
> > However, the primary program autodock3 when run, after 5-10 seconds I
> > get back an error:
> >
> > "Segmentation fault (core dump)"
> >
> > with no output or further error messages.  So I don't even know were to
> > start with this problem.  I've repeated the process with the software
> > included examples and I get the same error, so I believe this may be do
> > to a faulty compilation.
> >
> > Has anyone out there experience this kind of problem (under linux 2) or
> > does any one have any info that might be helpful to solving this
> > problem?
> >
> > Thanks for everyone's comments.
> >
> > David Smith
> >
> >
> >
> >
> >
> 
> -= This is automatically added to each message by mailing script =-
> CHEMISTRY@ccl.net -- To Everybody  | CHEMISTRY-REQUEST@ccl.net -- To Admins
> MAILSERV@ccl.net -- HELP CHEMISTRY or HELP SEARCH
> CHEMISTRY-SEARCH@ccl.net -- archive search    |    Gopher: gopher.ccl.net 70
> Ftp: ftp.ccl.net  |  WWW: http://www.ccl.net/chemistry/   | Jan: jkl@ccl.net

