From chemistry-request@server.ccl.net Mon Mar 25 01:42:06 2002
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From: Christian.Pilger@bc.boehringer-ingelheim.com
To: meenatul@bom2.vsnl.net.in
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Subject: AW: Histidine
Date: Mon, 25 Mar 2002 07:41:56 +0100
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Dear Meena,

the way I do this is to inspect each HIS residue manually and have a look on
the surrounding amino acids in terms of ionization state and hydrogen bond
donor/acceptor capabilities. In many cases you get a good hint about where
to put the proton, especially if you have a GLU or an ASP in hydrogen
bonding distance, there is a good chance, that the HIS will form a salt
bridge, hence it carries protons on both nitrogens. In analogy you can make
a decision to put the proton on N(delta) or N(epsilon) depending on the
closeness of HB donors/acceptors. In cases, where I can not make a clear
estimate, I arbitrarily put the proton on N(delta).

Cheers,

Christian
________________________________________________________________

   Dr. Christian Pilger
   Dept. Chemical Research / Structural Research
   K91-00-10
   Boehringer Ingelheim Pharma KG
   D-88397 Biberach/Germany
   Phone: 07351-545749
   Fax:     07351-5497924
   mailto: christian.pilger@bc.boehringer-ingelheim.com


From chemistry-request@server.ccl.net Mon Mar 25 03:06:34 2002
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From: "Shapiro, Stuart {Basi~Basel}" <STUART.SHAPIRO@Roche.COM>
Subject: ?s re variables in Stokes-Einstein eqn.
To: "'chemistry@ccl.net'" <chemistry@ccl.net>
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Dear Colleagues,

	In the Stokes-Einstein equation for the diffusion coefficient for spherical molecules, is the radius of the molecule under consideration taken to be the hydrodynamic radius, the radius of gyration, or some other kind of radius?  Also, in this equation is the viscosity taken to be the shear viscosity, intrinsic viscosity, kinematic viscosity, or some other kind of viscosity?

	Along the same lines, if you measure the viscosity of a solution using a Ubbeholde capillary viscometer, are you measuring the kinematic viscosity, the shear viscosity, the relative viscosity, or some other kind of viscosity?

	Kind address responses to me _directly_ at

stuart.shapiro@basileapharma.com

Thanks in advance to all responders,

S. Shapiro
stuart.shapiro@basileapharma.com


From chemistry-request@server.ccl.net Mon Mar 25 04:28:30 2002
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Date: Mon, 25 Mar 2002 10:28:13 -0800
From: Stefano Forli <forli@unisi.it>
Subject: QSAR equations
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Dear list,
I'm working on a pseudoreceptor model, using the PrGen software.
I'm writing to ask about QSAR equations, in particular, about the
physical meaning of the slope value.
It's well to obtain a good correlation with a big value of slope, or
not?
What is the optimal value?
Thanks

Stefano



-- 

***********************************
 Forli Stefano                    
 Dip. Farmaco Chimico Tecnologico  
 Universita' degli Studi di Siena  
 Via Aldo Moro                    
 I-53100 Siena, Italy              
 Phone: ++39 0577 234307      
 Fax: ++39 0577 234333         
***********************************

From chemistry-request@server.ccl.net Mon Mar 25 04:45:08 2002
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To: "Kiniu WONG \(Kin-Yiu\)" <kiniu@mps.ohio-state.edu>, chemistry@ccl.net
From: sergiusz kwasniewski <sergiusz.kwasniewski@luc.ac.be>
Subject: Re: CCL:TDDFT in terms of polarization propagator

Hi,

I only got one answer:

serge,

i'm pretty sure this has been done, have a look at the book by simons
and jorgenson [second quanitzation in chemistry i think its called?], or
some of the work of danny yeager

noj
-- 
  Dr. N.O.J. Malcolm                       n.malcolm@umist.ac.uk
  Chemistry Department                   
  UMIST, Sackville Street
  Manchester, England. M60 1QD

I guess this is about the book 'second quantization-based methods in QC' from
P Jorgenson and J Simons ?

Serge

At 07:53 AM 3/7/02 -0500, Kiniu WONG \(Kin-Yiu\) wrote:
>----- Original Message -----
>From: "sergiusz kwasniewski" <sergiusz.kwasniewski@luc.ac.be>
>To: <chemistry@ccl.net>
>Sent: Thursday, March 07, 2002 4:17 AM
>Subject: CCL:TDDFT in terms of polarization propagator
>
>
>> Hi,
>>
>> Does someone know whether TDDFT (or TDDFRT) has been derived in terms
>> of the polarization propagator (Green's functions). It would easen the
>> comparison with standard derivation of RPA (or TDHF).
>>
>> Thanks,
>>
>> Serge Kwasniewski


___________________________________________________

	Sergiusz Kwasniewski
	LUC SBG/TS
	Universitaire Campus Gebouw D
	3590 Diepenbeek
	BELGIUM

	tel(direct): 032 (0)11/268315
	fax	   : 032 (0)11/268301
	email      : sergiusz.kwasniewski@luc.ac.be
	http://www.luc.ac.be/Research/TheoChem
___________________________________________________


From chemistry-request@server.ccl.net Mon Mar 25 05:00:40 2002
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Date: Mon, 25 Mar 2002 11:00:27 -0800
From: Stefano Forli <forli@unisi.it>
Subject: QSAR equations: Addendum
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 I would also ask about the intercept value, and its implications in a
good correlation...
Thanks!

S.


-- 

***********************************
 Forli Stefano                    
 Dip. Farmaco Chimico Tecnologico  
 Universita' degli Studi di Siena  
 Via Aldo Moro                    
 I-53100 Siena, Italy              
 Phone: ++39 0577 234307      
 Fax: ++39 0577 234333         
***********************************

From chemistry-request@server.ccl.net Mon Mar 25 08:55:04 2002
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To: chemistry@ccl.net
From: sergiusz kwasniewski <sergiusz.kwasniewski@luc.ac.be>
Subject: question on vibronic coupling calculation

Hi everyone,

I'm trying to write a program to account for vibronic coupling on
UV/Visible absorption spectra. For the vibronic progression with
only one symmetric vibrational mode and up to 3 quanta, the Frank-Condon
approximation is fairly easy to implement. However, if I want to
include more vibrational modes, I encounter a small problem:

I(lambda) ~ SUM ( PRODUCT ( F.C.'s) * D )

where lambda is given in wavelength (nm), the sum is over the quanta (0-3),
and the product over the Frank-Condon factors corresponding to the different
vibrational modes.

Now: in order to describe the band shape factor D, I have to calculate
a factor (lambda - lambda(max))^2. How does this factor change while including
more than one vibrational frequency ?

What I found is: (lambda - (lambda(max) + SUM nu * omega))^2

where nu is the quantum (which is a constant in this summation) and omega
is the energy of the vibration, but then instead of having a series of 
6 additional peaks besides your lambda(max) (i.e. 3 per vibrational modes), 
these modes are coupled now 2 by 2 in order to give 3 additional peaks 
but with an almost doubled spacing (depending on the energies of the vibrations
off course).

Does anyone know if this is correct, the literature I found about vibronic
coupling doesn't explain this thoroughly.

I appreciate any kind of help !!

Serge


___________________________________________________

	Sergiusz Kwasniewski
	LUC SBG/TS
	Universitaire Campus Gebouw D
	3590 Diepenbeek
	BELGIUM

	tel(direct): 032 (0)11/268315
	fax	   : 032 (0)11/268301
	email      : sergiusz.kwasniewski@luc.ac.be
	http://www.luc.ac.be/Research/TheoChem
___________________________________________________


From chemistry-request@server.ccl.net Mon Mar 25 09:50:31 2002
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Date: Mon, 25 Mar 2002 15:50:08 +0100
From: Stefan Bromley <S.T.Bromley@tnw.tudelft.nl>
Subject: GULP with MPI/LAM
To: chemistry@ccl.net
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I have been runnning MD jobs with GULP (General Utility Lattice 
Program) on a 16 node Athlon based Beowulf cluster but have been 
unable to run consecutive MPI jobs without a remake of the source 
(just deleting the final source file and remaking - taking a second or 
two) each time. Although it works, it is a rather unsatisfactory way 
of working and limits me to one MPI job at a time.

It seems that every time GULP finishes it somehow manages to 
corrupt the LAM MPI libraries, and when a second run of GULP is 
attempted an error occurs just as the first step is to proceed:

******************************************************************************
  Output for configuration   1                                                        *
******************************************************************************
MPI_Recv: process in local group is dead (rank 0, 
MPI_COMM_WORLD)
Rank (0, MPI_COMM_WORLD): Call stack within LAM:
Rank (0, MPI_COMM_WORLD):  - MPI_Recv()
Rank (0, MPI_COMM_WORLD):  - MPI_Reduce()
Rank (0, MPI_COMM_WORLD):  - MPI_Allreduce()
Rank (0, MPI_COMM_WORLD):  - main()

Looking at the source code this seems to be the point in the code 
where the memory allocation takes place. I have therefore tried all 
combinations of -DMALLOC and -DF90 in the getmachine setup 
but none seems to fix the problem.

I am using LAM-MPI compiled with the GNU compilers and 
configured to use the pgf90 compiler under Linux.

Has anyone managed to compile a more robust LAM-
MPI/pgf90/GULP setup (or similar), or does anyone have any 
suggestions of how to do so. An mpirun of a consecutive GULP job 
with np 1 gives no problem only with 2 or more processors. I have 
also tried using MPICH but I couldn't even run/compile/link GULP 
sucessfully then. 

Many thanks for your help in advance.  

Stefan
________________________________________________________

Dr Stefan T. Bromley
Laboratory of Applied Organic Chemistry and Catalysis
DelftChemTech, Delft University of Technology
Julianalaan 136, 2628 BL Delft
The Netherlands

Phone  : + 31 1527 89418
 
e-mail  : S.T.Bromley@tnw.tudelft.nl
________________________________________________________

From chemistry-request@server.ccl.net Mon Mar 25 18:47:38 2002
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Hi!

I am using autodock3 for sometime. I went through the dockings a couple
of times. But when I read the ligand.macro.dlg.pdb in the sybyl window,
It just gives me different positions of the ligand molecule with the
macromolecule missing in the background.

Anybody knows solution to this problem?

Praveen


