From chemistry-request@ccl.net Mon Jul 12 09:46:07 2004
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From: Ian Hovell <HOVELL_at_cetem.gov.br>
To: "'chemistry'" <chemistry_at_ccl.net>
Subject: CCL: choice of computer for G03
Date: Mon, 12 Jul 2004 11:49:58 -0300
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Dear CCLers,
I'm looking for the ideal computer for running G03. I was wondering what
people on the list, when buying a new computer dedicated to Gaussian03,
would go fo? Would people go for cpu speed, cache memory, RAM or hard disk.
Where would the emphasise be? And what OS would you opt for. I'm sure these
questions have been asked for before so if any body can point me to a URL
they know, okay.
Thanks for your help and time.
Ian

From chemistry-request@ccl.net Mon Jul 12 09:49:26 2004
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Schrodinger is pleased to announce the latest versions of its drug discovery
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From chemistry-request@ccl.net Mon Jul 12 07:00:30 2004
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From: guntetz^at^charlotte.lfc.edu
Subject: Adding a new atom type to G03 UFF Calculation?
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Hello All,

I am currently trying to build in two new atom types into the UFF force field in Gaussian 03', but am having a bit of difficulty.  Has anyone attempted this before?  If so, could you possibly give me some pointers on how to go about it.  Test585.com is the only real clue that I have to work with right now, and it is just not cutting it.

Thanks,
Thomas Z. Gunter



From chemistry-request@ccl.net Mon Jul 12 09:50:02 2004
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Subject: RE: Question on molecular structure and QM
Date: Mon, 12 Jul 2004 10:54:40 -0400
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Wouldn't the isomers simply be different solutions to the same non-B-O Hamiltonian, just as the various states of a molecule are different solutions?  (By "the various states" I mean the ones that within the B-O approx. are labeled vibrational, rotational, and electronic). 

--David Shobe, Ph.D., M.L.S.
S|d-Chemie, Inc.
phone (502) 634-7409
fax (502) 634-7724

Don't bother flaming me: I'm behind a firewall.


-----Original Message-----
From: Computational Chemistry List [mailto:chemistry-request^at^ccl.net]On
Behalf Of Eric Scerri
Sent: Friday, July 09, 2004 3:00 AM
To: ccl
Subject: CCL:Question on molecular structure and QM




The following is a somewhat general philosophical question.
I would very much appreciate the comments of computational chemists.

In the philosophy of chemistry literature much has been made of the 
fact that molecular structure cannot be strictly deduced from QM.  I 
am referring to the work of Guy Wooley in the UK and Hans Primas at 
the ETH.

The basis of this claim is that structure comes after applying the 
Born-Oppenheimer approximation to fix the nuclei.  These authors 
claim that in this sense molecular structure has not been "reduced" 
to QM.

They point to the fact that the Hamiltonians for two isomers of an 
organic compound, for example, are identical in the absence of the 
B-O approximation and they conclude that a strictly QM calculation 
cannot therefore distinguish between the two structures in question.

I would be happy to pull some references together for anyone 
interested in studying the original articles.  But I just wanted to 
hear some general reactions to such claims.




-- 


Dr. Eric Scerri ,
UCLA,
Department of Chemistry & Biochemistry,
607 Charles E. Young Drive East,
Los Angeles,  CA 90095-1569
USA

E-mail :   scerri^at^chem.ucla.edu
tel:  310 206 7443
fax:  310 206 2061
Web Page:    http://www.chem.ucla.edu/dept/Faculty/scerri/index.html

Editor  of  Foundations of Chemistry
http://www.kluweronline.com/issn/1386-4238

Also see International Society for the Philosophy of Chemistry
http://www.georgetown.edu/earleyj/ISPC.html


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From chemistry-request@ccl.net Mon Jul 12 09:52:34 2004
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Subject: RE: time-dependent and time-independent QM
Date: Mon, 12 Jul 2004 10:57:16 -0400
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A possibly related question: there are two versions of the Hamiltonian, the time-dependent and the time-independent.  The former represents the evolution of a dynamic system; the latter represents the steady states of the system, and is the Hamiltonian used in most quantum-chemistry problems.  I've never really understood the relationship between the time-dependent and time-independent equations, especially since this is where all the "weirdness" of QM comes into play. 

--David Shobe, Ph.D., M.L.S.
S|d-Chemie, Inc.
phone (502) 634-7409
fax (502) 634-7724

Don't bother flaming me: I'm behind a firewall.



-----Original Message-----
From: Shobe, David 
Sent: Monday, July 12, 2004 10:55 AM
To: CCL computational chemistry list (E-mail)
Subject: RE: Question on molecular structure and QM


Wouldn't the isomers simply be different solutions to the same non-B-O Hamiltonian, just as the various states of a molecule are different solutions?  (By "the various states" I mean the ones that within the B-O approx. are labeled vibrational, rotational, and electronic). 

--David Shobe, Ph.D., M.L.S.
S|d-Chemie, Inc.
phone (502) 634-7409
fax (502) 634-7724

Don't bother flaming me: I'm behind a firewall.


-----Original Message-----
From: Computational Chemistry List [mailto:chemistry-request)at(ccl.net]On
Behalf Of Eric Scerri
Sent: Friday, July 09, 2004 3:00 AM
To: ccl
Subject: CCL:Question on molecular structure and QM




The following is a somewhat general philosophical question.
I would very much appreciate the comments of computational chemists.

In the philosophy of chemistry literature much has been made of the 
fact that molecular structure cannot be strictly deduced from QM.  I 
am referring to the work of Guy Wooley in the UK and Hans Primas at 
the ETH.

The basis of this claim is that structure comes after applying the 
Born-Oppenheimer approximation to fix the nuclei.  These authors 
claim that in this sense molecular structure has not been "reduced" 
to QM.

They point to the fact that the Hamiltonians for two isomers of an 
organic compound, for example, are identical in the absence of the 
B-O approximation and they conclude that a strictly QM calculation 
cannot therefore distinguish between the two structures in question.

I would be happy to pull some references together for anyone 
interested in studying the original articles.  But I just wanted to 
hear some general reactions to such claims.




-- 


Dr. Eric Scerri ,
UCLA,
Department of Chemistry & Biochemistry,
607 Charles E. Young Drive East,
Los Angeles,  CA 90095-1569
USA

E-mail :   scerri)at(chem.ucla.edu
tel:  310 206 7443
fax:  310 206 2061
Web Page:    http://www.chem.ucla.edu/dept/Faculty/scerri/index.html

Editor  of  Foundations of Chemistry
http://www.kluweronline.com/issn/1386-4238

Also see International Society for the Philosophy of Chemistry
http://www.georgetown.edu/earleyj/ISPC.html


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From chemistry-request@ccl.net Mon Jul 12 13:19:53 2004
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Date: Mon, 12 Jul 2004 13:17:45 -0500
From: "Thomas Z. Gunter" <guntetz*at*lfc.edu>
Subject: CCL:G03 new atom type for UFF question
To: "chemistry*at*ccl.net" <chemistry*at*ccl.net>
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Hello All,



I am currently trying to build in two new atom types into the UFF force 
field in Gaussian 03', but am having a bit of difficulty.  Has anyone 
attempted this before?  If so, could
you possibly give me some pointers on how to go about it.  Test585.com is 
the only real clue that I have to work with right now, and it is just not 
cutting it.



Thanks,

Thomas Z. Gunter



-- 
Using M2, Opera's revolutionary e-mail client: http://www.opera.com/m2/


From chemistry-request@ccl.net Mon Jul 12 13:11:18 2004
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Cc: CCL computational chemistry list (E-mail) <chemistry/at/ccl.net>,
   scerri/at/chem.ucla.edu
From: hinsen/at/cnrs-orleans.fr
Subject: Re: CCL:time-dependent and time-independent QM
Date: Mon, 12 Jul 2004 20:17:43 +0200
To: "Shobe, David" <dshobe/at/sud-chemieinc.com>
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On Jul 12, 2004, at 16:57, Shobe, David wrote:

> A possibly related question: there are two versions of the 
> Hamiltonian, the time-dependent and the time-independent.  The former 
> represents the evolution of a dynamic system; the latter represents 
> the steady states of the system, and is the Hamiltonian used in most 
> quantum-chemistry problems.  I've never really understood the 
> relationship between the time-dependent and time-independent 
> equations, especially since this is where all the "weirdness" of QM 
> comes into play.

The Hamiltonian is the same in the time-dependent and the 
time-independent Schroedinger equations. The time-dependent one is the 
starting point, it describes the time evolution of an arbitrary quantum 
state of a system. The time-independent equation results if one then 
asks which quantum states have no time evolution (other than a variable 
phase factor). The interest in these states is twofold:

1) They describe the stable states, which one is often interested in.
2) They contain all the time-dependent information as well, because the
    stable states (eigenstates of the Hamiltonian) are a basis of state 
space.
    For an arbitrary initial quantum state, calculate the projections on 
the
    stable states. Then multiply each projection with the (trivial) 
time-dependent
    phase factor and the corresponding stable state. Sum up everything, 
and you
    have the time evolution of the initial state.

Because of 2), the time-independent equation can be considered a 
particular approach to solve the time-dependent equation.

> Wouldn't the isomers simply be different solutions to the same non-B-O 
> Hamiltonian, just as the various states of a molecule are different 
> solutions?  (By "the various states" I mean the ones that within the 
> B-O approx. are labeled vibrational, rotational, and electronic).

Assuming that by "solution to a Hamiltonian" you mean its eigenstates, 
no, not in general, though often to a good approximation.

This leads back to the original question by Eric Scerri. I am not 
familiar with the articles he refers to, but I don't see why the B-O 
approximation would be crucial. With or without B-O, quantum mechanics 
gives the probability distribution of the atomic configurations. One 
can then search for well-defined maxima and call them "molecular 
structures", but that is an additional interpretation step made for 
convenience of discussion only. I suppose that all chemists are aware 
that molecules are not static, the atoms move around all the time. So 
"molecular structure" is a concept introduced as a convenience, it 
cannot be deduced strictly from quantum mechanics.

---------------------------------------------------------------------
Konrad Hinsen
Laboratoire Lion Brillouin, CEA Saclay,
91191 Gif-sur-Yvette Cedex, France
Tel.: +33-1 69 08 79 25
Fax: +33-1 69 08 82 61
E-Mail: hinsen/at/llb.saclay.cea.fr
---------------------------------------------------------------------




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Subject: RE: CCL:time-dependent and time-independent QM
Date: Mon, 12 Jul 2004 16:14:28 -0400
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Thread-Topic: CCL:time-dependent and time-independent QM
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From: "Shobe, David" <dshobe^at^sud-chemieinc.com>
To: <hinsen^at^cnrs-orleans.fr>,
   "CCL computational chemistry list (E-mail)" <chemistry^at^ccl.net>
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Where does the part where measuring a property of the system "resets" the quantum state of the system come in?   That's always been mysterious: how does the system "know" it's being measured?  Does the uncertainty principle rest on an assumption that one cannot make a measurement w/o temporarily adding one or more other particles to the system?  And can you really do that temporarily, or are you permanently enlarging the system when you add particles?  

Another problem I have with understanding the time dependent Schroedinger equation is that it's a differential equation, so you need initial/boundary conditions to solve it, right?  But the postulates imply that you can't know all the initial conditions...or can the initial "psi-0" function incorporate both what's known about the initial state and what's unknown?

--David Shobe, Ph.D., M.L.S.
S|d-Chemie, Inc.
phone (502) 634-7409
fax (502) 634-7724

Don't bother flaming me: I'm behind a firewall.





-----Original Message-----
From: hinsen^at^cnrs-orleans.fr [mailto:hinsen^at^cnrs-orleans.fr]
Sent: Monday, July 12, 2004 2:18 PM
To: Shobe, David
Cc: CCL computational chemistry list (E-mail); scerri^at^chem.ucla.edu
Subject: Re: CCL:time-dependent and time-independent QM


On Jul 12, 2004, at 16:57, Shobe, David wrote:

> A possibly related question: there are two versions of the 
> Hamiltonian, the time-dependent and the time-independent.  The former 
> represents the evolution of a dynamic system; the latter represents 
> the steady states of the system, and is the Hamiltonian used in most 
> quantum-chemistry problems.  I've never really understood the 
> relationship between the time-dependent and time-independent 
> equations, especially since this is where all the "weirdness" of QM 
> comes into play.

The Hamiltonian is the same in the time-dependent and the 
time-independent Schroedinger equations. The time-dependent one is the 
starting point, it describes the time evolution of an arbitrary quantum 
state of a system. The time-independent equation results if one then 
asks which quantum states have no time evolution (other than a variable 
phase factor). The interest in these states is twofold:

1) They describe the stable states, which one is often interested in.
2) They contain all the time-dependent information as well, because the
    stable states (eigenstates of the Hamiltonian) are a basis of state 
space.
    For an arbitrary initial quantum state, calculate the projections on 
the
    stable states. Then multiply each projection with the (trivial) 
time-dependent
    phase factor and the corresponding stable state. Sum up everything, 
and you
    have the time evolution of the initial state.

Because of 2), the time-independent equation can be considered a 
particular approach to solve the time-dependent equation.

> Wouldn't the isomers simply be different solutions to the same non-B-O 
> Hamiltonian, just as the various states of a molecule are different 
> solutions?  (By "the various states" I mean the ones that within the 
> B-O approx. are labeled vibrational, rotational, and electronic).

Assuming that by "solution to a Hamiltonian" you mean its eigenstates, 
no, not in general, though often to a good approximation.

This leads back to the original question by Eric Scerri. I am not 
familiar with the articles he refers to, but I don't see why the B-O 
approximation would be crucial. With or without B-O, quantum mechanics 
gives the probability distribution of the atomic configurations. One 
can then search for well-defined maxima and call them "molecular 
structures", but that is an additional interpretation step made for 
convenience of discussion only. I suppose that all chemists are aware 
that molecules are not static, the atoms move around all the time. So 
"molecular structure" is a concept introduced as a convenience, it 
cannot be deduced strictly from quantum mechanics.

---------------------------------------------------------------------
Konrad Hinsen
Laboratoire Lion Brillouin, CEA Saclay,
91191 Gif-sur-Yvette Cedex, France
Tel.: +33-1 69 08 79 25
Fax: +33-1 69 08 82 61
E-Mail: hinsen^at^llb.saclay.cea.fr
---------------------------------------------------------------------




From chemistry-request@ccl.net Mon Jul 12 12:15:08 2004
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From: Anil Korkut <ak2048/at/columbia.edu>
Sender: ak2048/at/columbia.edu
To: chemistry/at/ccl.net
Subject: normal modes problem/CHARMM
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I am doing an NMA calculation for a protein with 3000 atoms using charmm
simulation package.

I minimized my structure to a gradient of 1e-6 with 2000 steps of sttepest
descent followed by about 8000 steps of ABNR.

I know that the first six normal modes should have zero frequency.

However, I got no frequency values for the first two normal modes!!!!

The translational and rotational modes start at mode 3 and the vibrational
modes start at mode 9 instead of 7.

The frequency values are
VIBRAN> PRINT NORM MODE 1 THRU 16 DIPO

NORMAL MODES

1********** 2********** 3 -0.01 4 -0.01 5 0.00
6 0.00 7 0.00 8 0.01 9 1.51 10 1.76
11 2.40 12 3.03 13 3.40 14 3.76 15 4.05
16 4.29


I have done the same calculation with a different force field (opls-ua)
using TINKER and results were as expected (i.e. no blank modes, no 
negative
eigenvalues)

The nomal mode 7 from tinker has very similar freq. value to normal mode 9
> from charmm.

I also used BPTI as a sample protein and the same problem exists.

Does anyone have any idea what is going wrong here?

I can post my script, if anyone is interested.

Thanks

______________________________________________________________
Anil Korkut
Dept of Biochemistry and Mol. Biophysics
Columbia University,
630 West 168th St, BB204
New York, NY 10032
office ph (212) 305 1846
______________________________________________________________


From chemistry-request@ccl.net Mon Jul 12 13:35:04 2004
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Date: Mon, 12 Jul 2004 11:40:32 -0700
From: Carsten Detering <detering!at!u.washington.edu>
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Dear all,

Thanks to all who replied to my previous question about the transition 
state problem. Using Noeigentest in the keyword section worked.

I have two further questions now:
After having successfully optimized my transition state in the gas 
phase, I would like to optimize it in solution.
I used
#B3LYP/6-31g* opt SCRF=(PCM,TS,Modredundant,solvent=chloroform,READ) 
nosymmetry test

SCRF=PCM doesnt seem to allow a TS keyword though. Is there a way to 
optimize to a TS using the PCM model? What would the keyword section 
have to look like?

My second question concerns the optimization of the same structure to 
one its minima, also in solution. I have used

  #B3LYP/6-31g* opt SCRF=(PCM,solvent=chloroform,READ) nosymmetry test

with radii=uff and sphereonh=XX, but the calculation stops with

------
Using the following non-standard input for PCM:
  radii=uff
  sphereonh=39
  End of line while reading PCM input.
  Error termination via Lnk1e in /software/gaussian/g03_B.4/g03/l301.exe 
at Mon Jul 12 19:56:48 2004.
------

I am using cartesian coordinates in the input section.
Am I missing a parameter, or what is causing the calculation to stop?

Thanks a lot in advance for any helpful suggestions,

Carsten






From chemistry-request@ccl.net Mon Jul 12 15:45:29 2004
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From: hinsen!at!cnrs-orleans.fr
Subject: Re: CCL:time-dependent and time-independent QM
Date: Mon, 12 Jul 2004 22:52:04 +0200
To: "Shobe, David" <dshobe!at!sud-chemieinc.com>
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On 12.07.2004, at 22:14, Shobe, David wrote:

> Where does the part where measuring a property of the system "resets"  
> the quantum state of the system come in?   That's always been  
> mysterious:

That depends on who you ask, I think that discussion is still  
open-ended. The "collapse of the wave function" is part of the original  
Copenhagen interpretation of the meaning of the wave function. However,  
there are other interpretations. As the term "interpretation" implies,  
the choice of one does not change the maths - the equations and wave  
functions remain the same.

The real problem in that discussion is that "measurement" needs to be  
defined. In a pure quantum world, there are particles interacting, all  
subject to the same laws, and the whole universe is governed by a  
single huge wave function. No measurements, no problems. Various  
definitions of measurements have been proposed, but none has yet been  
found to be without problems. Some say that measuring implies human  
consciousness - hence the paradox known as "Schrvdinger's cat". Others  
say that measurement is an interaction with a classical object, but  
that would imply that quantum mechanics needs to be defined in terms of  
its own limiting case, classical mechanics.

>  how does the system "know" it's being measured?  Does the uncertainty  
> principle rest on an assumption that one cannot make a measurement w/o  
> temporarily adding one or more other particles to the system?  And can  
> you

The strict mathematical formulation of the uncertainty principle is in  
terms of wave functions, thus independent of any one interpretation.  
Many formulations in plain language depend on a choice of  
interpretation, however.

> Another problem I have with understanding the time dependent  
> Schroedinger equation is that it's a differential equation, so you  
> need initial/boundary conditions to solve it, right?  But the  
> postulates imply that you

Yes, you need to know the initial quantum state.

>  can't know all the initial conditions...or can the initial "psi-0"  
> function incorporate both what's known about the initial state and  
> what's unknown?

Right. That's again part of the interpretation problem. But not the  
worst in practice, as the question of time propagation of a given  
quantum state rarely occurs in real-life questions. That is perhaps  
another reason why the time-independent equation is so much more used  
in practice.

------------------------------------------------------------------------ 
-------
Konrad Hinsen
Laboratoire Leon Brillouin, CEA Saclay,
91191 Gif-sur-Yvette Cedex, France
Tel.: +33-1 69 08 79 25
Fax: +33-1 69 08 82 61
E-Mail: hinsen!at!llb.saclay.cea.fr
------------------------------------------------------------------------ 
-------




From chemistry-request@ccl.net Mon Jul 12 11:38:12 2004
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2004 July 12

Here is the summary of the answers I got to the question below. Thanks 
very much to all who responded (I hope I haven't omitted anyone).
Those interested in cases like s-cis-butadiene/s-trans-butadiene + a 
dienophile might wish to note #4 below,  and E. Goldstein, B. Beno, and 
K. N. Houk, JACS, 1996, 118, 6036.
=========
QUESTION

2004 July 8

The rate of formation of products Pa and Pb from quickly interconverting
conformers Ca and Cb is treated with the the Curtin/Hammett and
Winstein-Holness equations (the Curtin-Hammett principle, in particular,
is well-known): J. I Seeman, Chem Rev, 1983, 83, 83; E. L. Eliel, "From
Cologne to Chapel Hill", ACS, 1990, pp. 31-33.

Question: has anyone a reference to a discussion of the case of rapidly
interconverting conformers Ca and Cb, where Ca, although the minor
conformer, is the only one that can react with X to form a product CaX,
through transition state Ta; intuition aside, has someone explicitly
addressed whether the _experimental_ activation E is measuring the Ta-Ca
energy difference, or the Ta-Cb difference?

Thanks.

EL
-----------

#1
Per-Ola Norrby

    Provided that the interconversion is fast relative to the final 
reaction, the free energy of activation should be relative to the 
ensemble energy (which is slightly lower than the lowest of Ca and Cb).  
The apparent activation energy is taken from an expression where you 
consider the total concentration of reactant.  The sole effect of the 
pre-equilibrium is to make the effective concentration lower, with a 
concominant lowering of the rate which corresponds exactly to the free 
energy difference between the reacting conformer and the free energy of 
the ensemble.  You can get the latter by assuming a virtual species 
corresponding to the total concentration of the reagent, and use the 
standard Boltzmann expression.

    The above wasn't perfectly clear (I haven't digested my coffee yet), 
but it should be correct.  The math is available in the Ph.D. Thesis of 
Torben Rasmussen (Copenhagen 2001), and he took much of it from H 
Maskil, "The Physical Basis of Organic Chemistry", Oxford 1985.

    /Per-Ola
-- 
Per-Ola Norrby, Assoc. Professor, http://organisk.kemi.dtu.dk/PON/
Technical University of Denmark, Department of Chemistry
Building 201, Kemitorvet, DK-2800 Kgs. Lyngby, Denmark
Email: pon(at)kemi.dtu.dk  tel +45-45252123,  fax +45-45933968
==========
#2
Andreas Klamt

Errol,

sorry for replying with a theoretical aspect:
Do you really expect a unique answer? The answer will depend on the 
question, whether the exchange rate between Ca and Cb is larger or 
smaller than the reaction rate. In the first case you will observe Ta-Ca 
as activation energy, in the seond case Ca-Cb!!! because this step 
becomes rate determining. I am not sure whether you ever will observe 
Ta-Cb as activation energy.

Andreas

klamt(at)cosmologic.de
=================
#3
Philip Hultin

We have been dealing with a similar question, and have had some arguments
with referees on this question.

I don't know of any experimental demonstrations, but Seeman's paper does
make the point very clearly that populations DO matter, at least in what he
calls the "Case II Kinetics" scenario.  The total rate is a
population-weighted sum of the two individual rates, which implies that the
individual activation barriers play a population-weighted role in the
"apparent" activation barrier you would measure experimentally.

Please, let me know of any comments you receive on this question.

Dr. Philip G. Hultin
Associate Professor of Chemistry
University of Manitoba
Winnipeg, MB, Canada R3T 2N2
(vox) 204-474-9814
(fax) 204-474-7608
mailto:hultin(at)cc.umanitoba.ca
http://www.umanitoba.ca/chemistry/

=================
#4
Jose Ignacio Garcia-Laureiro

Dear Prof. Lewars,

Indeed, there is a very common situation in which that happens, namely the
s-cis/s-trans conformational equilibrium of open-chain dienes in 
Diels-Alder
reactions. For instance, only the s-cis conformer (BDc) of butadiene is 
able to react,
whereas the s-trans (BDt), the major conformer, is inactive towards the 
cycloaddition.
In these conditions, the experimental activation barrier is measuring 
the TS-BDt
energy difference, and this is because the same reasons operating in the 
Curtin-Hammett
equation: the preequilibrium constant s-cis/s-trans appears in the 
kinetic equation
as a multiplicative term, so that the apparent rate constant is in fact 
the product
between the kcis (representing the TS-BDc activation barrier), and K 
(the conformational
equilibrium constant, representing the s-trans - s-cis energy difference).
I hope this can help you.
Best regards.

Josi I. Garcma

++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++
Dr. Jose Ignacio Garcia-Laureiro, Investigador Cientmfico del CSIC
Depto. Quimica Organica. Instituto de Ciencia de Materiales de Aragon
Facultad de Ciencias (edificio D). Universidad de Zaragoza-CSIC
c/ Pedro Cerbuna, 12. E-50009 Zaragoza (Spain)
Phone: +34 976762271       e-mail: jig(at)unizar.es
Fax:     +34 976762077
http://wzar.unizar.es/acad/fac/cie/quiorg/catalisis/index.htm
==============




From chemistry-request@ccl.net Mon Jul 12 18:37:23 2004
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Thanks to a lot of help from those on this board, I've gotten over many
hurdles I've encountered in trying to use autodock without any linux or
modeling experience.  It seems now that the only problem I have is with
the 'finish work.'  I've gotten all the data my PI requested of me, but
now need to make some docked illustrations for some publications.  All
of my pdbq files used in the dockings however have a problem with
connectivity.  Once saved as a pdbq file, it gets pretty messy.  I've
attached a picture of FAD as an example.  If someone could please help
me in getting around this problem, I would greatly appreciate it.  I
also have downloaded opendx and compiled it on cygwin, but am unable to
compile CTC chemistry extensions for some reason using the cygwin
makefile provided.  I get the following error:
 
Make: *** [bin/addbonds] error 1
 
So, the only program I'll have to depicting my modeling is ViPEr that
came with ADT package and what I can do with PMV.  Anyone with useful
'networks' for ViPEr that care to share, it would be greatly
appreciated.  Also, is it possible to make a 'docking movie' with
ADT/ViPEr?  Thank you for your time
 
Will
ewlowe*at*helios.acomp.usf.edu
university of south florida
department of chemistry and biochemistry  

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<p class=3DMsoNormal><font size=3D2 face=3DArial><span =
style=3D'font-size:10.0pt;
font-family:Arial'>Thanks to a lot of help from those on this board, =
I&#8217;ve
gotten over many hurdles I&#8217;ve encountered in trying to use <span
class=3DSpellE>autodock</span> without any <span =
class=3DSpellE>linux</span> or
modeling experience. <span style=3D'mso-spacerun:yes'>&nbsp;</span>It =
seems now that
the only problem I have is with the &#8216;finish work.&#8217;<span
style=3D'mso-spacerun:yes'>&nbsp; </span>I&#8217;ve gotten all the data =
my PI
requested of me, but now need to make some docked illustrations for some
publications. <span style=3D'mso-spacerun:yes'>&nbsp;</span>All of my =
<span
class=3DSpellE>pdbq</span> files used in the dockings however have a =
problem with
connectivity.<span style=3D'mso-spacerun:yes'>&nbsp; </span>Once saved =
as a <span
class=3DSpellE>pdbq</span> file, it gets pretty messy.<span
style=3D'mso-spacerun:yes'>&nbsp; </span>I&#8217;ve attached a picture =
of FAD as
an example.<span style=3D'mso-spacerun:yes'>&nbsp; </span>If someone =
could please
help me in getting around this problem, I would greatly appreciate =
it.<span
style=3D'mso-spacerun:yes'>&nbsp; </span>I also have downloaded <span
class=3DSpellE>opendx</span> and compiled it on <span =
class=3DSpellE>cygwin</span>,
but am unable to compile CTC chemistry extensions for some reason using =
the <span
class=3DSpellE>cygwin</span> <span class=3DSpellE>makefile</span> =
provided.<span
style=3D'mso-spacerun:yes'>&nbsp; </span>I get the following =
error:<o:p></o:p></span></font></p>

<p class=3DMsoNormal><font size=3D2 face=3DArial><span =
style=3D'font-size:10.0pt;
font-family:Arial'><o:p>&nbsp;</o:p></span></font></p>

<p class=3DMsoNormal><font size=3D2 face=3DArial><span =
style=3D'font-size:10.0pt;
font-family:Arial'>Make: *** [bin/<span class=3DSpellE>addbonds</span>] =
error 1<o:p></o:p></span></font></p>

<p class=3DMsoNormal><font size=3D2 face=3DArial><span =
style=3D'font-size:10.0pt;
font-family:Arial'><o:p>&nbsp;</o:p></span></font></p>

<p class=3DMsoNormal><font size=3D2 face=3DArial><span =
style=3D'font-size:10.0pt;
font-family:Arial'>So, the only program I&#8217;ll have to depicting my
modeling is <span class=3DSpellE>ViPEr</span> that came with ADT package =
and what
I can do with PMV.<span style=3D'mso-spacerun:yes'>&nbsp; </span>Anyone =
with
useful &#8216;networks&#8217; for <span class=3DSpellE>ViPEr</span> that =
care to
share, it would be greatly appreciated.<span =
style=3D'mso-spacerun:yes'>&nbsp;
</span>Also, is it possible to make a &#8216;docking movie&#8217; with =
ADT/<span
class=3DSpellE>ViPEr</span>?<span style=3D'mso-spacerun:yes'>&nbsp; =
</span>Thank you
for your time<o:p></o:p></span></font></p>

<p class=3DMsoNormal><font size=3D2 face=3DArial><span =
style=3D'font-size:10.0pt;
font-family:Arial'><o:p>&nbsp;</o:p></span></font></p>

<p class=3DMsoNormal><font size=3D2 face=3DArial><span =
style=3D'font-size:10.0pt;
font-family:Arial'>Will<o:p></o:p></span></font></p>

<p class=3DMsoNormal><font size=3D2 face=3DArial><span =
style=3D'font-size:10.0pt;
font-family:Arial'><a =
href=3D"mailto:ewlowe*at*helios.acomp.usf.edu">ewlowe*at*helios.acomp.usf.edu</=
a><o:p></o:p></span></font></p>

<p class=3DMsoNormal><span class=3DGramE><font size=3D2 =
face=3DArial><span
style=3D'font-size:10.0pt;font-family:Arial'>university</span></font></sp=
an><font
size=3D2 face=3DArial><span =
style=3D'font-size:10.0pt;font-family:Arial'> of south =
</span></font><st1:State><st1:place><span
  class=3DSpellE><font size=3D2 face=3DArial><span =
style=3D'font-size:10.0pt;
  =
font-family:Arial'>florida</span></font></span></st1:place></st1:State><f=
ont
size=3D2 face=3DArial><span =
style=3D'font-size:10.0pt;font-family:Arial'><o:p></o:p></span></font></p=
>

<p class=3DMsoNormal><font size=3D2 face=3DArial><span =
style=3D'font-size:10.0pt;
font-family:Arial'>department of chemistry and biochemistry<span
style=3D'mso-spacerun:yes'>&nbsp; </span><o:p></o:p></span></font></p>

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