From owner-biophysics@net.bio.net Mon Dec 01 22:00:00 1997
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From: fujimoto@u.washington.edu (Bryant Fujimoto)
Newsgroups: bionet.biophysics
Subject: Re: Verification of the second law (reply to Bryant Fujimoto)
Date: 2 Dec 1997 06:58:29 GMT
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Pentcho Valev <RUMYM@BGEARN.ACAD.BG> writes:

>Bryant,
>   I read very carefully your last post and found it quite self-consistent,
>so I see no reason to comment on each item. Yes I agree that thermodynamics
>works, but only within a certain paradigm. In the same way the concept that
>heat is a substance (caloric) did work for quite a lot of time until the
>new paradigm (the law of conservation of energy) emerged.
>   Let us accept for the moment that delta G is the right measure of the
>work a chemical system does, under certain conditions, on another system.
>But let us also consider an alternative, and compare eventually the two
>interpretations.
>   Let the reaction

>      ATP  =  ADP  +  P                                      /1/

>drive another reaction, e.g.  B = C, isothermally and isobarically:

>      ATP + B  =  ADP + P + C                                /2/

>As one mole ATP is used up in the reaction, the energy of the system
>ATP-ADP-P  dereases by 20 KJ/mole (since the enthalpy of ATP hydrolysis
>is  -20 KJ/mole). Let us also assume that the enthalpy of /2/ is shown
>experimentally to be  -10 KJ/mole. This leads to the following quite
>simple conclusion.If one mole ATP had been just hydrolysed (without
>coupling), 20 KJ heat would have been released. Now, in the coupled
>reaction /2/, only 10 KJ heat are released. Therefore, the other 10 KJ
>energy coming from the ATP-ADP-P system have been transfered to the
>B-C system and have increased its energy. We may call this "energy accepted
>by the B-C system" (not "work done on the B-C system" since this last concept
>is reserved for delta G):

>    E = (delta H)o  -  (delta H)c                             /3/

>where (delta H)o is the enthalpy of the driving reaction (ATP = ADP + P)
>and (delta H)c is the enthalpy of the coupled reaction /2/.
>   Note how useful the relation /3/ is. First, it defines a valuable
>quantity - the energy accepted and stored by a chemical system. If, for
>instance, B = C is some biosynthesis,  /3/ gives the energy content of
>the respective structure acquired during the process. Second, /3/ is
>concentration-independent so far as both enthalpies are independent.
>Third, the experimental determination of /3/ is extremely easy.

>Let us now see what the delta G concept says about the same coupled
>reaction /2/. It says that, when /2/ is close to equilibrium, the work
>done by the ATP-ADP-P system on the B-C system is

>     W = -(delta Go + RTln((ADP)(P)/(ATP)))                      /4/

>where delta Go is the standard free energy of the reaction ATP = ADP + P.

>Note that E and W are independent. I spent a lot of effort in trying to
>show that they are incompatible, but failed. They are just independent -
>two different worlds - we are to choose the more cosy one. So let me
>describe three possible cases. In all of them the reactions /2/ are CLOSE
>TO EQUILIBRIUM, THE ENTHALPIES ARE THE SAME AND ONLY THE DELTA G VALUES
>OF THE ATP-ADP-P SYSTEM DIFFER.
>1. E = 10 KJ/mole, i.e. the system B-C accepts 10 KJ/mole energy. However
>delta G for the ATP system is -15 KJ/mole, i.e. the ATP system does
>15 KJ/mole work on the B-C system (W = 15 KJ/mole).

>2. E = 10 KJ/mole, i.e. the system B-C accepts 10 KJ/mole energy. However
>delta G for the ATP system is -5 KJ/mole, i.e. the ATP system does
>5 KJ/mole work on the B-C system (W = 5 KJ/mole).

>3. E = 10 KJ/mole, i.e. the system B-C accepts 10 KJ/mole energy. However
>delta G for the ATP system is 5 KJ/mole, i.e. the ATP system GETS
>5 KJ/mole work FROM the B-C system (W = -5 KJ/mole).

>All three cases are real (in the sense that the combinations of delta H and
>delta G values can exist) and, within the definitions, all statements in
>them are correct. However common sense tells us that it would be better
>to define "the energy the system B-C accepts" as "the work done on the B-C
>system"; i.e. to reject the physically meaningless delta G definition of
>work and adopt one whose usefulness seems obvious. In other words, I
>propose to adopt /3/ as a natural definition of chemical work.
>   Now I am waiting for your comments.

Pentcho

First of all, since /3/ is not a definition of work within the framework
of thermodynamics, any problems you may see with it will be the result
of your definition, not any problems with thermodynamics.  And what do
you propose to do for a reaction where the volume does change? It seems
odd that a definition for chemical work should only be applicable if the
reaction occurs in an incompressible fluid.

Since reaction /2/ contains the ATP->ADP+P system, what you want to do
is not so simple to arrange.  You need to adjust all the concentrations
(ATP, ADP, P, B and C).  Possible of course, but in order to have /2/
at equilibrium in case 3.  requires a larger concentration of B (relative
to C) than for case 1.  More about this point later.

I get the impression that you are bothered by the idea that the amount
of work which a reaction can do is dependent on the concentration of the
reactants and products. I am not bothered, it seems perfectly reasonable
to me.  Consider your three cases, you say that all three are near 
equilibrium.  If we assume they are all at equilibrium, then no further
net reaction occurs in any of the three cases, and no work occurs at all.
For every set of molecules which react in the forward direction, a set
reacts in the backwards direction.  i.e. Delta G = 0, seems the appropriate
measure for the amount of work that can be done, not E = 10 kJ/mole.  

Consider just the ATP hydrolysis for the moment.  With or without an
enzyme, both the forward and back reactions are present.  For the type of
systems we are discussing now, the back reaction is so slow that we can
neglect it.  However, that is because most of the time when we study
these systems the reaction is far from equilibrium (lots of ATP, little
ADP).  Consider the case where the hydrolysis is close to equilibrium,
which means a lot of ADP and P, and very little ATP.  Since at equilibrium,
the forward and back reactions are equal, does it really seem so odd that
the reaction cannot perform any useful work? (Delta G = 0).

Now consider B -> C.  If the concentration of B is so much larger than
that of C, that (Delta G) for the B -> C reaction is negative, then
a net forward reaction will be observed.  (Of course, it may not be
proceeding fast enough to be biologically useful, so the enzyme may
still be necessary for the organism to survive.)  Your case 3 would
seem to be such a case.  In order for (Delta G) for the ATP hydrolysis
to be positive, it would require that there be so little ATP present
(relative to the amount of ADP and P) that the back reaction was
faster than the forward reaction.  Inorder for the overall reaction
(/2/) to be at equilibrium, the (Delta G) for the B->C reaction alone,
must be negative, so that the forward B->C reaction was favored.  If
(Delta G) for the total reaction was slightly negative, reaction /2/
would proceed in the direction shown, and in that case the B->C reaction
does indeed do work on the ATP -> ADP+P reaction.  The B->C reaction goes
towards equilbrium, while the ATP hydrolysis is pushed farther away from
equilibrium.  This should not be surprising.  If the concentrations are
such that the back reaction of ATP -> ADP + P, was favored, you wouldn't
expect the forward reaction to be able to do any work would you?

Finally, it appears that you would be happier with a chemical work which
was the same for all three of your cases.  However, I would not. The
further away you are from equilibrium, the more out of balance the
forward and backward rates will be. It should take more work to push
the reaction still further out of equilibrium, because the system has
to overcome a greater tendency for the reaction to go the other way.

Regards,
Bryant

From owner-biophysics@net.bio.net Mon Dec 01 22:00:00 1997
Path: biosci!daresbury!not-for-mail
From: Pentcho Valev <RUMYM@BGEARN.ACAD.BG>
Newsgroups: bionet.biophysics
Subject: Chemical work (reply to Bryant Fujimoto)
Date: 2 Dec 1997 09:41:03 -0000
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Bryant, you wrote:>>>>>>>>>
Consider just the ATP hydrolysis for the moment.  With or without an
enzyme, both the forward and back reactions are present.  For the type of
systems we are discussing now, the back reaction is so slow that we can
neglect it.  However, that is because most of the time when we study
these systems the reaction is far from equilibrium (lots of ATP, little
ADP).  Consider the case where the hydrolysis is close to equilibrium,
which means a lot of ADP and P, and very little ATP.  Since at equilibrium,
the forward and back reactions are equal, does it really seem so odd that
the reaction cannot perform any useful work? (Delta G = 0).<<<<<<<<

It does seem odd to me. Let us assume that the equilibrium of ATP
hydrolysis

          ATP <-> ADP + P                                    /1/

were a bit more "normal", i.e. the back reaction were not so slow and
the equilibrium ATP concentration not so low. I hope you would agree that
both assumptions are realistic and have nothing to do with the second law.
However, as the ATP system drives the reaction  B -> C:

       ATP + B  -> ADP + P + C                                   /2/

the equilibrium of the ATP system would be restored by the not-so-slow
back reaction. Since this back reaction is endothermic, the whole process
amounts to a cycle in which heat is absorbed from the environment and
converted into.....?

    Two questions arise here. 1. Is this quantity into which the equilibrium
ATP system converts the heat valuable (potentially, of course - nobody has
analysed it yet)? If yes, I will show later that we can call it H-work
(H denotes enthalpy) as opposed to G-work (G is free energy) which is also
very important for living systems.

2. If the equilibrium of the ATP system is not "normal" and living systems
cannot build the above heat engine, can we suspect that they may have made
amendments so that some perfectioned reaction is much more suitable for
an isothermal heat engine? I believe we can - I need to think a bit more
and will present the case.

Best regards,
Pentcho

From owner-biophysics@net.bio.net Tue Dec 02 22:00:00 1997
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From: saudekv@synbio.tpgnet.net (Vladimir Saudek)
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Subject: Protein Modeller
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Synthelabo Biomoleculaire            
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From owner-biophysics@net.bio.net Tue Dec 02 22:00:00 1997
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From: Justin Lee <cjl2@columbia.edu>
Newsgroups: bionet.biophysics
Subject: Mini Analysis Program
Date: Wed, 03 Dec 1997 13:31:50 -0500
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--
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Phone (212) 305-3817
Fax (212) 305-5775
e-mail cjl2@columbia.edu
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From owner-biophysics@net.bio.net Tue Dec 02 22:00:00 1997
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From: smith@umes07.avl.co.at (Search Spaniel)
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From owner-biophysics@net.bio.net Wed Dec 03 22:00:00 1997
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From: "Miguel A. Talavera" <miguel.talavera@yale.edu>
Newsgroups: bionet.biophysics
Subject: General information about Centrifugation
Date: Thu, 04 Dec 1997 04:37:50 -0500
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I would like to know what type of information can you get from a
velocity sedimentation experiment, and from an equilibrium sedimentation
experiment. Also, what other alternate methods might give the each type
of information.




From owner-biophysics@net.bio.net Wed Dec 03 22:00:00 1997
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From: fujimoto@u.washington.edu (Bryant Fujimoto)
Newsgroups: bionet.biophysics
Subject: Re: Chemical work (reply to Bryant Fujimoto)
Date: 4 Dec 1997 09:04:52 GMT
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Pentcho Valev <RUMYM@BGEARN.ACAD.BG> writes:

>Bryant, you wrote:>>>>>>>>>
>Consider just the ATP hydrolysis for the moment.  With or without an
>enzyme, both the forward and back reactions are present.  For the type of
>systems we are discussing now, the back reaction is so slow that we can
>neglect it.  However, that is because most of the time when we study
>these systems the reaction is far from equilibrium (lots of ATP, little
>ADP).  Consider the case where the hydrolysis is close to equilibrium,
>which means a lot of ADP and P, and very little ATP.  Since at equilibrium,
>the forward and back reactions are equal, does it really seem so odd that
>the reaction cannot perform any useful work? (Delta G = 0).<<<<<<<<

>It does seem odd to me. Let us assume that the equilibrium of ATP
>hydrolysis

>          ATP <-> ADP + P                                    /1/

>were a bit more "normal", i.e. the back reaction were not so slow and
>the equilibrium ATP concentration not so low. I hope you would agree that
>both assumptions are realistic and have nothing to do with the second law.
>However, as the ATP system drives the reaction  B -> C:

>       ATP + B  -> ADP + P + C                                   /2/

>the equilibrium of the ATP system would be restored by the not-so-slow
>back reaction. Since this back reaction is endothermic, the whole process
>amounts to a cycle in which heat is absorbed from the environment and
>converted into.....?

In your example there are two pathways /1/ and /2/.  If the concentrations
of ATP, ADP and P are such that the hydrolysis of ATP will in fact drive
reaction /2/ forward, then pathway /1/ will show a net flow in the forward
direction as well.  That is under these conditions pathway /1/ will produce
a net hydrolysis of ATP, not a net production of ATP.  

As for it being odd that a chemical reaction at equilibrium can't do
any work - consider an electric battery, when the chemical reaction
inside is at equilibrium, the battery is dead.

>    Two questions arise here. 1. Is this quantity into which the equilibrium
>ATP system converts the heat valuable (potentially, of course - nobody has
>analysed it yet)? If yes, I will show later that we can call it H-work
>(H denotes enthalpy) as opposed to G-work (G is free energy) which is also
>very important for living systems.

I hope I didn't give you the impression that I didn't think the enthalpy
was important.  I only noted that it isn't a good representation of the
work being done.  Note that at constant P, if the system does only 
displacement work (i.e. no chemical work), then (Delta H) is the heat
absorbed by the system.

>2. If the equilibrium of the ATP system is not "normal" and living systems
>cannot build the above heat engine, can we suspect that they may have made
>amendments so that some perfectioned reaction is much more suitable for
>an isothermal heat engine? I believe we can - I need to think a bit more
>and will present the case.

Pentcho
  I'm sure you are already aware that your proposed heat engine violates
the laws of thermodynamics, and that you are not going to be deterred
by that.  So as you think about this, remember that all of the reactions
in your cycle will have both a forward and back rate. As noted above
for your ATP cycle, if you keep track of all the rates, you will see
that the heat engine will not work.  A mechanical analog of this is the
osmotic pressure perpetual motion machine you tried to build.  If you
remember, you were hoping to create a system where solvent would flow
from the left chamber to the right chamber at the upper membrane, and
from the right chamber to the left chamber at the lower membrane. 
As you reported, this didn't work.  You had left the reverse flow of
solvent at the two membranes (R->L at the upper membrane, and L->R at
the lower membrane) out of your considerations and you discovered that
they have to be considered when describing the system.

Regards,
Bryant 

From owner-biophysics@net.bio.net Wed Dec 03 22:00:00 1997
Path: biosci!daresbury!not-for-mail
From: Pentcho Valev <RUMYM@BGEARN.ACAD.BG>
Newsgroups: bionet.biophysics
Subject: Work done by a reaction at equilibrium
Date: 4 Dec 1997 16:29:14 -0000
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I wrote:>>>>>>>>>>>>>>
>It does seem odd to me. Let us assume that the equilibrium of ATP
>hydrolysis

>          ATP <-> ADP + P                                    /1/

>were a bit more "normal", i.e. the back reaction were not so slow and
>the equilibrium ATP concentration not so low. I hope you would agree that
>both assumptions are realistic and have nothing to do with the second law.
>However, as the ATP system drives the reaction  B -> C:

>       ATP + B  -> ADP + P + C                                   /2/

>the equilibrium of the ATP system would be restored by the not-so-slow
>back reaction. Since this back reaction is endothermic, the whole process
>amounts to a cycle in which heat is absorbed from the environment and
>converted into.....?<<<<<<<<<<<<<<<<<<<<<<

Bryant Fujimoto replied:>>>>>>>>>>>
In your example there are two pathways /1/ and /2/.  If the concentrations
of ATP, ADP and P are such that the hydrolysis of ATP will in fact drive
reaction /2/ forward, then pathway /1/ will show a net flow in the forward
direction as well.  That is under these conditions pathway /1/ will produce
a net hydrolysis of ATP, not a net production of ATP.<<<<<<<<<<<<<

I did not claim that there would be a net production of ATP. Let there be,
initially, a great amount of B and no C. Also, let the reaction  /1/ be at
equilibrium. At the end of the process, both reactions /1/ and /2/ would
be at equilirium. All along the back reaction in /1/ has absorbed heat
from the environment whereas the forward reaction has transfered, in /2/, this
energy to the B-C system. If B -> C is some biosynthesis, this energy can
be thought of as stored in the respective synthesized structure.

In fact, if the reaction B -> C is a biosynthesis, the reaction /2/ never
goes backwards, so the only problem biosystems face is the abnormal
equilibrium of /1/. They have solved this problem by replacing /1/ with
a reaction in which the equilibrium concentration of ATP is not so low and
the back reaction not so slow. However the price to pay was that one of
the reagents in this new reaction - H+, had to be constantly transfered
through the membrane. So H+ translocation is not an energy storage -
rather, it is a regulatory process. Of course, the story is much longer
than that.

Best regards,
Pentcho

From owner-biophysics@net.bio.net Wed Dec 03 22:00:00 1997
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From: Pentcho Valev <RUMYM@BGEARN.ACAD.BG>
Newsgroups: bionet.biophysics
Subject: Chemical work and delta G
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Bryant Fujimoto wrote:>>>>>>>>>>>
Finally, it appears that you would be happier with a chemical work which
was the same for all three of your cases.  However, I would not. The
further away you are from equilibrium, the more out of balance the
forward and backward rates will be. It should take more work to push
the reaction still further out of equilibrium, because the system has
to overcome a greater tendency for the reaction to go the other way.<<<<<<

I believe that your last sentence is based on wrong intuition - you just
feel that something should be done against a greater tendency and call it
work, but then refuse to consider the real energy transfer in the system -
after all, work production is always energy transfer - otherwise things
would become too mystical.

We can easily solve the problem by comparing the work done by the ATP
system with other works which do obey the dellta G definition. Let us
consider a simplest galvanic system:

     Zn2+ (high conc.), Zn II  Zn,  Zn2+ (low conc.)

The useful (electric) work done by this system does obey the delta G
definition, but note that the energy transfer is specific and definite:
HEAT IS ABSORBED FROM THE ENVIRONMENT AND CONVERTED INTO USEFUL WORK.

Now let us consider a simplest osmotic system:

     H+ (high conc.)             M                H+ (low conc.)

As H+ crosses the membrane (M) down the concentration gradient, it can
do osmotic work which also obeys the delta G definition. However, again,
HEAT IS ABSORBED FROM THE ENVIRONMENT AND CONVERTED INTO WORK. In other
words, we know the origin of the energy and can imagine the physical
picture of energy transfer to the system on which work is done.

In fact, my analysis of the work done by the ATP system was based on the
same principle. I defined the origin of the energy (it is the internal
energy of ATP molecules) and described quantitatively the transfer of
this energy to the system on wich work is done (it was the B-C system).
Unfortunately, this energy transfer does not obey the delta G definition -
it obeys another one based on the enthalpy concept, so it seems suitable
to name this kind of work "H-work", as opposed to "G-work" done in
galvanic and osmotic systems.

Of course, you may insist that, in the last case, delta G accounts for
something (e.g the distance from equilibrium or the tendency to move
towards equilibrium), but this something has nothing to do with the
ENERGY TRANSFERED FROM THE "WORKING" SYSTEM TO THE SYSTEM ON WHICH
WORK IS DONE. In other words, you would insist upon a definition of
work not based on the first law of thermodynamics.

Best regards,
Pentcho

From owner-biophysics@net.bio.net Thu Dec 04 22:00:00 1997
Newsgroups: bionet.biophysics
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From: "Ulrich T. Riedel" <Ulrich.T.Riedel@Bristol.ac.uk>
Subject: 0.002 mm Droplets: How to produce them?
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For my research I have to apply droplets (1000-2000 nanometer
(0.001-0.002 mm) in diameter and about 100 nm in height) to a surface to
protect the volume below the droplet during successive treatments.

Therefore the material of the droplets has to have the following
properties:

- the substance should be a fluid which turns into a solid with the
mentioned properties in a couple of minutes after application;
- it has to stick very well on an inorganic, polar surface
(hydroxyapatite with intercalated organic substance and water), which
may be uneven;
- it has to be chemically stable (meaning: it should not swell in water
and should not react in any way with acids);
- the surface of the substance should be completely dry and solid
(meaning no liquid layer apart from the always existing water layer
should be around).
- it should be possible to create little droplets of the above mentioned
size. The size can be slightly arbitrary, since it can be measured after
application.

Any ideas, what substance and which application technique could be used,
would be _HIGHLY_ appreciated.

Thanks and Regards,
  Ulrich Riedel

From owner-biophysics@net.bio.net Thu Dec 04 22:00:00 1997
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From: jamesl@healthtech.com (James W. Larkin)
Newsgroups: bionet.biophysics,bionet.molbio.proteins.fluorescent,sci.chem.electrochem
Subject: Call for Papers Advances in MOLECULAR LABELS, SIGNALING & DETECTION
Date: 5 Dec 1997 16:20:33 GMT
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Xref: biosci bionet.biophysics:3776 bionet.molbio.proteins.fluorescent:1768

First Announcement and Call for Papers

Cambridge Healthtech Institute’s Second Annual
Advances in MOLECULAR LABELS, SIGNALING & DETECTION: 
Enhancing Sensitivity, Accuracy and Speed
May 4-5, 1998
San Diego Hilton

Extending the limits of assay sensitivity and accuracy, at the same 
time meeting the demand for greater speed, requires the application 
of innovative techniques and systems.  The development of new probes 
and labels, homogeneous assay designs, and approaches which allow 
for the direct detection of compounds or specific binding events are 
having an impact in basic research, diagnostic and drug development 
segments.  Novel fluorescent and luminescent technology are also 
critical for the implementation of greater speed and automation.  
These advances are being applied to the detection, quantification 
and localization of gene sequences, proteins, infectious organisms 
and a variety of other targets.

Researchers are encouraged to submit a proposal  for presentation of 
their own work.  Recommendations for other speakers to be considered 
are also welcomed.  Among the topics to be covered are:

Novel Probes and Labels
New Homogeneous Assays
Methods for Direct (Non-amplified) Quantitation
Methods for Ultra-Sensitive Detection
Novel Fluorescent Assay Systems
New Luminescent Approaches

Please submit proposal or suggestions by e-mail or fax to:

Mary Chitty
Conference Director
e-mail:  mchitty@healthtech.com
fax:      617-630-1325
telephone: 617-630-1316

For full consideration and to allow time for followup, please submit 
proposal or suggestions by December 12, 1997.


From owner-biophysics@net.bio.net Fri Dec 05 22:00:00 1997
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From: "Dr E. Buxbaum" <EB15@le.ac.uk>
Newsgroups: bionet.biophysics
Subject: Re: General information about Centrifugation
Date: Fri, 05 Dec 1997 14:45:40 -0800
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Miguel A. Talavera wrote:
> 
> I would like to know what type of information can you get from a
> velocity sedimentation experiment, and from an equilibrium sedimentation
> experiment. Also, what other alternate methods might give the each type
> of information.

Still a good source of introductory information is "The
Ultracentrifuges" by Svedberg, despite being 50 years old.
"Ultracentrifugation - A Practical Approach" is also usefull and
somewhat more modern. Have a look at your library what they have, there
are quite a few good books out there.

From owner-biophysics@net.bio.net Sat Dec 06 22:00:00 1997
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From: "Jonathan B. Marder" <marder@agri.huji.ac.il>
Newsgroups: bionet.biophysics
Subject: Re: Verification of the second law (reply to Bryant Fujimoto)
Date: Sun, 7 Dec 1997 09:15:45 +0200
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Pentcho Valev wrote in message +ADw-65p1ju+ACQ-7ke+AEA-mserv1.dl.ac.uk+AD4-...
...
+AD4-   Let the reaction
+AD4-
+AD4-      ATP  +AD0-  ADP    P                                      /1/
+AD4-
+AD4-drive another reaction, e.g.  B +AD0- C, isothermally and isobarically:
+AD4-
+AD4-      ATP  B  +AD0-  ADP  P  C                                /2/
+AD4-
+AD4-As one mole ATP is used up in the reaction, the energy of the system
+AD4-ATP-ADP-P  dereases by 20 KJ/mole (since the enthalpy of ATP hydrolysis
+AD4-is  -20 KJ/mole). Let us also assume that the enthalpy of /2/ is shown
+AD4-experimentally to be  -10 KJ/mole. ...

Pentcho,
  Free energy (deltaG) is a much more useful concept than enthalpy for
looking at this.
You can easily split up the reaction into its component parts:
1. deltaG+AHs-ATP+AH0- +AD0- deltaG'+AHs-ATP+AH0- +- RT ln +AFs-ATP+AF0-/+AFs-ADP+AF0-
2. deltaG+AHs-B+AD0-C+AH0- +AD0- deltaG'+AHs-B+AD0-C+AH0- +- RT ln +AFs-B+AF0-/+AFs-C+AF0-

The overall deltaG for the coupled reaction is the total. Thus
deltaG+AHs-ATP+AH0- can be negative
and deltaG+AHs-B+AD0-C+AH0- positive, but it is the overall total which defines the
equilibrium of the
coupled reaction. This approach is straightforward and adequate even for
very complicated
systems where you may have to (additively) include many subsystems.
In contrast, using enthalpy changes is less useful since it doesn't
easily take account of
reactant concentrations. Furthermore, you forget that overall deltaG'
can be easily
measured simply by looking at the equilibrium concentrations under
standard conditions.

Pentcho,
  I really think that you are beating a dead horse. I suggest that you
go back to your original
perpetual motion example (the semipermeable membrane) and do a full
+ACI-deltaG+ACI- analysis taking
account of ALL the steps in the cycle. I think that you will find that
your subsequent ion-movement
models are simply a variant on the same idea. In each case, I think you
will find that the system will
arrive at equilibrium+ACE-

I hope that my comments are useful, but in any case, I do not intend to
pursue this until Pentcho or
someone else can come up with something more substantive.

Jonathan B. Marder   +ADw-MARDER+AEA-agri.huji.ac.il+AD4-
Department of Agricultural Botany, The Hebrew University of Jerusalem
Faculty of Agriculture, P.O.Box 12, Rehovot 76100, ISRAEL
Phone: +-972 8 9481918   Fax:   +-972 8 9467763
Web page:    http://www.agri.huji.ac.il/+AH4-marder




From owner-biophysics@net.bio.net Sat Dec 06 22:00:00 1997
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From: fujimoto@u.washington.edu (Bryant Fujimoto)
Newsgroups: bionet.biophysics
Subject: Re: Work done by a reaction at equilibrium
Date: 7 Dec 1997 09:59:06 GMT
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Pentcho Valev <RUMYM@BGEARN.ACAD.BG> writes:


>Pentcho wrote:>>>>>>>>>>>>>>
>>It does seem odd to me. Let us assume that the equilibrium of ATP
>>hydrolysis

>>          ATP <-> ADP + P                                    /1/

>>were a bit more "normal", i.e. the back reaction were not so slow and
>>the equilibrium ATP concentration not so low. I hope you would agree that
>>both assumptions are realistic and have nothing to do with the second law.
>>However, as the ATP system drives the reaction  B -> C:

>>       ATP + B  -> ADP + P + C                                   /2/

>>the equilibrium of the ATP system would be restored by the not-so-slow
>>back reaction. Since this back reaction is endothermic, the whole process
>>amounts to a cycle in which heat is absorbed from the environment and
>>converted into.....?<<<<<<<<<<<<<<<<<<<<<<

>Bryant Fujimoto replied:>>>>>>>>>>>
>In your example there are two pathways /1/ and /2/.  If the concentrations
>of ATP, ADP and P are such that the hydrolysis of ATP will in fact drive
>reaction /2/ forward, then pathway /1/ will show a net flow in the forward
>direction as well.  That is under these conditions pathway /1/ will produce
>a net hydrolysis of ATP, not a net production of ATP.<<<<<<<<<<<<<

>Pentcho wrote:>>>>>>>>>>>>>>
>I did not claim that there would be a net production of ATP. Let there be,
>initially, a great amount of B and no C. Also, let the reaction  /1/ be at
>equilibrium. At the end of the process, both reactions /1/ and /2/ would
>be at equilirium. All along the back reaction in /1/ has absorbed heat
>from the environment whereas the forward reaction has transfered, in /2/, this
>energy to the B-C system. If B -> C is some biosynthesis, this energy can
>be thought of as stored in the respective synthesized structure.

Pentcho
  You initially stated that the ATP hydrolysis was driving the B->C
reaction.  This means that /1/ cannot be at equilibrium.  When reading
your post, I missed the fact that you wanted /1/ to be at equilibrium.
That is, I missed the fact that you made two contradictory statements
about your system.

  If /1/ is at equilibrium and there is no C, then the hydrolysis of
ATP does not drive the B->C reaction.  For the particular initial
conditions which you specify (which probably do not occur naturally),
the B->C reaction drives the hydrolysis of ATP.

>In fact, if the reaction B -> C is a biosynthesis, the reaction /2/ never
>goes backwards, so the only problem biosystems face is the abnormal
>equilibrium of /1/. 

  Never say never.  What if the organism decides it doesn't need any
more C and shuts the biosynthesis down?  In any event, while the
biosynthesis is running reaction /2/ will never exhibit a _net_
backwards reaction.  However, there will be some back reaction, it
will just be much smaller than the forward reaction.  

  What do you mean by an abnormal equilibrium?  Reaction /1/ is not
at equilibrium in a living organism.  Its out of equilibrium, and the
organism uses that fact to drive other reactions.

Regards
Bryant

>They have solved this problem by replacing /1/ with
>a reaction in which the equilibrium concentration of ATP is not so low and
>the back reaction not so slow. However the price to pay was that one of
>the reagents in this new reaction - H+, had to be constantly transfered
>through the membrane. So H+ translocation is not an energy storage -
>rather, it is a regulatory process. Of course, the story is much longer
>than that.


From owner-biophysics@net.bio.net Sat Dec 06 22:00:00 1997
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From: fujimoto@u.washington.edu (Bryant Fujimoto)
Newsgroups: bionet.biophysics
Subject: Re: Chemical work and delta G
Date: 7 Dec 1997 10:40:06 GMT
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Pentcho Valev <RUMYM@BGEARN.ACAD.BG> writes:

>Bryant Fujimoto wrote:>>>>>>>>>>>
>Finally, it appears that you would be happier with a chemical work which
>was the same for all three of your cases.  However, I would not. The
>further away you are from equilibrium, the more out of balance the
>forward and backward rates will be. It should take more work to push
>the reaction still further out of equilibrium, because the system has
>to overcome a greater tendency for the reaction to go the other way.<<<<<<

>I believe that your last sentence is based on wrong intuition - you just
>feel that something should be done against a greater tendency and call it
>work, but then refuse to consider the real energy transfer in the system -
>after all, work production is always energy transfer - otherwise things
>would become too mystical.

>We can easily solve the problem by comparing the work done by the ATP
>system with other works which do obey the dellta G definition. Let us
>consider a simplest galvanic system:

>     Zn2+ (high conc.), Zn II  Zn,  Zn2+ (low conc.)

>The useful (electric) work done by this system does obey the delta G
>definition, but note that the energy transfer is specific and definite:
>HEAT IS ABSORBED FROM THE ENVIRONMENT AND CONVERTED INTO USEFUL WORK.

>Now let us consider a simplest osmotic system:

>     H+ (high conc.)             M                H+ (low conc.)

>As H+ crosses the membrane (M) down the concentration gradient, it can
>do osmotic work which also obeys the delta G definition. However, again,
>HEAT IS ABSORBED FROM THE ENVIRONMENT AND CONVERTED INTO WORK. In other
>words, we know the origin of the energy and can imagine the physical
>picture of energy transfer to the system on which work is done.

Pentcho
  I think we went through this once before, and I didn't give a very
good response, so lets try again.  Particularly, since it demonstrates
why you can't use the enthalpy for work.  Consider your simple osmotic
system.  The enthalpy for the transfer of H+ from the left to the right
at constant pressure is zero.  This is true regardless of whether any
work is done during this process or not.  Now, to understand why this
is so, you need to understand the physical interpretation of the
enthalpy.  Starting from the first law of thermodynamics and H=U+pV,
we can derive that at constant pressure (Delta H) is equal to the heat
absorbed by the system plus any non-displacement work done on the
system.  At constant P, 

  Wu = (non-displacement work) = (Total work) - (-p(Delta V))

(-p(Delta V) is the displacement work done on the system). So at
constant P

  (Delta H)  = q + Wu

Wu contains any chemical work which might be done. Up to this point,
we need only the first law of thermodynamics, so if you don't like
this, you will have to discard the first law as well.  This is why
using the enthalpy for the work is problematic, since it contains
both heat and work, and as we shall see, it can be distributed between
q and Wu in many different ways for the same value of Delta H.

Now, if the diffusion of H+ across the membrane is not coupled to any
reaction, then net diffusion of H+ does no chemical work and Wu=0.
Since (Delta H = 0), we get q = 0.  That is, no heat absorption.
So far so good.  What if the diffusion of H+ is coupled to a 
chemical reaction?  In that case Wu < 0 (the diffusion is doing
work on something else), and so since Delta H is still zero,
we get q > 0, and q = |Wu|.  That is the heat absorbed equals the
work done.  The more work done, the larger q is.

>In fact, my analysis of the work done by the ATP system was based on the
>same principle. I defined the origin of the energy (it is the internal
>energy of ATP molecules) and described quantitatively the transfer of
>this energy to the system on wich work is done (it was the B-C system).
>Unfortunately, this energy transfer does not obey the delta G definition -
>it obeys another one based on the enthalpy concept, so it seems suitable
>to name this kind of work "H-work", as opposed to "G-work" done in
>galvanic and osmotic systems.

As I point out, it doesn't obey your concept of H-work.  I don't
recall your giving a good reason why this doesn't obey "G-work"
as you call it.  After all, Delta G for the diffusion of H+ from left
to right in your system is negative, which means it can do work on
another system.  Delta G would be maximum available, how much is 
actually done depends on the details of the system. On the other hand,
(Delta H) is zero regardless of how much work is done, which it makes
it difficult to see how you would use it for the work.

>Of course, you may insist that, in the last case, delta G accounts for
>something (e.g the distance from equilibrium or the tendency to move
>towards equilibrium), but this something has nothing to do with the
>ENERGY TRANSFERED FROM THE "WORKING" SYSTEM TO THE SYSTEM ON WHICH
>WORK IS DONE. In other words, you would insist upon a definition of
>work not based on the first law of thermodynamics.

Pentcho
  I pointed out before that Delta G is maximun amount of
non-displacement work which a reaction can perform on its surroundings
(at constant T and P).  How much work is actually done depends on
the efficiency of the transfer.  There is no contradiction between
this and the first law.  Notice that my description of Delta G does
not claim it represents all the energy in the system, only that which
is available to do Wu.

Regards
Bryant 

From owner-biophysics@net.bio.net Sat Dec 06 22:00:00 1997
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From: Marcel Hofman <ECB9.ORCOM@skynet.be>
Newsgroups: bionet.biophysics
Subject: ECB9 ninth European congress on Biotechnology has a  website you might visit
Date: Sun, 07 Dec 1997 19:24:18 +0100
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ECB9 ninth European congress on Biotechnology has a  website you might
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From owner-biophysics@net.bio.net Sat Dec 06 22:00:00 1997
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From: Pentcho Valev <RUMYM@BGEARN.ACAD.BG>
Newsgroups: bionet.biophysics
Subject: What delta G cannot explain (reply to Bryant).
Date: 7 Dec 1997 12:01:56 -0000
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Bryant, when I wrote my previous message, I had not received your last one,
so mine was nervous and ultimative - sorry about that. Now I see that
the discussion still makes sense.

You are right that, for the osmotic system, the delta G concept is better
than the one based on the enthalpy. You are also right that the enthalpy
concept does not distinguish between Q and Wu. Still I insist that, except
for galvanic and osmotic systems, what I call H-work is the only
meaningful concept describing chemical work.

Let the reaction A -> B drive the reaction  C -> D :

       A + C -> B + D                                    /1/

The only question we ask for the moment is: How much energy is accumulated
by the C-D system for one stoichiometric unit of reaction? It is not
diffucult to see that this quantity is

       E = (delta H)c - (delta H)o                         /2/

where (delta H)o is the enthalpy change of the reaction  A -> B  and
(delta H)c is the enthalpy change of the coupled reaction /2/.

Now what is this E? Part of it may indeed come from the reaction A -> B,
but the other part is simply due to the fact that the reaction C -> D
is itself endo(exo)thermic. So E cannot be called true work. In the
osmotic system, the true work is delta G whereas the thermal component
in E makes it "contaminated" work.

   However, for ATP driven reactions, E is the ONLY quantity reflecting
the real energy flow in the system. It is again "contaminated" - we
can never know what part of E comes from ATP (i.e. is "true" work) and
what part is just absorbed from the environment. Still it is valuable
in itself - it is a direct measure of energy accumulation in living
systems. In this sense it does not reject the delta G concept of work -
it just explains something that delta G cannot explain. The whole problem
is whether this something makes sense. I still believe that the adequate
interpretation of energy accumulation in living systems makes a lot
of sense.

Best regards,
Pentcho

From owner-biophysics@net.bio.net Sat Dec 06 22:00:00 1997
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Newsgroups: bionet.biophysics
Subject: What thermodynamics cannot explain (reply to Bryant).
Date: 7 Dec 1997 11:00:20 -0000
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Bryant, unfortunately there is too much misunderstanding again - I am
again to blaim for imprecise statements and earlier mistakes. So I would
like to state the problem clearly and briefly - if nobody finds it
important, the discussion would be really pointless.
   Let there be an energy-consumming reaction:

                   B -> C                                     /1/

It could be a biosynthesis - B are the building blocks and C is some
biopolimer structure. We do not know where the equilibrium of the reaction
lies, but in any event it must be driven by some energy-transfering
reaction. The energy transfered is accumulated in the synthesized structure
and is expressed by the concept of H-work that I am trying in vain to
introduce.

Now please tell me: do you find the energy accumulated during biosynthesis
an important quantity? If yes, we will have to go beyond the thermodynamic
restrictions. But maybe this quantity is unimportant or just does not
exist? Then I see no reason to obtrude any more.

Best regards,
Pentcho

From owner-biophysics@net.bio.net Wed Dec 10 22:00:00 1997
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From: "Schuricht S.I.N.N." <cs@schuricht.de>
Newsgroups: bionet.biophysics
Subject: TESTING DEVICES  FOR   ENVIRONMENTAL   MEASURING   TECHNOLOGY
Date: Thu, 11 Dec 1997 10:40:29 +0100
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TESTING DEVICES  FOR   ENVIRONMENTAL   MEASURING   TECHNOLOGY

http://www.schuricht.de/schudynae/schuhome?pStockNo=17.463.30 
prices are DM(DeutschMark)


From owner-biophysics@net.bio.net Wed Dec 10 22:00:00 1997
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From: villowan@earthlink.net (Charlsie Patterson)
Newsgroups: bionet.biophysics
Subject: ]][[ Sr/Principal R & D Scientist B9710
Date: Thu, 11 Dec 1997 18:03:26 GMT
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My client company is a large, well established pharmaceutical
company, who is aggressively seeking to fill this position and several
others at the first of the year.  It is in the area of research and
development.  They offer excellent compensation and benefit, as well
as great growth potential.  The client company will pay all fees
associated with recruiting and placement of candidates. The position
is located in North Carolina.

Please refer to Job Listing B9710b  in all correspondence

To submit your CV or have any questions answered, please contact:

Ms. Charlsie Patterson
Technical and Bio-Science Recruiter
Global Staffing and Recruiting
(919) 871-0070
Fax: (919) 871-0030
email: techsearch@globals-r.com
and/or villowan@earthlink.net

Sr. Associate Research Scientist/Principal Associate Research
Scientist-R & D


Brief Description of the Position:

This position is for a research scientist who will stabilize
therapeutic plasma proteins using formulation and lypholization
techniques.  The incumbent will be a team member to develop new freeze
dryer cycles and will have the opportunity to work with various other
site projects.

Position Requirements:

MS in Life Sciences or Engineering with 2+ years or more of relevant
pharmaceutical experience or equivalent combination of education and
experience.  The successful candidate must have extensive experience
with protein biochemistry and methods of protein stabilization, be
proficient with analytical equipment (DSC, FTIR, HPLC, nIR) and be
able to interpret results.  The ability to analyze data independently,
as well as present the data within a team environment is a must.
Computer experience and familiarity with various databases helpful.

PLEASE NOTE:  Hepatitis B immunization is required.



From owner-biophysics@net.bio.net Wed Dec 10 22:00:00 1997
Path: biosci!daresbury!not-for-mail
From: Pentcho Valev <RUMYM@BGEARN.ACAD.BG>
Newsgroups: bionet.biophysics
Subject: Delta G vs. Delta H
Date: 11 Dec 1997 13:47:36 -0000
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In reply to Bryant Fujimoto

Bryant, my choice of delta H as a measure of chemical work is based on the
following simple physical picture:

The ATP system interacts with another system. As one mole ATP is used up,
the energy of the other system increases by 10 KJ. These 10 KJ are the
only real physical quantity showing the changed energetics of the second
system, so I am inclined to think of it as "work done on the second system".
Of course, I am ready to consider other definitions of "work done on the
second system", but expect them to be in harmony with the first law - if
work is done on the second system, its energy content should change
accordingly. (Of course, we neglect particular cases - work resulting in a
motion for instance is not accumulated but dissipated as heat).

As I find that these 10 KJ are the only reliable physical quantity, I
analyse them and find that they obey a delta H, not delta G definition:

          W = (delta H)c - (delta H)o = 10 KJ/mole               /1/

where (delta H)c is the enthalpy of the coupled reaction, whereas (delta H)o
id the enthalpy of ATP hydrolysis.

As you can see, I  started from a simple idea - I was interested in the
energy the second system had received, not in delta G, delta H, the second
law etc. I called this energy "work done on the second system", and only
then I started expressing it in terms of thermodynamic functions - it
proved a function of delta H, not of delta G.

What wrong do you find in my approach? Can you offer an analogous approach
leading to delta G - first you give some reasonable physical definition of
chemical work based on the first law, and then prove that this work SO
DEFINED is expressed by delta G? I am sure you can't. This is the whole
problem - delta G only formaly describes chemical work - it does not
correspond to any real energy transfer (except for galvanic and osmotic
reactions).

Best regards,
Pentcho

From owner-biophysics@net.bio.net Wed Dec 10 22:00:00 1997
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From: fujimoto@u.washington.edu (Bryant Fujimoto)
Newsgroups: bionet.biophysics
Subject: Re: What delta G cannot explain (reply to Bryant).
Date: 11 Dec 1997 11:48:01 GMT
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Pentcho Valev <RUMYM@BGEARN.ACAD.BG> writes:

>Bryant, when I wrote my previous message, I had not received your last one,
>so mine was nervous and ultimative - sorry about that. Now I see that
>the discussion still makes sense.

>You are right that, for the osmotic system, the delta G concept is better
>than the one based on the enthalpy. You are also right that the enthalpy
>concept does not distinguish between Q and Wu. Still I insist that, except
>for galvanic and osmotic systems, what I call H-work is the only
>meaningful concept describing chemical work.

>Let the reaction A -> B drive the reaction  C -> D :

>       A + C -> B + D                                    /1/

>The only question we ask for the moment is: How much energy is accumulated
>by the C-D system for one stoichiometric unit of reaction? It is not
>diffucult to see that this quantity is

>       E = (delta H)c - (delta H)o                         /2/

>where (delta H)o is the enthalpy change of the reaction  A -> B  and
>(delta H)c is the enthalpy change of the coupled reaction /2/.

>Now what is this E? Part of it may indeed come from the reaction A -> B,
>but the other part is simply due to the fact that the reaction C -> D
>is itself endo(exo)thermic. So E cannot be called true work. In the
>osmotic system, the true work is delta G whereas the thermal component
>in E makes it "contaminated" work.

Its not the true work due to an additional complication.  See below.

>   However, for ATP driven reactions, E is the ONLY quantity reflecting
>the real energy flow in the system. It is again "contaminated" - we
>can never know what part of E comes from ATP (i.e. is "true" work) and
>what part is just absorbed from the environment. Still it is valuable
>in itself 

I never said it wasn't important, I said it wasn't the work.

>- it is a direct measure of energy accumulation in living
>systems. In this sense it does not reject the delta G concept of work -
>it just explains something that delta G cannot explain. The whole problem
>is whether this something makes sense. I still believe that the adequate
>interpretation of energy accumulation in living systems makes a lot
>of sense.

Pentcho
  I certainly hope you didn't get the impression that I thought the
enthalpy was not important.  It certainly is.  I was making the point
that Delta G is a more appropriate quantity for thinking about the work
than Delta H.  In addition to the problem of separating q from Wu, an
additional complication with trying to use Delta H as a measure of the
work involved stems from the fact that H (and G, A, U, and S) are state
functions, while work and heat are not.  What this means is that if you
want to know what (Delta H) is for a process which takes a system from
state 1 to state 2, all you need to know is what those two states are,
you don't need to know how the system got from state 1 to state 2.
However, if you want to know how much work was involved, or how much
heat was absorbed, you have to know the path.  That is, the amount of
work involved (or heat absorbed) depends on how the system got from
state 1 to state 2.  This dependence is exploited to make refrigerators,
steam engines, etc.
  Delta G doesn't have the problem of distinguishing between q and Wu.
For a reversible reaction Delta G is Wu.  Second, for a non-reversible
reaction Delta G is maximum amount maximun amount of non-displacement
work which the driving reaction can perform.  This doesn't mean that it
will perform that much, if the coupling is inefficient, less will be
done.  For the reaction being driven, Delta G is the minimum amount of
work which needs to be done to cause the reaction to proceed.  If the
coupling is inefficient, more will be needed.  So you can at least
think about the limits of how much chemical work can be provided by a
driving reaction, or how much is needed by the reaction being driven.
  The reason that Delta G will depend on the concentration (a fact that
seems to bother you) is that we are considering the net reaction, not
just the result of a single collision.  If the concentrations are such
that the back reaction is favored, then it will take more work to get a
net forward reaction, than if the reaction is initially at equilibrium.
This is what Delta G is about, and it is more in keeping with our
concepts of work.  You should not be able to get any work out of a
reaction at equilibrium.
  Now Delta H is something else.  It has its own uses, and people do
measure and think about it.  It shows up in the temperature dependence
of equilibrium and rate constants, and in bond enthapies, etc.  It just
isn't thought of as a kind of work.  If you want to use it as a measure
of accumulated energy, then you are trying to define an enthalpy of
formation for an organism.  This is can be done in principle.  In
practice the measurements might not be possible.

Regards,
Bryant

From owner-biophysics@net.bio.net Wed Dec 10 22:00:00 1997
Path: biosci!webtv.net!uunet!in5.uu.net!news-hh.maz.net!unlisys!news.snafu.de!fu-berlin.de!cpk-news-hub1.bbnplanet.com!cam-news-hub1.bbnplanet.com!news.bbnplanet.com!prodigy.com!nntp.earthlink.net!usenet
From: villowan@earthlink.net (Charlsie Patterson)
Newsgroups: bionet.biophysics
Subject: [Sr/Assoc. Research Scientist]
Date: Wed, 10 Dec 1997 18:47:53 GMT
Organization: EarthLink Network, Inc.
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My client company is a large established  pharmaceutical company
aggressively seeking to fill this position at the first of the year.
It is in the area of research and development.  They offer excellent
compensation and benefit, as well as great growth potential.  The
client company will pay all fees associated with recruiting and
placement of candidates. The position is located in North Carolina.

Please refer to Job Listing B-9785 in all correspondence

To submit your CV or have any questions answered, please contact:

Ms. Charlsie Patterson
Technical and Bio-Science Recruiter
Global Staffing and Recruiting
(919) 871-0070
Fax: (919) 871-0030
email: techsearch@globals-r.com
and/or villowan@earthlink.net

Sr./Assoc. Research Scientist

Brief Description of the Position:

Conduct assays to support the development and characterization of new
biological products.  The incumbent will also be part of a  team that
will interact closely with early stages of process scale up and with
the QA development and establishment of numerous new assays.  (i.e.
robotics immunological and real time on-line assays) and advanced
characterization of protein products.  The incumbent will collaborate
closely with projects in New Product Biochemistry, Pathogen Safety and
Process Research Sections.  The incumbent will work at the laboratory
bench and have good oral and written communication skills to keep
accurate experimental records, communicate research goals and results
on a frequent schedule.

Position Requirements:

BS in Biochemistry, Analytical chemistry, or closely related field
with at least 2 years of relevant job experience.  Experience with
operating and maintaining Hewlett Package HPLCs, BioSepara ProSys
HPLCs and Beckman BioMek Robotics systems is desired.  A demonstrated
ability to keep clear records, recognize and implement needed
experimental controls, communicate with team members, and meet time
lines is required.  A background with HPLC, enzymatic, and/or
immunological assays is required.  Experience with mass spectrometry,
amino acid analysis, sequence analysis, peptide mapping, disulfide
assignment and/or glycoprotien analysis is needed. GLP/GMP experience,
analytical methods validation, experience in automation, robotics,
on-line assays, a familiarity with the well-characterized biological
concept will contribute to the success of a candidate.


From owner-biophysics@net.bio.net Wed Dec 10 22:00:00 1997
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From: villowan@earthlink.net (Charlsie Patterson)
Newsgroups: bionet.biophysics
Subject: ]][[ Research Scientist/Senior Research Scientist B-9785
Date: Thu, 11 Dec 1997 00:15:00 GMT
Organization: EarthLink Network, Inc.
Lines: 43
Message-ID: <66nbbg$apj@argentina.earthlink.net>
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My client company is a large, well established pharmaceutical
company, who is aggressively seeking to fill this position at the
first of the year.  It is in the area of research and development.
They offer excellent compensation and benefit, as well as great growth
potential.  The client company will pay all fees associated with
recruiting and placement of candidates. The position is located in
North Carolina.

Please refer to Job Listing B-9817 in all correspondence

To submit your CV or have any questions answered, please contact:

Ms. Charlsie Patterson
Technical and Bio-Science Recruiter
Global Staffing and Recruiting
(919) 871-0070
Fax: (919) 871-0030
email: techsearch@globals-r.com
and/or villowan@earthlink.net


Brief Description of the Position:

The incumbent will be a member of the Process Engineering Group of the
Technology Department and will contribute to the development of new
purification processes for plasma proteins.  The process optimization
work will center around unit operations as chromatography, membrane
separation, and filtration.  Major focuses will be the scale-up from
macro-bench to pilot-scale and beyond.  The incumbent will
particularly interface with project engineering and play a major role
in the realization projects of the new processes.

Position Requirements:

Requires a Ph.D./MS degree in Chemical Engineering: minimum experience
of four plus years in process development or manufacturing, preferably
in the pharmaceutical or biotechnology industries.  Must be familiar
with GLP/GMP rules and conditions.  Experience in project engineering
as well as working knowledge in protein chemistry is preferred

PLEASE NOTE:  A Hepatitis B immunization is required



From owner-biophysics@net.bio.net Fri Dec 12 22:00:00 1997
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From: prismx@earthlink.net (Claire Haller)
Newsgroups: bionet.neuroscience,bionet.biophysics,bionet.cellbiol,bionet.general,sci.misc
Subject: SCIENCE-WEEK: Headlines (12 Dec 97) Content Increased
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Xref: biosci bionet.neuroscience:20972 bionet.biophysics:3795 bionet.cellbiol:8565 bionet.general:28899

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10. Persistence of the DNA Form of an RNA Virus
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From owner-biophysics@net.bio.net Sat Dec 13 22:00:00 1997
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From: med050@aix.zam.kfa-juelich.de (d.gembris)
Newsgroups: bionet.neuroscience,bionet.biophysics,de.sci.biologie,sci.med.physics,sci.techniques.mag-resonance,sci.med.informatics
Subject: Announcement: new brain-research WWW site
Date: 14 Dec 1997 21:28:20 GMT
Organization: Forschungszentrum Juelich GmbH (KFA)
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Keywords: fMRI, BOLD, MR, MRI, functional MR, modelling,
          Bloch equations, brain, neural activation,
          non-invasive
Xref: biosci bionet.neuroscience:20979 bionet.biophysics:3796

We want to announce that the Institute of Medicine
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Regards, Daniel Gembris

************************************************************
********** research center Juelich GmbH , Germany **********
************************************************************
******                                                ******
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************************************************************
**************** (I)nstitute for (ME)dicine ****************
************************************************************
******                                                ******
******            Daniel Gembris, MR-group            ******
******                                                ******
******  email  : d.gembris@fz-juelich.de              ******
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******  tel    : ++49 - 2461 - 61 - 2107              ******
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******                                                ******
************************************************************
************************************************************

From owner-biophysics@net.bio.net Sun Dec 14 22:00:00 1997
Path: biosci!daresbury!not-for-mail
From: Pentcho Valev <RUMYM@BGEARN.ACAD.BG>
Newsgroups: bionet.biophysics
Subject: What is chemical work?
Date: 15 Dec 1997 15:02:43 -0000
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Message-ID: <673gqj$8g@mserv1.dl.ac.uk>
Original-To: biophys@dl.ac.uk

Bryant Fujimoto wrote:>>>>>>>>>>>>>>>>>>>>>>>
Now for a discussion about chemical work.  If the total work is W, as in

   dU = Q + W

then, the "useful" work is

  Wu = W -(displacement work)

At constant pressure the displacement work is -P(Delta V).  (If the
system is not a constant pressure, then you have to integrate -PdV over
the volume change.)  So

  Wu = W + P(Delta V)

If there is only chemical and displacement work being done, then Wu is
the chemical work. Now the definition of H is

  H = U + PV                                                   /1/

so

  dH = dU + PdV + VdP = Q + W + PdV + VdP = Q + Wu +VdP

At constant pressure dP = 0 and

  dH = Q + Wu                                                   /2/

Which as we can see, is not the work.  The definition of G is

  G = H - TS                                                    /3/

so (at constant pressure)

  dG = dH - TdS - SdT = Q + Wu - TdS - SdT

>From the definition of the entropy we have Q = TdS for a reversible
reaction, so

  dG = Wu - SdT

So at constant temperature (dT = 0) and pressure, for a reversible
process

  dG = Wu                                                         /4/

The only things I have used are the first law, and the definitions
of H, G, and S.<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<<

No, Bryant, something is missing in your analysis. /3/ only formally
defines chemical work - the "operative" definition is different - it
is ad hoc definition - it defines chemical work so as to satisfy the
second law, and in so doing it can produce the absurd result that the
work production is a process opposite to the real energy flow.

Let the reaction  A -> B  drive the reaction  C -> D:

         A + C -> B + D                                       /5/

Let us also make the realistic assumption that, as the reaction proceeds,
the energy of the system  A-B decreases whereas that of the system C-D
increases. On the other hand, if /5/ is close to equilibrium, THE WORK
DONE BY THE SYSTEM  A-B  ON THE SYSTEM  C-D  is given by

        delta G = delta Go  +  RTln((B)/(A))                 /6/

where delta Go is the standard free energy of the reaction A -> B.
Now the concentrations in /6/ can be such that, as the reaction /5/
is still close to equilibrium, delta G is positive - e.g. 5 KJ/mole.

Now please try to understand the absurdity of the situation. The value
of delta G shows that the work done by the system A-B on the system C-D
is NEGATIVE, i.e. it is the system  C-D that does work on the system A-B.
On the other hand, the energy flow is in the opposite direction - from the
system A-B to the system C-D. Please forget for a while about chemistry
and see how this sounds in most general terms:

THE SYSTEM X DOES WORK ON THE SYSTEM Y. IN THE PROCESS, THE ENERGY OF X
INCREASES AND THAT OF Y DECREASES.

I simply do not understand how science has tolerated such an absurdity
for so many years. What is even more deplorable is that this does not
bother anybody.

Best regards,
Pentcho

From owner-biophysics@net.bio.net Sun Dec 14 22:00:00 1997
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From: fujimoto@u.washington.edu (Bryant Fujimoto)
Newsgroups: bionet.biophysics
Subject: Re: Delta G vs. Delta H
Date: 15 Dec 1997 10:52:12 GMT
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Pentcho Valev <RUMYM@BGEARN.ACAD.BG> writes:


>In reply to Bryant Fujimoto

>Bryant, my choice of delta H as a measure of chemical work is based on the
>following simple physical picture:

>The ATP system interacts with another system. As one mole ATP is used up,
>the energy of the other system increases by 10 KJ. These 10 KJ are the
>only real physical quantity showing the changed energetics of the second
>system, so I am inclined to think of it as "work done on the second system".
>Of course, I am ready to consider other definitions of "work done on the
>second system", but expect them to be in harmony with the first law - if
>work is done on the second system, its energy content should change
>accordingly. (Of course, we neglect particular cases - work resulting in a
>motion for instance is not accumulated but dissipated as heat).

If you think about what happens when two chemical reactions are coupled,
there are not two systems, but three.  The third one is the environment in
which the reaction takes place (the solvents and any other solutes for
a liquid phase reaction).  Your analysis ignores energy flows to or
from the surroundings.

>As I find that these 10 KJ are the only reliable physical quantity, I
>analyse them and find that they obey a delta H, not delta G definition:

>          W = (delta H)c - (delta H)o = 10 KJ/mole               /1/

>where (delta H)c is the enthalpy of the coupled reaction, whereas (delta H)o
>id the enthalpy of ATP hydrolysis.

>As you can see, I  started from a simple idea - I was interested in the
>energy the second system had received, not in delta G, delta H, the second
>law etc. I called this energy "work done on the second system", and only
>then I started expressing it in terms of thermodynamic functions - it
>proved a function of delta H, not of delta G.

But the energy received is not the work and furthermore, not all of
Delta H is received.  For an exothermic reaction, some of Delta H
can represent heat given off by the reaction, not energy received.
Also, the amount of energy received depends on the efficiency of the
coupling between the driving and receiving reactions, and this simply
isn't reflected in Delta H.

>What wrong do you find in my approach? Can you offer an analogous approach
>leading to delta G - first you give some reasonable physical definition of
>chemical work based on the first law, and then prove that this work SO
>DEFINED is expressed by delta G? I am sure you can't. This is the whole
>problem - delta G only formaly describes chemical work - it does not
>correspond to any real energy transfer (except for galvanic and osmotic
>reactions).

Pentcho
  In addition to my above comments, what I find wrong with your
approach is that equating Delta H to any type of work contradicts the
first law of thermodynamics.  The energy transferred is not the work.
The energy transferred is independent of the process used to go from
the initial to the final state.  The work does depend on it.  Therefore
Delta H cannot be a work.  As I stated before, if Delta G is negative,
then Delta G is the maximum useful work the system can perform on its
environment.

Now for a discussion about chemical work.  If the total work is W, as in

   dU = Q + W

then, the "useful" work is

  Wu = W -(displacement work)

At constant pressure the displacement work is -P(Delta V).  (If the
system is not a constant pressure, then you have to integrate -PdV over
the volume change.)  So 

  Wu = W + P(Delta V)

If there is only chemical and displacement work being done, then Wu is
the chemical work. Now the definition of H is

  H = U + PV

so

  dH = dU + PdV + VdP = Q + W + PdV + VdP = Q + Wu +VdP

At constant pressure dP = 0 and

  dH = Q + Wu

Which as we can see, is not the work.  The definition of G is

  G = H - TS

so (at constant pressure)

  dG = dH - TdS - SdT = Q + Wu - TdS - SdT

From the definition of the entropy we have Q = TdS for a reversible
reaction, so

  dG = Wu - SdT

So at constant temperature (dT = 0) and pressure, for a reversible
process

  dG = Wu

The only things I have used are the first law, and the definitions
of H, G, and S.

Finally, what don't you like about the enthalpy, that you keep trying
to redefine it as something else?  Its not the work (though it is
related to it), and its not the energy (though for reactions in solution
it is close).  Why can't you just let the enthalpy be the enthalpy?
Its a perfectly good, well defined quantity and lots of people study it.

Regards,
Bryant

From owner-biophysics@net.bio.net Sun Dec 14 22:00:00 1997
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From: Mike Croning <michael.croning@yale.edu>
Newsgroups: bionet.biophysics
Subject: In vitro chambers - custom fabrication facilities
Date: Mon, 15 Dec 1997 10:54:43 -0500
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For a number of years R. Felix Garcia has been designing and
manufacturing in vitro chambers for neuroscience research in
collaboration with researchers at Yale University Medical School and
elsewhere.  Our speciality is in chamber designs constructed from
plexiglass, stainless steel and aluminium.  Many designs are available
'off the shelf', with custom designs for your application being produced
at little extra cost.


Current production chambers include:-

**Cell dissociation chamber**

For dissociation of neurons from mammalian CNS tissue for patch clamp
and optical recordings according to the method of Kay and Wong (Kay AR.
Wong RK. Isolation of neurons suitable for patch-clamping from adult
mammalian central nervous systems. J Neurosci Methods. (1986).
16(3):227-38.  The chamber incorporates a plexiglass jacket (for
circulation of heated water), and a glass inner chamber where the
nervous tissue is incubated with digestive enzymes.

Publications arising from neurons dissociated in this chamber:-

Patch clamp recording
Jiang C. Haddad GG. A direct mechanism for sensing low oxygen levels by
central neurons. Proc Natl Acad Sci U S A. (1994), 91(15):7198-201.

Single cell microfluorimetry
Friedman JE. Haddad GG. Major differences in Ca2+i response to anoxia
between neonatal and adult rat CA1 neurons: role of Ca2+o and Na+o. J
Neurosci. (1993), 13(1):63-72.


**Superfusion ('fully-submerged') brain slice recording chamber**

For electrophysiological recordings.  The design is two part, consisting
of the chamber proper and a separate water jacket for preheating the
aqueous perfusate.  The recording chamber volume is small (<0.5 ml),
enabling very rapid solution exchange (» 20 s).  The design is very
similar to that reported by Roger Nicolls lab (Nicoll RA. Alger BE. A
simple chamber for recording from submerged brain slices. J Neurosci
Methods. (1981) 4(2):153-6).


**Interface brain-slice chamber**

For electrophysiological recordings.  When it is desired to maintain
brain slices at a gas-liquid interface on a flat plate plexiglass
surface.  The design is very similar to the original report of this
chamber type (Haas HL. Schaerer B. Vosmansky M. A simple perfusion
chamber for the study of nervous tissue slices in vitro. J Neurosci
Methods. (1979) 1(4):323-5).  The chamber consists of a plexiglass plate
which sits on a heated humidfying chamber that both heats the perfusate
and the gas flowing over the slices.  The chamber can incorporate either
a heating wire for electrical heating via a thermostatic heating
controller, or a stainless-steel tubular coil for circulation of warmed
water to heat the chamber.


**Enviromental chamber**

For exposure of rodents to controlled breathing mixtures.  Chamber
includes all hardware to maintain a gas-regulated and air-tight
envioment including provisions for connection of an internal oxygen
probe, and gas flow tubes for mixing of gases.


Enquiries can be passed via email sent to michael.croning@yale.edu or
directly to:-


R. Felix Garcia
745 Orange
Apt. 1
New Haven, CT 06511, USA

From owner-biophysics@net.bio.net Sun Dec 14 22:00:00 1997
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From: "jmouse" <jmouse18@hotmail.com>
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Subject: Career related to biology
Date: Mon, 15 Dec 1997 16:58:05 -0400
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i'm doing a project on careers related to biology, can somebody give me some
information? (as detail as possible) Thanks.



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From: Pentcho Valev <RUMYM@BGEARN.ACAD.BG>
Newsgroups: bionet.biophysics
Subject: Elaboration on chemical work
Date: 16 Dec 1997 09:59:52 -0000
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In reply to Bryant Fujimoto

Bryant, my previous message was negative - I tried to show that delta G
gives a description of chemical work incompatible with the real energy flow.
Let me develop the positive aspect of the concept of chemical work.

The example: The reactions  A -> B  and  C -> D  are coupled in

          A + C -> B + D                                       /1/

For one stoichiometric unit of reaction, the energy increase of the C-D
system is 10 KJ/mole. On the other hand, as /1/ is close to equilibrium,
delta G for the C-D system is -5 KJ/mole.

Now we have to choose between two interpretations:

1. According to the second law, the A-B system receives 5 KJ/mole work.

2. In contradiction to the second law, the C-D system receives 10 KJ/mole
work.

I hope you would agree that the former interpretaion is absurd. There could
be no reason in the belief that the energy of the A-B system DECREASES,
the energy of the C-D system INCREASES, and yet the A-B system RECEIVES
5 KJ/mole work. This contradicts directly the first law of thermodynamics.

As for the latter interpretation, these 10 KJ/mole are REAL energy the
C-D system has received. The only problem is whether we can call them WORK.
In fact, these 10 KJ are the enthalpy of the reaction  C-D, i.e.

           delta H(C-D) = Q + Wu                                    /2/

You are absolutely right that /2/ is not exactly the work obtained - it
includes also Q. On the other hand, physically, this is the only interesting
quantity as far as the energy flow is concerned. Let us forget for a while
about second law problems and try to sketch the general methodology of
bioenergetics. Aren't we to divide the system into subsystems and describe
how much energy each subsystem gains or loses? Then of course we may
concentrate on mechanisms, but still this general approach seems essential.
If so, why should we deal with a definition of chemical work having nothing
to do with the energy flow? Just to defend a principle wrongly attributed
to living systems? Why don't we just use /2/ as a REAL quantity - we may
not call it WORK - let it be "ENERGY INCREASE". As this new methodology
develops, we would be able to answer an important question - how energy
flows and accumulates in living systems, to juxtapose energy movement
with different concepts of order etc. Also, there would be no need at
all to refute the second law - it would be clear that to speak of work
production occuring in a direction opposite to the real energy flow is
just nonsense. However, until this new approach develops, we will continue
the unproductive argument about the formal definition of chemical work -
whether it is energy of "tendency" etc.

Best regards,
Pentcho

From owner-biophysics@net.bio.net Mon Dec 15 22:00:00 1997
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                        VIII  MEDITERRANEAN  CONFERENCE  ON
                MEDICAL  AND  BIOLOGICAL  ENGINEERING AND COMPUTING

                                   Medicon'98
                                            
                        June 14-17, 1998, Lemesos, Cyprus


Organized and Sponsored by:
    Department of Computer Science, University of Cyprus
    The Cyprus Association of Medical Physics and Biomedical Engineering

Co-Sponsored by:
    IEEE Engineering in Medicine and Biology Society
    European Society for Engineering and Medicine

In cooperation with:
    International Federation for Medical and Biological Engineering (IFMBE)   
    Associazione Italiana di Ingegneria Medica e Biologica
    Croatian Medical & Biological Engineering Society
    Greek Society for Biomedical Engineering
    Israel Society for Medical & Biological Engineering
    Slovene Society for Medical & Biological Engineering
    Societe des Electriciens et des Electroniciens (Club Francais des 
    Technologies Biomedicales)
    Spanish Society of Biomedical Engineering
    Institute of Electrical and Electronics Engineers (IEEE Cyprus Section)
    Institution of Electrical Engineers (IEE Cyprus Centre)

In association with:
    Cyprus Institute of Neurology and Genetics
    Higher Technical Institute
    United Kingdom Liaison Committee for Sciences Allied to Medicine & 
    Biology (S.A.M.B.)

PROGRAMME COMMITTEE
D Adam (Israel)                         J P Morucci (France)
K Athanasiou (USA)                      A Nicolaides (UK)
T Bajd (Slovenia)                       M Nyssen (Belgium)
M Bracale (Italy)                       N Ouzounoglou (Greece)
J E W Beneken (Netherlands)             N Pallikarakis (Greece)
S Cerutti (Italy)                       P Rabichong (France)
A G Constantinides (UK)                 L M Roa (Spain)
K Copeland (UK)                         V C Roberts (UK)
G Dimitrov (Bulgaria)                   M Sawan (Canada)
N Dimitrova (Bulgaria)                  S Sideman (Israel)
U. Faust (Germany)                      J A E Spaan (The Netherlands)
H Hutten (Austria)                      V A Spasic (Yugoslavia)
G Inbar (Israel)                        N Sphiris (Greece)
F Kajiya (Japan)                        U Stanic (Slovenia)
Z Kollitsi (Greece)                     Y Istefanopoulos (Turkey)
K Kouris (Cyprus)                       D Tsaptsinos (UK)
D Koutsouris (Greece)                   K Turker (Australia)
I Krekule (Czech Republic)              E M Tzanakou (USA)
S Laxminarayan (USA)                    N Zamboglou (Germany)
R Magjarevic (Croatia)                  

ORGANIZING COMMITTEE
Conference Co-Chairs: Stelios Christofides (CAMPBE, Cyprus),
		    : Constantinos S Pattichis (University of Cyprus, Cyprus)
Program Chair       : Christos N Schizas (University of Cyprus, Cyprus)
International Chair : Elpida Keravnou-Papailiou (University of Cyprus, Cyprus)
Exhibits Chair      : Yiannis Theodoulou (CAMPBE, Cyprus)
Treasurer           : Prodromos Kaplanis (CAMPBE, Cyprus)
Publications        : Spyros Spyrou (Higher Technical Institute, Cyprus)
Social Program      : George Christodoulides (CAMPBE, Cyprus)

Medicon'98 is the 8th in the series of regional meetings in the Mediterranean
of the International Federation for Medical and Biological Engineering
(IFMBE). The goal of Medicon'98 is to provide updated information on the
state of the art on Medical and Biological Engineering and Computing. The
program will consist of both invited and submitted papers on new developments
in these fields. Medicon'98 will focus primarily on the following topics:

TOPICS OF INTEREST
 *  Biomechanics/Implants
 *  Biosignal Processing and Analysis
 *  Cardiovascular Systems
 *  Cellular Engineering
 *  Clinical Engineering
 *  Health Care Technology Assessment
 *  High Performance Computing in Medicine
 *  Instrumentation
 *  Intelligent Systems in Medicine
 *  Medical Imaging
 *  Medical Multimedia Workstations and Databases
 *  Models of Physiological Systems
 *  Neuromuscular Systems
 *  Patient Monitoring
 *  Radiation Protection
 *  Radiotherapy
 *  Rehabilitation Engineering
 *  Telemedicine
 *  Virtual Reality in Medicine

SPECIAL SESSIONS
Proposals for plenary and special sessions are invited. For further details
please contact Constantinos Pattichis, by January 30, 1998.

KEYNOTE LECTURES
 *  Information Technology in Biomedicine Leaping into 2000, Swamy
Laxminarayan (USA)
 *  Integrated Telemedicine Networks and Added Value Services, Stelios
Orphanoudakis (Greece)
 *  Computational Intelligence: Status and Trends in Medical Diagnostic
Systems, Evangelia Micheli-Tzanakou (USA)


BEST STUDENT PAPER AWARDS
In memory of Dick Poortvliet, dinstinguished biomedical engineer and active
member of IEEE Region 8, the IEEE Cyprus Section will organize during
Medicon'98 a student paper contest. To qualify, a student or group of
students must contribute a significant part of the paper and be the primary
author(s).  The submission should clearly indicate that the paper is to be
considered for the best student paper award, the amount of contribution made
by the student, the current level of study, and the address including fax or
e-mail.

INTERNATIONAL EXHIBITION
The conference will provide the attendees with the opportunity of examining
state-of-the-art technology (in biomedical and medical physics
instrumentation, computer hardware and software) and establishing useful
interactions with representatives of manufacturers, vendors, and publishers.

PAPER SUBMISSION
Papers are invited, but not limited, to theabove topics of interest.

Authors are stongly encouraged to submit a PostScript version of their full
paper by anonymous ftp to zeus.cc.ucy.ac.cy, and put the paper in the
directory /incoming/medicon98. Files should be uniquely named:
<author-surname.firstname>.ps. In addition, authors should notify by e-mail
to med98@turing.cs.ucy.ac.cy the title of the paper, the corresponding author
and address, and the first two choices for the topics of interest as given
above, under which the paper can be classified.

Alternatively, papers can be submitted in paper format (one original and two
copies). These submissions should be accompanied with a diskette with the
paper in MS Word format, or TEX on IBM PC or MAC, including all figures. In
an accompanying letter, authors should specify the title of the paper, the
corresponding author and address, and the first two choices from the topics
of interest as given above, under which the paper can be classified.

The papers must be completed within 6 pages, including figures, tables and
references, and should be written in English. An A4 size format with 2,5 cm
margin on all four sides should be used. They should be prepared in
one-column format, single spaced, in Arial or similar type style of 10
points.  Centered at the top of the first page should be the complete title,
author name(s), affiliation(s) and mailing address(es), including electronic
mailing(s) address(es). This is followed by a blank space and then the
abstract, up to 15 lines, followed by the main text.

Submission of a proposed paper implies a commitment from one of the authors
to present the paper if accepted.

ADDRESS FOR PAPER SUBMISSIONS
Medicon'98, Department of Computer Science, University of Cyprus, 75
Kallipoleos Str, P.O. Box 537, CY-1678 Nicosia, CYPRUS.

CONFERENCE PROCEEDINGS
Submitted papers will be reviewed by at least two referees and all accepted
papers will be published on CD-ROM. A copy of the proceedings will be given
to each participant at the conference. After the conference, the proceedings
will be available from the publisher.

A few selected authors will be invited to publish extended versions of their
papers in a special issue of the IEEE Transactions on Information Technology
in Biomedicine (T-ITB). All papers submitted for publication in the
Transactions will be subject to a further peer-review process prior to
publication in the T-ITB.


AUTHORS SCHEDULE
 *  Paper submission					January 30, 1998
    (Receival acknowledgment will follow)
    
 *  Notification of acceptance				March 30, 1998
    (List of all accepted papers will be posted at
    the WWW page of the conference)


REGISTRATION
Full conference registration fee includes admission to all sessions, welcome
reception, and a copy of the proceedings. Early registration is highly
recommended in order to save both time and money.

Early registration (before April 30, 1998)        	Cyp.Pounds 140
Late registration (after April 30, 1998)          	Cyp.Pounds 160
Students                                          	Cyp.Pounds  70

Note: Cyp.Pound 1 ~= US$2

Make all cheques payable to CYDEM TOURS Ltd or charge your Credit card. Mail
or fax your payment to the address of the official travel agent.

OFFICIAL TRAVEL AGENT
Aristos C Demetriou, CYDEM TOURS Ltd, P.O. Box 4134, Nicosia, CYPRUS.
Tel: +357-2-773865/451300, Fax: +357-2-457297, Email: cydem@spidernet.com.cy.


ABOUT CYPRUS
Cyprus is an island situated at the north-east corner of the Mediterranean
Sea at the cross-roads of three continents, Europe, Asia and Africa. Its
geographically significant position both for trade and military purposes has
been one of the main reasons for Cyprus' turbulent history. The passing from
the island of different conquerors has helped to blend the character of the
Cypriots. Here the visitor may enjoy magnificent pottery and sculpture,
ancient ruins all over the island, Byzantine monasteries, churches and
medieval monuments of great architectural value. The people of Cyprus are
traditionally warm and welcoming. Their language is Greek but English is
spoken in all shops, restaurants, hotels, banks and government offices. Life
on the island is leisurely and safe. Greek food should be tried. Greek Meze,
consisting of as many as thirty dishes, starting with salads, dips, tasty
local dishes and kebabs is something the visitor should not miss.

CLIMATE
Cyprus has what is called a Mediterranean climate, that is hot summers but
moderate winters. July and August are the hottest months. Temperatures during
the day vary from 32 - 38 deg. C, so bring light clothes, sandals and
sunglasses. Temperature falls during the evening but remains warm. Sea water
is warm and inviting so don't forget your swimsuits.

TRANSPORT
Cyprus is easily accessible by air. Larnaca airport is forty-five minutes
drive from the Hawaii Beach Hotel at Lemesos. A taxi ride from the airport
costs around Cyp.Pounds 20. Pafos airport on the other hand is one hour and
twenty minutes drive from the Hotel at Lemesos and costs around Cyp.Pounds 30
by taxi.


MORE INFORMATION
Constantinos S Pattichis
Department of Computer Science
University of Cyprus
75 Kallipoleos Street,
CY-1678 Nicosia
CYPRUS

Tel no  :  +357-2-338705/06
Fax no  :  +357-2-339062
Email   :  pattichi@turing.cs.ucy.ac.cy

Stelios Christofides
Medical Physics Department
Nicosia General Hospital
P.O. Box 4039
CY-1450 Nicosia
CYPRUS

Tel no  :  +357-2-301306
Fax no 	:  +357-2-369170
Email   :  g.h.library@cytanet.com.cy

INFORMATION ON WWW
Please refer to this WWW page. It contains the latest information for
Medicon'98.

URL : http://www.ucy.ac.cy/ucy/cs/med98/med98.htm



From owner-biophysics@net.bio.net Mon Dec 15 22:00:00 1997
Path: biosci!agate!howland.erols.net!cpk-news-hub1.bbnplanet.com!news.bbnplanet.com!baron.netcom.net.uk!netcom.net.uk!newsfeed2.uk.ibm.net!news.ibm.net.il!ibm.net!news.biu.ac.il!news.huji.ac.il!not-for-mail
From: "Jonathan B. Marder" <marder@agri.huji.ac.il>
Newsgroups: bionet.biophysics
Subject: Definition of work (for Pentcho)
Date: Tue, 16 Dec 1997 15:39:02 +0200
Organization: Hebrew University
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Pentcho raised the difficulty of defining chemical work. Perhaps the
following general definition of work will be useful:-

 "Work performed on a system is the act of moving that system away from
equilibrium".

In a sense, this simply restates an aspect of the second law of
thermodynamics,
so Pentcho will object. On the other hand this definition appears
applicable to work in all its forms.

--
Jonathan B. Marder   <MARDER@agri.huji.ac.il>
Department of Agricultural Botany, The Hebrew University of Jerusalem
Faculty of Agriculture, P.O.Box 12, Rehovot 76100, ISRAEL
Phone: +972 8 9481918   Fax:   +972 8 9467763
Web page:    http://www.agri.huji.ac.il/~marder



From owner-biophysics@net.bio.net Mon Dec 15 22:00:00 1997
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From: "Jonathan B. Marder" <marder@agri.huji.ac.il>
Newsgroups: bionet.biophysics
Subject: Re: Elaboration on chemical work
Date: Tue, 16 Dec 1997 15:29:25 +0200
Organization: Hebrew University
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Pentcho Valev wrote in message +ADw-675jeo+ACQ-hq9+AEA-mserv1.dl.ac.uk+AD4-...
...
+AD4-Let me develop the positive aspect of the concept of chemical work.
+AD4-
+AD4-The example: The reactions  A -+AD4- B  and  C -+AD4- D  are coupled in
+AD4-
+AD4-          A  C -+AD4- B  D                                       /1/
+AD4-
+AD4-For one stoichiometric unit of reaction, the energy increase of the C-D
+AD4-system is 10 KJ/mole. On the other hand, as /1/ is close to
equilibrium,
+AD4-delta G for the C-D system is -5 KJ/mole.
...
Pentcho, you've lost me already. What is the +ACI-energy increase+ACI- of C-D
and how can it be different to deltaG? This is a blatant contradiction.
If /1/ is at equilibrium, and deltaG or C-+AD4-D is -5 kJ/mol, then this
means that deltaG for A-+AD4-B is +-5 kJ/mol. Anything else is incorrect.




From owner-biophysics@net.bio.net Tue Dec 16 22:00:00 1997
Path: biosci!MARA.FI.UBA.AR!icie96
From: icie96@MARA.FI.UBA.AR (1995 Congress)
Newsgroups: bionet.biophysics
Subject: ICIE 98
Date: 16 Dec 1997 16:53:23 -0800
Organization: BIOSCI International Newsgroups for Molecular Biology
Lines: 83
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=09=09=09LLAMADO A LA PRESENTACION DE TRABAJOS

=09=09IV CONGRESO INTERNACIONAL EN INGENIERIA INFORMATICA
=09=09=09=09=09ICIE'98

=09=09=09=09 16 y 17 de Abril de 1998
=09=09=09=09Departamento de Computacion.
=09=09=09=09   Facultad de Ingenier=A1a
=09=09=09=09Universidad de Buenos Aires.
=09=09=09=09=09ARGENTINA


Por cuarto an^o consecutivo se desarrolla el CONGRESO INTERNACIONAL EN=20
INGENIERIA INFORMATICA, organizado por el Departamento de Computacion de
la Facultad de Ingenier=A1a de la Universidad de Buenos Aires.=20
El mismo se llevara a cabo los d=A1as 16 y 17 de abril de 1998.

Pueden ser presentados trabajos de todas las =A0reas de aplicacion que se=
=20
encuadren dentro de las siguientes caracter=A1sticas: 1) Resultados de trab=
ajos=20
de investigacion en el area de aplicacion, 2) Soluciones a problemas en la
industria, los negocios el gobierno o areas relacionadas o 3) Propuestas
Acadamicas o Tecnologicas innovadoras.

Los temas del congreso abarcan:
Sistemas Basados en Conocimiento, Redes Neuronales, Sistema Difusos,=20
Inteligencia Artificial, Bases de Datos, Algebra Computacional, Lenguajes d=
e
 Computacion, Tecnolog=A1a Orientada a Objetos, Multimedia, Vision por=20
Computadora, Robotica, Networking, Ingenier=A1a de Software, Investigaci=A2=
n=20
Operativa, Sistemas Distribuidos y Redes, Sistemas de Tiempo Real,=20
Educacion en Informatica y otras =A0reas relacionadas.

Las personas o grupos de investigacion y desarrollo interesadas en
presentar su trabajos deben enviar un resumen (500 palabras) por e-mail=20
a: icie@mara.fi.uba.ar o cuatro (4) copias escritas en espan^ol, portugues
o ingles a:

Comite de Programa ICIE '98.
Departamento de Computacion.
Facultad de Ingenier=A1a.
Universidad de Buenos Aires. Paseo Colon 850. 4to Piso. (1063)
Capital Federal. ARGENTINA.

En caso de hacerlo por correo normal se agradecer=A0 la inclusion de un=20
disquete con el archivo correspondiente, el cual debe estar escrito en=20
letra Arial o Times New Roman, de un taman^o de 12 puntos, espaciado
sencillo y un maximo de 15 paginas en tama=A4o A4. Los margenes deben ser
de 2,5 cm por lado. Las paginas deben ser numeradas en lapiz en la parte
posterior y en la primer hoja se debe indicar tambien el area de
aplicacion al que pertenece el trabajo.

FECHAS IMPORTANTES
Presentacion de resumenes:=0906/02/98
Comunicacion de Aceptacion:=0906/03/98
Presentacion de la version definitiva:=0913/03/98

Tanto la version de evaluaci=A2n como la version definitiva puede ser
enviada por e-mail a icie@mara.fi.uba.ar en formato RTF.
La presentacion de un trabajo facultara al Departamento de Computacion de
la Facultad de Ingenier=A1a de la Universidad de Buenos Aires a publicarlo =
en=20
los Anales del ICIE' 98. No obstante es conveniente adjuntar una
autorizacion con la firma de sus autores. Los trabajos recibidos despues
de los plazos establecidos no seran incluidos en los Anales.



=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=
=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D
Comite de Programa ICIE '98.
Departamento de Computaci=A2n.
Facultad de Ingenier=A1a.
Universidad de Buenos Aires.
Paseo Col=A2n 850. 4to Piso. (1063)
Capital Federal. ARGENTINA.

e-mail: icie96@mara.fi.uba.ar
=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=
=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D=3D


From owner-biophysics@net.bio.net Tue Dec 16 22:00:00 1997
Path: biosci!bcm.tmc.edu!news.msfc.nasa.gov!newsfeed.internetmci.com!207.97.14.174!europa.clark.net!152.158.16.55!newsfeed2.uk.ibm.net!news.ibm.net.il!ibm.net!news.biu.ac.il!news.huji.ac.il!not-for-mail
From: "Jonathan B. Marder" <marder@agri.huji.ac.il>
Newsgroups: bionet.biophysics
Subject: Re: Definition of chemical work
Date: Wed, 17 Dec 1997 11:49:56 +0200
Organization: Hebrew University
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Pentcho Valev wrote in message +ADw-677u9l+ACQ-hlc+AEA-mserv1.dl.ac.uk+AD4-...
+AD4-
+AD4-Jonathan Marder wrote:+AD4-
...
+AD4- +ACI-Work performed on a system is the act of moving that system away from
+AD4-equilibrium+ACI-.
...
+AD4-
+AD4-Yes Jonathan I object but not simply because you redefine delta G as a
+AD4-measure of chemical work. This definition contradicts our basic
+AD4-understanding of physical reality.

If this contradicts your understanding of physical reality, then we
obviously understand physical reality differently.

+AD4-Please consider a most general picture:
+AD4-
+AD4-A system does work, isothermally, on the surroundings. How?

First problem, once you say +ACI-isothermally+ACI- it is already unclear where
your system begins and ends. Are the heat sources/sinks part of the
system?

+AD4-There are two possibilities:
+AD4-
+AD4-1. The system uses its internal energy for doing work. Obviously in
this
+AD4-case its internal energy decreases in the process.


Yes, the system moves TOWARDS equilibrium, so is able to DO work.
This is my definition applied in the opposite direction.

+AD4-
+AD4-2. The system, like an ideal gas, uses external energy for doing work.
+AD4-In this case its internal energy remains the same.
+AD4-

Now you have a different system which includes the external energy
source.
Entry of energy from the external source moves the combined system
towards equilibrium - same applies as above.

+AD4-Please note that in both cases the internal energy of the system CANNOT
+AD4-INCREASE. Now your definition allows the system, in principle, to
+AD4-INCREASE its internal energy while doing work.


If, in the second case, the system is extended to include the external
energy source, your statement becomes invalid.

Regards,
Jonathan B. Marder   +ADw-MARDER+AEA-agri.huji.ac.il+AD4-
Department of Agricultural Botany, The Hebrew University of Jerusalem
Faculty of Agriculture, P.O.Box 12, Rehovot 76100, ISRAEL
Phone: +-972 8 9481918   Fax:   +-972 8 9467763
Web page:    http://www.agri.huji.ac.il/+AH4-marder




From owner-biophysics@net.bio.net Tue Dec 16 22:00:00 1997
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From: biohelp (BIOSCI Administrator)
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Subject: BIOSCI/bionet miniFAQ & Fundraiser
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-------------------------------------------------------
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From owner-biophysics@net.bio.net Tue Dec 16 22:00:00 1997
Path: biosci!daresbury!not-for-mail
From: Pentcho Valev <RUMYM@BGEARN.ACAD.BG>
Newsgroups: bionet.biophysics
Subject: Definition of chemical work
Date: 17 Dec 1997 07:17:09 -0000
Lines: 37
Sender: lpddist@mserv1.dl.ac.uk
Distribution: bionet
Message-ID: <677u9l$hlc@mserv1.dl.ac.uk>
Original-To: biophys@dl.ac.uk


Jonathan Marder wrote:>>>>>>>>>>>>>>>>>>>
Pentcho raised the difficulty of defining chemical work. Perhaps the
following general definition of work will be useful:-
 "Work performed on a system is the act of moving that system away from
equilibrium".
In a sense, this simply restates an aspect of the second law of
thermodynamics,
so Pentcho will object. On the other hand this definition appears
applicable to work in all its forms.<<<<<<<<<<<<<<<<<<<<

Yes Jonathan I object but not simply because you redefine delta G as a
measure of chemical work. This definition contradicts our basic
understanding of physical reality. Please consider a most general picture:

A system does work, isothermally, on the surroundings. How? There are two
possibilities:

1. The system uses its internal energy for doing work. Obviously in this
case its internal energy decreases in the process.

2. The system, like an ideal gas, uses external energy for doing work.
In this case its internal energy remains the same.

Please note that in both cases the internal energy of the system CANNOT
INCREASE. Now your definition allows the system, in principle, to
INCREASE its internal energy while doing work.

Here is the crux of the problem. The second law is a principle forbiding
an alleged absurdity in physical reality - e.g. cyclical isothermal
conversion of heat into work. However its extension in the chemical world
leads to another absurdity - a system which does work on the surroundings
and increases its internal energy in the process. We are to choose - if
one is absurdity, the other is not, and vice versa.

Best regards,
Pentcho

From owner-biophysics@net.bio.net Tue Dec 16 22:00:00 1997
Path: biosci!bcm.tmc.edu!news.msfc.nasa.gov!newsfeed.internetmci.com!193.174.75.126!news-was.dfn.de!news-fra1.dfn.de!news.kfa-juelich.de!aix.zam.kfa-juelich.de!med050
From: med050@aix.zam.kfa-juelich.de (d.gembris)
Newsgroups: bionet.neuroscience,bionet.biophysics,de.sci.biologie,sci.med.physics,sci.techniques.mag-resonance,sci.med.informatics
Subject: Re: Announcement: new brain-research WWW site
Date: 17 Dec 1997 15:51:06 GMT
Organization: Forschungszentrum Juelich GmbH (KFA)
Lines: 12
Distribution: world
Message-ID: <678sda$cr6@zam201.zam.kfa-juelich.de>
References: <671j1k$llk@zam201.zam.kfa-juelich.de>
NNTP-Posting-Host: aix.zam.kfa-juelich.de
Keywords: fMRI, BOLD, MR, MRI, functional MR, modelling,
Xref: biosci bionet.neuroscience:20993 bionet.biophysics:3811

To all webmasters of MR-sites: Could you please set
a link to our pages? We have already set links to
several other MRI-Sites.

If you do so please notify me with a short eMail:

d.gembris@fz-juelich.de

Thanks a lot.

Daniel Gembris
Research Center Juelich

From owner-biophysics@net.bio.net Tue Dec 16 22:00:00 1997
Path: biosci!agate!logbr