From owner-biophysics@net.bio.net Sun Feb 01 22:00:00 1998
Newsgroups: bionet.biophysics
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From: aekentsi@midway.uchicago.edu (alex emil kentsis)
Subject: Re: stray light
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Date: Mon, 2 Feb 1998 14:18:59 GMT
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i am not sure if you are asking about background light levels, as from an
ambient light leak, or about this strange phenomenon we've encountered. if
the solution level in teh observation cuvette is below a certain level,
the fluorimeter produces curved baselines. we think it's due to teh
elevation of the meniscus in the cuvette which somehow produces stray
light. if the meniscus is covered with a piece of tape or the solution
volume increased so that it's far away from teh incident beam, the anomaly
disappears. very strange.

 David Scott (djs17@york.ac.uk) wrote:
: Hia
: Does anyone out there know anything about stray light in a fluorimeter
: and how to calculate/correct/get rid of it?
: We have an application where this may be a problem
: Thanks in advance

: Dave Scott

From owner-biophysics@net.bio.net Sun Feb 01 22:00:00 1998
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From: "Marc W. Slutzky" <mslutzky@nwu.edu>
Newsgroups: bionet.biophysics
Subject: APS March Meeting
Date: Mon, 02 Feb 1998 11:16:32 -0600
Organization: Northwestern University, Evanston, IL.  USA
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I am looking for a roommate for the American Physics Society March
Meeting in L.A.  I am a graduate student in Biomedical Engineering at
Northwestern University.  I'm looking for a non-smoking roommate from
March 14th-20th.  If interested, please email me at mslutzky@nwu.edu  .
Thank you

--

Marc W. Slutzky
Northwestern University, Evanston, IL.  USA
mslutzky@nwu.edu



From owner-biophysics@net.bio.net Mon Feb 02 22:00:00 1998
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From: Christophe GOEURY <goeury@lien.u-nancy.fr>
Newsgroups: sci.bio.technology,sci.med.physics,sci.physics.electromag,bionet.biophysics,can.med.misc,fr.sci.biometrie,sci.engr.biomed,sci.materials,sci.med.telemedicine
Subject: phantom simulated dielectric properties of human tissues
Date: Tue, 03 Feb 1998 17:09:46 +0100
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Hello,
I'm a french seeker and I'm working in bioelectromagnetism.
I would like to use a phantom for simulating the dielectric 
properties of human tissues in the ELF freqency range(0-100kHz).
Would you send me informations and documentations about existing
products and phantom if you have. In the negative, would you
give me links of whatever else.
Thanks very much and I'm waiting for you.

Christophe GOEURY
--

From owner-biophysics@net.bio.net Mon Feb 02 22:00:00 1998
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From: Medical Electronics Lab <rosing@physiology.wisc.edu>
Newsgroups: sci.bio.technology,sci.med.physics,sci.physics.electromag,bionet.biophysics,can.med.misc,fr.sci.biometrie,sci.engr.biomed,sci.materials,sci.med.telemedicine
Subject: Re: phantom simulated dielectric properties of human tissues
Date: Tue, 03 Feb 1998 12:57:17 -0600
Organization: Dept. Physiology, U. Wisconsin
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Uncle Al wrote:
> We always use undergraduates.  They are abundant, self-housing,
> acceptable models for human beings (except the pre-meds and jocks), and
> can be charged course credits.  If it works in undergrads we go to
> rats.  There are strict rules for using rats, and they are expensive.

:-)  Grads and med students make useful phantoms too.

Patience, persistence, truth,
Dr. mike

From owner-biophysics@net.bio.net Mon Feb 02 22:00:00 1998
Path: biosci!bloom-beacon.mit.edu!panix!howland.erols.net!ix.netcom.com!news
From: Uncle Al <UncleAl0@ix.netcom.com>
Newsgroups: sci.bio.technology,sci.med.physics,sci.physics.electromag,bionet.biophysics,can.med.misc,fr.sci.biometrie,sci.engr.biomed,sci.materials,sci.med.telemedicine
Subject: Re: phantom simulated dielectric properties of human tissues
Date: Tue, 03 Feb 1998 09:19:00 -0800
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Christophe GOEURY wrote:
> 
> Hello,
> I'm a french seeker and I'm working in bioelectromagnetism.
> I would like to use a phantom for simulating the dielectric
> properties of human tissues in the ELF freqency range(0-100kHz).
> Would you send me informations and documentations about existing
> products and phantom if you have. In the negative, would you
> give me links of whatever else.
> Thanks very much and I'm waiting for you.
> 
> Christophe GOEURY
> --

We always use undergraduates.  They are abundant, self-housing,
acceptable models for human beings (except the pre-meds and jocks), and
can be charged course credits.  If it works in undergrads we go to
rats.  There are strict rules for using rats, and they are expensive.

-- 
Uncle Al Schwartz
UncleAl0@ix.netcom.com ("zero" before @)
http://pw2.netcom.com/~uncleal0/uncleal.htm
http://www.ultra.net.au/~wisby/uncleal.htm
http://www.guyy.demon.co.uk/uncleal/uncleal.htm
 (Toxic URLs! Unsafe for children, Democrats, and most mammals)
"Quis custodiet ipsos custodes?"  The Net!

From owner-biophysics@net.bio.net Mon Feb 02 22:00:00 1998
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From: david kony <David.Kony@cabe.unige.ch>
Newsgroups: bionet.biophysics
Subject: polysaccharides database
Date: Tue, 03 Feb 1998 20:03:17 +0100
Organization: Universite de Geneve (CABE)
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hi!

I'm looking for NMR or/and X-RAY data concercing polysaccharides.

thank you for any information you can give me.

bye,

david

From owner-biophysics@net.bio.net Mon Feb 02 22:00:00 1998
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From: Brian M Burkhart <burkhart@hwi.buffalo.edu>
Newsgroups: bionet.biophysics
Subject: dielectric constant of a membrane bilayer
Date: Tue, 03 Feb 1998 14:30:17 -0500
Organization: Hauptman-Woodward Medical Research Institute
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I would be interested to see some discussion of the dielectric constant
properties of the interior of a membrane bilayer.  Gradient towards the
center? Or is the 80/2 model sufficient?  How similar are various
organic solvent systems to the membrane bilayer (n-alcohols, glacial
acetic acid, alkanes, fatty acids, etc)

-- 
Brian M Burkhart, Ph.D.
Hauptman-Woodward Medical Research Institute
73 High Street Buffalo, NY 14203
Phone: (716)856-9600 x313  FAX: (716)852-6086

From owner-biophysics@net.bio.net Tue Feb 03 22:00:00 1998
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From: Schmidt.GEMETEC@t-online.de (Peter Schmidt)
Newsgroups: sci.bio.technology,sci.med.physics,sci.physics.electromag,bionet.biophysics,can.med.misc,fr.sci.biometrie,sci.engr.biomed,sci.materials,sci.med.telemedicine
Subject: Re: phantom simulated dielectric properties of human tissues
Date: 3 Feb 1998 19:53:10 GMT
Organization: GEMETEC Aachen mbH
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To: goeury@lien.u-nancy.fr, goeury@lien.u-nancy.fr

Hello, Christophe GOEURY 

I made my thesis paper in biotechnological engineering on a field theory
topic. Modelling was one of the tasks to do. I cannot instantly give you
the proper source, but there is an excellent book on bioelectrical
capabilities of tissue written by J. P. Reilly (sp. as far as I can
remember).

This does not give you the phantom, but for basic research this might be
a good point to start.

The IEEE Journal on ?Biotechnology or Biomedical Engineering? also
regularly delivers articles about modelling.

Please mail me (and do not forget to remove the "antispm" thing in the
reply-to address;-) if you need more information, i can look it up for
you in my paper.

You wrote:
> 
...
> I would like to use a phantom for simulating the dielectric
> properties of human tissues in the ELF freqency range(0-100kHz).

well, there is not only dielecticity, but also ionic conduction.
Especially the low range bears some interestin unlinearities
(stimulation!).

> Would you send me informations and documentations about existing
> products and phantom if you have. In the negative, would you
> give me links of whatever else.
...

CU on the net,

Peter Schmidt
-- 
Schmidt.GEMETEC@t-online.de (Dipl.-Ing. Peter B. Schmidt)
GEMETEC Aachen mbH, Germany http://home.t-online.de/home/GEMETEC-AC
Snail: Pauwelsstrasse 19, D-52074 Aachen, Germany
Voice: +49 241 44 68 224, Fax: +49 241 44 68 229


From owner-biophysics@net.bio.net Tue Feb 03 22:00:00 1998
Path: biosci!CUB.UCA.EDU!RDJ0288
From: RDJ0288@CUB.UCA.EDU
Newsgroups: bionet.biophysics
Subject: (none)
Date: 4 Feb 1998 13:40:53 -0800
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sUBCRIBE BIOPHYS@NET.BIO.NET RICHARD JOHNSON

From owner-biophysics@net.bio.net Tue Feb 03 22:00:00 1998
Path: biosci!daresbury!not-for-mail
From: Alex Spirov <spirov@iephb.ru>
Newsgroups: bionet.biophysics
Subject: Preprint on line: PARASITIC MOBILE GENETIC ELEMENTS IN SIMULATIONS OF EVOLUTION
Date: 4 Feb 1998 19:34:17 -0000
Lines: 90
Sender: lpddist@mserv1.dl.ac.uk
Distribution: bionet
Message-ID: <6bafrp$hjf@mserv1.dl.ac.uk>
MIME-Version: 1.0
Original-To: "'bionet.info-theory'" <bio-info@dl.ac.uk>,
 "'bionet.general'"
 <bioforum@dl.ac.uk>,
 "'bionet.biophysics'"
 <biophys@dl.ac.uk>,
 "'bionet.biology.computational'"
 <comp-bio@dl.ac.uk>,
 "'bionet.molbio.evolution'"
 <mol-evol@dl.ac.uk>

        This announcement is being cross-posted to several newsgroups.
        Please, excuse the duplication.

Dear All,

The following paper is now available=20
as HTM Pages:

http://www.iephb.ru/~spirov/te-tech/te-tech.htm

and as ZIP-compressed
PostScript file via anonymous ftp from:

ftp://ftp.iephb.ru/pub/spirov/te_tech.zip (528 KB)


These materials are submitted to "Evol.Comp.Journal".=20

Title: "VARIABLE-LENGTH GENOMES, OPERATORS OF TRANSPOSITION AND =
PARASITIC MOBILE GENETIC ELEMENTS IN SIMULATIONS OF EVOLUTION"

Authors: Alexander V. Spirov and Alexander B. Kazansky

ABSTRACT

The progress in the field of evolutionary self-learning algorithms is =
primarily associated with the development of the set of operators, =
realising the process of evolutionary search and adaptation. It is a =
matter of fact, that the low "evolvability" of neo-darwinian population =
with the classical set of evolutionary operators put a fundamental =
limitation on the effectivity and universality of evolutionary =
computations, based on this type of evolving system. The realisation of =
this fact stimulates the constant interest of specialists in the field =
of evolutionary computations to the achievements in evolutionary and =
molecular biology. Godsends of nature can be adapted and applied to =
evolutionary algorithms for perfection of the instrument for solving of =
the hard optimisation problems. The creative role of viruses and =
virus-like elements in evolution attracts nowadays a great interest of =
evolutionary biologists as well as specialists in evolutionary =
computations.

In this work we put forward a new approach to evolutionary algorithms - =
Transposable Elements (TE) technique. This technique was evaluated and =
tested by the example of solving of biological, as well as classical =
test behavioural problems (the John Muir's trail in ant's navigation =
problem).

The approach is based on the application of new algorithms, modelling =
co-evolution of host population and a set of selfish/parasite mobile =
genetic elements (transposons). These elements have ability to insertion =
in the host's genome and to move from one genome site to another. =
Besides, transposons are heritable and can be transmitted to the next =
generations as well as to the other host during 'contacts'.

Our TE technique presupposes the application of special new TE operators =
of evolutionary computations along with classical ones. The TE operators =
act on genes-strings of variable length just as known variable-length =
operators of duplication, elimination and random addition.

The TE technique is effective in cases, when traditional neo-darwinian =
populations in framework of classical approaches loses the evolvability. =
This technique gives selection advantage to functionally redundant, more =
complex programs in the bottlenecks of evolutionary process.

The developed method was successfully applied to the simulation of =
biological evolution and to solving of ant's navigation test for =
non-standard variant of trail. The possibilities for application of =
proposed technique for solving GA-hard problems has being discussed as =
well.

KEYWORDS: self-organisation, evolution, transposons, genetic algorithms, =

genetic networks, artificial life, evolutionary biology.

(13 pages, 9 color illus.)

	PS: The PS-file was generated by WinWord 7 and tested
by GhostScript viewer for Windows.=20

________________________
Alexander V.Spirov (PhD)
The Sechenov Institute of Evolutionary Physiology & Biochemistry, Thorez =
Pr. 44, S.-Petersburg, 194223, Russia
phone/fax +7 (812)552 3219;  fax + 7 (812)552-3012 =
http://www.iephb.ru/~spirov/; Email spirov@iephb.ru
and
Institute for High-Performance Computing & Data Bases, P.O. Box 71, =
St.Petersburg 194291, RUSSIA



From owner-biophysics@net.bio.net Tue Feb 03 22:00:00 1998
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From: Linda Chamberlain <rteam@netzone.com>
Newsgroups: bionet.biophysics
Subject: Conference Announcement
Date: Wed, 04 Feb 1998 10:16:45 -0700
Organization: Alcor Life Extension Foundation
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You are invited to attend a conference on advances in life extension 
and cryopreservation.  For more information on the Alcor Life 
Extension Foundation and this year's Conference:

http://www.alcor.org 
(click on the blue Phoenix icon, then on "Conference")



Presentations, Talks and Panels by:

Fred Chamberlain
Linda Chamberlain
Michael Cloud
Mike Darwin
Robert Ettinger
Greg Fahy, Ph.D.
Ralph Merkle, Ph.D.
Marvin Minsky, Ph.D. (tbc)
Dave Pizer
Paul Segall, Ph.D.
Hal Sternberg, Ph.D.
Brian Wowk, Ph.D.

Lodging: $99/night, single or double room, $119 for four people.  Be
sure to tell the reservation clerk that you are attending the Alcor
Conference and give them the following code: ALC.

Fifty rooms held through March 4, 1998.  For additional information,
contact the Chamber of Commerce in Scottsdale at (800)877-1117 or in
Phoenix at (602)254-5521 (No toll free Ch.Comm in Phoenix!)

For frugal conference attendees, there are two Super 8 Motels near
the airport and conference hotel with shuttles.  The toll-free
reservation number is 1-800-800-8000.

Conference Cost: Full package includes all presentations and
materials, Saturday luncheon and Saturday evening banquet. 

Regular Rate... if received by March 3, 1998...$149 

Late Rate... if received by April 2, 1998...$179 

Door Rate......$195 

Register by phone: (800) 367-2228 - Ask for Joe Hovey.  Visa or
MasterCard accepted; you may mail registration - see below: You may
mail your registration and payment to: 1998 Alcor Conference, 7895 E.
Acoma Dr., Ste. 110, Scottsdale, AZ 85260. Please make check payable
to Alcor Foundation, and give us your full name, address, and phone
number.  Your check will be your receipt; please pick up tickets at
the Conference.

Friday, April 3, 1998

7:00-10:00 pm	Welcome: Registration, Reception

Saturday, April 4, 1998

9:00-9:15 am	Introduction - Fred Chamberlain, Alcor President/CEO
9:15-10:30 am	Greg Fahy, Ph.D. - "CryoPreservation of the Human Brain"
10:30-11:30 am	Mike Darwin - "Newly Developed and Emerging
                                                      Technologies for
Human CryoPreservation"

11:30-1:30 pm	Luncheon (provided with registration, or available 
                                separately, see fee below)

1:30-2:30 pm	Brian Wowk, Ph.D. - "Toward Human Vitrification"
2:30-3:30 pm	Fred & Linda Chamberlain, , Alcor CEO and Alcor
                                      CryoTranport Manager - "Cryonics
Rescue Systems"
3:30-4:30 pm	Ralph Merkle, Ph.D. - "Nanotechnology Update and
Molecular 				 
                                                                 Repair
of the Brain" 
4:30-5:30 pm	Paul Segall, Ph.D. and Hal Sternberg, Ph.D. - 
                                                "Advances in Low
Temperature Medicine"

7:00-7:30 pm	Reception; no host bar

7:30-11:00 pm	Banquet

8:30-11:00 pm	Panel: What's in It for Me? -  Marvin Minsky, Ph.D. (tbc)

	
Sunday, April 5, 1998

TRACK-I

8:45-9:30 am	Bus to Alcor Facility
9:30-11:15 am	Alcor Tour and Sign-up Party
11:15-11:45 am	Bus returns to Conference Site

TRACK-II

9:30-11:45		Panel: Identity and Reanimation - Fred Chamberlain

11:45 am-1:30 pm	Lunch (on your own)

1:30-2:30 pm	Alan Stoner & Mark Thompson - Smith Barney's
                                "Cryonics Wealth Preservation Programs"
2:30-3:30 pm	Michael Cloud - "How to Make the Idea of  Cryonics
                                                         Infectious"
3:30-4:00		Break	
4:00-4:30 pm	Dave Pizer - "A Retirement Community and Safe
                                                    Storage
Alternatives"	
4:30-5:00 pm	Robert Ettinger - "Where are we headed?"
5:00-5:30 pm	Closing Comments - Linda Chamberlain

END OF EMAIL
Linda Chamberlain (linda@alcor.org)
CryoTransport Manager
Alcor Life Extension Foundation
Non-profit cryonic suspension services since 1972.
7895 E. Acoma Dr., Suite 110, Scottsdale AZ 85260-6916
Phone (602) 922-9013  (800) 367-2228   FAX (602) 922-9027
info@alcor.org for general requests
http://www.alcor.org

From owner-biophysics@net.bio.net Tue Feb 03 22:00:00 1998
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From: kfoster@red.seas.upenn.edu (Kenneth R Foster)
Newsgroups: sci.bio.technology,sci.med.physics,sci.physics.electromag,bionet.biophysics,can.med.misc,fr.sci.biometrie,sci.engr.biomed,sci.materials,sci.med.telemedicine
Subject: Re: phantom simulated dielectric properties of human tissues
Followup-To: sci.bio.technology,sci.med.physics,sci.physics.electromag,bionet.biophysics,can.med.misc,fr.sci.biometrie,sci.engr.biomed,sci.materials,sci.med.telemedicine
Date: 4 Feb 1998 17:21:16 GMT
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: > I would like to use a phantom for simulating the dielectric
: > properties of human tissues in the ELF freqency range(0-100kHz).
: > Would you send me informations and documentations about existing
: > products and phantom if you have. In the negative, would you
: > give me links of whatever else.
: 

All kidding aside, it depends on how accurately you want to model the body, 
and what the mechanical properties of the phantom need to be.

In this frequency range the loss tangent of tissue is very high, i.e. you
do not have to worry too much about the permittivity.  For most purposes
a simple saline solution should work.  If you want to model anatomical
structures, you will need to use some kind of gelling agent, taking care
to keep the conductivity appropriate for tissue. Some conductivity data
are in my review in the CRC Reviews on Biomedical Engineering published
a few years ago, but other sources are available also.

If you need to correctly model the permittivity as well, you are in trouble
since there is no convenient (or feasible, I think() way to get the high
permittivity values of tissue at low frequencies using simple phantom
liquids.

In case you are interested, there will be a conference on electrical 
bioimpedance in Barcelona, April 5-9, 1998, and a lot of people there would 
undoubtably be interested in your work.  

See

Contact Prof. Pere Riu  priu@eel.upc.es 
Departament d'Enginyeria Electrsnica
Universitat Politicnica de Catalunya
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From owner-biophysics@net.bio.net Tue Feb 03 22:00:00 1998
Path: biosci!agate!howland.erols.net!news-peer.gip.net!news-lond.gip.net!news.gsl.net!gip.net!nntp.news.xara.net!xara.net!server5.netnews.ja.net!daresbury!not-for-mail
From: Pentcho Valev <RUMYM@BGEARN.ACAD.BG>
Newsgroups: bionet.biophysics
Subject: Dielectric constant of biomembranes
Date: 4 Feb 1998 09:34:22 -0000
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Brian M Burkhart <burkhart@hwi.buffalo.edu> wrote:>>>>>>>>>>>>
I would be interested to see some discussion of the dielectric constant
properties of the interior of a membrane bilayer.  Gradient towards the
center? Or is the 80/2 model sufficient?  How similar are various
organic solvent systems to the membrane bilayer (n-alcohols, glacial
acetic acid, alkanes, fatty acids, etc)<<<<<<<<<<<<<<<<<<<<

I would also like to see a discussion on the same topic and tried to
initiate it a few times but failed. There are at least two extremely
interesting bioenergetic implications related to a possible variation
of the dielectric constant both along and across the membrane. Let me
briefly describe them.

1. If the dielectric constant varies ALONG the membrane and if Donnan
transmembrane potential difference is established, the combination of the
following two universally accepted facts: a) that the potential is
uniform on each side of the membrane b) that the transmembrane potential
difference is equal to the ratio of the surface charge density and the
capacitance - leads inevitably to the incredible result that, even at
(Donnan) equilibrium, there are local lateral and, accordingly,
transmembrane fluxes of some ion, e.g. H+.


2. Let us consider the following equilibrium system:

   pH 7           M1              pH 2            M2            pH 7

where M1 and M2 are membranes permeable only to H+ and whose dielectric
constants are respectively high and low. What should be noted is that
the surface charge density (H+ concentration) is higher on the LEFT side
of M1 than on the RIGHT side of M2, but both places are at the SAME
electrical potential. In other words, there is a H+ concentration difference
between the far sides of the membranes, but no potential difference.
If, in a thought experiment, the two membranes approach each other until the
space between them becomes microscopic, we obtain a model of a membrane whose
dielectric constant varies ACROSS it. What is remarkable however is that
in the case of Donnan equilibrium there is a transmembrane concentration but
no potential difference, i.e. we can expect a transmembrane H+ flux.

My description is incomplete and therefore contains contradictions (it is
strange to speak of equilibrium and a transmembrane flux at the same time),
but everything could be clarified in a discussion.

Pentcho Valev

From owner-biophysics@net.bio.net Wed Feb 04 22:00:00 1998
Path: biosci!CCVAX.SINICA.EDU.TW!mbmtchan
From: mbmtchan@CCVAX.SINICA.EDU.TW (ming-tsair Chan)
Newsgroups: bionet.biophysics
Subject: PI Positions
Date: 5 Feb 1998 02:32:34 -0800
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From owner-biophysics@net.bio.net Wed Feb 04 22:00:00 1998
From: mjts@usa.net
Newsgroups: bionet.biophysics
Subject: help
Date: Thu, 05 Feb 1998 08:51:59 GMT
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In a photoelectic experiment, if light of  wavelength is first
0.0000004m.
The wavelength is then changed to 0.0000003m, but the intensity is
kept constant.

Why for the same intensity, the number of photons is smaller by ¾ and
the current is then decreased ?
And what actually ‘intensity’ means ?


From owner-biophysics@net.bio.net Wed Feb 04 22:00:00 1998
Path: biosci!bloom-beacon.mit.edu!senator-bedfellow.mit.edu!usenet
From: "Timothy E. Vaughan" <tvaughan@epore.mit.edu>
Newsgroups: sci.med.physics,bionet.biophysics
Subject: Re: phantom simulated dielectric properties of human tissues
Date: Wed, 04 Feb 1998 09:14:26 -0500
Organization: Harvard-MIT Division of Health Sciences and Technology
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Peter Schmidt wrote [and I snipped]:

> I made my thesis paper in biotechnological engineering on a field theory
> topic. Modelling was one of the tasks to do. I cannot instantly give you
> the proper source, but there is an excellent book on bioelectrical
> capabilities of tissue written by J. P. Reilly (sp. as far as I can
> remember).

The title of Reilly's book, if it is the one I am thinking of,
is"Electrical Stimulation and Electropathology", and it is from
Cambridge University Press, 1992.

Another potentially useful starting point is and article by K. R. Foster
and H. P. Schwan: "Dielectric properties of tissues and biological
materials: A critical review", which is in Critical Reviews in Biomedical
Engineering, vol. 17, Issue 1 (1989).

> This does not give you the phantom, but for basic research this might be
> a good point to start.

This is true of the Foster and Schwan article, too.




From owner-biophysics@net.bio.net Wed Feb 04 22:00:00 1998
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From: prismx@scienceweek.com (Claire Haller)
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12. Motor Proteins and Organelle Transport
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From owner-biophysics@net.bio.net Sat Feb 07 22:00:00 1998
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From: "Jonathan B. Marder" <marder@agri.huji.ac.il>
Newsgroups: bionet.biophysics
Subject: Re: Dielectric constant of biomembranes
Date: Sun, 8 Feb 1998 12:23:18 +0200
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Pentcho Valev wrote in message =
+ADw-6b9cmu+ACQ-d43+AEA-mserv1.dl.ac.uk+AD4-...
...
+AD4-
+AD4-1. If the dielectric constant varies ALONG the membrane and if =
Donnan
+AD4-transmembrane potential difference is established, the combination =
of the
+AD4-following two universally accepted facts: a) that the potential is
+AD4-uniform on each side of the membrane b) that the transmembrane =
potential
+AD4-difference is equal to the ratio of the surface charge density and =
the
+AD4-capacitance - leads inevitably to the incredible result that, even =
at
+AD4-(Donnan) equilibrium, there are local lateral and, accordingly,
+AD4-transmembrane fluxes of some ion, e.g. H.
+AD4-
...
Pentcho, this is really not so mysterious. There are lateral movements =
of ions until electroCHEMICAL equilibrium is reached. Once this happens, =
there will be no more net ion fluxes. I see no problem with membrane =
patches attracting concentrations of particular ions - in fact I expect =
that this is documented in the literature.




From owner-biophysics@net.bio.net Sat Feb 07 22:00:00 1998
Path: biosci!OUT.HIX.COM!publisher
From: publisher@OUT.HIX.COM ("HIX")
Newsgroups: bionet.biophysics
Subject: *** HIXCD/8 *** HIXCD/8 *** HIXCD/8 ***
Followup-To: poster
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-- English description is at the end --

---------------------------------------------------------------------------
-- Elofordulhat, hogy ezt a levelet tobb peldanyban kapod meg. Ez azt
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-- program nem tudott megfeleltetni egymasnak. Mivel egyszeri ertesitesrol
-- van szo, remelem, ezt a kis kellemetlenseget nem veszed zokon.
-- Ez a level a To: mezoben lathato cimedre erkezett.
---------------------------------------------------------------------------

Szia!

Keszuloben van egy jubileumi HIXCD a HIX 8. szuletesnapjara, februar
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                       hixcd@hix.com
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English description:

This letter is to announce a non-profit CDROM containing the 8-year long
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From owner-biophysics@net.bio.net Sun Feb 08 22:00:00 1998
Path: biosci!daresbury!not-for-mail
From: Pentcho Valev <RUMYM@BGEARN.ACAD.BG>
Newsgroups: bionet.biophysics
Subject: Membrane capacitance
Date: 9 Feb 1998 08:08:17 -0000
Lines: 33
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Message-ID: <6bmdhh$gsq@mserv1.dl.ac.uk>
Original-To: biophys@dl.ac.uk

Jonathan Marder wrote:>>>>>>>>>>>>>>>>>>
Pentcho, this is really not so mysterious. There are lateral movements
of ions until electroCHEMICAL equilibrium is reached. Once this happens,
there will be no more net ion fluxes. I see no problem with membrane
patches attracting concentrations of particular ions - in fact I expect
that this is documented in the literature.<<<<<<<<<<<<<<<<<<<

It seems to me that there will be lateral fluxes even at equilibrium
(although half of my mind rejects this as absurd). Let us have a close
look at the situation:

                         pH 2

-------high-capacitance---------low-capacitance-----------------------

                         pH 7

The membrane is permeable only to H+. If (at equilibrium) the potential in
each compartment is uniform (this is universally accepted), there will be
a lateral gradient of H+ concentration close to the membrane - e.g., in
the lower compartment, the H+ concentration will be higher at the
high-capacitance patch than at the low-capacitance one. As the potential is
uniform, we should expect a lateral H+ flux from the high-capacitance patch
to the low-capacitance one (in the lower compartment).

The other possible assumption is that, at equilibrium, the potential in
each compartment is not uniform. We could analyse this situation as well
but it is clear even without analysis that, if correct, the assumption
would disturb the established theoretical paradigm to such an extent that
practically a new theory will have to be built.

Best regards,
Pentcho

From owner-biophysics@net.bio.net Sun Feb 08 22:00:00 1998
Path: biosci!daresbury!not-for-mail
From: Pentcho Valev <RUMYM@BGEARN.ACAD.BG>
Newsgroups: bionet.biophysics
Subject: Membrane capacitance
Date: 9 Feb 1998 08:27:13 -0000
Lines: 33
Sender: lpddist@mserv1.dl.ac.uk
Distribution: bionet
Message-ID: <6bmel1$hnk@mserv1.dl.ac.uk>
Original-To: biophys@dl.ac.uk

Jonathan Marder wrote:>>>>>>>>>>>>>>>>>>
Pentcho, this is really not so mysterious. There are lateral movements
of ions until electroCHEMICAL equilibrium is reached. Once this happens,
there will be no more net ion fluxes. I see no problem with membrane
patches attracting concentrations of particular ions - in fact I expect
that this is documented in the literature.<<<<<<<<<<<<<<<<<<<

It seems to me that there will be lateral fluxes even at equilibrium
(although half of my mind rejects this as absurd). Let us have a close
look at the situation:

                         pH 2

-------high-capacitance---------low-capacitance-----------------------

                         pH 7

The membrane is permeable only to H+. If (at equilibrium) the potential in
each compartment is uniform (this is universally accepted), there will be
a lateral gradient of H+ concentration close to the membrane - e.g., in
the lower compartment, the H+ concentration will be higher at the
high-capacitance patch than at the low-capacitance one. As the potential is
uniform, we should expect a lateral H+ flux from the high-capacitance patch
to the low-capacitance one (in the lower compartment).

The other possible assumption is that, at equilibrium, the potential in
each compartment is not uniform. We could analyse this situation as well
but it is clear even without analysis that, if correct, the assumption
would disturb the established theoretical paradigm to such an extent that
practically a new theory will have to be built.

Best regards,
Pentcho

From owner-biophysics@net.bio.net Tue Feb 10 22:00:00 1998
Path: biosci!agate!logbridge.uoregon.edu!news.maxwell.syr.edu!newsfeed.nacamar.de!uni-erlangen.de!lrz-muenchen.de!not-for-mail
From: Gerald Mathias <Gerald.Mathias@Physik.Uni-Muenchen.DE>
Newsgroups: bionet.biophysics
Subject: Re: help
Date: Wed, 11 Feb 1998 13:27:32 +0100
Organization: [posted via] Leibniz-Rechenzentrum, Muenchen (Germany)
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Intensity means the amount of energy per second per m*m. As the
waveleght is shortent the amount of energy per photon is increased, so
you nead less photons for the some intensity.


From owner-biophysics@net.bio.net Wed Feb 11 22:00:00 1998
Path: biosci!daresbury!not-for-mail
From: Nick Art <Art@EMBL-Hamburg.DE>
Newsgroups: bionet.biophysics
Subject: Entropy question
Date: 12 Feb 1998 17:48:17 -0000
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Dear All,


I hope if someone could tell me the difference between
the statistical entropy and thermodynamic entropy.


Many thanks,

Nick


From owner-biophysics@net.bio.net Wed Feb 11 22:00:00 1998
From: 133@109.com
Newsgroups: bionet.biophysics
Subject: NLREG - Nonlinear & linear statistical regression program - 34 0212180124 CMI
Date: Thu, 12 Feb 98 18:01:25
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-- 34: bionet.biophysics 0212180124 --


From owner-biophysics@net.bio.net Wed Feb 11 22:00:00 1998
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From: fujimoto@u.washington.edu (Bryant Fujimoto)
Newsgroups: bionet.biophysics
Subject: Re: Entropy question
Date: 12 Feb 1998 21:26:27 GMT
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Nick Art <Art@EMBL-Hamburg.DE> writes:

>Dear All,


>I hope if someone could tell me the difference between
>the statistical entropy and thermodynamic entropy.


If by statistical entropy, you mean the entropy defined in
statistical mechanics, it is assumed that it is the same as
the thermodynamic entropy.  Measurements of the entropy using
the methods of statistical mechanics have always yielded the
same result as measurements using the results of thermodynamics.

Bryant Fujimoto

From owner-biophysics@net.bio.net Thu Feb 12 22:00:00 1998
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From: M.Makris@shef.ac.uk (E Demoncheaux)
Newsgroups: bionet.biophysics
Subject: General question
Date: 13 Feb 1998 14:52:10 GMT
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Could someone explain the difference between kinetic and thermodynamic 
stability?


From owner-biophysics@net.bio.net Thu Feb 12 22:00:00 1998
Path: biosci!daresbury!not-for-mail
From: Pentcho Valev <RUMYM@BGEARN.ACAD.BG>
Newsgroups: bionet.biophysics
Subject: Boltzmann's and thermodynamic entropy
Date: 13 Feb 1998 14:23:23 -0000
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Bryant Fujimoto wrote:>>>>>>>>>
Nick Art <Art@EMBL-Hamburg.DE> writes:
>Dear All,
>I hope if someone could tell me the difference between
>the statistical entropy and thermodynamic entropy.

If by statistical entropy, you mean the entropy defined in
statistical mechanics, it is assumed that it is the same as
the thermodynamic entropy.  Measurements of the entropy using
the methods of statistical mechanics have always yielded the
same result as measurements using the results of thermodynamics.<<<<<<<

We have already discussed that, Bryant, on a suitable model devised by
R. Alberty (do you remember?). We found that, in order for Boltzmann's
(klnW) and thermodynamic entropy to coincide, some systems must
SPONTANEOUSLY move from a MORE probable to a LESS probable state. So I
hope you would agree with the following answer: If systems can
spontaneously move from a more probable to a less probable state, the two
entropies coincide. If not, not.

In my opinion, spontaneous movement from a more probable to a less probable
state is a LOGICAL absurdity, but I may be wrong.

Best regards,
Pentcho

From owner-biophysics@net.bio.net Thu Feb 12 22:00:00 1998
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From: Marc Roussel <roussel@henri.chem.uleth.ca>
Newsgroups: bionet.biophysics
Subject: Re: General question
Date: Fri, 13 Feb 1998 12:20:09 -0700
Organization: Department of Chemistry and Biochemistry, University of Lethbridge
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E Demoncheaux wrote:
> Could someone explain the difference between kinetic and thermodynamic
> stability?

Easily done by example:  Diamonds are thermodynamically unstable
relative to graphite at standard temperature and pressure which means
that their free energy is higher than that of graphite.  Thus, every
diamond that has ever been dug out of the ground is slowly converting to
graphite.  (Contrary to the popular saying, diamonds are not forever.) 
However, diamonds are kinetically stable in the sense that the rate
constant for this conversion is immeasurably small.

				Marc R. Roussel
				(roussel@uleth.ca)
				Department of Chemistry and Biochemistry
				University of Lethbridge

From owner-biophysics@net.bio.net Thu Feb 12 22:00:00 1998
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From: fujimoto@u.washington.edu (Bryant Fujimoto)
Newsgroups: bionet.biophysics
Subject: Re: Boltzmann's and thermodynamic entropy
Date: 13 Feb 1998 20:51:52 GMT
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Pentcho Valev <RUMYM@BGEARN.ACAD.BG> writes:

>Bryant Fujimoto wrote:>>>>>>>>>
>Nick Art <Art@EMBL-Hamburg.DE> writes:
>>Dear All,
>>I hope if someone could tell me the difference between
>>the statistical entropy and thermodynamic entropy.

>If by statistical entropy, you mean the entropy defined in
>statistical mechanics, it is assumed that it is the same as
>the thermodynamic entropy.  Measurements of the entropy using
>the methods of statistical mechanics have always yielded the
>same result as measurements using the results of thermodynamics.<<<<<<<

>We have already discussed that, Bryant, on a suitable model devised by
>R. Alberty (do you remember?). We found that, 

We?  Speak for yourself, don't try to speak for me.

>in order for Boltzmann's
>(klnW) and thermodynamic entropy to coincide, some systems must
>SPONTANEOUSLY move from a MORE probable to a LESS probable state. 

No.  In order for them to coincide, experimental measurements of
the entropy using statistical mechanics must agree with experimental
measurements of the entropy using thermodynamics.  Since they do,
the assumption that they are the same is accepted.

>So I
>hope you would agree with the following answer: If systems can
>spontaneously move from a more probable to a less probable state, the two
>entropies coincide. If not, not.

I don't remember how you came to conclude this, but its incorrect.

Regards,
Bryant


From owner-biophysics@net.bio.net Thu Feb 12 22:00:00 1998
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From: Thierry Leclipteux <thierry@stat.fmv.ulg.ac.be>
Newsgroups: bionet.biophysics
Subject: gold conjugates
Date: Fri, 13 Feb 1998 14:01:29 +0100
Organization: ulg
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I have a problem in conjugating a monoclonal antibody to 20 nm gold
particles.  Monoclonal pi is close to 6.5 and several trials have been
performed at ph 7, 8 and even 9 without significant increase in the
conjugate sensitivity.  In our procedure 0.01 mg IgG are incubated with
1 ml of gold particules (at 0.01 %).
I am looking for a protocol which enables me to increase this conjugate
sensitivity.
Thanks for replying either in the news or by e-mail.

From owner-biophysics@net.bio.net Fri Feb 13 22:00:00 1998
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From: Mike Marsh <mmarsh@centenary.edu>
Newsgroups: bionet.biophysics
Subject: Re: General question
Date: Sat, 14 Feb 1998 01:09:21 -0600
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To: E Demoncheaux <M.Makris@shef.ac.uk>



E Demoncheaux wrote:

> Could someone explain the difference between kinetic and thermodynamic
> stability?

E. Demoncheaux,

for a good explanation, consult a college-level organic chemistry
textbook.

in short:
thermodynamic stability means that the species is at a lower energy
relative to some reference value (e.g. the energy of the reactant or the
energy of the product)

kinetic stability usually denotes a metastable (i.e. thermondynamically
metastable) species whose energy could be lowered by a reaction, but the
kinetics of such reaction are prohibitive.

-mike

by the way,
can anybody tell me where i should go to do doctoral work in structural
biology??  i currently have applications in at scripps research inst,
baylor college of medicine, and u.c.s.d.


From owner-biophysics@net.bio.net Fri Feb 13 22:00:00 1998
Path: biosci!daresbury!not-for-mail
From: Pentcho Valev <RUMYM@BGEARN.ACAD.BG>
Newsgroups: bionet.biophysics
Subject: Boltzmann's vs. thermodynamic entropy
Date: 14 Feb 1998 12:45:34 -0000
Lines: 38
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I wrote:
>So I
>hope you would agree with the following answer: If systems can
>spontaneously move from a more probable to a less probable state, the two
>entropies coincide. If not, not.

Bryant Fujimoto replied:>>>>>>>>>>>>
I don't remember how you came to conclude this, but its incorrect.<<<<<<<

Let me remind you. Consider the following system:

---------------------------------------------------------------------------

                    A + B <-> C + D

---------membrane-permeable-only-to-D--------------------------------------

                         D

------------------------piston--------------------------------------------


This is a semi-grand ensemble: The EXOTHERMIC gas reaction A + B <-> C + D
undergoes an isothermal reversible course as D in the lower compartment
pushes a piston and expands. As heat is released by the system, the
thermodynamic entropy of the system DECREASES. On the other hand, this
reversible course has its spontaneous conterpart (D can expand irreversibly,
without pushing the piston). If, in the spontaneous process, the system
moves to a MORE probable state, Boltzmann's entropy INCREASES and does not
coincide with the thermodynamic entropy. If, in the spontaneous process,
the system moves to a LESS probable state (some people claimed so),
Boltzmann's entropy decreases, like the thermodynamic entropy.

As you can see, the problem is real and quite independent of my
personality.

Best regards,
Pentcho

From owner-biophysics@net.bio.net Sat Feb 14 22:00:00 1998
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From: mmisha@nmr.mgh.harvard.edu (M. Papisov)
Newsgroups: bionet.biophysics
Subject: Re: Boltzmann's and thermodynamic entropy
Date: Fri, 13 Feb 1998 14:14:03 -0500
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In article <6c1l0r$5lm@mserv1.dl.ac.uk>, Pentcho Valev
<RUMYM@BGEARN.ACAD.BG> wrote:

The "thermodynamic enthropy" has been invented simply to acknowledge that
not all energy can be transformed into work. Nobody could explain why at
the time. Entropy was *just a member in the thermodynamic equation*. In
the simplest case (a system is being heated, there are no chemical
reactions), thermodynamic enthropy equaled to heat capacity. Anyway,
nobody knew, at the time where, the heat might go. 

In turn, the statistical explanation of enthropy was offered simply to
demonstrate where the energy actually goes, and why it can not be
completely transformed into work.

So, there is no "coincidence" or "non-coincidence": "statistical enthropy"
is simply a mechanistic explanation of thermodynamic enthropy. If you know
*exactly* how energy can be distributed between components of your system,
you can calculate a "theoretical" value that is very close to the
experimentally determined (thermodynamic) enthropy. If you don't know what
is going on in your system (like in old good days), or if the system is
too complex, you have no chance to come up with any reasinable theoretical
estimate. 

Obviously, ALL thermodynamic systems can move from a more probable to a
less probable states and back. This is what they do all the time. Lower
probability does not mean that the state is "more difficult" to reach, it
is just that you can encounter that state less frequently. If there is a
state to which a system _can not_ move, the probability of that state
would be zero.

Regards

MP

PS: Entropy has nothing to do with order. Any objections?


        > Bryant Fujimoto wrote:>>>>>>>>>
        > Nick Art <Art@EMBL-Hamburg.DE> writes:
        > >Dear All,
        > >I hope if someone could tell me the difference between
        > >the statistical entropy and thermodynamic entropy.
        > 
        > If by statistical entropy, you mean the entropy defined in
        > statistical mechanics, it is assumed that it is the same as
        > the thermodynamic entropy.  Measurements of the entropy using
        > the methods of statistical mechanics have always yielded the
        > same result as measurements using the results of
thermodynamics.<<<<<<<
        > 
        > We have already discussed that, Bryant, on a suitable model devised by
        > R. Alberty (do you remember?). We found that, in order for Boltzmann's
        > (klnW) and thermodynamic entropy to coincide, some systems must
        > SPONTANEOUSLY move from a MORE probable to a LESS probable state. So I
        > hope you would agree with the following answer: If systems can
        > spontaneously move from a more probable to a less probable
state, the two
        > entropies coincide. If not, not.
        > 
        > In my opinion, spontaneous movement from a more probable to a
less probable
        > state is a LOGICAL absurdity, but I may be wrong.
        > 
        > Best regards,
        > Pentcho

______________He who rides on a tiger never dismounts________________

Please delete the very first letter in my email address to reply. 

Nobody at all, including my past, current and future employers, 
is responsible for whatever is written above. 

From owner-biophysics@net.bio.net Sat Feb 14 22:00:00 1998
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From owner-biophysics@net.bio.net Sat Feb 14 22:00:00 1998
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From: Alan Loberto <alan.loberto@virgin.net>
Newsgroups: bionet.biophysics
Subject: Magnetic affect on growth
Date: Sun, 15 Feb 1998 17:13:44 +0000
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I have a dying question and that is;
"Will a magnetic field have an affect on Bacterial growth?"
I would be very grateful if one would reply via e-mail to
alan.loberto@virgin.net
Thanks a lot
Alan Loberto

From owner-biophysics@net.bio.net Sat Feb 14 22:00:00 1998
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From: shahar stein <steinsXX@inter.net.il>
Newsgroups: bionet.biophysics
Subject: what is phantom
Date: Sun, 15 Feb 1998 11:21:43 +0200
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sorry for the ignorance but what is "phantom"?

From owner-biophysics@net.bio.net Sun Feb 15 22:00:00 1998
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From: fujimoto@u.washington.edu (Bryant Fujimoto)
Newsgroups: bionet.biophysics
Subject: Re: Boltzmann's vs. thermodynamic entropy
Date: 16 Feb 1998 09:23:48 GMT
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Pentcho Valev <RUMYM@BGEARN.ACAD.BG> writes:

>I wrote:
>>So I
>>hope you would agree with the following answer: If systems can
>>spontaneously move from a more probable to a less probable state, the two
>>entropies coincide. If not, not.

>Bryant Fujimoto replied:>>>>>>>>>>>>
>I don't remember how you came to conclude this, but its incorrect.<<<<<<<

>Let me remind you. Consider the following system:

>---------------------------------------------------------------------------

>                    A + B <-> C + D

>---------membrane-permeable-only-to-D--------------------------------------

>                         D

>------------------------piston--------------------------------------------


>This is a semi-grand ensemble: The EXOTHERMIC gas reaction A + B <-> C + D
>undergoes an isothermal reversible course as D in the lower compartment
>pushes a piston and expands. As heat is released by the system, the
>thermodynamic entropy of the system DECREASES. On the other hand, this
>reversible course has its spontaneous conterpart (D can expand irreversibly,
>without pushing the piston). If, in the spontaneous process, the system
>moves to a MORE probable state, Boltzmann's entropy INCREASES and does not
>coincide with the thermodynamic entropy. If, in the spontaneous process,
>the system moves to a LESS probable state (some people claimed so),
>Boltzmann's entropy decreases, like the thermodynamic entropy.

>As you can see, the problem is real and quite independent of my
>personality.

What does your personality have to do with this?  I certainly haven't
referred to it.  Do you want me to?  If so, why?

It is possible to use thermodynamics to determine the entropy of both
the initial and final states, without having to worry about whether
the process you wish to use is reversible.  Since comparisons of these
sorts of calculations with calculations of statistical mechanics yield
good agreement, what is the problem?  The fact is that, experimental
results contradict your assertion.  Until you can point to an actual
reaction, which behaves the way you think it will, you have nothing
comparable.  Keep in mind, your system is undergoing an isothermal
expansion.  If you simply expand a non-reacting gas isothermally,
heat will flow _into_ the system.  So, how do you know that your
exothermal reaction will give off more heat than is necessary to keep
the temperature constant due to the expansion?  You haven't named the
reaction, and until you can, you don't have a demonstration of anything.

Regards,
Bryant

P.S.  What does thermodynamics mean by reversible?


From owner-biophysics@net.bio.net Sun Feb 15 22:00:00 1998
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From: szia@hanga.enzim.hu (Andras Szilagyi)
Newsgroups: bionet.biophysics
Subject: Re: Boltzmann's vs. thermodynamic entropy
Date: 16 Feb 1998 18:43:02 GMT
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On 14 Feb 1998 12:45:34 -0000, Pentcho Valev <RUMYM@BGEARN.ACAD.BG> wrote:

>---------------------------------------------------------------------------
>
>                    A + B <-> C + D
>
>---------membrane-permeable-only-to-D--------------------------------------
>
>                         D
>
>------------------------piston--------------------------------------------
>
>
>This is a semi-grand ensemble: The EXOTHERMIC gas reaction A + B <-> C + D
>undergoes an isothermal reversible course as D in the lower compartment
>pushes a piston and expands. As heat is released by the system, the
>thermodynamic entropy of the system DECREASES. On the other hand, this
>reversible course has its spontaneous conterpart (D can expand irreversibly,
>without pushing the piston). If, in the spontaneous process, the system
>moves to a MORE probable state, Boltzmann's entropy INCREASES and does not
>coincide with the thermodynamic entropy. If, in the spontaneous process,
>the system moves to a LESS probable state (some people claimed so),
>Boltzmann's entropy decreases, like the thermodynamic entropy.

Pentcho, we discussed this earlier. I'm surprised that you still don't
understand this example. Any non-isolated subsystem of a system will
spontaneously move from a MORE probable state to a LESS probable state if
the WHOLE system can move from a LESS probable state to a MORE probable
state by this. That is how life evolved, for example. In other words: if
the system is not isolated--and yours is not--then its entropy can
spontaneously decrease.

In your example, the internal energy of the system decreases during the
process. The environment takes up heat and this additional energy is
distributed among the degrees of freedom of the environment. This
distribution can be done in a very high number of ways, thus the
thermodynamic probability (for the WHOLE system) will increase. The
entropy of the WHOLE system will increase.

Andras


From owner-biophysics@net.bio.net Sun Feb 15 22:00:00 1998
Path: biosci!musc.edu!vakseri
From: vakseri@musc.edu (Ilya Vakser)
Newsgroups: bionet.biophysics
Subject: Postdocs/Graduate Students in Protein Docking and Structure Prediction
Date: 16 Feb 1998 11:24:59 -0800
Organization: Medical University of South Carolina
Lines: 35
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Distribution: world
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Applications are invited for postdoctoral and graduate student positions
in my laboratory at the Medical University of South Carolina. 
The positions were advertised in November, however, due to the delayed
release of funds, I post them again.

The main subjects of the research in the laboratory are computational
studies of molecular recognition, docking methodology, structure
prediction, and applications to signal transduction pathways and other
molecular systems. For more information, see the lab's web site at
http://reco3.musc.edu. The following positions are immediately
available:

Postdoctoral fellow
Development of flexible docking techniques for small ligands. Docking
methodology for computer-aided drug design.

Postdoctoral fellow
Modeling of integral membrane receptors. Structure prediction based on
the principles of molecular recognition.

Graduate student
General development of protein docking methodology.

Strong programming skills in C are required for all positions. 

To apply send or email a letter and CV with names of 3 referees. 

Ilya A. Vakser
Assistant Professor of Pharmacology
Department of Cell and Molecular Pharmacology
Medical University of South Carolina
171 Ashley Avenue
Charleston, SC 29425

Email: vakseri@musc.edu, Phone:(803)792-2471, Fax:(803)792-2475

From owner-biophysics@net.bio.net Sun Feb 15 22:00:00 1998
From: mmisha@nmr.mgh.harvard.edu (M. Papisov)
Newsgroups: bionet.biophysics
Subject: Re: Magnetic affect on growth
Date: Mon, 16 Feb 1998 12:29:11 -0500
Organization: MGH & HMS
Lines: 76
Message-ID: <mmisha-1602981229110001@misha.mgh.harvard.edu>
References: <34E72248.38C@virgin.net>
NNTP-Posting-Host: misha.mgh.harvard.edu
Path: biosci!agate!howland.erols.net!cpk-news-hub1.bbnplanet.com!news.bbnplanet.com!baron.netcom.net.uk!netcom.net.uk!newsfeed.wizvax.net!news.mv.net!newspump.wustl.edu!news.fas.harvard.edu!oitnews.harvard.edu!hpngsv01.mgh.harvard.edu!misha.mgh.harvard.edu!user

In article <34E72248.38C@virgin.net>, alan.loberto@virgin.net wrote:

        > I have a dying question and that is;
        > "Will a magnetic field have an affect on Bacterial growth?"
        > I would be very grateful if one would reply via e-mail to
        > alan.loberto@virgin.net

I personally have no idea, but because it's a "dying question", here is a
couple of references:

    1
AN 81247674
AU Aarholt E.  Flinn EA.  Smith CW.
TI Effects of low-frequency *magnetic* fields on *bacterial* *growth* rate.
SO Physics in Medicine & Biology.  26(4):613-21, 1981 Jul.
JC p6j
CP England
AB A large number of cultures of the bacterium E. coli have been grown in weak
   alternating *magnetic* fields of square waveform, at frequencies of 50 Hz
   and 16.66 Hz. Control cultures were simultaneously grown under ambient
   conditions identical except for the almost complete absence of any
   *magnetic* *field*. The mean generation time (MGT) for a culture subjected
   to alternating *magnetic* fields is significantly reduced by comparison
   with that for the control cultures. Application of the F-ratio test
   indicates a probability of less than one  in two million that the effects
   observed are due to chance. A marked threshold effect is observed, along
   with strong indications of periodicity in the graph of MGT against
   *magnetic* *field* strength. Within the limits of experimental error, these
   effects correspond to integral changes in the number of *magnetic* flux
   quanta linking an individual *bacterial* cell during the process of
   division.
DE *Escherichia coli/gd [*Growth* & Development].  *Magnetics.
IS 0031-9155
PT Journal Article.
LG English
EM 8111.

    2
AN 87113862
AU Pantev TP.  Minkova MI.
TI [Direct and mediated action of a permanent *magnetic* *field* on biological
   objects]. [Russian]
TT Priamoe i oposredovannoe deistvie postoiannogo magnitnogo polia na
   biologicheskie ob''ekty.
SO Kosmicheskaia Biologiia i Aviakosmicheskaia Meditsina.  20(6):73-6, 1986
   Nov-Dec.
JC kxc
CP USSR
AB The effect of a constant *magnetic* *field* (CMF) of H = 2.3 X 10(5) A/m
   (2900 Oe) on the viability and radiosensitivity of E. coli B and the effect
   of magnetically activated water (MAW) on the radioresistance of rats were
   examined. The exposure did not influence the *growth* kinetics of E. coli
   B. Cell cultivation in the magnetically pretreated nutrient medium
   enhanced the *bacterial* *growth*. Preliminary exposure of *bacterial*
   cells to a CMF for 24 and 48 hrs increased and that for 72 hrs decreased
   their radioresistance. Twice a day the experimental weanlings were given
   MAW and the controls--tap water. The postradiation longevity of the MAW
   rats proved extended as compared to that of the controls. The MAW rats
   showed a greater osmotic stability of erythrocytes, a higher concentration
   of nucleic acids, and a larger count of leucocytes.
DE Animal.  Comparative Study.  English Abstract.  Escherichia coli/ph
   [Physiology].  Gamma Rays.  *Magnetics.  Radiation Dosage.  Radiation
   Tolerance.  Rats.  Space Flight.  Time Factors.  Water/pd [Pharmacology].
   X-Rays.
RN 7732-18-5 (Water).
IS 0321-5040
PT Journal Article.
LG Russian
EM 8705.

______________He who rides on a tiger never dismounts________________

Please delete the very first letter in my email address to reply. 

Nobody at all, including my past, current and future employers, 
is responsible for whatever is written above. 

From owner-biophysics@net.bio.net Mon Feb 16 22:00:00 1998
Path: biosci!daresbury!not-for-mail
From: Pentcho Valev <RUMYM@BGEARN.ACAD.BG>
Newsgroups: bionet.biophysics
Subject: Boltzmann's versus thermodynamic entropy
Date: 17 Feb 1998 08:39:09 -0000
Lines: 53
Sender: lpddist@mserv1.dl.ac.uk
Distribution: bionet
Message-ID: <6cbibd$5m0@mserv1.dl.ac.uk>
Original-To: biophys@dl.ac.uk


Andras Szilagyi wrote:>>>>>>>>>>>>>>>>>>>>>>>>
On 14 Feb 1998 12:45:34 -0000, Pentcho Valev <RUMYM@BGEARN.ACAD.BG> wrote:

>---------------------------------------------------------------------------
>
>                    A + B <-> C + D
>
>---------membrane-permeable-only-to-D--------------------------------------
>
>                         D
>
>------------------------piston--------------------------------------------
>
>
>This is a semi-grand ensemble: The EXOTHERMIC gas reaction A + B <-> C + D
>undergoes an isothermal reversible course as D in the lower compartment
>pushes a piston and expands. As heat is released by the system, the
>thermodynamic entropy of the system DECREASES. On the other hand, this
>reversible course has its spontaneous conterpart (D can expand irreversibly,
>without pushing the piston). If, in the spontaneous process, the system
>moves to a MORE probable state, Boltzmann's entropy INCREASES and does not
>coincide with the thermodynamic entropy. If, in the spontaneous process,
>the system moves to a LESS probable state (some people claimed so),
>Boltzmann's entropy decreases, like the thermodynamic entropy.

Pentcho, we discussed this earlier. I'm surprised that you still don't
understand this example. Any non-isolated subsystem of a system will
spontaneously move from a MORE probable state to a LESS probable state if
the WHOLE system can move from a LESS probable state to a MORE probable
state by this. That is how life evolved, for example. In other words: if
the system is not isolated--and yours is not--then its entropy can
spontaneously decrease.
In your example, the internal energy of the system decreases during the
process. The environment takes up heat and this additional energy is
distributed among the degrees of freedom of the environment. This
distribution can be done in a very high number of ways, thus the
thermodynamic probability (for the WHOLE system) will increase. The
entropy of the WHOLE system will increase.<<<<<<<<<<<<<<<<<<<<<<

Andras, I do not see any contradiction between my statement and your
explanation, so there is certainly nothing which I don't understand at
that level. Still I find it awkward to accept that, as the system
(rather, only D) expands spontaneously and never returns to the initial
point, it moves from a MORE probable to a LESS probable state. Your
explanation is formally correct but it contradicts my intuition.
Unfortunately I am incompetent in statistical mechanics and cannot offer
a more reasonable objection. Still my conclusion remains valid: The
two entropies may coincide but ONLY IF SYSTEMS CAN SPONTANEOUSLY MOVE
FROM A MORE PROBABLE TO A LESS PROBABLE STATE.

Best regards,
Pentcho

From owner-biophysics@net.bio.net Mon Feb 16 22:00:00 1998
Path: biosci!internet!biosci!not-for-mail
From: biohelp (BIOSCI Administrator)
Newsgroups: bionet.biophysics
Subject: BIOSCI/bionet miniFAQ & Fundraiser
Date: 17 Feb 1998 02:00:05 -0800
Organization: BIOSCI International Newsgroups for Molecular Biology
Lines: 233
Sender: daemon@net.bio.net
Distribution: world
Message-ID: <199802171000.CAA11764@net.bio.net>
NNTP-Posting-Host: net.bio.net

(LAST REVISION: 30-JUL-95)

This BIOSCI "miniFAQ" is designed to answer the questions that come up
the *most frequently*.  The main BIOSCI FAQ (Frequently Asked
Questions) is accessible on the World Wide Web at URL
http://www.bio.net/.

If you can not find an answer to your question in this or other
documentation, the BIOSCI technical support staff answers e-mail
queries sent to

		       biosci-help@net.bio.net

We can only answer questions about the use of the newsgroups and
mailing lists.  We unfortunately do not have the staff to do Internet
information searches or answer scientific questions.  Please post
those to the appropriate BIOSCI/bionet newsgroups.


	Contents:
	--------
	0) BIOSCI NEEDS YOUR SUPPORT!!

	1) Using the WWW to access the BIOSCI/bionet newsgroups.

	2) What to do about "spams," i.e., junk mail, ads, etc.

	3) Examples of subscribing and unsubscribing to the mailing lists.

	4) The BIOSCI user address and research interest directory.


0) BIOSCI NEEDS YOUR SUPPORT!!
------------------------------
BIOSCI's government funding has been expended, and we are now
operating solely from advertising revenue that we have raised from our
Web site at http://www.bio.net/.  We need just a few minutes of your
time to help us serve you.

You can do two important things which will take very little time for
you individually and will immensely help us continue to help you.

First, please use our WWW system at http://www.bio.net/ to access the
archives.  You can post or reply to messages via your Web browser as
described in item #1 below.  Your usage helps attract sponsors. If you
contact any of our sponsors, please be sure to thank them for
supporting BIOSCI. It is critical for them to get this feedback if
they are to continue their sponsorship for the long term.

Second, if you work for a company or organization that provides
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this message on to your marketing or marketing communications
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interested, they can then contact us for further information at our
tech support address, biosci-help@net.bio.net.


1) Using the WWW to access the BIOSCI/bionet newsgroups.
--------------------------------------------------------
As of 10 December 1995, all BIOSCI/bionet full newsgroups are
accessible through the World Wide Web (WWW) at URL http://www.bio.net.
One can read and reply publicly or privately to both recent postings
and archived messages through one's Web browser if it is configured
properly to send e-mail.  Each newsgroup is equipped with its own WAIS
index.  The main BIOSCI home page also has access to the BIO-JOURNALS
Table of Contents database WAIS index and the BIOSCI user address
database described in another item further below.


2) What to do about "spams," i.e., junk mail, ads, etc.
-------------------------------------------------------
BIOSCI is a set of parallel USENET newsgroups (the "bionet" groups),
mailing lists, and a hypermail archive at URL http://www.bio.net/.
The same postings are distributed on all media (except for a small
number of mailing-list-only groups at net.bio.net).  Unfortunately it
is becoming a despicable practice on the Internet (by a few people out
to make a fast buck) to do automated mass postings to thousands of
newsgroups and mailing lists.  These attempts to grab free advertising
are refered to as "spams" in the usual, somewhat boneheaded, net
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spams originate on the USENET groups and then are passed on to the
mailing lists.  However, spammers also get lists of mailing addresses
and hit these too, so neither medium is immune.

What should you do personally if you get junk mail?
---------------------------------------------------
Just delete it and move on without reading it further.  Filing a
protest is becoming increasingly useless because spammers are often
disguising the addresses where the messages are sent from.  Unless you
really understand Internet mail systems, your attempt at protest by
sending replies to the message will often end up being sent to the
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What can BIOSCI/bionet do to protect its newsgroups?
----------------------------------------------------
The only solution currently available is to moderate the newsgroup.
If this newsgroup is already moderated, then you are in good shape.
Moderation protects the USENET distribution from about 95% of the
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time to review each message before it goes out.  We have set up
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This takes no more time than that needed to read the message and pass
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Most newsgroups currently have a discussion leader who is responsible
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addresses are listed in the BIOSCI Information Sheet which is
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hit with too many junk postings, please contact the discussion leader
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Please do not assume that by simply posting a complaint to the
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to rely on the discussion leaders of each newsgroup to report problems
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We will moderate any of our newsgroups if the discussion leader tells
us that the readership of the group wishes to do so and if a moderator
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entails only a few minutes of work each day.

Moderating a newsgroup will resolve probably 95% of the junk postings
on the USENET distribution.  Unfortunately there are easy ways for
determined spammers to override the moderation mechanism on USENET,
but we can protect our e-mail subscribers from unwanted postings if
the newsgroup is moderated.  You can also access our newsgroups over
the WWW at URL http://www.bio.net.  While this Web interface will not
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yet another way, besides using USENET news, to keep the junk out of
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3) Examples of subscribing and unsubscribing to the mailing lists.
------------------------------------------------------------------
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Gory details are in the BIOSCI Information sheets on the Web at
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METHODS-AND-REAGENTS list at both of our two BIOSCI sites:

Users in the Americas and Pacific Rim countries who use the BIOSCI
------------------------------------------------------------------
node at computer net.bio.net:
----------------------------

A) Determine the "listname" which is the <=8 character mail address
                                         ^^^^^^^^^^^^^
   for the group.  These can be found in the BIOSCI Info. Sheet.  For
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Users in Europe, Africa, and Central Asia who use the BIOSCI node at
--------------------------------------------------------------------
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-------------------------------------------------

To subscribe and unsubscribe to/from the BIOSCI lists, you need to
specify the full USENET newsgroup name with "bionet-news." prepended.
The USENET newsgroup names are listed in the BIOSCI Information sheet
on the Web at http://www.bio.net/.  For the METHODS-AND-REAGENTS list
the USENET newsgroup name is bionet.molbio.methds-reagnts, thus the
appropriate commands are

    sub bionet-news.bionet.molbio.methds-reagnts

    unsub bionet-news.bionet.molbio.methds-reagnts

These commands are included in a message addressed to mxt@dl.ac.uk,
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    unsub bionet-news

Please note that if the address in the list is different than the one
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4) The BIOSCI user address and research interest directory.
-----------------------------------------------------------
Please take this opportunity to add your name, address, and research
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not already done so.

You can fill out the address form directly through our Web page at URL
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The address database is reindexed nightly for WWW access (the URL is
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Please check your database entry from time-to-time to see if your
address information is still up-to-date.  Because of our limited
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From owner-biophysics@net.bio.net Mon Feb 16 22:00:00 1998
Path: biosci!daresbury!uninett.no!news.maxwell.syr.edu!newspeer.monmouth.com!news.monmouth.com!tr-ppp8.monmouth.com!user
From: NOSPAM-Glen@AvivInst.com (Glen Ramsay)
Newsgroups: bionet.biophysics
Subject: Re: Magnetic affect on growth
Date: Tue, 17 Feb 1998 11:31:32 -0500
Organization: Aviv Instruments
Lines: 19
Message-ID: <NOSPAM-Glen-1702981131320001@tr-ppp8.monmouth.com>
References: <34E72248.38C@virgin.net> <mmisha-1602981229110001@misha.mgh.harvard.edu>
NNTP-Posting-Host: tr-ppp8.monmouth.com
X-Newsreader: Yet Another NewsWatcher 2.1.8

In article <mmisha-1602981229110001@misha.mgh.harvard.edu>,
mmisha@nmr.mgh.harvard.edu (M. Papisov) wrote:

>         > I have a dying question and that is;
>         > "Will a magnetic field have an affect on Bacterial growth?"
>         > I would be very grateful if one would reply via e-mail to
>         > alan.loberto@virgin.net
> 

Check the bionet.journals.contents newsgroup.  Periodically they list the
table of contents for a journal on the effects of magnetic / eletronic
fields on life.  Sorry, but I can't remember the name of the journal.

Glen

-- 
   Glen Ramsay, Ph.D.
   Aviv Instruments
   Glen@(NoSpam)AvivInst.com

From owner-biophysics@net.bio.net Mon Feb 16 22:00:00 1998
Path: biosci!agate!logbridge.uoregon.edu!news-peer.gip.net!news-raspail.gip.net!news.gsl.net!gip.net!newscore.univie.ac.at!news.iif.hu!szia
From: szia@hanga.enzim.hu (Andras Szilagyi)
Newsgroups: bionet.biophysics
Subject: Re: Boltzmann's versus thermodynamic entropy
Date: 17 Feb 1998 13:50:46 GMT
Organization: IIF
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On 17 Feb 1998 08:39:09 -0000, Pentcho Valev <RUMYM@BGEARN.ACAD.BG> wrote:

>Andras, I do not see any contradiction between my statement and your
>explanation, so there is certainly nothing which I don't understand at
>that level. Still I find it awkward to accept that, as the system
>(rather, only D) expands spontaneously and never returns to the initial
>point, it moves from a MORE probable to a LESS probable state. Your
>explanation is formally correct but it contradicts my intuition.
>Unfortunately I am incompetent in statistical mechanics and cannot offer
>a more reasonable objection. Still my conclusion remains valid: The
>two entropies may coincide but ONLY IF SYSTEMS CAN SPONTANEOUSLY MOVE
>FROM A MORE PROBABLE TO A LESS PROBABLE STATE.

So it contradicts your intuition that the entropy of an open system can
spontaneously decrease? If yes, then there is something very wrong with
your intuition. Personal incredulity is not an argument, it only
demonstrates that you have not tried hard enough to understand things.

I think that actually it does not make much sense to speak about
spontaneous and non-spontaneous processes in an open system. If the
system is open (i.e. anything can be made with it from outside) then any
processes are spontaneous that are forced by the environment, regardless
of any probabilities.

Your example would be good if the system were an isolated system. But it
is not.

Andras


From owner-biophysics@net.bio.net Mon Feb 16 22:00:00 1998
Path: biosci!news.ohsu.edu!not-for-mail
From: Matt Jones <jonesmat@ohsu.edu>
Newsgroups: bionet.biophysics
Subject: Re: General question
Date: 17 Feb 1998 22:38:47 GMT
Organization: Vollum Institute
Lines: 26
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In article <34E49CE9.2781@henri.chem.uleth.ca> Marc Roussel,
roussel@henri.chem.uleth.ca writes:
> Diamonds are thermodynamically unstable
>relative to graphite at standard temperature and pressure which means
>that their free energy is higher than that of graphite.  Thus, every
>diamond that has ever been dug out of the ground is slowly converting to
>graphite.

Maybe another way to say this is in terms of an energy diagram for the
reaction: imagine a bell-shaped curve with the left "foot" higher than
the right "foot", so that there is a hill in between. The height of the
curve at each point represents the energy of the reaction (e.g., diamond
turning to graphite), so that diamond (on the left) has a higher energy
than graphite. Given an infinite time, all dimaonds will sooner or later
slide across the reaction towards graphite, so diamond is less
thermodynamically stable than graphite. However, before diamond can turn
to graphite, it has to surmount an energy barrier (the hill). The lower
the hill between the two states, the faster things can go over it, and
the faster the reaction will proceed. If the hill is very high, then
diamond will be kinetically stable, because only very rarely does an
individual diamond crystal attain enough energy (from heat in the ground,
or whatever) to climb over this energy barrier.

Helpful, or more confusing?

-Matt

From owner-biophysics@net.bio.net Mon Feb 16 22:00:00 1998
Path: biosci!agate!logbridge.uoregon.edu!newsfeed.direct.ca!news-peer.sprintlink.net!news.sprintlink.net!Sprint!worldnet.att.net!news.u.washington.edu!fujimoto
From: fujimoto@u.washington.edu (Bryant Fujimoto)
Newsgroups: bionet.biophysics
Subject: Re: Boltzmann's versus thermodynamic entropy
Date: 17 Feb 1998 21:32:43 GMT
Organization: University of Washington
Lines: 24
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Pentcho Valev <RUMYM@BGEARN.ACAD.BG> writes:

>Andras, I do not see any contradiction between my statement and your
>explanation, so there is certainly nothing which I don't understand at
>that level. Still I find it awkward to accept that, as the system
>(rather, only D) expands spontaneously and never returns to the initial
>point, it moves from a MORE probable to a LESS probable state. Your
>explanation is formally correct but it contradicts my intuition.

Your intuition is wrong.  You haven't even proved which way the
heat will flow.  How do you know heat will flow out of the chamber?
You haven't accounted for the heat necessary to maintain the 
temperature as you expand your system.

>Unfortunately I am incompetent in statistical mechanics and cannot offer
>a more reasonable objection. Still my conclusion remains valid: The
>two entropies may coincide but ONLY IF SYSTEMS CAN SPONTANEOUSLY MOVE
>FROM A MORE PROBABLE TO A LESS PROBABLE STATE.

If your conclusion is valid, then why is it contradicted by every
test ever made to compare statisical mechanical and thermodynamic
entropies?  

Bryant

From owner-biophysics@net.bio.net Mon Feb 16 22:00:00 1998
Path: biosci!UCONNVM.UCONN.EDU!RHODES
From: RHODES@UCONNVM.UCONN.EDU
Newsgroups: bionet.biophysics
Subject: Trying to cut housing cost @ KC
Date: 17 Feb 1998 04:03:42 -0800
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I know it's pretty close to the last minute, BUT...
my plans for the biophys meetings got a little fouled up.

I'm looking for someone to share a room at KC.  I have made
reservations in a place 3 blocks north of the center, but
will gladly cancel those if someone has space available.

So - -
* If you have space in your room and/or
* are interested in sharing to reduce your housing costs
* (or if you simply need a place)
* are male, nonsmoker

give me a call or drop me an email.

Thanks! - see you there!!

|-----------------------------O==O----------------------------|
| David G. Rhodes             O==O  Phone 860-486-5413        |
| School of Pharmacy; U-92    O==O  Fax   860-486-4998        |
| University of Connecticut   O==O                            |
| Storrs, CT  06269-2092      O==O  rhodes@uconnvm.uconn.edu  |
|_____________________________O==O____________________________|
I love deadlines - especially the "whoosh" sound as they go flying by.

From owner-biophysics@net.bio.net Tue Feb 17 22:00:00 1998
Path: biosci!CHEM.UFL.EDU!tan
From: tan@CHEM.UFL.EDU (Weihong Tan)
Newsgroups: bionet.biophysics
Subject: Postdoctoral positions at University of Florid
Date: 17 Feb 1998 19:44:27 -0800
Organization: BIOSCI International Newsgroups for Molecular Biology
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Distribution: world
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	Applications are invited for two postdoctoral positions at the
Department of Chemistry and the UF Brain Institute, University of Florida.
The successful applicant should have a strong background in ANY ONE of the
following areas: biophysics, optical microscopy and spectroscopy, scanning
probe microscopy, bioanalytical chemistry, or neuroscience. We are
carrying out exciting research work in the following areas: novel optical
microscopy for biomedical imaging and sensing; single biomolecule
detection and manipulation; biochemical sensors and in-vivo monitoring; a
novel new form of patch clamp technique and its application. We are also
studying important biomedical problems such as the molecular and
subcellular mechanisms of ischemic stroke, ion channel imaging and
manipulation, DNA hybridization in single living cells. These research
activities are funded by the National Science Foundation, the Office of
Naval Research, Department of Defense and The Arnold Beckman Foundation.
These two positions are expected to be as long as three years. The
successful applicant will be expected to show both individual initiative
and ability to work as a team member. At University of Florida we have
excellent working and living environment.  Interested applicants should
make an initial contact with Prof. Tan through e-mail, or send a CV with
two reference letters to the following address:

Prof. Weihong Tan
Department of Chemistry and The UF Brain Institute
University of Florida
Gainesville, FL 32611-7200
352-846-2410
E-mail: tan@chem.ufl.edu




From owner-biophysics@net.bio.net Tue Feb 17 22:00:00 1998
Path: biosci!daresbury!not-for-mail
From: Pentcho Valev <RUMYM@BGEARN.ACAD.BG>
Newsgroups: bionet.biophysics
Subject: Boltzmann vs. thermodynamic entropy
Date: 18 Feb 1998 14:17:58 -0000
Lines: 63
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Message-ID: <6ceqim$guo@mserv1.dl.ac.uk>
Original-To: biophys@dl.ac.uk


I wrote:
>Andras, I do not see any contradiction between my statement and your
>explanation, so there is certainly nothing which I don't understand at
>that level. Still I find it awkward to accept that, as the system
>(rather, only D) expands spontaneously and never returns to the initial
>point, it moves from a MORE probable to a LESS probable state. Your
>explanation is formally correct but it contradicts my intuition.

Bryant Fujimoto replied:>>>>>>>>>>>>>>>
Your intuition is wrong.  You haven't even proved which way the
heat will flow.  How do you know heat will flow out of the chamber?
You haven't accounted for the heat necessary to maintain the
temperature as you expand your system.<<<<<<<<<<<<<<

I explained this some time ago and still believe that it is obvious. The
system is analogous to a liquid-vapor system, the only difference being
that in this case the reaction is exothermic. As D (or the vapor in the
liquid-vapor system) expands isothermally and reversibly, the chemical
reaction releases exothermic heat dQexo and, in addition, the system does
work of expansion PdV. So

       dQabsorbed = PdV - dQexo                                 /1/

where P is the partial pressure of D (or the vapor) and dQexo is positive
in this case and negative for the liquid-vapor system.

If dQexo > PdV, we obtain

     dS = dQabs/T  < 0                                           /2/

i.e. the entropy of the system decreases. I don't think there is problem
with this.

Then I wrote:
>Unfortunately I am incompetent in statistical mechanics and cannot offer
>a more reasonable objection. Still my conclusion remains valid: The
>two entropies may coincide but ONLY IF SYSTEMS CAN SPONTANEOUSLY MOVE
>FROM A MORE PROBABLE TO A LESS PROBABLE STATE.

Bryant replied:>>>>>>>>>>>>>>>>>>
If your conclusion is valid, then why is it contradicted by every
test ever made to compare statisical mechanical and thermodynamic
entropies?<<<<<<<<<<<<<<<<<

Bryant, my conclusion is an "if.." statement and is not contradicted by
any test. However I have not proved, although my wrong intuition tells
me so, that the expanded state is MORE probable than the initial state.
So at the moment I am forced to accept Andras' interpretation of
probability in terms of entropy: the expanded state is LESS probable than
the initial state, but this is compensated for by events in the environment,
so the probability of the system + the environment increases in the
spontaneous process. If I find a reasonable argument, I will present it
for discussion.

By the way, why don't you describe an intersting test comparing Boltzmann's
and thermodynamic entropy? I know your answer - read the books| - and will
certainly do so, but meanwhile you, as you have already read them,  can
say something interesting - can't you? Otherwise I will have to do this
after reading the books, but this will take time.

Best regards,
Pentcho

From owner-biophysics@net.bio.net Tue Feb 17 22:00:00 1998
Path: biosci!agate!logbridge.uoregon.edu!news.maxwell.syr.edu!newscore.univie.ac.at!news.iif.hu!szia
From: szia@hanga.enzim.hu (Andras Szilagyi)
Newsgroups: bionet.biophysics
Subject: Re: Boltzmann vs. thermodynamic entropy
Date: 18 Feb 1998 15:04:20 GMT
Organization: IIF
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X-Newsreader: slrn (0.9.4.1 UNIX)

On 18 Feb 1998 14:17:58 -0000, Pentcho Valev <RUMYM@BGEARN.ACAD.BG> wrote:

>By the way, why don't you describe an intersting test comparing Boltzmann's
>and thermodynamic entropy? I know your answer - read the books| - and will
>certainly do so, but meanwhile you, as you have already read them,  can
>say something interesting - can't you? Otherwise I will have to do this
>after reading the books, but this will take time.

Just a suggestion. It was Boltzmann who first proved, using very deep
considerations, that the thermodynamic entropy and the thermodynamic
probability are always proportional with each other (and the
proportionality constant is the Boltzmann constant). Perhaps you should
read the original work of Boltzmann if you really want to get to the core
of these things. I haven't read them myself, but I would like too.

Andras


From owner-biophysics@net.bio.net Tue Feb 17 22:00:00 1998
Path: biosci!agate!howland.erols.net!cpk-news-hub1.bbnplanet.com!cpk-news-feed4.bbnplanet.com!cpk-news-feed1.bbnplanet.com!news.bbnplanet.com!nih.gov!helix.nih.gov!malini
From: Malini Viswanathan <malini@helix.nih.gov>
Newsgroups: bionet.biophysics
Subject: BIAcore
Date: Wed, 18 Feb 1998 17:40:12 -0500
Organization: National Institutes of Health
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I have a question regarding BIAcor - are there references about two
state kinetic models that have been analyzed or predicted using
the BIA. I've tried to look through some references, but have not come
across any for a two state kinetic model. 
	Sorry if this newsgroup is not the right one to post to, any
suggestions regarding that would also be welcome.

Thanks in advance
Malini


--------------------
Malini Viswanathan
Bldg 37, 2B10,NIH
Bethesda,MD 20892-4255


From owner-biophysics@net.bio.net Tue Feb 17 22:00:00 1998
Path: biosci!daresbury!uninett.no!news.maxwell.syr.edu!newsfeed.direct.ca!news.u.washington.edu!fujimoto
From: fujimoto@u.washington.edu (Bryant Fujimoto)
Newsgroups: bionet.biophysics
Subject: Re: Boltzmann vs. thermodynamic entropy
Date: 18 Feb 1998 21:40:00 GMT
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Pentcho Valev <RUMYM@BGEARN.ACAD.BG> writes:


>I wrote:
>>Andras, I do not see any contradiction between my statement and your
>>explanation, so there is certainly nothing which I don't understand at
>>that level. Still I find it awkward to accept that, as the system
>>(rather, only D) expands spontaneously and never returns to the initial
>>point, it moves from a MORE probable to a LESS probable state. Your
>>explanation is formally correct but it contradicts my intuition.

>Bryant Fujimoto replied:>>>>>>>>>>>>>>>
>Your intuition is wrong.  You haven't even proved which way the
>heat will flow.  How do you know heat will flow out of the chamber?
>You haven't accounted for the heat necessary to maintain the
>temperature as you expand your system.<<<<<<<<<<<<<<

>I explained this some time ago and still believe that it is obvious. The
>system is analogous to a liquid-vapor system, the only difference being
>that in this case the reaction is exothermic. As D (or the vapor in the
>liquid-vapor system) expands isothermally and reversibly, the chemical
>reaction releases exothermic heat dQexo and, in addition, the system does
>work of expansion PdV. So

>       dQabsorbed = PdV - dQexo                                 /1/

You seem to be assuming that the internal energy of the system is
constant for an isothermal expansion.  This is true for a ideal
gas which is not undergoing any reaction.  Not necessarily true
otherwise.

>where P is the partial pressure of D (or the vapor) and dQexo is positive
>in this case and negative for the liquid-vapor system.

>If dQexo > PdV, we obtain

>     dS = dQabs/T  < 0                                           /2/

>i.e. the entropy of the system decreases. I don't think there is problem
>with this.

>Then I wrote:
>>Unfortunately I am incompetent in statistical mechanics and cannot offer
>>a more reasonable objection. Still my conclusion remains valid: The
>>two entropies may coincide but ONLY IF SYSTEMS CAN SPONTANEOUSLY MOVE
>>FROM A MORE PROBABLE TO A LESS PROBABLE STATE.

>Bryant replied:>>>>>>>>>>>>>>>>>>
>If your conclusion is valid, then why is it contradicted by every
>test ever made to compare statisical mechanical and thermodynamic
>entropies?<<<<<<<<<<<<<<<<<

>Bryant, my conclusion is an "if.." statement and is not contradicted by
>any test. However I have not proved, although my wrong intuition tells
>me so, that the expanded state is MORE probable than the initial state.

This was supposed to a reversible process.  Why should the expanded
state always be expected to have a higher entropy than the initial state?
Do you know what thermodynamics means by reversible?   Perhaps one of
the sources of your misunderstandings is that you think that reversible
and spontaneous mean the same thing in thermodynamics.

>So at the moment I am forced to accept Andras' interpretation of
>probability in terms of entropy: the expanded state is LESS probable than
>the initial state, but this is compensated for by events in the environment,
>so the probability of the system + the environment increases in the
>spontaneous process. If I find a reasonable argument, I will present it
>for discussion.

>By the way, why don't you describe an intersting test comparing Boltzmann's
>and thermodynamic entropy? I know your answer - read the books| - and will
>certainly do so, but meanwhile you, as you have already read them,  can
>say something interesting - can't you? Otherwise I will have to do this
>after reading the books, but this will take time.

Pentcho
  I have already described it, several times.  I pointed out that it
is possible to calculate the entropy of a system using the results of
thermodynamics and it is possible to calculate the entropy using the
results of statistical mechanics.  So far, whenever it has been done
the results agree to within experimental error.  What more is necessary?

For example, McQuarrie and Simon calculate the entropy of N2 at 298.15K
and 1 atm in two different ways. 

From thermodynamics,

 S(T) = Int[0..Ttr] (Cp/T)dT  + (Delta H_tr)/T
      + Int[Ttr..Tm] (Cp/T)dT + (Delta H_fus)/T
      + Int[Tm..Tb] (Cp/T)dT + (Delta H_vap)/T
      + Int[Tb..T] (Cp/T)dT

where 
  Cp is the heat capacity at constant pressure (1 atm)
  Int[Ta..Tb] refers to an integral from Ta to Tb, 
  Ttr and (Delta H_tr) are the temperature of a solid phase transition
in N2 at 35.61K and the enthalpy change for that transition,
  Tm and (Delta H_fus) are the melting temperature and heat of fusion,
  Tb and (Delta H_vap) are the boiling temperature and heat of vaporization.

All of these quantities are experimentally measurable, and performing
the integrals yields 

   S(298.15K, 1atm) = 191.6 J/(mole K)   [Result of Thermodynamics]

From statistical mechanics,

 S = k_B ln(Q) + k_BT (partial ln(Q)/partial T)N,V

where k_B is Boltzmann's constant, Q is the cannoical partition function
(not to be confused with the reaction quotient which is also called Q),
and the last term is the partial derivative of ln(Q) with respect to T
at constant composition and volume.  Q can be calculated, it depends
on the mass of a nitrogen atom, the bond length of N2, and vibrational
force constant of N2, the energy and degeneracy of the ground electronic
state.  These are all measureable by different experiments than that
used above. The result is

   S(298.15K, 1atm) = 191.5 J/(mole K).   [Result of Stat. Mech.]

Regards,
Bryant 
 

From owner-biophysics@net.bio.net Tue Feb 17 22:00:00 1998
Path: biosci!agate!logbridge.uoregon.edu!news-peer.gip.net!news.gsl.net!gip.net!news-peer.sprintlink.net!news.sprintlink.net!Sprint!newsfeed.nacamar.de!univ-lyon1.fr!citi2.fr!bomsel.cochin.inserm.fr!user
From: bomsel@lovelace.infobiogen.fr (Morgane BOMSEL)
Newsgroups: bionet.biophysics
Subject: new web site on cell membranes
Date: 18 Feb 1998 16:36:40 GMT
Organization: CITI2 - Universite Rene Descartes, Paris
Lines: 6
Message-ID: <bomsel-1802981747530001@bomsel.cochin.inserm.fr>
NNTP-Posting-Host: bomsel.cochin.inserm.fr

a new site on cell membranes has been opened, for information and
discussion, on the web at
the following address: http://www.univ-paris5.fr/ELM
you can also send comments at alfsen@bisance.citi2.fr
we are waiting for your prosa
 ELM , sort of ULM

From owner-biophysics@net.bio.net Tue Feb 17 22:00:00 1998
From: mmisha@nmr.mgh.harvard.edu (M. Papisov)
Newsgroups: bionet.biophysics
Subject: Re: Magnetic affect on growth
Date: Wed, 18 Feb 1998 18:24:14 -0500
Organization: MGH & HMS
Lines: 30
Message-ID: <mmisha-1802981824140001@misha.mgh.harvard.edu>
References: <34E72248.38C@virgin.net> <mmisha-1602981229110001@misha.mgh.harvard.edu> <NOSPAM-Glen-1702981131320001@tr-ppp8.monmouth.com>
NNTP-Posting-Host: misha.mgh.harvard.edu
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In article <NOSPAM-Glen-1702981131320001@tr-ppp8.monmouth.com>,
NOSPAM-Glen@AvivInst.com (Glen Ramsay) wrote:

        > In article <mmisha-1602981229110001@misha.mgh.harvard.edu>,
        > mmisha@nmr.mgh.harvard.edu (M. Papisov) wrote:
        > 
        > >         > I have a dying question and that is;
        > >         > "Will a magnetic field have an affect on Bacterial
growth?"
        > >         > I would be very grateful if one would reply via e-mail to
        > >         > alan.loberto@virgin.net
        > > 
        > 
        > Check the bionet.journals.contents newsgroup.  Periodically they
list the
        > table of contents for a journal on the effects of magnetic / eletronic
        > fields on life.  Sorry, but I can't remember the name of the journal.
        > 
        > Glen

Glen, it was not me who had a dying question. Please make quotations correctly.

MP

______________He who rides on a tiger never dismounts________________

Please delete the very first letter in my email address to reply. 

Nobody at all, including my past, current and future employers, 
is responsible for whatever is written above. 

From owner-biophysics@net.bio.net Tue Feb 17 22:00:00 1998
Path: biosci!daresbury!not-for-mail
From: Pentcho Valev <RUMYM@BGEARN.ACAD.BG>
Newsgroups: bionet.biophysics
Subject: Boltzmann vs. thermodynamic entropy
Date: 18 Feb 1998 15:35:10 -0000
Lines: 63
Sender: lpddist@mserv1.dl.ac.uk
Distribution: bionet
Message-ID: <6cev3e$lfr@mserv1.dl.ac.uk>
Original-To: biophys@dl.ac.uk


I wrote:
>Andras, I do not see any contradiction between my statement and your
>explanation, so there is certainly nothing which I don't understand at
>that level. Still I find it awkward to accept that, as the system
>(rather, only D) expands spontaneously and never returns to the initial
>point, it moves from a MORE probable to a LESS probable state. Your
>explanation is formally correct but it contradicts my intuition.

Bryant Fujimoto replied:>>>>>>>>>>>>>>>
Your intuition is wrong.  You haven't even proved which way the
heat will flow.  How do you know heat will flow out of the chamber?
You haven't accounted for the heat necessary to maintain the
temperature as you expand your system.<<<<<<<<<<<<<<

I explained this some time ago and still believe that it is obvious. The
system is analogous to a liquid-vapor system, the only difference being
that in this case the reaction is exothermic. As D (or the vapor in the
liquid-vapor system) expands isothermally and reversibly, the chemical
reaction releases exothermic heat dQexo and, in addition, the system does
work of expansion PdV. So

       dQabsorbed = PdV - dQexo                                 /1/

where P is the partial pressure of D (or the vapor) and dQexo is positive
in this case and negative for the liquid-vapor system.

If dQexo > PdV, we obtain

     dS = dQabs/T  < 0                                           /2/

i.e. the entropy of the system decreases. I don't think there is problem
with this.

Then I wrote:
>Unfortunately I am incompetent in statistical mechanics and cannot offer
>a more reasonable objection. Still my conclusion remains valid: The
>two entropies may coincide but ONLY IF SYSTEMS CAN SPONTANEOUSLY MOVE
>FROM A MORE PROBABLE TO A LESS PROBABLE STATE.

Bryant replied:>>>>>>>>>>>>>>>>>>
If your conclusion is valid, then why is it contradicted by every
test ever made to compare statisical mechanical and thermodynamic
entropies?<<<<<<<<<<<<<<<<<

Bryant, my conclusion is an "if.." statement and is not contradicted by
any test. However I have not proved, although my wrong intuition tells
me so, that the expanded state is MORE probable than the initial state.
So at the moment I am forced to accept Andras' interpretation of
probability in terms of entropy: the expanded state is LESS probable than
the initial state, but this is compensated for by events in the environment,
so the probability of the system + the environment increases in the
spontaneous process. If I find a reasonable argument, I will present it
for discussion.

By the way, why don't you describe an intersting test comparing Boltzmann's
and thermodynamic entropy? I know your answer - read the books| - and will
certainly do so, but meanwhile you, as you have already read them,  can
say something interesting - can't you? Otherwise I will have to do this
after reading the books, but this will take time.

Best regards,
Pentcho

From owner-biophysics@net.bio.net Wed Feb 18 22:00:00 1998
Path: biosci!UCONNVM.UCONN.EDU!RHODES
From: RHODES@UCONNVM.UCONN.EDU
Newsgroups: bionet.biophysics
Subject: Biophysics meeting housing
Date: 19 Feb 1998 04:04:35 -0800
Organization: BIOSCI International Newsgroups for Molecular Biology
Lines: 16
Sender: daemon@net.bio.net
Distribution: world
Message-ID: <980219.070331.EST.RHODES@UConnVM.UConn.Edu>
NNTP-Posting-Host: net.bio.net

I posted a note here a couple of days ago but am still looking ....

If you have space in your room or would like to share mine, please
get in touch with me soon so we can save some $$$$.  I have a room
about 3 blocks from the center, but would like to avoid paying for
the whole thing.

Once again, male - nonsmoking preferred.   Thanks 10^6 - see you in KC!

|-----------------------------O==O----------------------------|
| David G. Rhodes             O==O  Phone 860-486-5413        |
| School of Pharmacy; U-92    O==O  Fax   860-486-4998        |
| University of Connecticut   O==O                            |
| Storrs, CT  06269-2092      O==O  rhodes@uconnvm.uconn.edu  |
|_____________________________O==O____________________________|
I love deadlines - especially the "whoosh" sound as they go flying by.

From owner-biophysics@net.bio.net Thu Feb 19 22:00:00 1998
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From: prismx@scienceweek.com (Claire Haller)
Newsgroups: bionet.neuroscience,bionet.biophysics,bionet.cellbiol,bionet.general,sci.misc
Subject: SCIENCE-WEEK: Headlines (20 Feb 98)
Date: Thu, 19 Feb 1998 21:28:56 GMT
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5. On the Bose-Einstein Condensate
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From owner-biophysics@net.bio.net Fri Feb 20 22:00:00 1998
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From: smd <smd3804@aros.net>
Newsgroups: bionet.biophysics
Subject: ***IT REALLY WORKS***YOU MUST READ THIS!!
Date: Sat, 07 Feb 1998 15:24:51 -0700
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A must for you to read::
A little while back, I was browsing these newsgroups,
just like you are now, and came across an article similar to
this that that said "YOU COULD MAKE THOUSANDS OF DOLLARS WITHIN
WEEKS WITH ONLY AN INITIAL INVESTMENT OF $6.00!!!"
So I thought YEAH RIGHT, SCAM, just like most of you are
thinking now!! But I was curious, so I kept reading. Anyway,
it said that you send $1.00 to each of the six names and
addresses stated in the article.
You then place your own name and address at the bottom of the
list at #6, and post the article in at least 200 newsgroups
(there are thousands) no catch, that was it.
The main difference with this system and others is that you
have a mailing list of 6 instead of 5...this means that your
average gain will be app. 15x higher!!!

So after thinking it over, and talking to a few people first,
I thought about trying it. I figured what have I got to lose
except 6 stamps and $6.00 right?
Unlike most I was still VERY skeptical and a little worried
about the legal aspects of it all. So I checked it out with the
U.S. post office (1-800-725-2161) and they confirmed that it is
indeed legal!! THEN I INVESTED MY $6.00......
WELL, GUESS WHAT...within 7 days, I started getting money in
the mail!!!
I was shocked! I still figured it would end soon, and did not
give it a second thought. But the money just kept coming in.
In my first week I had made about $20.00 to $30.00 dollars.
By the end of the second week I had made well over $1000.00!!
In the third week I had over $10,000 and its still coming in
rapidly...
It was well worth the $6.00 and the six stamps, I spent more
than that on one go with the lottery!!!
Let me tell you how it worls and, more importantly, why it works
...also, make sure you print a copy of this article NOW(and save
it to your hard drive for use later), so you can get the
information of it as and when you need it.
The process is very simple and consists of three easy steps:

STEP 1: get 6 separate pieces of paper and write the following
on each piece of paper "PLEASE PUT ME ON YOUR MAILING LIST."
Now get 6 U.S. $1.00 bills and place them inside each of the 6
pieces of paper so the bill cannot be seen through the envelope
"this helps against thievery."
Next, place one paper inside each of the six envelopes and seal
them...You should now have 6 sealed envelopes, each with a piece
of paper stating the above phrase, your name and address, and
the $1.00 bill.

WHAT YOU ARE DOING IS CREATING A SERVICE THAT IS ABSOLUTELY
LEGAL.
NOW mail the six envelopes to the addresses below:



#1 G. GARRISON
 3013 MONICA DR WEST
 COLORADO SPRINGS, CO 80916
 U.S.A.

#2 R. NICKERSON
 5700 BLACK LAKE BLVD.
 OLYMPIA, WA 98512
 U.S.A.

#3 Y. WONG
 121 SEAMEN AVE 2D
 NEW YORK, NY 10034
 U.S.A.

#4 R.A. DORAN
 42 FALCON ROAD
 MEIR PARK, STOKE ON 