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Subject: Re: Time and its existance -- From: tdp@ix.netcom.com(Tom Potter)
Subject: Re: Physics GRE -- From: jac@ibms46.scri.fsu.edu (Jim Carr)
Subject: Re: Tampere Replication -- From: jac@ibms46.scri.fsu.edu (Jim Carr)
Subject: particle temperatures -- From: "Chris Birch"
Subject: Re: Please Solve an Argument for me... -- From: mmcirvin@world.std.com (Matt McIrvin)
Subject: free electron gas -- From: Tevfik Uret
Subject: Re: Temperature measurements and blackbody radioation : limit 4000 K ? -- From: rjg@d31rz0.Stanford.EDU (Richard J. Green)
Subject: Re: Is there any theory on mass-transportation? Like the transporters on Star Trek. -- From: Doug Craigen
Subject: Re: matter at relatavistic speeds. -- From: Doug Craigen
Subject: Re: Question on Fractals Dimension and Entropy -- From: Big Ears
Subject: Re: Creation VS Evolution -- From: singtech@teleport.com (Charles Cagle)
Subject: Re: Creation VS Evolution -- From: singtech@teleport.com (Charles Cagle)
Subject: This Week's Finds in Mathematical Physics (Week 96) -- From: baez@math.ucr.edu (John Baez)
Subject: Re: NASA lies, again. -- From: singtech@teleport.com (Charles Cagle)
Subject: Re: But which way does it really flow? -- From: Richard Mentock
Subject: Re: Freezing Water -- From: Richard Mentock
Subject: Code HEXTIME for the numerical solution of the Space-Time multigroup -- From: dmitri@cdc.net (Dmitri Alperovitch)
Subject: Re: NASA lies, again. -- From: singtech@teleport.com (Charles Cagle)

Articles

Subject: Re: Time and its existance
From: tdp@ix.netcom.com(Tom Potter)
Date: 17 Dec 1996 18:01:14 GMT
One body's mass is another body's media ( Time and space ).
This can be expressed as:
   mass(A) * G = distance(B)^3
                 --------------
                 time(common)^2
   mass(B) * G = distance(A)^3
                 --------------
                 time(common)^2
Where:
G is the universal gravitational constant,
which does no more than make both sides of
the equation balance. If "G" was set equal to
one, then the units of mass would follow
after the units of time and distance were defined.
Time(common) is the common period ( divided by 2 pi )
shared by interacting bodies. Time is what two interacting
bodies share, and what is unique to each body is their
distance from the common center they share.
Distance(A) and distance(B) are the distances
from each body to the system center of mass.
Classical physics treats distance as the distance
between two bodies, but this introduces an 
assymetry and an error which must be corrected
by a "reduced mass" adjustment.
-------------
The distance between two independent intereacting 
bodies, or between a body and the center of mass
it shares with another body, can be expressed as:
      distance = interaction time * C
Where "C" is the universal distance per interaction time
constant, better known as "the speed of light".
-----------
We can then restate the equations that
express the relationships between two bodies as:
   mass(A) * G = ( interaction time(B) * C)^3 
                 -------------------------
                 time(common)^2
   mass(B) * G = ( interaction time(A) * C)^3
                 ----------------------------
                 time(common)^2
-------------
If we divide both side of the equation by C^3
we get:
   mass(A) * G = interaction time(B)^3 
   -----------   -------------------------
       C^3       time(common)^2
   mass(B) * G = interaction time(A)^3 
   -----------   -------------------------
       C^3       time(common)^2
Now, I assert that G / C^3 is nothing more
than a universal time per mass constant,
and that time can be expressed most simply
in terms of a time, and that this time
is a simplier ( and less precise ) expression
of the media that it represents.
In other words, we perceive objects, which
possess the property of mass ( Basically
a composite time property ), as varying in
media composed of time and space ( basically
an interaction time expressed as space to
differentiate it from the common time shared
by interacting bodies ( period time )).
Now, the mass of a body is a simplified, 
composite expression of the media of
the body that it is interacting with.
The bottom line is, that media is a
more basis, and more complete definition
of mass, and the most fundamental way to
define both mass and media, is in terms
of the interaction time between a body
and the center it shares with another "body",
and the common time it share with the other body.
The universe is a composite of "standing waves",
and time is the ratio of these waves. 
All else, including mass, objects and media, follows from time.
If anyone is interested in a more complete
explanation of this, visit my Web site.
Tom Potter      http://pobox.com/~tdp
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Subject: Re: Physics GRE
From: jac@ibms46.scri.fsu.edu (Jim Carr)
Date: 9 Dec 1996 02:56:57 GMT
jjtom4@imap2.asu.edu writes:
>
>       Advice?
 The best preparation is teaching recitations as an undergrad.  The 
 highest score they had seen at Michigan State came from such a case. 
 That person quit ABD, however.  It is no guarantee of success. 
 Get a good nights sleep. 
 Don't worry about your score while writing the exam. 
>	What's a "good" score?  
 One good enough to get into the place where you want to go.  Anything 
 more is irrelevant.  What that level is depends greatly from place to 
 place as well as on other factors, like letters, undergrad research 
 involvement, grades, and the reputation of the school that gave you 
 those grades.  Your teachers at ASU can tell you what they look for, 
 and there are publications that list averages and minimum scores for 
 different places that are probably available in your department. 
-- 
 James A. Carr        |  "The half of knowledge is knowing
    http://www.scri.fsu.edu/~jac/       |  where to find knowledge" - Anon. 
 Supercomputer Computations Res. Inst.  |  Motto over the entrance to Dodd 
 Florida State, Tallahassee FL 32306    |  Hall, former library at FSCW. 
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Subject: Re: Tampere Replication
From: jac@ibms46.scri.fsu.edu (Jim Carr)
Date: 9 Dec 1996 03:08:52 GMT
Alan_Douglas@mindlink.bc.ca (Alan Douglas) writes:
>
>But surely others should still try to repeat the experiment, if for no
>other reason than to refute it.  
 As I mentioned in another article in this thread, there are at least 
 two conditions that must be met before someone tries to repeat an 
 experiment: they have to know about it (when did you read the article 
 in Physica C?) and they have to have the expertise and interest to 
 do the experiment (the UAH group that cites the paper are theorists).  
 Further, they have to believe it is worth their time and effort and 
 budget to mount the experiment.  Given the history of such claims 
 in the past, groups that have the relevant expertise might have 
 chosen to bide their time. 
>Or is the scientific method only to be applied when convenient? 
 Bogus results sometimes go away on their own, either fading away 
 or as an erratum.  This is very convenient.  We have lots of time 
 and there are many people doing physics who might get around to 
 it if they thought it was worth the effort. 
-- 
 James A. Carr        |  "The half of knowledge is knowing
    http://www.scri.fsu.edu/~jac/       |  where to find knowledge" - Anon. 
 Supercomputer Computations Res. Inst.  |  Motto over the entrance to Dodd 
 Florida State, Tallahassee FL 32306    |  Hall, former library at FSCW. 
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Subject: particle temperatures
From: "Chris Birch"
Date: Tue, 17 Dec 1996 18:14:41 GMT
I need to calculate the approximate temperatures of particles at ground
level after being released from a stack at high temperature. I am assuming
a worst case scenario. The (metallic) particles are released from an 18m
stack at 1000C and are very small (<10um).  If I assume that the particles
fall straight to the ground and disregard things like the effects of wind
and solar irradiation how hot will they be at ground level.
Any help with the above would be appreciated.
Thanks in advance
Chris Birch
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Subject: Re: Please Solve an Argument for me...
From: mmcirvin@world.std.com (Matt McIrvin)
Date: Tue, 17 Dec 1996 18:59:33 GMT
In article , Anthony James Bentley
 wrote:
> ps Did someone *really* try to redefine pi as 3 ? How precious!
This is such a frequently asked question that I think it's in the
top-level FAQ for all of Usenet! (The answer is: Not quite-- the
story is much more complicated than that. See the FAQ for details;
I think they still post it to news.answers from time to time.)
-- 
Matt McIrvin   
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Subject: free electron gas
From: Tevfik Uret
Date: Tue, 17 Dec 1996 18:24:13 +0200
hello, i am looking for an information of specialities of free electron
gas. Where can i found info about this on the net ?
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Subject: Re: Temperature measurements and blackbody radioation : limit 4000 K ?
From: rjg@d31rz0.Stanford.EDU (Richard J. Green)
Date: 17 Dec 1996 12:12:22 -0800
In article <32AD339A.7A9F@nl.compuware.com>,
C++ Freak   wrote:
>Any ideas on this ?
One way to measure the temperatures in flames and plasmas is through
spectroscopy. Techniques such as Cavity Ring-Down Spectroscopy (CRDS) or
Degenerate Four-Wave Mixing (DFWM) can be used to measure the rotational
temperatures of free-radicals (such as CH, OH and CH3) in a position 
sensitive manner.
A problem can be encountered: a person who has a thermometer knows what
the temperature is; a person who has two thermometers isn't sure.
Regards,
Rich Green
-- 
------------------------------------------------------------------
Richard J. Green                           Dept. of Chemistry
rjg@lyman.Stanford.EDU                     Stanford University     
http://www-leland.Stanford.EDU/~redcloud   Stanford, CA 94305-5080
"Remember the days of yore,
"Learn the lessons of the generation that came before you."
       -Deuteronomy 32:7
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Subject: Re: Is there any theory on mass-transportation? Like the transporters on Star Trek.
From: Doug Craigen
Date: Tue, 17 Dec 1996 10:20:26 -0600
MHL wrote:
> 
> It's completely nonsense. That's why I never watch Star Trek. :)
Actually that's one of the things I enjoy about Star Trek.  I think it 
would be great fun to be one of the writers who gets to make up a 
technical term soup wherever its needed in a script. 
|++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++|
| Doug Craigen                                                 |
|                                                              |
| If you think Physics is no laughing matter, think again .... |
|    http://cyberspc.mb.ca/~dcc/phys/humor.html                |
|++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++|
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Subject: Re: matter at relatavistic speeds.
From: Doug Craigen
Date: Tue, 17 Dec 1996 10:35:39 -0600
Stephen C. Woodworth wrote:
> 
> My question is probably stupid, but here goes!
> 
> When matter approaches the speed of light, it's mass increases towards
> infinite( so I've heard).
> since mass is equal to density times volume, the only way I see for the
> mass to increase is for mass to be added. If my understanding is not
> flawed, then my question is At what level is the mass added?
> 
> Is it at the quark and gluon level, making the particles more complex, or
> forming new particles?
> 
> Is it at the atomic level, simply adding more atoms?
> 
> I appreciate any answers or corrections!
> thanks for your time!
"Relativistic mass" is not the addition of any new particles, but rather an 
increase given to each individual particle.  What exactly is meant by 
"relativistic mass" is something else...
Another effect that you may have cited tending to lead to infinite densities is 
the length contraction, which similarly is not a subtraction of particles.
|++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++|
| Doug Craigen                                                 |
|                                                              |
| If you think Physics is no laughing matter, think again .... |
|    http://cyberspc.mb.ca/~dcc/phys/humor.html                |
|++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++|
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Subject: Re: Question on Fractals Dimension and Entropy
From: Big Ears
Date: Wed, 18 Dec 1996 04:32:25 +0800
crs wrote:
> That having been said, there is more than one way to define the fractal
> dimension.  Among these are:  
>(1) The so-called "Hausdorff dimension,"
> which depends only on the structure of the divided space.  This is the
> most usually encountered definition.  The most frequently cited examples
> used to illustrate this definition are the Cantor set, the Sierpinski
> gasket and the Koch snowflake.  
>(2) The correlation dimension, which is
> defined in terms of the scaling of the change in the number of pairwise
> correlations between particles in a dynamical system as the interaction
> length is increased.  In this case, the dimension is an exponent.  
>(3)The Lyapunov dimension, usually illustrated in terms of a baker's
> transformation in which dough is stretched and folded many times (The
> definition would take a fair amount of space to explain.).  
>(4) The information dimension, which is concerned with the change in the
> quantity of information as the system is subdivided into smaller and
> smaller cells.  This definition arises in terms of the limit as the size
> of each sample cell goes to zero - so
> d(I) = lim (e -> 0) I(e)/log(1/e)
> where e is the size of the cell and I is the quantity of information.
> Information is defined as you have defined entropy.
About the definition of these dimensions, I would like to learn if they
are consistency and how is the relation between them qualitatively! Why
there are so many definition? It really confused me. But the fractals
are concerning the H-dimension. Is it also related to other dimensions
in other ways as well?
Besides, I read some materials the correlation integral. Is it the same
stuff as the correlation dimension?
Also for the Lyapunov D, is it related to Lyapunov exp. ?
Fong
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Subject: Re: Creation VS Evolution
From: singtech@teleport.com (Charles Cagle)
Date: Tue, 17 Dec 1996 13:02:54 -0800
In article <32AE0D63.BE8@pilot.infi.net>, Jerry  wrote:

>   I AM is merely a property of space and time. The living die and the 
>memory of the living exists in space and time. This memory becomes life
>anew from a collective sense. Thus the Prophets of God dealt with a
>scientific property of space and time and not the creator of space and
>time.
>  The God of the Universe is a higher level. This level of God is concerned
>with MAN and the continuity of the creation all over the Universe. It could
>care less what the little individual thinks. Each of us is only one little
>part of the creation over one little part of time.
>Jerry (Jewish Prophet of Truth)
Jerry, you are a false prophet.  You represent the intellectual sterility
of the Jewish faith that I am faced with each time I enter a synagogue. 
You wonder why your God has abandoned you? (Actually, you don't wonder
about much since you think you are intellectually gifted beyond the simple
minded masses).  He has abandoned you because you have abandoned Him.
-- 
C. Cagle
SingTech
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Subject: Re: Creation VS Evolution
From: singtech@teleport.com (Charles Cagle)
Date: Tue, 17 Dec 1996 13:06:31 -0800
In article <32B0BF50.143D@pilot.infi.net>, Jerry  wrote:

 >That God "I AM" is an evolved entity.
>Jerry (Jewish Prophet of a higher God)
You are merely a false prophet with his head up his ass.
-- 
C. Cagle
SingTech
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Subject: This Week's Finds in Mathematical Physics (Week 96)
From: baez@math.ucr.edu (John Baez)
Date: 16 Dec 1996 16:17:30 -0800
This Week's Finds in Mathematical Physics - Week 96
John Baez
Lots of cool papers have been appearing which I've been neglecting
in my attempts to write expository stuff about string theory, lattices,
category theory, and all that.  It's time to start catching up!
Let me start with the following book:
1) J. Scott Carter, Daniel E. Flath and Masahico Saito,
"The Classical and Quantum 6j-Symbols", Princeton University
Press, Princeton, 1995.  ISBN 0-691-02730-7.
Ever since Jones discovered the Jones polynomial invariant of knots,
an amazing story has been unfolding about the relation between algebra
and 3-dimensional topology.  Some key players in this story are the 
"quantum groups": certain noncommutative algebras analogous to the 
commutative algebras of functions on groups.   In fact, not merely
are they analogous, they depend on a parameter, usually called
Planck's constant or hbar, and in the classical limit where hbar -> 0
they actually reduce to algebras of functions on familiar groups.  The 
simplest case is "quantum SU(2)", which reduces in the classical
limit to the group SU(2) of 2x2 unitary matrices with determinant 1.
Ironically, it's good old "classical SU(2)" that governs the quantum 
mechanical theory of angular momentum.   Quantum SU(2) was first 
discovered by people working on physics in 2-dimensional spacetime,
where when you quantize certain systems you also need to quantize their
group of symmetries!  
Nowadays, mathematicians find it simpler to work with the closely 
related "quantum SL(2)", a quantization of the the group SL(2) 
of all 2x2 complex matrices with determinant 1.  The above book is 
largely about quantum SL(2) and its applications to topology.
All quantum groups give rise to invariants of knots, links, and 
tangles.  They also give rise to 3-dimensional topological quantum 
field theories of "Turaev-Viro type".   This is a kind of quantum field
theory you can define on a 3-dimensional spacetime that you've triangulated,
i.e., chopped up into tetrahedra.  One of the main things you want to 
compute in a quantum field theory is the "partition function", and we say
the Turaev-Viro theories are "topological" because you get the same answer
for the partition function no matter how you triangulate the 3-dimensional
manifold corresponding to your spacetime: the partition function only 
depends on the topology of the manifold.  The SU(2) Turaev-Viro theory,
the first one to be discovered, is also one of the most interesting because,
modulo a few subtle points, this theory is just quantum gravity in 
3 dimensions (see "week16").  The basic idea, though, is that you compute 
the partition function by summing over all ways of labelling the edges of 
your tetrahedra by "spins" j = 0, 1/2, 1, 3/2, etc..  Ponzano and Regge 
had tried to set up 3-dimensional quantum gravity this way previously, 
but there were problems getting the sum to converge.  The neat thing about 
the quantum group is that you only sum over spins less than some fixed spin 
depending on the value of hbar.  Since the sums are finite, they automatically 
converge.  
It turns out that in these Turaev-Viro theories you are not actually
taking advantage of all the structure of the quantum group.  Using the
extra structure, you can also use quantum groups to define certain 
*4-dimensional* topological quantum field theories, those of 
"Crane-Yetter-Broda" type.  Here you triangulate a 4-dimensional manifold 
and, in the SU(2) case, you label both the 2d faces the 3d tetrahedra with 
spins.  Actually, lots of people think the Crane-Yetter-Broda theories are 
boring, because they look sort of boring if you only examine their 
implications for 4-dimensional topology.   However, they become interesting 
when you realize that, like all topological quantum field theories defined 
using triangulations, they are "extended topological quantum field theories".  
Roughly speaking this means that they have implications for all
dimensions below the dimension they live in.  
In particular, the Crane-Yetter-Broda theories spawn 3-dimensional 
topological quantum field theories of "Chern-Simons-Reshetikhin-Turaev" 
type, and most people agree that *these* are interesting.  I like to 
emphasize, however, that a deep understanding of these 3-dimensional
progeny requires an understanding of their seemingly innocuous 4-dimensional
ancestors.  Also, there are a lot of interesting relationships between
the SU(2) Crane-Yetter-Broda model and quantum gravity in 4 dimensions, which
we are just beginning to understand.  See "week56" for a bit about this.
If you haven't yet joined the fun, Carter, Saito, and Flath's book is a 
great place to start learning about the marvelous interplay between 
algebra, topology, and physics in 3 and 4 dimensions.  Needless to say, 
it doesn't cover all the ground I've sketched above.  Instead, it focuses 
on a rather specific and concrete aspect: the 6j symbols.  This should
make it especially handy for beginners who aren't familiar with category
theory, path integrals, and all that jazz.  
What are the 6j symbols, anyway?  Here I need to get a wee bit more technical.
The "classical" 6j symbols are important in the representation theory of 
plain old classical SU(2), while the "quantum" ones are analogous gadgets 
applicable to quantum SU(2).  In either case the idea is the same.  SU(2), 
classical or quantum, has different representations corresponding to different 
spins j = 0, 1/2, 1, 3/2, etc..  (If you don't know what I mean by this, try 
"week5".)  If we take three representations j1, j2, and j3, we can tensor 
them either like this:
(j1 tensor j2) tensor j3
or like this
j1 tensor (j2 tensor j3)
The tensor product is associative, but that doesn't mean that the
above two representations are *equal*.  They are only *isomorphic*.
This *isomorphism* can be thought of as just a big fat matrix, and
the entries in this matrix are a bunch of numbers, the 6j symbols.  
Turaev and Viro used the quantum 6j symbols to define the original 
Turaev-Viro model.   It goes like this: first you chop your 3-dimensional
manifold up into tetrahedra, and then you consider all possible ways
of labelling the edges with spins.  Each tetrahedron gets labelled with
6 spins since it has 6 edges, and from these spins we can compute a 
number: the 6j symbol.  Then we multiply all these together, one for each 
tetrahedron, and finally we sum over labellings to get the partition function.
Marvelously, the identities satisfied by the 6j symbols are precisely what's 
needed to make the result independent of the triangulation!  See "week38" for
an explanation of this seeming miracle: it's actually no miracle at all.
2) E. Guadagnini, L. Pilo, Three-manifold invariants and their relation 
with the fundamental group, 22 pages in LaTeX available as hep-th/9612090.
Fans of topological field theory may like this one, though I must
admit I haven't gotten around to doing more than reading the abstract
yet.  In this paper the authors give evidence for the conjecture
that among 3-manifolds M for which the Chern-Simons invariant CS(M) is
nonzero, the absolute value |CS(M)| only depends on the fundamental
group of M.  Chern-Simons theory depends on a choice of group; they 
prove the conjecture for certain manifolds ("lens spaces") when
the group is SU(2), and give numerical evidence when the gauge group
is SU(3).  
What's interesting about this to me is that |CS(M)|^2 is just the
Turaev-Viro theory partition function, so this conjecture is saying
that the Turaev-Viro theories discussed above have a tendency to notice
only the fundamental group. 
3) Michael Reisenberger and Carlo Rovelli, "Sum over surfaces" form
of loop quantum gravity, preprint available as gr-qc/9612035.
This wonderful paper should really push forwards our understanding
of the loop representation of quantum gravity.  I talked a little
bit about the basic idea in "week86".  In the loop representation,
a state of quantum gravity at a given moment is represented by a bunch
of knotted loops or "spin networks" in space.  What's the spacetime
picture?  Well, if you have a surface in spacetime and look at it
at one moment of time, it typically looks like a bunch of loops... so
maybe the spacetime picture of quantum gravity is that spacetime is
packed with 2-dimensional surfaces, all tangled up.  Interestingly,
this is also very reminiscent of the picture of quantum gravity in 
string theory! 
I've been working on this sort of idea ever since I wrote a paper
suggesting that the loop representation and string theory might be
two faces of the same ideas (see "week18").  Since then, most of the 
time I've been trying to understand how these ideas relate to the 
Crane-Yetter-Broda theories, and trying to set up the necessary *algebra* 
(n-category theory) to deal nicely with surfaces in 4-dimensional spacetime.
But there are many other angles from which one can attack this problem,
and one of the best is to start directly from Einstein's equations
for general relativity, try to quantize them using the path-integral
approach, and see how the path integral can be written as a sum over
surfaces.  Reisenberger has already begun work on this in the context of
"simplicial quantum gravity" - where you chop spacetime up into 
the 4-dimensional analog of tetrahedra.   But during the Vienna workshop
on canonical quantum gravity this summer, we talked about a different,
still more direct approach (see "week89").  The idea is to copy standard
quantum field theory, write the propagator describing time evolution
as a time-ordered exponential, and interpret the terms in the resulting
sum as surfaces in spacetime.  It's all very analogous to traditional
Feynman diagrams, where you write the propagator as a sum over diagrams,
but now the "Feynman diagrams" are 2-dimensional surfaces.   (Again, this
is reminiscent of string theory - but with many important differences.)
There is much more to say, but I think I'll leave it at that.... 
Over in the world of n-categories there is also some very interesting 
stuff happening, which I will discuss more next week.  I'm almost done
writing a paper with James Dolan on the definition of n-categories, but 
in the meantime some other folks have been coming up with other definitions of
n-categories, so we will soon be in the position to compare definitions and
see how similar or different they are, and start erecting the formalism
needed to deal with all these topological quantum field theories and
"sums over surfaces" in a really elegant way!  Everything looks like its
fitting together.  At least, that's my momentary optimistic feeling.  
Perhaps it's just the fact that classes are over that is making me so happy.  
Yes, it's probably just that.
-----------------------------------------------------------------------
Previous issues of "This Week's Finds" and other expository articles on
mathematics and physics, as well as some of my research papers, can be
obtained by anonymous ftp from math.ucr.edu; they are in the
subdirectory pub/baez.  The README file lists the contents of all the
papers.  On the World-Wide Web, you can get these files by going to
http://math.ucr.edu/home/baez/
A complete index of the old issues of "This Week's Finds" is available
at
http://math.ucr.edu/home/baez/twf.html
but if you are cursed with a slow connection and just want a jumping-off
place to the olds issues, go to
http://math.ucr.edu/home/baez/twfshort.html
For the latest issue, go to
http://math.ucr.edu/home/baez/this.week.html
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Subject: Re: NASA lies, again.
From: singtech@teleport.com (Charles Cagle)
Date: Tue, 17 Dec 1996 13:51:08 -0800
In article <32b2bc70.2511968899@news.smart.net>, stephani@smart.net wrote:
that C. Cagle had written:
>>There you go; admitting freely that your choice of friends includes a
>>number of 'Welfare Queens in White Coats'.
>
>I just wonder if you have a point here, or if you're parroting some
>party line or talk show host.  It's clear you don't know any
>government employees; it's also clear that you are uninterested in the
>facts, except where they back up your hastily-formed opinion.
Your half witted response indicates that it is you that has little
interest in the facts.  I know lots of gov't employees.  And my opinion,
oh swami know it all who knows nothing, has taken nigh on fifty years to
form.  Perhaps that's 'hastiness' where you come from.
>>
>>> Like all other human beings, some government workers are
>>>worth their pay, some are not, and some don't get paid nearly enough for
>>>what they do.  There are some really good people working for the
>>>government who could make quite a bit more money working in the private
>>>sector, but who choose public service.
>>
>>Probably because its easier.
>
>I work for the government.  I've done the private sector thing too,
And probably couldn't cut it in the real world.
>and I recognize that there are some people in the private sector who
>work very hard indeed.  
No doubt why you couldn't make it.
>But the job I have now takes more of my time
>and energy than anything else I've attempted to do, graduate school
>included.
Probably because you are utterly incompetent at what you do.  Most likely
you are a personification of the Peter Principle.  The fact that you are
'attempting' to do your job says it all.
>>
>>>  It really pisses me off when some
>>>jerk mouths off about how evil (or lazy, inefficient, etc.) the government
>>>and government workers are without having any real evidence to back it up.
>>
>>I wonder who programmed that into your head?  Couldn't be you, right?  So,
>>you get pissed off do you when someone 'pushes your button' by conforming
>>to a set of parameters which you yourself have set up?  Exactly whose
>>problem to do suppose that is?  And you refer to others as 'jerks'? :-)
>>
>>As far as evidence to back it up...wow!  What a laugh!  There's
>>practically nothing but evidence.  If we could just put the armor plating
>>that you apparently have on your head on our Army tanks why we would be
>>invincible. :-).
>
>Okay, so, where is this evidence?  The fact that some departments in
>government have been inefficient in spending the taxpayers' money
>(something I will not gainsay) does not mean that government workers
>are lazy. 
Just cowards who will not stand up and make a fuss about the waste and
theft.  But why should they?  Because they are without honor and will
stand by and allow theft and incompetence to reign because it is from such
they gain their own sustenance.
> You are stating that anyone who works for the government
>must _on that account_, be lazy, ineffectual, or stupid.  
I didn't use those terms, but now that you've put it like that...Because
you haven't seen it can only mean you are too *lazy* to look for it, too
*ineffectual* to find it, and too *stupid* to recognize it when you are
immersed head first in it. 
>I've seen no
>evidence of that, even in the tattier publications; I have seen
>opinions (like yours) put forth without evidence.  I'm still waiting
>for that evidence.
 Likely, you, being blind to your own incompetence, will never recognize
the evidence.
>>>People are people. Even government workers.
>>
>>Gee and I thought gov't workers were parasites.  You learn something
every day.
>
>Name-calling makes you look foolish.
While attempting to defend the indefensible merely establishes your
blindness and lack of conscience.
-- 
C. Cagle
SingTech
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Subject: Re: But which way does it really flow?
From: Richard Mentock
Date: Tue, 17 Dec 1996 17:05:32 -0500
A Level Physics Group wrote:
> 
> Dear Southern half of the Planet (and anywhere else for that matter),
> 
> We are after the result to an experiment that you may be able to help us
> with. Our A-Level physics teacher will not believe us when we say that
> water drains in a spiral that flows in a different direction depending
> on which hemisphere it is in. He insists that it makes no difference and
> that it is dependant on the design of your bath! Oh well.
> 
> We would appreciate any help from anyone (no matter where in the world
> they are) who could try emptying their bath and recording whether the
> water drains clockwise or anticlockwise. We are particularly interested
> in result from the southern hemisphere and from places on or near the
> equator.
> 
> Please email the results to spiralwater@lpbsnet.demon.co.uk
> 
> The results of this research will be posted as we process them.
> 
> Thank you for your assistance, Langley Park School for Boys.
This is in the physics FAQ
http://math.ucr.edu/home/baez/physics/bathtub.html
The answer is:  
your teacher is right.
-- 
D.
mentock@mindspring.com
http://www.mindspring.com/~mentock/index.htm
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Subject: Re: Freezing Water
From: Richard Mentock
Date: Tue, 17 Dec 1996 17:07:17 -0500
SBobst wrote:
> 
> Which freezes faster at -10 deg. F,
>   8 oz of boiling water at 212 deg. F, or
>   8 oz of water at 70 deg. F?
> 
> How can I calculate the amount of time it will take both to freeze? :)
Depends on a lot of things which you haven't included:  size and
shape of container, amount of moisture in the air, air pressure...
See the physics FAQ: 
http://math.ucr.edu/home/baez/physics/hot_water.html
-- 
D.
mentock@mindspring.com
http://www.mindspring.com/~mentock/index.htm
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Subject: Code HEXTIME for the numerical solution of the Space-Time multigroup
From: dmitri@cdc.net (Dmitri Alperovitch)
Date: 17 Dec 1996 22:07:17 GMT
Mikhail Alperovitch
Code HEXTIME for the numerical solution of the Space-Time multigroup 
neutron diffusion and delayed precursor equations in 3D geometry
------------------------------------------------------------------------------------------
Code HEXTIME has been developed to solve Space-Time multigroup 
neutron diffusion & delayed precursor equations in 3D geometry using 
implicit finite-difference, alternative-triangular and power iterations 
methods.  The code allows to simulate nuclear reactor core transients 
initated by moving control rods, the dynamic reactivity calculation at 
different space points, neutron lifetime and effective delayed neutron 
fraction calculations.  Code was written in FORTRAN 77 for PC or UNIX 
workstations.
If you have any questions, please e-mail me at: dmitri@cdc.net
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Subject: Re: NASA lies, again.
From: singtech@teleport.com (Charles Cagle)
Date: Tue, 17 Dec 1996 14:12:35 -0800
In article <58uu92$cao@trojan.neta.com>, blair@trojan.neta.com (Blair P
Houghton) wrote:
>Charles Cagle  wrote:
>>jwalters@clark.net (Jim Walters) wrote:
>>>By the way, I don't work for NASA.  However I have lived within commuting
>>>distance of Washington, DC for almost seven years now, and a lot of my
>>>friends and acquaintances are US government employees.  Some of them even
>>>work for NASA. 
>>
>>There you go; admitting freely that your choice of friends includes a
>>number of 'Welfare Queens in White Coats'.
>
>Y'know, applying that sort of insult to some of the most
>intelligent and productive people ever to grace human
>history makes you look like a complete idiot.
And your defense of those people establishes that you are without moral
conscience.
>>>There are some really good people working for the
>>>government who could make quite a bit more money working in the private
>>>sector, but who choose public service.
>>
>>Probably because its easier.
>
>Almost always because it's challenging and satisfying.  I
>happen to work in a place where there are a surprising
>number of former NASA engineers, whether employees or
>subcontractors, and the reason they give most for leaving
>NASA is that the private-sector money for their skills is
>far too large to turn down.
Most likely the place you work is sucking the gov't tit.  So they changed
jobs because the money was better.  Shows you they weren't so dedicated
after all but merely intellectual whores such as yourself.
>>>  It really pisses me off when some
>>>jerk mouths off about how evil (or lazy, inefficient, etc.) the government
>>>and government workers are without having any real evidence to back it up.
>>
>>I wonder who programmed that into your head?  Couldn't be you, right?  
>
>And perhaps you can tell us who programmed your irrational
>anti-government-worker prejudice into your head?
>
>>So, you get pissed off do you when someone 'pushes your button' by conforming
>>to a set of parameters which you yourself have set up?
>
>So you don't like it when someone recognizes that you're
>being a jerk?
>
>The attitude you displayed was tantamount to a troll for
>people on this net who would disagree with you; 
That's right and you slack jawed bottom feed, you took the bait, didn't you?
>especially
>considering that the attitude is abhorrent and almost
>anyone (except maybe Randy Weaver) could find it in
>themselves to disagree with you.
You lockstepp moron.  You think what the Gov't did to Weaver was right? 
If so, may they do the same to you and your family.
>Jim was in fact expressing what amounts to the community
>standard, and I'm confident the community applauded it.
Hey, Mr. herd instinct....is that how you do science and form your
opinions?  By consensus?
>>Exactly whose problem to do suppose that is?
>
>Apparently it's yours.  He's got a valid point and you're
>a prejudiced jerk.
>
>>And you refer to others as 'jerks'? :-)
>
>Sounds like he knows one when he sees one, jerk.
This is fun, playing you along.  Seeing you make your incompetent runs and
trying to get off the hook, but the hook is set and you are the fish.  Too
bad you aren't fit for anything but fertilizer.
>>As far as evidence to back it up...wow!  What a laugh!  There's
>>practically nothing but evidence.
>
>"Practically nothing but evidence."  That's not evidence.
>And anecdotes won't do, either.  You made a generalization
>about everyone who works for NASA and you'll either have to
>back that up or eat the crow you're roasting for yourself.
>Silence or evasion will of course be inferred to agree that
>you're a coward and a liar.
What, and join company with you?  Never!
>>>People are people. Even government workers.
>>
>>Gee and I thought gov't workers were parasites.  You learn something
every day.
>
>Today we learned that Charles Cagle is an abusive and irrational
>loser who has nothing better to do than insult his betters.
>
>                                --Blair
>                                  "You jerk."
And we learned that Blair P Houghton considers himself the better of all
who know of his utter incompetence and dishonestly and inability to
demonstrate rationality
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