Subject: Re: "Essential" reality (was: When did Nietzsche wimp out?)
From: meron@cars3.uchicago.edu
Date: Tue, 29 Oct 1996 00:22:41 GMT
In article <327524A3.4B40@sdd.hp.com>, Steven Hines writes:
>meron@cars3.uchicago.edu wrote:
>>
>> In article <3274E91F.5247@sdd.hp.com>, Steven Hines writes:
>> >Russell Turpin wrote:
>> >>[snip]
>> >> There is no faith to which one
>> >> must leap, no metaphysical tenets that one must accept.
>> >
>> >Don't you have to believe that every event has a cause? Doesn't
>> >acceptance of this proposition constitute a "passage of faith"?
>> >
>> Assume, yes, believe, no. There is a difference. Science is self
>> checking and self correcting. It makes assumptions, draws conclusions
>> and checks the conclusions versus experimantal data. But the
>> assumptions aren't sacred and if the data fails to support your
>> conclusions you may be forced to modify your assumptions. It is the
>> continuous cross checking that distinguishes assumptions from beliefs.
>
>Okay.
>
>I think I have a basic understanding of the model scientists
>use in settling on hypotheses, theories, and laws. I accept that
>each of these must be consistent with observations in order to hold
>up and that theories that do not stand up to experimental rigor are
>discarded in time.
>
>I write the above paragraph in the hopes of establishing some common
>ground here and so you do not think that I am attempting to discard
>science and its accomplishments.
>
It was rather obvious from the beginning that this is not your
intention.
>That being said, I have a hard time seeing how one can experimentally
>determine that some events do not have causes and still be doing
>science. That is, if a scientist observes an event, looks for a cause,
>and finds none, what is the consensus among other scientists in the field?
>Honestly... are they likely to say, "Ah, this event has no cause"
>or instead will they say (perhaps to themselves) "This scientist has
>not looked hard enough, or in the right places."
>
OK, lets use some example, then we can return to the general issues.
Assume we've a hydrogen atom in an excited state (meaning that the
electron is not at the lowest energy state possible). We know, both
experimentally and theoretically (from quantum mechanics) that
eventually there will be a transition, the electron will end up at the
ground state and a photon carrying the excess energy will be emitted.
We can calculate what is the probability per unit time for such an
event to occur and how lon, on the average, we've to wait for it to
occur. But, we cannot predict at what moment exactly it'll occur and
according to all we know such prediction is impossible.
So, if you ask "what was the cause for the transition" I can tell you
that it was caused by the system not being in its ground state and by
its coupling withthe radiation field. But then you can say "yes, but
why did it happen at the specific moment it did" and I'll answer
"according to all we know no cause can be specified for this".
So (now we're back to the general stuff) you can ask "how can you be
sure that this apparent lack of cause is how things really work, not
just a failure on your part to look deep enough. How do you know that
there is no better theory which explains this which you cannot
explain." And my answer is "I'm not sure and, what's more important,
I know that I'll never be sure that I've the best theory possible.
And, it doesn't matter."
You see, science is pragmatic, one may even say opportunistic. Unlike
religions and some philosophies it is not trying to come with the
ultimate answers to everything (no cracks about 42, please). And it
is not claiming absolute certainties. What it does is to try to come
with as good answers and descriptions as it can given existing
information, in the full knowledge that better answers and
descriptions may be forthcoming in the future. It is not claimming
infallibility, thus when existing models are modified or replaced by
newer ones it considers the change to be progress, not admission of
failure.
>What I mean to say is that I can't see how science can proceed unless
>is assumes beforehand that observed phenomena can be explained
>(isn't that, after all, the job?).
Yes, it is its job, and it assumes that observed phenomena can be
explained, in some fashion. How much of an explanation is full
explanation, that changes over time.
>But what about this assumption? Is it forced to stand up to the
> same rigor as the hypotheses, theories and laws?
What to you mean "stand to the same rigor". If you mean "prove that
the best explanation possible was achieved" that's unprovable.
>That is, how can one know for certain that _all_ avenues
>have been traveled in search of a cause, but to no avail, and that
>therefore the phenomena has no cause? How many scientists would
>accept this?
As I said, absolute certainties are for religion, not science.
Science only offers the best current explanations.
>
>If the proposition "all events have causes" cannot be proven or
>disproven by experimentation, then isn't it true that the proposition
>is being accepted on faith?
No, it is accepted as working assumption, to be modifiesd as needed.
It already has been heavily modified in the transition from classical
to quantum mechanics, where the concept of cause is way weaker than it
used to be.
Mati Meron | "When you argue with a fool,
meron@cars.uchicago.edu | chances are he is doing just the same"
Subject: Re: "Essential" reality (was: When did Nietzsche wimp out?)
From: turpin@cs.utexas.edu (Russell Turpin)
Date: 28 Oct 1996 18:30:47 -0600
-*-------
In article <327524A3.4B40@sdd.hp.com>, Steven Hines wrote:
> That being said, I have a hard time seeing how one can experimentally
> determine that some events do not have causes and still be doing
> science. That is, if a scientist observes an event, looks for a cause,
> and finds none, what is the consensus among other scientists in the
> field? Honestly... are they likely to say, "Ah, this event has no
> cause" or instead will they say (perhaps to themselves) "This
> scientist has not looked hard enough, or in the right places."
It's a bit more complex than that. Summarizing far too
simplistically, one can create physical systems that are
identical (actually mirror opposites in some measures), separate
them, and then observe their deviance from deterministic behavior
to identify which elements of behavior are intrinisically(*)
non-deterministic. Some fairly rigorous bounds can be placed on
the "intrinsically" in the previous sentence: determinism can be
preserved only by faster-than-light communication, effects
preceding their cause, multiple universes, and other oddities.
Strictly speaking, one isn't *compelled* to believe that the
universe is inherently non-deterministic at bottom, but only to
consider this as one possibility from other -- equally weird and
disturbing -- choices. The best popular introduction I have seen
to this is "Quantum Reality" by Nick Herbert, which should be
available through major bookstores.
Now, obviously, physics might be wrong about this in some crucial
regard. Einstein thought so. But it is evidence of how much
more important evidence is to preferred metaphysical assumptions
that physics as a field is guided by the former, not the latter.
> ... But what about this assumption? Is it forced to stand up
> to the same rigor as the hypotheses, theories and laws? ...
Some of the key experimental evidence are the famous dual slit
experiment and Aspect's experiment.
> ... That is, how can one know for certain that _all_ avenues
> have been traveled in search of a cause, ...
No physical theory is known "for certain." But the evidence is
pretty strong.
Russell
--
The difference between life and a movie script is that the script has
to make sense. -- Humphrey Bogart
Subject: Re: A photon - what is it really ?
From: parendt@nmt.edu (Paul Arendt)
Date: 29 Oct 1996 00:18:13 GMT
I said:
>>- When photons travel through a medium, they are being continually absorbed
>> and re-emitted by the medium (its atoms or molecules or larger systems).
Lloyd Johnson points out:
>Usually when a photon is absorbed, then re-emitted, it is emitted in
>some random direction. Yet when a photon travels through glass, you
>say it is continually absorbed and re-emitted. Why then is it
>preferentially emitted in the original direction?
An excellent question!!! I've been away from Usenet for a few days, and this
thread has expanded beyond belief... browsing the replies, however, I think
there are several things that have not been pointed out, and some things
that have been misunderstood.
(emerging from bait shop, fishing lures hooked to hat... setting down a huge
metal can. **** THHHHUUUUNNNNKKKKK!!!! **** Inscription on side: "Very Big
Can-o-Worms." **** CCCCCCRRRREEEEEAAAAAAKKK...**** .... opening the can,
very slightly:)
Judging from the newsgroups this thread is in, the readership is very large
and diversified. I'd like to clarify a few things first off:
There are several different wavelengths of relevance here. One is the
wavelength of the photons involved, which is given by the photons' energy
or frequency (energy/Planck's constant). Divide the speed of light IN VACUUM,
c, by this frequency and you get the (vacuum) wavelength of the photon.
Another frequency of relevance is that of the natural oscillations of the
medium you're considering;
these can be atomic, nuclear, molecular, crystal, or other transitions (quantum
mechanically speaking). This frequency gives you another wavelength, by the
same method as above. Finally, there is a length scale involved in the spatial
distance (averaged, if you like) between the molecules or other oscillators in
the medium. This gives you yet another length scale. When the photons'
wavelengths is near EITHER of the other length scales, special stuff happens
and we gotta be careful in describing the photons' behavior.
For the standard example (visible light in glass), the separation between
molecules is around 10^-8 or 10^-7 cm. Visible light, on the other hand,
has a wavelength of several times 10^-5 cm... much larger than the typical
interatomic separation.
We are also safely away from the nearest relevant natural oscillation frequency
of glass, which is in the UV (shorter wavelength than visible). It is these
properties which allow us to choose whether we use "classical electrodynamics"
(CED) to describe what's going on (easier in this case, but less general), or
"quantum electrodynamics" (QED...pain-in-the-A** in this case, but applicable
to other frequencies, and containing classical EM as a limit). When someone
talks about "index of refraction" of a medium, or "wavefront" of a photon
or set of photons, they are implicitly in the classical limit; decrease the
wavelength of our photons to the hard X-ray or gamma-ray regime, and you won't
see anyone talking about the index of refraction at those wavelengths!
Why? Because the description is inappropriate and not very useful.
Some terminology definition is necessary at this point as well. In QED, we
describe the "scattering" of photons via what are known as "virtual"
transitions.
A free electron can "wiggle" as it likes... so that incoming photons of
any wavelength can be absorbed by it, and re-emitted. If a photon is absorbed
and re-emitted RIGHT AWAY (with the same wavelength but possibly with a new
direction), it's called a "virtual" transition; one where the excited electron
sans photon is never directly observed. It is also called "elastic scattering"
of the photon (the "elastic" refers to the photon's wavelength not changing).
So, whenever I say "scatter", I actually MEAN "virtually absorbed and
re-emitted";
they are the SAME thing. In a molecule, metal, crystal, or whatever, the
electrons are confined to "wiggle" in certain ways only... these are the
transitions between the quantum-mechanical "states" of the system.
Now, it is natural to ask HOW this virtual absorption and re-emission leads
to the slowing of light in a medium, and why the direction isn't totally
randomized. Read on...
(**** CRRRRREEEEAAAAKKKKK **** as we open the can of worms a bit more, but
still not all the way)
I'll now assume that the reader has some idea of quantum mechanics, and
I'll try to describe how normal optics comes out of this quirky QED....
Pretend, for simplicity, that we have a bunch of molecules with only one
transition possible, say a UV transition from glass. Now, let's follow
a visible-light photon as it goes through the glass. Wait... we're already
in trouble!!! It turns out that we CAN'T say what happens to the photon,
unless we observe it to have happened! This is an EXTREMELY important point.
Now, several things are possible as the photon goes through the glass:
1. It can go through unchanged, without interacting with ANY of the molecules.
2. It can "scatter" (be virtually absorbed and re-emitted) off exactly one
of the molecules.
3. It can "scatter" off two of the molecules
4. and beyond... you get the picture!
Now, I'll be talking about the "amplitude" for a process to happen... if you
haven't had any QM (quantum mechanics) you can substitute the word
"probability" where you see "amplitude", but you'll run into trouble in
following how the
probablilities don't seem to add quite right. The "amplitude" is a complex
number, or 2D vector if you like, whose length gives the probablility for a
process to have happened.
Now, the amplitude for number 1 above to happen is quite large!! Photons would
be quite happy to pass through a medium without anything happening.
Let's look at number 2, the single scattering event. For an isolated molecule,
the likelihood of scattering is much less than that of passing through
unharmed, so it seems that our photon will not even see the glass we've put
in front of it. The scattering amplitude goes as the amplitude for the
absorption and re-emission (not very likely if the photon isn't at just the
right frequency), and has the fine-structure constant (about 1/137) in the
numerator, making it quite small indeed (it always has length smaller than 1,
even if you take the 1/137 out).
But wait... there are MANY ways number 2 can happen; the photon can scatter
off any of the 10^(23 +- 5) or so molecules that are present.
The amplitude for number 2 to happen is the sum of all the ways it can happen,
so all of a sudden number 2 is MUCH more likely than number 1! Furthermore,
the photon's wavelength is much larger than the typical intermolecular
separation (as noted above), so MANY of the scattering sites are seen by
the photon at approximately the same "phase." This leads to some
magical sort of stuff happening:
All of a sudden, the most likely direction for scattering becomes the original
direction of the photon, with the next most likely direction being directly
backward... contrast this with the more random direction associated with
scattering by a single molecule. This has EVERYTHING to do with the number
of scattering sites that are approximately at the same phase, and with
the fact that we haven't observed which molecule actually absorbed and
re-emitted the photon. If we do this latter observation, the photon all
of a sudden gets scattered all over the place again... and the single
molecule scattering results get reproduced!!! Spooky, but wonderful. It
is the fact that amplitudes are vectors (complex numbers...as opposed to
probablilites which are always real numbers)
that makes this happen... when the amplitudes point the same direction they
are "in phase" and add "coherently." You then get a BIG probablility for those
events which can happen many different ways with the same phase... the forward
and backward directions survive while the other directions' probablilities are
swamped out. Basically, if the photon makes a 10 degree turn, the molecules
on the "inside bend" of the turn have their contributions cancelled by those
on the "outside bend". You can change this: take away selected molecules so
that those that are left are those which contribute in phase for scattering
into a 10 degree bend, and you'll find that you've likely produced a "prism"
which favors the 10 degree bend in the classical "index-of refraction"
treatment (although other, much more complicated, arrangements, are possible)
... this is left as an exercise ;-) !
(ooops... opened the can-o-worms too far... closing it a bit again now)
Anyway, this is where the term "coherent forward scattering" comes from, which
was brought up by another poster. It could just as easily and correctly have
been called "coherent virtual absorption and re-emission."
Back to the different ways the photon can pass through... if it is scattered
TWICE, the amplitude for scattering is much higher than for scattering once,
due again to the large number of molecules present. One might think that it
just keeps getting more and more likely to scatter lots and lots of times,
but the amplitude peaks for a certain number of scattering events, and finally
goes back down for larger numbers. The reason is that the amplitude for N
scattering events to occur goes roughly as
(matrix element for scattering/137)^N,
which is always smaller than (1/137)^N, which gets pretty darn small
for large N!
The amplitude for the N scattering events goes up like the above times:
number of molecules (M), for one scattering event
M(M-1) for two
... smaller than M^N for N events.
So, no matter what our M (number of molecules) is, it finally becomes LESS
likely for more scattering events to occur. The most likely number of
events goes (as you might guess) up linearly with the thickness of the
glass. The time spent "during" each scattering event is VERY small, of the
order of
(Planck's constant/energy difference between photon and transition energy)
where Planck's constant is about 10^-34 Joules-seconds, in familiar units.
For a UV transition and visible photon, we get about 10^-32 seconds that
the molecule can "keep" the photon before conservation of energy forces it
to give it up. Thus, "virtual" transitions still make themselves felt,
especially when a LOT of them could have occurred.
Why did I just say "could have?" As mentioned above, we don't KNOW what the
photon did from when it was emitted until when it was detected! The process of
passing through the glass is entirely probablilistic; repeating the experiment
with an identical photon and you'll get different answers for, among other
things:
- how long it took
- the EXACT direction it comes out
- the phase when it is detected
- etc.
This all falls nicely (although it's difficult) from the QED treatment. You
never have to introduce ideas like: susceptibility of the material, index of
refraction, etc. However, these concepts are VASTLY easier to use when one
is in the classical regime, and it's easier to think of the "wavelike"
properties of the light than the "particle" properties. But, the originators
of this thread were interested in PHOTONS... particles of light.
To sum up:
- the photons are slowed down from "c" by virtual absorption and emission,
or "scattering" if you prefer;
- They travel at "c", whenever you are able to "see" them between
successive scattering events... the absorptions slow them down macroscopically.
If the wavelength is large compared to the distance between scatterers, you
can use classical ideas to simplify the interpretation of what goes on.
I hope that this has answered more questions than it brings up!!!
- Paul Arendt
Subject: Re: Why is the sky blue?
From: rrd@fc.hp.com (Ray Depew)
Date: 28 Oct 1996 23:38:30 GMT
About seeing stars in daylight from the bottom of a well, long tube,
etc.:
The last time this came up on alt.folklore.urban (and it was
crossposted then, too), it was revealed as a joke. A Boy Scout Joke,
no less. A good old-fashioned Boy Scout Summer Camp Joke, right
up there with left-handed smoke shifters and snipe hunts.
In late afternoon, when everybody's feeling too tired to climb
mountains or carve neckerchief slides but dinner's still an hour
or two away, some of the older Scouts start talking about working
on their Astronomy merit badge. One of them says he's going to go
identify some constellations, and everybody waits for a tenderfoot
to say "You can't see stars in the daytime!"
When the know-it-all tenderfoot finally says that, one of the older
Scouts sides with the tenderfoot and challenges the stargazer to
prove that it can be done.
Meanwhile, one of the other older Scouts says "I'm thirsty" and gets
himself a big glass of water. He sips quietly, and watches the
proceedings with interest.
So the stargazer takes a long tube, like a mailing tube or a fly-rod
case, and a compass, and figures out an imaginary bearing on some
constellation or star that is not visible in the summer -- Orion, for
instance -- just to make it plausible. He then orients the tube just
so, and invites the older skeptic to "take a look." The guy looks,
is suitably impressed, and says so. Other Scouts take turns looking
through the tube, and are also amazed that it works.
Finally the know-it-all Tenderfoot lets his curiosity overcome his
better judgement. He swallows his pride and asks if he might take
a look. The daylight astronomer obliges. The tenderfoot squats,
peers through the tube -- "you have to wait for your eyes to adjust,"
he is advised -- and the aforementioned thirsty Scout pours the glass
of water down the tube.
Regards | "It does not do to
Ray Depew rrd@fc.hp.com | leave a live dragon out of
Integrated Circuits Business Division | your calculations."
Hewlett Packard Co, Fort Collins, CO | -- Tolkien
Subject: Re: What is the Cause of Time Dilation?
From: savainl@pacificnet.net (Louis Savain)
Date: Tue, 29 Oct 1996 01:54:51 GMT
In article <32743114.2A57@onramp.net>, Larry Richardson
wrote:
[One more before leaving. Couldn't resist]
>Louis Savain wrote:
>>
>> Sorry, that's not what I'm saying. I'm saying that the traveling
>> twins first accelerates away (1) from the earth bound twin, then
>> applies negative acceleration (deceleration) (2) to come to a "stop",
>> then accelerates (3) toward the earth bound twin and again decelerates
>> (4) to come to a final stop. That's two equal and opposite
>> accelerations going away and two equal and opposite accelerations
>> coming back. Unless I'm missing something that is obvious to others,
>> it seems that the net total acceleration is zero. The 4 of them
>> cancel each other out. This could not be the reason for the time
>> dilation, IMO.
>>
>
>Every time the traveller accelerates to create a net velocity with
>respect to the clock being used for comparison without a
>counterbalancing equal acceleration by that clock, the diparity between
>clocks becomes greater.
Sorry, I can't agree with this. Accelerations are vector
quantities. Their effects are directed. If the accelerations are
opposite and equal over the course of the twin's trajectory, their net
effect is null. There is no need to counterbalance with the other
clock. It is already counterbalanced. I still think that time
dilation has nothing to do with the accelerations of the traveling
twin. Also, the explanation that the traveling twin changes frames
and as a result, the change of frames somehow messes up the clock is
equally lacking in explanatory power. The way I see it, the traveling
clock will slow down on the first leg of voyage and slow even more on
the second leg. Direction does not matter. Are these the only
explanations of the twin paradox going around? If so, I'm afraid
they're not any good, IMO. Sorry. Still, I'm willing to change my
mind if someone can show me mathematically how the net zero
accelerations affect the traveling clock.
A long time ago I remember reading an account of the twin paradox
that invoked the action of the entire mass of the universe as a
possible factor. Sounds to me like this explanation is even worse
than the other ones. Does anyone know about this? If so, would you
care to comment on it?
It's amazing how the physics community would rather stand on their
heads and do a collective neutron dance, than consider absolute motion
as the simple and easy solution to this problem. Why is that? What
is there to loose besides a few inflated egos? Absolute motion does
not invalidate SRT, i.e., the relativity of observed motion. Nor does
it invalidate the constancy of the speed of light. SRT, IMO, is like
a federal mandate without the appropriate funding. It postulates (at
least most physicists claim that it does) that the only form of motion
is relative motion, and yet does not offer a cause-and-effect
explanation for that relativity. The funny thing is, physicists just
kick back as if this were no problem at all. Since when did science
decide that cause and effect was no longer pertinent? The logic of
cause and effect is the be-all of physics, as far as I can tell. This
is why the lack of a cause-and-effect explanation for relative motion
is such a monstrous hole in the theory of relativity and the sooner we
come to realize this, the better.
Is someone deliberately trying to keep the masses from figuring out
the cause of the constancy of the speed of light. It might be my
paranoia kicking into overdrive but I don't think so. I haven't seen
a single sensible reason why relativists absolutely refuse to have
anything to do with absolute motion when it would instantly explain so
many things in one fell swoop. Why the reticence? Did someone
decided that Occam's razor somehow lost its sharpness when it came to
relativity? Or are some people afraid that its application might
inadvertently do away with a few huevos in the process? :-)
> A crude analogy would be to have two cars at
>the same place with identical mileage on their odometers, then driving
>one of them a few miles away. You couldn't get their odometers to match
>once again by driving the car that had moved back to meet the car that
>hadn't moved even though the movement exhibited some symmetry.
It's a good thing you said this is a crude analogy. Very crude, I'd
say. :-) Comparing lengths traveled with the rates of clocks can
only lead to confusion at best and wrong conclusions at worst.
Best regards,
Louis Savain
Subject: Re: Question on Force, Work, and Torque was: Emory's Professors
From: brindle@lf.hp.com (Mark Brindle)
Date: 29 Oct 1996 01:15:03 GMT
Lloyd R. Parker (lparker@larry.cc.emory.edu) wrote:
: Mark Brindle (brindle@lf.hp.com) wrote:
MB: So, Lloyd, it's *MATHEMATICALLY IMPOSSIBLE* to formulate Planck's
MB: equation in terms of Joules/m^2 -- because *any* such form would
MB: constitute a *general proof* that Watts and Joules are identical.
LP: But you CAN express Planck's equation in J/m^3.
So, what's your point? I've *always* maintained that Planck's equation
describes the power-per-unit-area of a black body radiator -- and J/m^3
is a *direct* measure of power/area.
Are you *still* claiming that black bodies can be described in terms of
of "energy" or "energy-per-unit-area"? Well, you're still DEAD WRONG!
MB: Words are cheap, Lloyd; in *hard sciences* like chemistry/physics
MB: they're *useless* as ammunition against *MATHEMATICAL EQUATIONS*.
LP: Uh, no, Mark, perhaps if you had a real, liberal arts college education,
LP: you'd realize words are as useful in science as any other discipline.
LP: For example, explanations -- theories -- are formulated in words.
And *idiots* interpret the words incorrectly. If you have something
quantitative to say, there's *absolutely no substitute* for equations;
if you have nothing quantitative to say, you really don't understand
what you're talking about -- at least in the sense of "hard science".
MB: Planck's *EQUATION* says: There is *NO SUCH THING* as "the energy"
MB: of a black body radiator
LP: Hmmm... Wall says you there is the energy density. Guess what -- Silk's
LP: book also does the same thing. Energy density. And total energy density
LP: = aT^4, where a = 7.56 X 10^(-15) erg/cm^3 K^4.
Thanks, you have *AGAIN* proved my point. There is *NO SUCH THING*
as "the energy" of a black body radiator. By the numbers, Lloyd:
1) Energy is an *EXTENSIVE* property!
2) Temperature is an *INTENSIVE* property!
3) Extensive and intensive properties are *DIFFERENT*!
4) Your quote from Silk's book *PROVES* that you are DEAD WRONG.
5) Silk says that "energy_density" depends *ONLY* upon temperature.
6) Silk's equation *PROVES* that erg/cm^3 is an *INTENSIVE* property!
7) With help from Silk and Wall, *you* have *PROVEN* yourself an IDIOT!
MB: Words are cheap, Lloyd. In the *hard sciences* you need *EQUATIONS*;
MB: if you can't *SHOW US AN EQUATION* from Newtonian physics that uses
MB: Joules Of Gravity, you're just shoveling bullshit. Shovel on, Lloyd!
LP: Words may be cheap to an engineer. I'll remind you, Silk refers to
LP: "short wavelength gravitons," "energy of a graviton," and "characteristic
LP: energy distribution of gravitons."
So, I take it that you *CAN'T* come up with a Newtonian *equation*
that uses Joules Of Gravity? Thanks for *AGAIN* proving my point,
Lloyd; for *you*, words are EXTREMELY cheap and easy to come by...
...especially compared to equations,
Mark
"There's no point in being precise when you don't know what you're
talking about."
- unknown, apparently someone who's met Lloyd
Subject: Re: "Essential" reality (was: When did Nietzsche wimp out?)
From: Steven Hines
Date: Mon, 28 Oct 1996 17:17:48 -0800
Matt Austern wrote:
>
> Steven Hines writes:
>
> > As I consider these two actions, though, I have a hard time seperating
> > them. What is different between having the notion that "every event
> > has a cause" and having the notion that "the universe is lawful"?
> > If an event happens _and_ the universe is lawful, how can the event
> > not have a cause? Isn't an event without a cause arbitrary (not following
> > any law)? What kind of law is: "uncaused things happen occasionally"?
>
> If you sit and look at a particular tritium atom long enough, you
> might find that it will suddenly decay into an isotope of helium. As
> far as today's physics is concerned, though, there isn't any way to
> predict just when it will decay. We can predict the probability that
> it will decay, but its decay at any particular instant is, as far as
> we know, uncaused.
>
> Some physicists believe that there really is some cause for the atom
> decaying at one instant instead of another instant, and that we just
> haven't found out yet what the cause is. At this point, though, there
> is no evidence that those physicists are right.
All right. But consider this:
Richard Harter, to whom my paragraph above was first addressed, wrote:
> Urk. Not only do you not have to believe that every event has a
> cause, you'll do well to lay any such notion firmly aside if you're
> going to come to terms with modern physics. What you do have to "do"
> is accept *as a working hypothesis* that the universe is lawful.
Now, it may be that physicists disagree as to whether or not the decay
has been caused. As Richard says, I should discard my notion that
every event has a cause.
But Richard also says that I should accept a working hypothesis that
the universe is lawful. So: what about the physicists who do _not_
believe that the decay you talk about is caused? That is, some group
that believes that it is futile to search for the mechanism causing
the decay, because there isn't one. Do these physicists continue
to work under Richard's hypothesis that the universe is lawful?
For my part, I can't see how it is possible. If the decay is
spontaneous and uncaused, then no law can describe it. I suppose you
could try: "Decay is spontaneous and uncaused", but how are you going
to prove or disprove it through experimentation? And if no law can
describe it, the hypothesis that the universe is lawful must be
discarded.
Once again I find myself holding the position that holding the notion that
"all events have causes" is the same as working with the hypothesis that
"the universe is lawful." If you discard the first, how can you keep
the second?
In the end, of course, there are those other physicists who believe
that the decay does have a cause, despite the lack of evidence. They are
continuing their search because their job demands that they search for
the law that describes the phenomenon. They assume that there is one to
find, and may spend their careers looking. Thus, they have accepted
Richard's working hypothesis that the universe is lawful. Haven't they
also accepted that all events have causes?
-----------------
Steve Hines
shines@sdd.hp.com
Subject: Re: Hermeneutics and the difficulty to count to three...
From: moggin@nando.net (moggin)
Date: 29 Oct 1996 03:54:02 GMT
candy@mildred.ph.utexas.edu (Jeff Candy):
> Each of your posts follows the same recipe: two parts empty prose,
> one part insult, and a dash of bad metaphor. What is your goal
> in writing?
moggin :
> |> In this, particular discussion, it's to defend myself against
> |> pig-ignorant attacks from people like you. And yours, pray tell?
Jeff:
|> > I tried to be as polite as possible in my last post.
moggin:
|> Then perhaps you should stop trying. I'm serious. Your earlier
|> posts were entirely polite. I replied in kind, and you dropped the
|> subject. Your last post, in contrast, was just an attack. Again I
|> replied in kind; now you've re-acquired a degree of your politeness.
|> Go figure.
Jeff:
>After reading a good number of your posts, I noticed that you were
>devoting (what I thought was) an inordinate amount of time to heaping
>insults. If you're really interested in making a point, I don't see
>how that can help.
I already replied to this point -- you deleted the answer and then
repeated yourself. "As I've observed to others in this discussion, if
you intend to play Emily Post, you'll have to do more than criticize _me_
(at least if you hope to make your partisanship a wee bit less glaring)."
Jeff:
|> > One main point -- namely, that most of your posts include an insult --
|> > was unavoidable. To call my comments "pig-ignorant" is not reasonable.
moggin:
|> In our earlier exchange (the one about the Sokal affair, a few days
|> ago), your comments were perfectly civil, and I replied to you in the
|> same style. But you ignored that dialogue in order to claim that each
|> of my posts was insulting. Thus you're a person who chooses ignorance,
|> the better to make fraudulent claims. (There's plenty more like you
|> around here.)
Jeff:
>You were indeed civil to me previously. Now read my passage above again:
>I said "most" of your posts, not "each".
Bullshit. You said, "Each of your posts follows the same recipe:
two parts empty prose, one part insult, and a dash of bad metaphor."
_Then_ you retreated to "most." You're headed in the right direction;
the next step to is march from "most" back to "some," and then consider
_which_ posts contain insults, and why. There's no rush, but you might
want to stop making accusations until you've done some thinking. (If
you need a hint, you'll find it in my comments immediately below.)
moggin:
>l Please note that I'm the very soul of courtesy. When you were civil,
>I I offered you a civil response -- when you wanted to exchange insults,
>I accomodated you there, as well. (Or perhaps you wanted just to dish
>l them out?)
Jeff:
>I've never wanted to "exchange insults".
See above.
Jeff:
|> > What I think was stated explicitly. I can restate it very succinctly
|> > if you wish: gamma -> 1 is an approximation which captures the
|> > relevant physics in most situations. One can, and should, use this
|> > approximation in most applications. On this, I know I'm right.
|> > There. Done.
moggin:
|> If I understand correctly, you're trotting out the Indy-cars, bridge-
|> building, moon-shots argument again. But that was never a matter of any
|> dispute -- it's obvious to everyone concerned that Newton is good enough
|> for good ol' boys and government work. So if that's the only conclusion
|> you want to reach, congratulations -- we've been there from the start.
Jeff:
lCan I translate this as:
l"Correct. However, Newton is wrong in a different, more subtle sense"
I'm agreeing (as I have from the start) that Newton's errors are
small enough to ignore while performing many common tasks. Isn't that
obvious?
moggin:
|> I see. So when you attack me with falsehoods and insults, that's
|> just fine -- but when I reply, you suddenly adopt a high moral tone.
Jeff:
>-> Which falsehoods?
>-> Which insults (other than to imply that you insult others alot, and
> spend too much time coloring your language needlessly)?
"Each of your posts follows the same recipe: two parts empty prose,
one part insult, and a dash of bad metaphor." (Insult and falsehood.)
"I submit that your difficulties in this matter were a result of your
willingness to argue without having thought carefully about what it was
you wanted to say." (Insult.) "After reading many of your posts (and
you do produce a prodigious amount), I offered two tentative conclusions:
(i) your posts contain more insults than original ideas (ii) you argue
at length about a subject you had not thought about. (More insults.)
moggin:
|> Of course I'm not claiming to say anything original about Newton:
|> I've been clear about that. I made what I once thought was a widely
|> accepted statement, only to find myself being attacked, months later,
|> by people yelling things like, "You idiot! Don't you know that's
|> widely accepted?" Welcome to the party.
Jeff:
>I am sympathetic to the fact that there is no shortage of loudmouths on
>this group (sci.physics) yelling "you idiot" without due provocation.
>I also apologize if anything I say is off the mark because I've not
>read every article which preceded this out-of-control thread. But
>now its evolved into a very unfocused argument about Derrida and
>all kinds of other foggy stuff, and I'm not convinced anything was
>every *properly* resolved at a more fundamental level. You could
>simply summarize for me your most basic assumptions (if you indeed
>argue from such) in this matter, *or* you could tell me to just go
>away because you can't be bothered regurgitating what you consider
>to have been stated sufficiently well already.
What matter are you concerned with? And what do you want my
basic assumptions about? Six months ago, during one of the periodic
round-robins between alt.postmodern, talk.origins, and sci.skeptic, I
gave Newton as a counter-example to the proposition that "scientific
theories are never wrong." Recently a post turned up quoting part of
that conversation. Several members of talk.origins and sci.skeptic
saw the post, read my earlier comments, and felt compelled to dispute
me. Michael Siemon called me a complete idiot, Bob Casanova accused
me of playing semantic games, and Matt Silberstein asked, in what may
have been plaintive tones, "But what about Indy cars?" The ensuing
flame-war was cross-posted to rec.arts.books and sci.physics (in all
likelihood by Noel Smith). The rest is history.
>Recap: Its never been clear to me exactly what your position on
>approximation in physics is. What is it?
Please explain how one takes a position on approximation. What
are my choices?
-- moggin