https://books.google.com/books?id=ccFHXMDXFdEC&newbks=1&newbks_redir=0&printsec=frontcover&dq=Causation+and+Explanation+Campbell,+O%27Rourke,+Silverstein&hl=en&source=gb_mobile_entity#v=onepage&q=Causation%20and%20Explanation%20Campbell%2C%20O'Rourke%2C%20Silverstein&f=false
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Frank C. Wimberly
140 Calle Ojo Feliz,
Santa Fe, NM 87505

505 670-9918
Santa Fe, NM

On Tue, Aug 20, 2024, 5:12 PM Frank Wimberly <wimber...@gmail.com> wrote:

>
> > I hate thought experiments. But I need this one.
>
> See:
>
> Book Chapter3: Actual Causes and Thought Experiments
> By
>
> Clark Glymour ,
>
> Frank Wimberly
>
> MIT Press 2007
>
> ---
> Frank C. Wimberly
> 140 Calle Ojo Feliz,
> Santa Fe, NM 87505
>
> 505 670-9918
> Santa Fe, NM
>
> On Tue, Aug 20, 2024, 2:53 PM Santafe <desm...@santafe.edu> wrote:
>
>> Second inadequate reply, to Glen, unhappily similar to the first to Jon:
>>
>> > On Aug 19, 2024, at 23:37, glen <geprope...@gmail.com> wrote:
>>
>> > There's so much I'd like to say in response to 3 things: 1) to
>> formalize and fail is human, 2) necessary (□) vs possible (◇) languages,
>> and 3) principle vs generic/privied models. But I'm incompetent to say them.
>> >
>> > So instead, I'd like to ask whether we (y'all) think a perfectly rigid
>> paddle, embedded in a perfectly rigid solid, with a continual twisting
>> force on the handle, exhibits "degenerative" symmetry? Of course, such
>> things don't exist; and I hate thought experiments. But I need this one.
>>
>> I got lost here because I don’t know what “degenerative” symmetry is
>> meant to refer to.  In context of your next para, I see a contrast between
>> discrete symmetries, such as the rotations that would preserve a
>> crystalline unit cell, versus continuous symmetries, which I need as a
>> formal model to derive restoring forces.  Is “degenerative” somehow another
>> term for the continuous ones?
>>
>> The question when a continuum model can be seen as a limit of discrete
>> models on finer and finer grains, and when one needs it to be an
>> independent construct, is interesting.  It feels like it goes back to the
>> Eleatics.
>>
>> I have often thought that Zeno’s paradoxes nicely illustrate the things
>> you can’t do if you have a mechanics that mathematizes only positions.
>> Hamilton sweeps those limitations away by making momentum an independent
>> coordinate in a phase space, and in that way granting it status as an
>> independent property of objects from their positions (in classical
>> mechanics).   All the consequences of Noether’s theorem, conservations,
>> restoring forces, etc., are formulated in terms of these independent and
>> dual properties.  With the advent of quantum mechanics, their independence
>> becomes even more foundational to the picture of what exists, as a system
>> in a momentum eigenstate is really in a completely distinct state from one
>> in a position eigenstate.  The two are differentiated in something like the
>> way traveling waves and standing waves are differentiated in various wave
>> mechanicses.
>>
>> > Similarly, if the paddle+solid could only be in 1 of 2 states, rotation
>> 0° and rotation 180°, and would move instantly (1/∞) from one to the other,
>> with `NaN` force at every other angle and 100% force at the 2 angles. This
>> seems like symmetry as well, but not degenerative. And we could go on to
>> add more states to the symmetry (3, 4, ...) to get groups all the way up to
>> ∞, somewhere in between where the embedding material becomes liquid, then
>> gas, etc. and the "symmetry" is better expressed as a cycle/circle. But I'm
>> not actually asking questions about 1D symmetry groups. My question is more
>> banal, or tacit, or targeted to those who think with their bodies. When all
>> the other non-Arthur peasants try to pull Excalibur out of the stone, my
>> guess is they're not thinking it exhibits degenerative symmetry. And that
>> implies that normal language is not possible. It's impoverished, for this
>> concept. Math-like languages are necessary in the sea of all possible
>> languages. The would-be King *must* use math to describe the degenerative
>> symmetry. (Missed opportunity in Python's Holy Grail, if you ask me. "I
>> didn't vote for you!”)
>>
>> Here I end with the same one I ended the reply to Jon: I strongly bet
>> that much of what people think they believe for “Natural” reasons are
>> actually learned beliefs through formal systems.  I don’t think farmers
>> before Newton had a Cartesian and Newtonian concept of space x time, or
>> that they would have been bothered by Einstein.  I don’t think they would
>> have cared about Einstein any more than they cared about Newton.  They had
>> some ontology of “things", and the “places” that things *occupy*.  And
>> probably an ontology of keeping appointments, which in a more formal world
>> might entail something analogous to a “theory of mind” construction about
>> what other people are doing somewhere else “at the same time” as you are
>> doing your thing here.  But my default assumption would be that any of this
>> only ever took on the rigidities of a Cartesian system after the lived
>> practice of Newtonian mechanics had started to make some of its rigid
>> entailments part of routine experience.  Then it became a struggle to let
>> that go when Minkowskian geometry required something different.
>>
>> I don’t mean to be perverse and excessive in denying the implications of
>> folk physics: Probably, had farmers been dragged through it (strongly
>> against their will), they would have found QM’s notion that what we
>> _should_ call a _thing_ can be characterized by “being at” multiple
>> “places” more difficult than Newton’s “thing at a single place”.  But I’m
>> not sure how much trouble it would have been.  Considering the worldviews
>> people are proud to claim they hold in various religious and superstitious
>> traditions, the things asked from modern physics seem relatively benign as
>> imaginative lifts.
>>
>> Would be nice to have something substantive to say about any of this,
>> that would deserve to last.  But I don’t think I do.
>>
>> Eric
>>
>>
>>
>>
>>
>>
>>
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>
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