I'll see your bet with: 
<https://pedermisager.org/blog/seven_basic_rules_for_causal_inference/>

On August 20, 2024 5:59:20 PM PDT, Frank Wimberly <wimber...@gmail.com> wrote:
>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
>---
>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.
>>>

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