1. Forum
  2. Usenet
  3. SCI.PHYSICS.RESEARCH

  • "Three billiard balls collide simultaneously" revisited after 20 years

    From Carl K@21:1/5 to All on Tue Nov 29 13:59:16 2022
    Greetings,

    I used a new perfect (but simple) Newtonian physics engine to reverse a billiards break. The simulation surprised me. I expected it to re-form a stationary triangle of balls and spit out the cue ball. It did not.

    This means that classical physics is non-deterministic and not practically reversible.

    The simulator is perfect in that it keeps times, positions, and velocities
    as expressions--3*sqrt(7)/7--rather than using numeric approximations. Its worlds are 2D with circles, infinite walls, and elastic collisions.

    When trying to understand the results, I found a useful thread from sci.physics.research from almost 20 years ago. I eventually also found a
    few references in the philosophy of science.

    If you're interested in classical physics, determinism, or reversibility,
    see the details, short videos, and open-source code here (free): https://towardsdatascience.com/perfect-infinite-precision-game-physics-in-python-part-2-360cc445a197
    The old sci.physics.research thread: https://groups.google.com/g/sci.physics.research/c/xOCFItVlnro?pli=1

    - Carl

    --- SoupGate-Win32 v1.05
    * Origin: fsxNet Usenet Gateway (21:1/5)
  • From Phillip Helbig (undress to reply@21:1/5 to Carl K on Tue Nov 29 23:19:00 2022
    In article <f228b69d-cd2b-47ba-b503-56ea2a37617an@googlegroups.com>,
    Carl K <carlk@msn.com> writes:

    I used a new perfect (but simple) Newtonian physics engine to reverse a billiards break. The simulation surprised me. I expected it to re-form a stationary triangle of balls and spit out the cue ball. It did not.

    This means that classical physics is non-deterministic and not practically reversible.

    It does not mean that it is non-deterministic. Make a movie of the
    billiard break and run it backwards: perfectly valid physics. Classical physics is reversible.

    That it is not reversible in practice is a different matter, but that
    was known before the simulation.

    The simulator is perfect in that it keeps times, positions, and velocities
    as expressions--3*sqrt(7)/7--rather than using numeric approximations. Its worlds are 2D with circles, infinite walls, and elastic collisions.

    But even 3*sqrt(7)/7 or whatever, when it comes down to actually
    calculating something, will be used a finite approximation.

    Taking a broader view, questions such as whether classical physics is deterministic and/or reversible aren't determined by simulations. There
    are some complicated processes which simulations can shed light on, but
    with regard to fundamental issues, one must know the fundamental issues
    when programming the simulation.

    --- SoupGate-Win32 v1.05
    * Origin: fsxNet Usenet Gateway (21:1/5)
  • From Michael Moroney@21:1/5 to All on Wed Dec 7 13:36:56 2022
    On 11/30/2022 2:19 AM, Phillip Helbig (undress to reply) wrote:
    In article <f228b69d-cd2b-47ba-b503-56ea2a37617an@googlegroups.com>,
    Carl K <carlk@msn.com> writes:

    I used a new perfect (but simple) Newtonian physics engine to reverse a
    billiards break. The simulation surprised me. I expected it to re-form a
    stationary triangle of balls and spit out the cue ball. It did not.

    This means that classical physics is non-deterministic and not practically >> reversible.

    It does not mean that it is non-deterministic. Make a movie of the
    billiard break and run it backwards: perfectly valid physics. Classical physics is reversible.

    That it is not reversible in practice is a different matter, but that
    was known before the simulation.

    Is it chaotic in a way, that is, a tiny change in the backwards action
    causes a completely different outcome?

    --- SoupGate-Win32 v1.05
    * Origin: fsxNet Usenet Gateway (21:1/5)
  • From Phillip Helbig (undress to reply@21:1/5 to .std.spaamtrap.com on Thu Dec 8 23:23:43 2022
    In article <tmqftd$1pem$3@gioia.aioe.org>, Michael Moroney <moroney@world= .std.spaamtrap.com> writes:
    On 11/30/2022 2:19 AM, Phillip Helbig (undress to reply) wrote:
    In article <f228b69d-cd2b-47ba-b503-56ea2a37617an@googlegroups.com>,
    Carl K <carlk@msn.com> writes:

    I used a new perfect (but simple) Newtonian physics engine to revers=
    e a
    billiards break. The simulation surprised me. I expected it to re-fo=
    rm a
    stationary triangle of balls and spit out the cue ball. It did not.

    This means that classical physics is non-deterministic and not pract=
    ically
    reversible.

    It does not mean that it is non-deterministic. Make a movie of the billiard break and run it backwards: perfectly valid physics. Classi=
    cal
    physics is reversible.

    That it is not reversible in practice is a different matter, but that
    was known before the simulation.

    Is it chaotic in a way, that is, a tiny change in the backwards action
    causes a completely different outcome?

    Right. Even if one could specify the positions and velocities as well
    as allowed by the uncertainty principle, after just twelve collisions
    the uncertainty in a ball's position would be larger than the size of
    the table.

    --- SoupGate-Win32 v1.05
    * Origin: fsxNet Usenet Gateway (21:1/5)
  • From Carl K@21:1/5 to All on Thu Dec 8 23:24:58 2022
    Summary:

    I'm the original poster. I recently found a reference with a simpler
    example illustrating the issue.
    Imagine this simple Newtonian example from Lee [2016, https://dl.acm.org/doi/pdf/10.1145/2912149]: Three balls of unequal mass
    in the line; the left is moving right, the middle ball is stationary; the
    right ball is moving left. This seems to show different results depending
    on whether the left ball hits first or the right ball hits first. Prof.
    Lee concludes that the Newtonian system is mathematically "incomplete" in
    the sense that it does not include its limits (Here, the limit as the time delta between the hits goes to zero).

    Details:

    I'm interested in the mathematical properties of Newtonian physics and a
    few days ago found this paper by Prof. Edward A. Lee of U. of California, Berkeley. Fundamental Limits of Cyber-Physical Systems Modeling, November
    2016, ACM Transactions on Cyber-Physical Systems 1(1):1-26

    He gives the example above in section 4, on page 17. I worked it out with
    his suggested masses of 1/5, 1, and 5 and before velocities 1, 0, -1 and,
    as he said, got different sets of after velocities. Specifically, I used
    my simple physics engine and got <-73/27, -40/27, -5/9> vs <-31/9, -7/9,
    -2/3>.

    He closes the paper with a discussion of issues such as interleaving,
    butterfly effect, superposition, and determinism. If interested, please
    see the paper (starting near page 18) for more details.

    His lab works on real-world physical systems, so he also discusses more realistic models (for example, one with springs).

    I personally love his example. I find it much more compelling than other similar attempts to understand the mathematical structure of Newtonian
    physics (e.g. Norton's dome, Suppes' 2D symmetric 3-particle collision,
    and various 2D "game engine" collisions.)

    - Carl
    https://medium.com/@carlmkadie

    --- SoupGate-Win32 v1.05
    * Origin: fsxNet Usenet Gateway (21:1/5)