Aristotle principles of dynamics
Grzegorz M. Koczan
Information about the origin and purpose of this note: The note was made available by the author (Dr. G. M. Koczan) to Professor Arkadiusz Jadczyk for popularization, discussion and verification by publishing it on the professor's scientific blogs.
Aristotle is the author of a series of coherent writings on physics written around the same time, which are now consolidated and known as the work of Physics (Aristotle 350 BC, Leśniak 1968). In this work, Aristotle gave several proportions of the motion of bodies. It is difficult to explain why these proportions are currently so poorly exposed and why only one of them is usually analyzed. A selective analysis of proportions, however, leads to an wrong or misunderstood Aristotle principle of motion. Based on the translation of Physics, the author proposes a broader and more coherent system of reconstruction of Aristotle principles of dynamics (Koczan 2021, 2023).
Aristotle proportion of motion in Book VII of Physics can be represented quite faithfully by the following proportionality. Namely, the ratio of the distance s to the time t is proportional to the ratio of the driving factor (force F) to the measure of the body quantity (mass m): s/t~F/m. In Book IV of Physics, there are proportions that can be expressed by the proportionality of the motion time t to the density of the medium d: t~d or equivalently in the form s/t~1/d. In Aristotle, the density of the medium is a measure of the resistance of the medium, so often the proportion from Book IV is written in the form: s/t~F/f, where f is the measure of resistance. Both reconstructions (s/t~F/m and s/t~F/f) of Aristotle dynamics are known from the history of physics and are current reconstructions, but practically they have never been confronted simultaneously.
The author decided to simply combine both proportionalities resulting from Aristotle's proportions into one proportionality, which can be expressed as: s/t=F/(fm) or equivalently F=fmv using the velocity symbol v=s/t. The resulting relationship is equivalent to the original proportions, except for the equals sign. The physical truth of the obtained equation F=fmv now depends on the interpretation of the measure of resistance f, as well as the force F. If f is interpreted ad hoc literally as a resistance force, then the equation under consideration will not be confirmed in physical reality. However, if f is just a drag coefficient proportional to the density of the medium, and F is the force driving the motion (i.e. the force opposing the drag, and thus de facto equal to it), then the equation will have the correct physical sense. Such an equation describes the movement of a body under the influence of a strong resistance proportional to velocity, according to Newtonian dynamics. This agreement is based on quasi-stationary states. Thus, the equation F=fmv can be called Aristotle second principle of motion, which is physically correct for quasi-stationary or stationary states.
From Aristotle's second principle of motion follows the law of rest, or Aristotle zeroth principle of motion. It says that in a medium with resistance to motion, the body tends to rest if there is no force driving the motion. The zeroth principle (law of rest) is true and is consistent with Aristotle Physics.
The most difficult situation in the analysis of the equation F=fmv is when f=0 and F=0, because then the velocity can have any value (including infinite or zero). It is not true that Aristotle in a similar context rejected all non-zero values of velocity (infinite and finite), because he was aware of the indestructibility of motion and postulated the eternity of circular motion. Thus, in the present situation, the body can, according to Aristotle, move uniformly in a circle or be at rest. It is worth adding that in the macroscopic sense, rest can be treated as a circular motion with a radius approaching zero, and locally a radius approaching infinity can be treated as a rectilinear motion (generalized circle). In this way, Aristotle first principle of motion can be described based on uniform circular motion.
Aristotle's zeroth, first and second principles still need to be supplemented with the third principle, which tells us what the drag coefficient f depends on. As already mentioned, the drag coefficient depends directly on the density of the medium d. In addition, the greater the density ρ and the greater the weight of the body, the lower the drag coefficient. Thus, Aristotle third principle of motion has the form of proportionality f~d/ρ. This proportionality in the context of the density of the medium d is undoubtedly consistent with Aristotle Physics, and in the context of the density of the body ρ, one can have some doubts whether Aristotle did not mean F here.
Arystoteles (350 p.n.e.), tłum. Leśniak K. (1968), Fizyka (Physics), Corpus Aristotelicum 184a‒267b, PWN Warszawa.
Koczan G. M. (2021), [Aristotle's Defense: reconstruction of his dynamics not contradictory to the observation], preprint, www.researchgate.net/publication/356554413, DOI:10.13140/RG.2.2.10119.52647.
Koczan G. M., monograph submitted in April (2023) for review: [DEFENSE OF ARISTOTLE'S “PHYSICS” – Mathematically unified reconstruction of consistent with observation Aristotle's dynamic], Wydawnictwo SGGW.
P.S.3. 8:14 The double compactified universe with the conformal infinity cap (double Dupin cyclide) connecting our space-time with its polar opposite universe:Beatitude is God’s aim for humanity; get this supremegood for thyself first that thou mayst distribute it entirely to thyfellow-beings.He who acquires for himself alone, acquires ill though hemay call it heaven and virtue.Sri Aurobindo
About synchronicity. Seconds ago I received the following message from the Author of this note on Aristotle's dynamics:
ReplyDelete"However, there is something in the ether - some sort of intersecting chain of events. Just today I started working hard on the composition of the monograph - in the middle of the month I am supposed to submit."
Have finished the proof of Proposition 10!
ReplyDeleteNew scam comes by email:
ReplyDelete"Dear Author,
We are delighted to inform you that you have been provisionally selected for the Best Researcher Award at the upcoming International Research Awards on Gravitational Waves . We believe that your remarkable contributions to the field make you an excellent candidate for this prestigious award."
See:
https://www.researchgate.net/post/Is-this-a-new-scam-or-something-reliable/8
Pod (113) :
ReplyDeletethe group of linear transformation ->
the group of linear isometries
Lub po prostu isometries, bo czy izometrie mogą być nieliniowe?
ReplyDeleteIf p = [[X]] and Y ∈ N ->
ReplyDeleteIf X ∈ N and Y ∈ N
I have chnaged the Definition 2. I am not sure if it is for better.
Deletethat is the collection of all tangent spaces ->
ReplyDeletethat is the union of all tangent spaces
"that is the union of all tangent spaces"
Deleteor that is the disjoint union of the collection of all tangent spaces
disjoint union byłoby bardziej precyzyjne ale czy w związku z tym postawisz kropkę nad U w (126) i następnych?
DeleteW każdym razie czy zmienisz słowo collection?
Replaced Collection by disjoint union. The dot over set union is optional but not necessary, as tangent spaces at different points are by definition (of tangent vectors at a point) automatically disjoint.
DeletePrzypominam się z zamianą pod wzorem (113):
Deletethe group of linear transformation ->
the group of linear isometries
Fixed. Thanks.
DeleteStarted writing 8.5.
Tak rozmyślam sobie nad izometriami. W zasadzie to mogą być one afiniczne więc nieliniowe. Więc słowo linear chyba powinno pozostać.
ReplyDeleteThanks. Will fix tomorrow.
DeleteZastanawiam się czy bundle to zbiór fibers, czy raczej bundle to zbiór elementów należących do fibers.
ReplyDeleteAs a set it is a disjoint union of fibers. Anything else is not precise enough.
Delete
DeleteTo mi nie wyjaśnia - bo co to jest union of fibers?
Czy "union of fibers" to zbiór którego elementami są fibers czy raczej "union of fibers" to zbiór w którym fibers są jego podzbiorami? Symbol we wzorze (126) wskazywałby, że to drugie.
Bo gdyby miało by być to pierwsze to (126) chyba powinien wyglądać jakoś tak:
TPN = {TpPN : p ∈ PN}
A może TPN to jest jakiś iloczyn kartezjański.
DeleteSuppose PN is a circle. The fibers of TPN are tangent lines to the circle. You can make it into a Cartesian product in this case, but in general the tangent bundle is non-trivial. Set-theoretically it is a product, but topologically it is not.
DeleteTPN like any other tangent bundle is a set of points, where a point is an ordered pair (p,v) where p is a point of PN, and v is a tangent vector to PN at this point.
DeleteA fiber at p is a subset consisting of all pairs (p,v), where p is fixed.
W (130) brak =
ReplyDeleteFixed, updated. You are very constructive. Thank you!
DeleteAdded a dot over the union symbol in (129). There it is necessary!
DeleteNie widzę tej kropki w (129).
DeleteStrona 26 wiersz 1:
always exist. ->
always exists.
strona 26:
Deletewe have two linear condition ->
we have two linear conditions
Thanks, fixed. Finishing 8.3.
DeleteDot in (129) exists now for sure. Thanks.
DeleteFinished Sec. 8.3 - light rays circling at infinity. Now we can go beyond the 4D universe - to its 5D neighborhood, paying attention to the 5D reality left and right. Opening the windows and looking outside.
ReplyDeleteNie mogę przebrnąć przez stronę 25.
ReplyDeleteCzy wzory (126) i (127) są identyczne? Czy raczej niosą inną treść?
"T" : Tangent
Delete"T calligraphic": Tautological
Both names start with "T"
Czyli tangent bundle to nie jest to samo co tautological bundle?
DeleteCzyli tangent fiber to nie jest to samo do tautological fibre?
Jeśli tak to w pracy za mało jest uwypuklona ta różnica - zbyt płynne jest przejście z 8.1 to 8.1.1
Tangent fibre is 4-dimensional. Tautological fibre is 1-dimensional. Will make it clear in future versions.
DeleteNad wzorem (129) widnieje nazwa orthogonal bundle. Czy to to samo co tangent bundle?
DeleteOrthogonal bundle has five-dimensional fibers. Tangent bundle has 4-dimensional fibers. 4=5-1. Tangent space is identified with a quotient: 5 d vector space of vectors orthogonal to X divided by 1 d vector subspace spanned by X itself.
DeleteThe section 6.6 can repeated ->
ReplyDeleteThe section 6.6 can be repeated
Corrected. Thanks.
DeleteZastanawiam się czy to jest poprawny zapis:
DeleteDefinition 5. With p = [[X]], q = [[Y ]] ∈ N
Czy rzut punktu może należeć do zbioru z którego rzutujemy?
Chyba może być i tak i siak.
Dzięki za ten wiersz.
Napis:
Definition 5. With p = [[X]], q = [[Y ]] ∈ PN
nie wzbudziłby moich powyższych pytań.
Fixed. Thanks.
Delete