Recent content by wrobel

  1. wrobel

    I Mechanics problem: A Weight and a Mass Suspended from a String

    not always but in the absence of friction
  2. wrobel

    I Mechanics problem: A Weight and a Mass Suspended from a String

    Then it is indeed a simple application of the torque equation.
  3. wrobel

    I Mechanics problem: A Weight and a Mass Suspended from a String

    Is ##\ell## a rod that connected to the sphere perpendicular and such that they both form a rigid body?
  4. wrobel

    I Mechanics problem: A Weight and a Mass Suspended from a String

    You need the torque equation with respect to the point O to the whole system and a lot of geometry.
  5. wrobel

    Random Photos

  6. wrobel

    I Questions about these Trigonometry Graphs involving sin() and cos()

    When you consider level sets ##\{(x,y)\mid f(x,y)=const\}## it is important to find critical points of the function ##f## and understand which kind these critical points are. So first find the points such that ##df=0##. It is like drawing a phase portrait of a Hamiltonian system with the...
  7. wrobel

    I Prove projection of a measurable set from product space is measurable

    I think you need a lemma from p.289 S Lang
  8. wrobel

    B Why is the set {(x,y)∈Ω×R|y=f(x)} a manifold?

    The open set ##\Omega\subset\mathbb{R}^m## with the standard coordinates is a coordinate patch in this graph, so the graph is a manifold
  9. wrobel

    Why is Hamilton's Principle assumed to be valid for non-holonomic systems?

    There are articles by Alexandre Karapetyan where he shows that the nonholonomic constraints can be considered as a limit case of some field of viscous friction forces. Alexandre Karapetyan Realization of nonholonomic constraints by viscouse friction and stability of rotation of Celtic stone"...
  10. wrobel

    Why is Hamilton's Principle assumed to be valid for non-holonomic systems?

    Exactly! You do not have a functional to differentiate. Speaking informally, what you write is an infinite dimensional differential form of ##\delta q## and this differential form can not be presented as a differential of the Action functional for the nonholonomic case. Nobody doubts the...
  11. wrobel

    Why is Hamilton's Principle assumed to be valid for non-holonomic systems?

    Let's drop the dependence on ##t## in the function ##L## and in the constraints. Can you deduce your formulas from such a definition: $$\delta S:=\frac{d}{d\varepsilon}\Big|_{\varepsilon=0}\int L(q(t,\varepsilon), q_t(t,\varepsilon))dt=0,\quad a_{ij}(q(t,\varepsilon))q_t^i(t,\varepsilon)=0,$$...
  12. wrobel

    Why is Hamilton's Principle assumed to be valid for non-holonomic systems?

    Detail it please. It is the core of the whole of our issues. I gave the definition in #9 now it is important that you explain what you mean.
  13. wrobel

    Why is Hamilton's Principle assumed to be valid for non-holonomic systems?

    May I ask a question first. vanhees71: Please give a definition of a stationary point of the functional ##S## in the nonholonomic case.
  14. wrobel

    Why is Hamilton's Principle assumed to be valid for non-holonomic systems?

    I am sure that d'Alembert completely agrees with the experiment. That is not the point.
  15. wrobel

    Why is Hamilton's Principle assumed to be valid for non-holonomic systems?

    We have different views on this theory, so I prefer not to start the discussion again, but merely provide the topic starter with references and proofs. Let him decide by himself.
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