Differentiability And Fractality In Dynamics Of Physical Systems
eBook - ePub

Differentiability And Fractality In Dynamics Of Physical Systems

  1. 300 pages
  2. English
  3. ePUB (mobile friendly)
  4. Available on iOS & Android
eBook - ePub

Differentiability And Fractality In Dynamics Of Physical Systems

About this book

Using Cartan's differential 1-forms theory, and assuming that the motion variables depend on Euclidean invariants, certain dynamics of the material point and systems of material points are developed. Within such a frame, the Newtonian force as mass inertial interaction at the intragalactic scale, and the Hubble-type repulsive interaction at intergalactic distances, are developed.

The wave-corpuscle duality implies movements on curves of constant informational energy, which implies both quantizations and dynamics of velocity limits.

Analysis of motion of a charged particle in a combined field which is electromagnetic and with constant magnetism implies fractal trajectories. Mechanics of material points in a fractalic space is constructed, and various applications — fractal atom, potential well, free particle, etc. — are discussed.

Contents:

  • Principles of Motion in Invariantive Mechanics
  • Inertial Invariantive Motion of the Material Point
  • Field Invariantive Theories
  • Ondulatory Invariantive Theories. Wave-Corpuscule Duality
  • Invariantive Mechanics of Systems of Material Points
  • The Photon in Invariantive Ondulatory Theories
  • Lagrangian Approach in Invariantive Mechanics
  • Considerations on Invariantive Mechanics
  • Invariantive Mechanics of Rigid Body
  • Covariant Formulation of Conservation Laws in Invariantive Mechanics
  • Invariantive Mechanics and Informational Energy
  • Chaos Via Fractality in Gravitational Dynamical Systems
  • Fractality at Small Scale. Fractal Model of the Atom
  • Extended Fractal Hydrodynamic Model with an Arbitrary Fractal Dimension and Its Implications
  • Theory of Fractional Scale Relativity and Some Applications


Readership: Master, PhD students and professional researchers in the field of physics.
Key Features:

  • Theory of 1-forms is applied to dynamics of material points systems
  • Non-differentiability as a possible property of complex systems
  • The role played by informational energy in the definition of the constants of motion is discussed

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Information

Publisher
WSPC
Year
2015
eBook ISBN
9789814678407

Chapter 1

Principles of Motion in Invariantive Mechanics

1.1.The Euler-Lagrange and Hamilton’s equations obtained by means of exterior forms

Let
figure
be a function of class C2, called Lagrangian, where q ≡ (q1, q2, …, qn) are the generalized coordinates,
figure
are the generalized velocities, and t is the time. Let also S be the action, defined by the exterior 1-form
figure
Theorem 1.1. The total derivative of the action with respect to time yields the Hamilton-Jacobi equation [1]
figure
Indeed, if the functional dependence
figure
as well as the definition of generalized momenta
figure
are accepted, the total derivative of S with respect to time is
figure
(N.B. Here and hereafter, the summation symbol and the summation indices shall be omitted).
Since, according to (1.3)
figure
relations (1.7) and (1.8) lead to (1.4), where the Hamiltonian H is defined as
figure
Theorem 1.2. Closeness of the 1-form (1.3)
figure
reduces to Euler-Lagrange equations [1]
figure
and the integral of motion [1]
figure
Written explicitly, relation (1.10) becomes
figure
According to (1.1), we can write
figure
On the other hand, operators d and δ commute, so that
figure
Equation (1.3) can then be written as
figure
Using the Hamiltonian defined by (1.9) and the fact that variations δq and δt are arbitrary, equation (1.16) yields (1.11) and (1.12). If, in particular, L does not explicitly depend on time, then (1.12) reduces to the energy conservation law
figure
As one can see, the 1-form (1.3) can also be written as
figure
where the generalized momentum p is defined by
figure
Theorem 1.3. Closeness of the 1-form (1.18)
figure
reduces to Hamilton’s canonical equations [1]
figure
together with the integral of motion [1]
figure
Explicitating (1.20), we have
figure
Since H = H(p, q, t), one can write
figure
and (1.23), after some simple manipulation, becomes
figure
Equating to zero the coefficients of variations δq, δp, and δt, equations (1.21) and (1.22) follow immediately. In particular, if H does not explicitly depend on time, (1.22) reduces to the energy conservation law (1.17).

1.2.The Cartan motion principle

The previous results allow us to operate with both Lagrange function L and Hamilton’s function H. This means that, as long as the canonical...

Table of contents

  1. Cover Page
  2. Title
  3. Copyright
  4. Dedication
  5. Preface
  6. Contents
  7. 1. Principles of Motion in Invariantive Mechanics
  8. 2. Inertial Invariantive Motion of the Material Point
  9. 3. Field Invariantive Theories
  10. 4. Ondulatory Invariantive Theories. Wave-Corpuscule Duality
  11. 5. Invariantive Mechanics of Systems of Material Points
  12. 6. The Photon in Invariantive Ondulatory Theories
  13. 7. Lagrangian Approach in Invariantive Mechanics
  14. 8. Considerations on Invariantive Mechanics
  15. 9. Invariantive Mechanics of Rigid Body
  16. 10. Covariant Formulation of Conservation Laws in Invariantive Mechanics
  17. 11. Invariantive Mechanics and Informational Energy
  18. 12. Chaos Via Fractality in Gravitational Dynamical Systems
  19. 13. Fractality at Small Scale. Fractal Model of the Atom
  20. 14. Extended Fractal Hydrodynamic Model with an Arbitrary Fractal Dimension and its Implications
  21. 15. Theory of Fractional Scale Relativity and Some Applications
  22. Index

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