Hamiltonian form of general averaged systems

1992 ◽  
Vol 3 (1) ◽  
pp. 115-123
Author(s):  
Yu. G. Pavlenko ◽  
S. I. Zelenskii
Author(s):  
Nathalie Deruelle ◽  
Jean-Philippe Uzan

This chapter covers the equations governing the evolution of particle distribution and relates the macroscopic thermodynamical quantities to the distribution function. The motion of N particles is governed by 6N equations of motion of first order in time, written in either Hamiltonian form or in terms of Poisson brackets. Thus, as this chapter shows, as the number of particles grows it becomes necessary to resort to a statistical description. The chapter first introduces the Liouville equation, which states the conservation of the probability density, before turning to the Boltzmann–Vlasov equation. Finally, it discusses the Jeans equations, which are the equations obtained by taking various averages over velocities.


2018 ◽  
Vol 28 (10) ◽  
pp. 101102 ◽  
Author(s):  
Volker Mehrmann ◽  
Riccardo Morandin ◽  
Simona Olmi ◽  
Eckehard Schöll

Author(s):  
Xuncheng Huang ◽  
Guizhang Tu

The Hamiltonian equation provides us an alternate description of the basic physical laws of motion, which is used to be described by Newton's law. The research on Hamiltonian integrable systems is one of the most important topics in the theory of solitons. This article proposes a new hierarchy of integrable systems of1+2dimensions with its Hamiltonian form by following the residue approach of Fokas and Tu. The new hierarchy of integrable system is of fundamental interest in studying the Hamiltonian systems.


1990 ◽  
Vol 68 (9) ◽  
pp. 719-722 ◽  
Author(s):  
Hubert H. Shen

The evolution of the vorticity in time for 2D inviscid flow and in Lagrangian time for 3D viscous flow is written in Hamiltonian form by introducing Bose operators. The addition of the viscous and convective terms, respectively, leads to an interpretation of the Hamiltonian contribution to the evolution as Langevin noise.


Author(s):  
T. M. Cherry

Letbe a system of differential equations of Hamiltonian form, the characteristic function H being independent of t and expansible in a convergent series of powers of x1, … xn, y1, … yn in which the terms of lowest degree are


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