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Contour Dynamics with Symplectic Time Integration

โœ Scribed by P.W.C. Vosbeek; R.M.M. Mattheij


Book ID
102586649
Publisher
Elsevier Science
Year
1997
Tongue
English
Weight
498 KB
Volume
133
Category
Article
ISSN
0021-9991

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โœฆ Synopsis


Here u is the component of the velocity field in the x-direction and v the component in the y-direction. From

In this paper we consider the time evolution of vortices simulated by the method of contour dynamics. Special attention is being paid this we can see that we are dealing with a Hamiltonian to the Hamiltonian character of the governing equations and in system with Hamiltonian ฯช. A very important property particular to the conservational properties of numerical time integraof such a system is the concept of preservation of area (see tion for them. We assess symplectic and nonsymplectic schemes. [10]) which in our case is equivalent to conservation of For the former methods, we give an implementation which is both mass. Operators which have this property, are called symefficient and yet effectively explicit. A number of numerical examplectic. The solution operator of a Hamiltonian system is ples sustain the analysis and demonstrate the usefulness of the approach. แฎŠ 1997 Academic Press thus a symplectic operator. Since we like to solve this Hamiltonian system numerically, it is important, especially for long-time calculations, to preserve the area. This is


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the numerical solutions have a property of area preserving, -the discretization error in the energy integral does not have a secular term, which means that the accumulated truncation errors in angle variables increase linearly with the time instead of quadratic growth, -the symplectic integrators ca