Geometric integration: numerical solution of differential equations on manifolds

Since their introduction by Sir Isaac Newton, di erential equations have played a decisive role in the mathematical study of natural phenomena. An important and widely acknowledged lesson of the last three centuries is that critical information about the qualitative nature of solutions of di erentia...

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Published inPhilosophical transactions of the Royal Society of London. Series A: Mathematical, physical, and engineering sciences Vol. 357; no. 1754; pp. 945 - 956
Main Authors Budd, C.J., Iserles, A.
Format Journal Article
LanguageEnglish
Published The Royal Society 15.04.1999
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Summary:Since their introduction by Sir Isaac Newton, di erential equations have played a decisive role in the mathematical study of natural phenomena. An important and widely acknowledged lesson of the last three centuries is that critical information about the qualitative nature of solutions of di erential equations can be determined by studying their geometry. Perhaps the most important example of this approach was the formulation of the laws of mechanics by Alexander Rowan Hamilton, which allowed deep geometric tools to be used in understanding the dynamics of complex systems such as rigid bodies and the Solar System. Conserved quantities of a Hamiltonian system, such as energy, linear and angular momentum, could be understood in terms of the symmetries of the underlying Hamiltonian function, its ergodic properties determined from the underlying symplectic nature of the formulation and constraints on the system could be incorporated in a natural manner. The Hamiltonian geometric formulation of many other problems in science modelled by ordinary and partial di erential equations, such as ocean dynamics, nonlinear optics and elastic deformations, continues to play a vital role in our qualitative understanding of these systems. An equally important geometric approach to the study of di erential equations is the application of symmetry-based methods pioneered by Sophus Lie. Exploiting underlying symmetries of a partial or ordinary di erential equation, it can be often greatly simpli ed and sometimes solved altogether in closed form. Such methods, which lie at the heart of the construction of self-similar solutions of di erential equations and the symmetry reduction of complex systems, have become increasingly popular with the development of symbolic algebra packages. It is no coincidence that the most important equations of mathematical physics are precisely those for which geometric and symmetry-based methods are most e ective. Arguably, these equations are really a shorthand for the deep underlying symmetries in nature that they encapsulate.
Bibliography:istex:883A0161361D622281B56F57277AD0F46934C41C
ark:/67375/V84-CMNFGP8M-1
Theme Issue 'Geometric integration: numerical solution of differential equations on manifolds' compiled by C. J. Budd and A. Iserles
ISSN:1364-503X
1471-2962
DOI:10.1098/rsta.1999.0360