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ID:39211073
大小:807.38 KB
页数:55页
时间:2019-06-27
《【理想流体的哈密尔描述】hamilton description of ideal fluid》由会员上传分享,免费在线阅读,更多相关内容在学术论文-天天文库。
1、Hamiltoniandescriptionoftheideal¯uid*†P.J.MorrisonDepartmentofPhysicsandInstituteforFusionStudies,UniversityofTexas,Austin,Texas78712-1060TheHamiltonianviewpointof¯uidmechanicalsystemswithfewandin®nitenumberofdegreesoffreedomisdescribed.Rudimentaryconceptsof®nite-degree-of-freedomHamiltoniandynamics
2、arereviewed,inthecontextofthepassiveadvectionofascalarortracer®eldbya¯uid.Thenotionsofintegrability,invariant-tori,chaos,overlapcriteria,andinvariant-toribreakuparedescribedinthiscontext.Preparatorytotheintroductionof®eldtheories,systemswithanin®nitenumberofdegreesoffreedom,elementsoffunctionalcalcu
3、lusandactionprinciplesofmechanicsarereviewed.Theactionprinciplefortheidealcompressible¯uidisdescribedintermsofLagrangianormaterialvariables.Hamiltoniansystemsintermsofnoncanonicalvariablesarepresented,includingseveralexamplesofEulerianorinviscid¯uiddynamics.Liegrouptheorysuf®cientforthetreatmentofre
4、ductionisreviewed.ThereductionfromLagrangiantoEulerianvariablesistreatedalongwithClebschvariabledecompositions.StabilityinthecanonicalandnoncanonicalHamiltoniancontextsisdescribed.Suf®cientconditionsforstability,suchasRayleigh-likecriteria,areseentobeonlysuf®cientinthegeneralcasebecauseoftheexistenc
5、eofnegative-energymodes,whicharepossessedbyinteresting¯uidequilibria.Linearlystableequilibriawithnegativeenergymodesarearguedtobeunstablewhennonlinearityordissipationisadded.Theenergy-Casimirmethodisdiscussedandavariantofitthatdependsuponthenotionofdynamicalaccessibilityisdescribed.Theenergycontento
6、faperturbationaboutageneral¯uidequilibriumiscalculatedusingthreemethods.[S0034-6861(98)00102-0]CONTENTSV.TutorialonLieGroupsandAlgebras,Reduction,andClebschVariables491A.TutorialonLiegroupsandLiealgebras491I.Introduction4681.Liegroups492II.RudimentsofHamiltonianSystemswithFew2.Liealgebras493Degreeso
7、fFreedom,Illustratedby3.Realizationandrepresentation495PassiveAdvectioninTwo-DimensionalFluids469B.Reduction496A.Amodelfortwo-dimensional¯uidmotion4691.Reductionof®nite-dimensionalsystems496B.Passivea
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