描述
开 本: 大16开纸 张: 胶版纸包 装: 精装是否套装: 否国际标准书号ISBN: 9787040369441丛书名: 非线性物理科学
《非线性物理科学：微分方程群性质理论讲义》提供了确定和利用微分方程对称性的李群方法简明和清晰的介绍，并提供了在气体动力学和其他非线性模型中的大量应用，以及《非线性物理科学：微分方程群性质理论讲义》作者在这个经典领域的卓越贡献。《非线性物理科学：微分方程群性质理论讲义》中还包含在其他现代书籍中不曾涉及的一些非常有刚的材料，例如：Ovsyannikow教授发展的部分不变解理论，该理论提供了求解非线性微分方程和研究复杂数学模型强有力的工具。
Editor’s preface
Preface
1 One-parameter continuous transformation groups admitted by
differential equations
1.1 One-parameter continuous transformation group
1.1.1 Definition
1.1.2 Canonical parameter
1.1.3 Examples
1.1.4 Auxiliary functions of groups
1.2 Infinitesimal operator of the group
1.2.1 Definition and examples
1.2.2 Transformation of functions
1.2.3 Change of coordinates
1.3 Invariants and invariant manifolds
1.3.1 Invariants
1.3.2 Invariant manifolds
1.3.3 Invariance of regularly defined manifolds
1.4 Theory of prolongation
1.4.1 Prolongation of the space
1.4.2 Prolonged group
1.4.3 First prolongation of the group operator
1.4.4 Second prolongation of the group operator
1.4.5 Properties of prolongations of operators
1.5 Groups admitted by differentialequations
1.5.1 Determining equations
1.5.2 First-order ordinary differential equations
1.5.3 Second-orderordinarydifferentialequations
1.5.4 Heat equation
1.5.5 Gasdynamic equations
1.6 Lie algebra of operators
1.6.1 Commutator. Definition of a Lie algebra
1.6.2 Properties of commutator
1.6.3 Lie algebra of admitted operators
2 Lie algebras and local Lie groups
2.1 Lie algebra
2.1.1 Definition and examples
2.1.2 Subalgebra and ideal
2.1.3 Structure of finite-dimensionalLie algebras
2.2 Adjoint algebra
2.2.1 Inner derivation
2.2.2Adjoint algebra
2.2.3 Inner automorphisms of a Lie algebra.
2.3 Local Lie group
2.3.1 Coordinates in a group
2.3.2 Subgroups
2.3.3 Canonical coordinates of the first kind
2.3.4 First fundamental theorem of Lie
2.3.5 Second fundamental theorem of Lie
2.3.6 Properties ofcanonicalcoordinate systems of the first
kind
2.3.7 Third fundamental theorem of Lie
2.3.8 Lie algebra of a local Lie group
2.4 Subgroup, normal subgroup and factor group
2.4.1 Lemma on commutator
2.4.2 Subgroup
2.4.2 Subgroup
2.4.3 Normal subgroup
2.4.4 Factor grop
2.5 Inner automorphisms of a group and of its Lie algebra
2.5.1 Inner automorphism.
2.5.2 Lie algebra of GA and adjoint algebra of Lr
2.6 Local Lie group of transformations
2.6.1 Introduction
2.6.2 Lie’s first theorem.
2.6.3 Lie’s second theorem
2.6.4 Canonical coordinates of the second kind
3 Group invariant solutions of differential equations
3.1 Invariants of the group GNr
3.1.1 Invariance criterion
3.1.2 Functional independence
3.1.3 Linearly unconnected operators
3.1.4 Integration of jacobian systems
3.1.5 Computation ofinvariance
……
The theory of differential equations has two aspects of
investigation，namely local and global，no matter whether the
equations arise from applied problems of physics and mechanics or
from abstract speculations （which is rather frequent in modern
mathematics）.The local aspect is characterized by dealing with the
inner structure of a family of solutions and its investigation in a
neighborhood of a certain point.The global approach deals with
solutions definedin some domain and having a given behavior on its
boundary.
It would certainly be erroneous to oppose these directions to
each other.However，it is no good to ignore the differences in
approaches either.While the global approach necessitates the
functional analytic apparatus，the local viewpoint allows one to get
along with algebraic means only.A brilliant example of a profound
local consideration is the famous Cauchy-Kovalevskaya theorem which
is，in fact，an algebraic statement.Moreover，it is an easy matter to
notice that the theory of boundary value problems also makes an
essential application of various algebraic properties of the whole
family of solutions. Therefore，the local aspect of the algebraic
theory of differential equations is quite vital.
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