eBook ISBN:  9781470404390 
Product Code:  MEMO/178/838.E 
List Price:  $70.00 
MAA Member Price:  $63.00 
AMS Member Price:  $42.00 
eBook ISBN:  9781470404390 
Product Code:  MEMO/178/838.E 
List Price:  $70.00 
MAA Member Price:  $63.00 
AMS Member Price:  $42.00 

Book DetailsMemoirs of the American Mathematical SocietyVolume: 178; 2005; 133 ppMSC: Primary 51; 53; 70
This paper is a study of the elastic problems on simply connected manifolds \(M_n\) whose orthonormal frame bundle is a Lie group \(G\). Such manifolds, called the space forms in the literature on differential geometry, are classified and consist of the Euclidean spaces \(\mathbb{E}^n\), the hyperboloids \(\mathbb{H}^n\), and the spheres \(S^n\), with the corresponding orthonormal frame bundles equal to the Euclidean group of motions \(\mathbb{E}^n\rtimes SO_n(\mathbb{R})\), the rotation group \(SO_{n+1}(\mathbb{R})\), and the Lorentz group \(SO(1,n)\).
The manifolds \(M_n\) are treated as the symmetric spaces \(G/K\) with \(K\) isomorphic with \(SO_n(R)\). Then the Lie algebra \(\mathfrak{g}\) of \(G\) admits a Cartan decomposition \(\mathfrak{g}=\mathfrak{p}+\mathfrak{k}\) with \(\mathfrak{k}\) equal to the Lie algebra of \(K\) and \(\mathfrak{p}\) equal to the orthogonal comlement \(\mathfrak{k}\) relative to the trace form. The elastic problems on \(G/K\) concern the solutions \(g(t)\) of a left invariant differential systems on \(G\) \[\frac{dg}{dt}(t)=g(t)(A_0+U(t)))\] that minimize the expression \(\frac{1}{2}\int_0^T (U(t),U(t))\,dt\) subject to the given boundary conditions \(g(0)=g_0\), \(g(T)=g_1\), over all locally bounded and measurable \(\mathfrak{k}\) valued curves \(U(t)\) relative to a positive definite quadratic form \((\, , \,)\) where \(A_0\) is a fixed matrix in \(\mathfrak{p}\).
These variational problems fall in two classes, the EulerGriffiths problems and the problems of Kirchhoff. The EulerGriffiths elastic problems consist of minimizing the integral \[\tfrac{1}{2}\int_0^T\kappa^2(s)\,ds\] with \(\kappa (t)\) equal to the geodesic curvature of a curve \(x(t)\) in the base manifold \(M_n\) with \(T\) equal to the Riemannian length of \(x\). The curves \(x(t)\) in this variational problem are subject to certain initial and terminal boundary conditions. The elastic problems of Kirchhoff is more general than the problems of EulerGriffiths in the sense that the quadratic form \((\, , \,)\) that defines the functional to be minimized may be independent of the geometric invariants of the projected curves in the base manifold. It is only on two dimensional manifolds that these two problems coincide in which case the solutions curves can be viewed as the nonEuclidean versions of L. Euler elasticae introduced in 174.
Each elastic problem defines the appropriate leftinvariant Hamiltonian \(\mathcal{H}\) on the dual \(\mathfrak{g}^*\) of the Lie algebra of \(G\) through the Maximum Principle of optimal control. The integral curves of the corresponding Hamiltonian vector field \(\vec{\mathcal{H}}\) are called the extremal curves.
The paper is essentially concerned with the extremal curves of the Hamiltonian systems associated with the elastic problems. This class of Hamiltonian systems reveals a remarkable fact that the Hamiltonian systems traditionally associated with the movements of the top are invariant subsystems of the Hamiltonian systems associated with the elastic problems.
The paper is divided into two parts. The first part of the paper synthesizes ideas from optimal control theory, adapted to variational problems on the principal bundles of Riemannian spaces, and the symplectic geometry of the Lie algebra \(\mathfrak{g},\) of \(G\), or more precisely, the symplectic structure of the cotangent bundle \(T^*G\) of \(G\).
The second part of the paper is devoted to the solutions of the complexified Hamiltonian equations induced by the elastic problems. The paper contains a detailed discussion of the algebraic preliminaries leading up to \(so_n(\mathbb{C})\), a natural complex setting for the study of the left invariant Hamiltonians on real Lie groups \(G\) for which \(\mathfrak{g}\) is a real form for \(so_n(\mathbb{C})\). It is shown that the EulerGriffiths problem is completely integrable in any dimension with the solutions the holomorphic extensions of the ones obtained by earlier P. Griffiths. The solutions of the elastic problems of Kirchhoff are presented in complete generality on \(SO_3(\mathbb{C})\) and there is a classification of the integrable cases on \(so_4(\mathbb{C})\) based on the criteria of KowalewskiLyapunov in their study of the mechanical tops. Remarkably, the analysis yields essentially only two integrables cases analogous to the top of Lagrange and the top of Kowalewski. The paper ends with the solutions of the integrable complex Hamiltonian systems on the \(SL_2(\mathbb{C})\times SL_2(\mathbb{C})\), the universal cover of \(SO_4(\mathbb{C})\).
ReadershipGraduate students and research mathematicians interested in differential equations.

Table of Contents

Chapters

1. Introduction

2. Cartan decomposition and the generalized elastic problems

3. The maximum principle and the Hamiltonians

4. The leftinvariant symplectic form

5. Symmetries and the conservation laws

6. Complexified elastic problems

7. Complex elasticae of Euler and its $n$dimensional extensions

8. Cartan algebras, root spaces and extra integrals of motion

9. Elastic curves for the case of Lagrange

10. Elastic curves for the case of Kowalewski


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This paper is a study of the elastic problems on simply connected manifolds \(M_n\) whose orthonormal frame bundle is a Lie group \(G\). Such manifolds, called the space forms in the literature on differential geometry, are classified and consist of the Euclidean spaces \(\mathbb{E}^n\), the hyperboloids \(\mathbb{H}^n\), and the spheres \(S^n\), with the corresponding orthonormal frame bundles equal to the Euclidean group of motions \(\mathbb{E}^n\rtimes SO_n(\mathbb{R})\), the rotation group \(SO_{n+1}(\mathbb{R})\), and the Lorentz group \(SO(1,n)\).
The manifolds \(M_n\) are treated as the symmetric spaces \(G/K\) with \(K\) isomorphic with \(SO_n(R)\). Then the Lie algebra \(\mathfrak{g}\) of \(G\) admits a Cartan decomposition \(\mathfrak{g}=\mathfrak{p}+\mathfrak{k}\) with \(\mathfrak{k}\) equal to the Lie algebra of \(K\) and \(\mathfrak{p}\) equal to the orthogonal comlement \(\mathfrak{k}\) relative to the trace form. The elastic problems on \(G/K\) concern the solutions \(g(t)\) of a left invariant differential systems on \(G\) \[\frac{dg}{dt}(t)=g(t)(A_0+U(t)))\] that minimize the expression \(\frac{1}{2}\int_0^T (U(t),U(t))\,dt\) subject to the given boundary conditions \(g(0)=g_0\), \(g(T)=g_1\), over all locally bounded and measurable \(\mathfrak{k}\) valued curves \(U(t)\) relative to a positive definite quadratic form \((\, , \,)\) where \(A_0\) is a fixed matrix in \(\mathfrak{p}\).
These variational problems fall in two classes, the EulerGriffiths problems and the problems of Kirchhoff. The EulerGriffiths elastic problems consist of minimizing the integral \[\tfrac{1}{2}\int_0^T\kappa^2(s)\,ds\] with \(\kappa (t)\) equal to the geodesic curvature of a curve \(x(t)\) in the base manifold \(M_n\) with \(T\) equal to the Riemannian length of \(x\). The curves \(x(t)\) in this variational problem are subject to certain initial and terminal boundary conditions. The elastic problems of Kirchhoff is more general than the problems of EulerGriffiths in the sense that the quadratic form \((\, , \,)\) that defines the functional to be minimized may be independent of the geometric invariants of the projected curves in the base manifold. It is only on two dimensional manifolds that these two problems coincide in which case the solutions curves can be viewed as the nonEuclidean versions of L. Euler elasticae introduced in 174.
Each elastic problem defines the appropriate leftinvariant Hamiltonian \(\mathcal{H}\) on the dual \(\mathfrak{g}^*\) of the Lie algebra of \(G\) through the Maximum Principle of optimal control. The integral curves of the corresponding Hamiltonian vector field \(\vec{\mathcal{H}}\) are called the extremal curves.
The paper is essentially concerned with the extremal curves of the Hamiltonian systems associated with the elastic problems. This class of Hamiltonian systems reveals a remarkable fact that the Hamiltonian systems traditionally associated with the movements of the top are invariant subsystems of the Hamiltonian systems associated with the elastic problems.
The paper is divided into two parts. The first part of the paper synthesizes ideas from optimal control theory, adapted to variational problems on the principal bundles of Riemannian spaces, and the symplectic geometry of the Lie algebra \(\mathfrak{g},\) of \(G\), or more precisely, the symplectic structure of the cotangent bundle \(T^*G\) of \(G\).
The second part of the paper is devoted to the solutions of the complexified Hamiltonian equations induced by the elastic problems. The paper contains a detailed discussion of the algebraic preliminaries leading up to \(so_n(\mathbb{C})\), a natural complex setting for the study of the left invariant Hamiltonians on real Lie groups \(G\) for which \(\mathfrak{g}\) is a real form for \(so_n(\mathbb{C})\). It is shown that the EulerGriffiths problem is completely integrable in any dimension with the solutions the holomorphic extensions of the ones obtained by earlier P. Griffiths. The solutions of the elastic problems of Kirchhoff are presented in complete generality on \(SO_3(\mathbb{C})\) and there is a classification of the integrable cases on \(so_4(\mathbb{C})\) based on the criteria of KowalewskiLyapunov in their study of the mechanical tops. Remarkably, the analysis yields essentially only two integrables cases analogous to the top of Lagrange and the top of Kowalewski. The paper ends with the solutions of the integrable complex Hamiltonian systems on the \(SL_2(\mathbb{C})\times SL_2(\mathbb{C})\), the universal cover of \(SO_4(\mathbb{C})\).
Graduate students and research mathematicians interested in differential equations.

Chapters

1. Introduction

2. Cartan decomposition and the generalized elastic problems

3. The maximum principle and the Hamiltonians

4. The leftinvariant symplectic form

5. Symmetries and the conservation laws

6. Complexified elastic problems

7. Complex elasticae of Euler and its $n$dimensional extensions

8. Cartan algebras, root spaces and extra integrals of motion

9. Elastic curves for the case of Lagrange

10. Elastic curves for the case of Kowalewski