Mechanics in Differential GeometryWalter de Gruyter, 20/03/2012 - 588 من الصفحات No detailed description available for "Mechanics in Differential Geometry". |
المحتوى
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3 TANGENT BUNDLE VECTOR FIELD AND LIE ALGEBRA | 59 |
4 COTANGENT BUNDLE AND COVECTOR FIELDS | 75 |
5 TENSOR ALGEBRA AND TENSOR FIEDS | 83 |
6 EXTERIOR DIFFERENTIAL FORMS | 94 |
2 SYMPLECTIC GEOMETRY | 258 |
CHAPTER 3 A MODERN EXPOSITION OF MECHANICS | 285 |
2 HAMILTONIAN MECHANICS | 306 |
3 COMPARISON OF THE LAGRANGIAN AND HAMILTONIAN FORMULATIONS | 334 |
4 HAMILTONJACOBI MECHANICS | 370 |
5 INTRODUCTION TO PERTURBATIONS | 409 |
EXERCISES | 460 |
CHAPTER 4 THE NBODY PROBLEM AN ORIGINAL METHOD FOR LARGE Ν | 481 |
7 LIE DERIVATIVE LIE GROUP AND LIE ALGEBRA | 122 |
8 INTEGRATION OF FORMS | 173 |
9 RIEMANNIAN GEOMETRY | 192 |
EXERCISES | 234 |
CHAPTER 2 SYMPLECTIC GEOMETRY | 253 |
2 THE NBODY PROBLEM IN STATISTICAL MECHANICS | 523 |
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GLOSSARY OF SYMBOLS | 557 |
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عبارات ومصطلحات مألوفة
basis canonical equations canonical transformation chart components configuration space constant coordinates corresponding covector deduce defined denoted diffeomorphism differentiable manifold differentiable mapping differential equations differential form dx² dx³ element expressed exterior differential Əqi F₁ form of degree function Given Hamilton Hamilton-Jacobi equation Hamiltonian Hamiltonian vector field integral curve integral invariant introduce Lagrange equations Lagrangian Let us consider Lie derivative linear matrix mechanics motion equations neighborhood obtained one-form one-parameter orbit p-form P₁ perturbated phase space Poisson bracket problem Proof pull-back recall respect Riemannian solution symplectic Talpaert tangent vector tensor field tensor of type theorem variables vector bundle vector field vector space velocity written X₁ zero ӘР др хо