Book contents
- Frontmatter
- Contents
- Foreword by Sir William McCrea, FRS
- Preface to the fourth edition
- CHAPTER I KINEMATICAL PRELIMINARIES
- CHAPTER II THE EQUATIONS OF MOTION
- CHAPTER III PRINCIPLES AVAILABLE FOR THE INTEGRATION
- CHAPTER IV THE SOLUBLE PROBLEMS OF PARTICLE DYNAMICS
- CHAPTER V THE DYNAMICAL SPECIFICATION OF BODIES
- CHAPTER VI THE SOLUBLE PROBLEMS OF RIGID DYNAMICS
- CHAPTER VII THEORY OF VIBRATIONS
- CHAPTER VIII NON-HOLONOMIC SYSTEMS. DISSIPATIVE SYSTEMS
- CHAPTER IX THE PRINCIPLES OF LEAST ACTION AND LEAST CURVATURE
- CHAPTER X HAMILTONIAN SYSTEMS AND THEIR INTEGRAL-INVARIANTS
- CHAPTER XI THE TRANSFORMATION-THEORY OF DYNAMICS
- CHAPTER XII PROPERTIES OF THE INTEGRALS OF DYNAMICAL SYSTEMS
- CHAPTER XIII THE REDUCTION OF THE PROBLEM OF THREE BODIES
- CHAPTER XIV THE THEOREMS OF BRUNS AND POINCARÉ
- CHAPTER XV THE GENERAL THEORY OF ORBITS
- CHAPTER XVI INTEGRATION BY SERIES
- INDEX OF AUTHORS QUOTED
- INDEX OF TERMS EMPLOYED
CHAPTER I - KINEMATICAL PRELIMINARIES
Published online by Cambridge University Press: 05 August 2012
- Frontmatter
- Contents
- Foreword by Sir William McCrea, FRS
- Preface to the fourth edition
- CHAPTER I KINEMATICAL PRELIMINARIES
- CHAPTER II THE EQUATIONS OF MOTION
- CHAPTER III PRINCIPLES AVAILABLE FOR THE INTEGRATION
- CHAPTER IV THE SOLUBLE PROBLEMS OF PARTICLE DYNAMICS
- CHAPTER V THE DYNAMICAL SPECIFICATION OF BODIES
- CHAPTER VI THE SOLUBLE PROBLEMS OF RIGID DYNAMICS
- CHAPTER VII THEORY OF VIBRATIONS
- CHAPTER VIII NON-HOLONOMIC SYSTEMS. DISSIPATIVE SYSTEMS
- CHAPTER IX THE PRINCIPLES OF LEAST ACTION AND LEAST CURVATURE
- CHAPTER X HAMILTONIAN SYSTEMS AND THEIR INTEGRAL-INVARIANTS
- CHAPTER XI THE TRANSFORMATION-THEORY OF DYNAMICS
- CHAPTER XII PROPERTIES OF THE INTEGRALS OF DYNAMICAL SYSTEMS
- CHAPTER XIII THE REDUCTION OF THE PROBLEM OF THREE BODIES
- CHAPTER XIV THE THEOREMS OF BRUNS AND POINCARÉ
- CHAPTER XV THE GENERAL THEORY OF ORBITS
- CHAPTER XVI INTEGRATION BY SERIES
- INDEX OF AUTHORS QUOTED
- INDEX OF TERMS EMPLOYED
Summary
The displacements of rigid bodies.
The name Analytical Dynamics is given to that branch of knowledge in which the motions of material bodies, considered as due to the mutual interactions of the bodies, are discussed by the aid of mathematical analysis.
It is natural to begin this discussion by considering the various possible types of motion in themselves, leaving out of account for a time the causes to which the initiation of motion may be ascribed; this preliminary enquiry constitutes the science of Kinematics. The object of the present chapter is to establish a number of kinematical theorems which will be required in the rest of the work.
Kinematics is in itself an extensive subject, for a complete account of which the student is referred to treatises dealing exclusively with it, e.g. that of Koenigs (Paris, 1897). In what follows we shall confine our attention to theorems which are of utility in the applications of Kinematics to Dynamics.
We shall say that a material body is rigid when the mutual distance of every pair of specified points in it is invariable, so that the body does not expand or contract or change its shape in any way, although it may change its position with reference to surrounding objects.
If a rigid body is moved from one position to another, the change of position is called a displacement of the body.
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- Publisher: Cambridge University PressPrint publication year: 1988