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 VI - THE SOLUBLE PROBLEMS OF RIGID DYNAMICS
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 motion of systems with one degree of freedom: motion round a fixed axis, etc.
We now proceed to apply the principles which have been developed in the foregoing chapters in order to determine the motion of holonomic systems of rigid bodies in those cases which admit of solution by quadratures.
It is natural to consider first those systems which have only one degree of freedom. We have seen (§ 42) that such a system is immediately soluble by quadratures when it possesses an integral of energy: and this principle is sufficient for the integration in most cases. Sometimes, however (e.g. when we are dealing with systems in which one of the surfaces or curves of constraint is forced to move in a given manner), the problem as originally formulated does not possess an integral of energy, but can be reduced (e.g. by the theorem of § 29) to another problem for which the integral of energy holds; when this reduction has been performed, the problem can be integrated as before.
The following examples will illustrate the application of these principles.
(i) Motion of a rigid body round a fixed axis.
Consider the motion of a single rigid body which is free to turn about an axis, fixed in the body and in space. Let I be the moment of inertia of the body about the axis, so that its kinetic energy is ½Iθ2 where θ is the angle made by a moveable plane, passing through the axis and fixed in the body, with a plane passing through the axis and fixed in space. […]
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- Publisher: Cambridge University PressPrint publication year: 1988