Book contents
- Frontmatter
- PRELIMINARY DISSERTATION
- PHYSICAL ASTRONOMY
- BOOK I
- CHAPTER I DEFINITIONS, AXIOMS, &c
- CHAPTER II VARIABLE MOTION
- CHAPTER III ON THE EQUILIBRIUM OF A SYSTEM OF BODIES
- CHAPTER IV MOTION OF A SYSTEM OF BODIES
- CHAPTER V THE MOTION OF A SOLID BODY OF ANY FORM WHATEVER
- CHAPTER VI ON THE EQUILIBRIUM OF FLUIDS
- CHAPTER VII MOTION OF FLUIDS
- BOOK II
- BOOK III
- BOOK IV
- Index
- Errata
CHAPTER V - THE MOTION OF A SOLID BODY OF ANY FORM WHATEVER
Published online by Cambridge University Press: 29 August 2010
- Frontmatter
- PRELIMINARY DISSERTATION
- PHYSICAL ASTRONOMY
- BOOK I
- CHAPTER I DEFINITIONS, AXIOMS, &c
- CHAPTER II VARIABLE MOTION
- CHAPTER III ON THE EQUILIBRIUM OF A SYSTEM OF BODIES
- CHAPTER IV MOTION OF A SYSTEM OF BODIES
- CHAPTER V THE MOTION OF A SOLID BODY OF ANY FORM WHATEVER
- CHAPTER VI ON THE EQUILIBRIUM OF FLUIDS
- CHAPTER VII MOTION OF FLUIDS
- BOOK II
- BOOK III
- BOOK IV
- Index
- Errata
Summary
169. If a solid body receives an impulse in a direction passing through its centre of gravity, all its parts will move with an equal velocity; but if the direction of the impulse passes on one side of that centre, the different parts of the body will have unequal velocities, and from this inequality results a motion of rotation in the body round its centre of gravity, at the same time that the centre is moved forward, or translated with the same velocity it would have taken, had the impulse passed through it. Thus the double motions of rotation and translation are produced by one impulse.
170. If a body rotates about its centre of gravity, or about an axis, and is at the same time carried forward in space ; and if an equal and contrary impulse be given to the centre of gravity, so as to stop its progressive motion, the rotation will go on as before it received the impulse.
171. If a body revolves about a fixed axis, each of its particles will describe a circle, whose plane is perpendicular to that axis, and its radius is the distance of the particle from the axis. It is evident, that every point of the solid will describe an arc of the same number of degrees in the same time ; hence, if the velocity of each particle be divided by its radius or distance from the axis, the quotient will be the same for every particle of the body. This is called the angular velocity of the solid.
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- Mechanism of the Heavens , pp. 82 - 109Publisher: Cambridge University PressPrint publication year: 2009First published in: 1831