Volume 183001

Mechanics / By Henry Kater and Dionysius Lardner.

  • Henry Kater
Date:
1830
Catalogue details

Licence: Public Domain Mark

Credit: Mechanics / By Henry Kater and Dionysius Lardner. Source: Wellcome Collection.

    155/408 page 129
    earth and planets, or that of a common spinning-top, are examples of this. The cases, however, which will be considered in the present chapter, are chiefly those in which the axis is immovable, or at least where its motion has no relation to the phenomena under investigation. Instances of this are so frequent and obvious, that it seems scarcely necessary to particularise them. Wheel- work of every description, the moving parts of watches and clocks, turning lathes, mill-work, doors and lids on hinges, are all obvious examples. In tools or other in- struments which work on joints or pivots, such as scissors, shears, pincers, although the joint or pivot be not abso- lutely fixed, it is to be considered so in reference to the mechanical effect. In some cases, as in most of the wheels of watches and clocks, fly-wheels and chucks of the turning lathe, and the arms of wind-mills, the body turns continually in the same direction, and each of its points traverses a complete circle during every revolution of the body round its axis. In other instances the motion is alternate or recipro- cating, its direction being at intervals reversed. Such is the case in pendulums of clocks, balance-wheels of chro- nometers, the treddle of the lathe, doors and lids on hinges, scissors, shears, pincers, &c. When the alter- nation is constant and regular, it is called oscillation or vibration, as in pendulums and balance-wheels. (181.) To explain the properties of an axis of rota- tion it will be necessary to consider the different kinds of forces to the action of which a body moveable on such an axis may be submitted, to show how this action depends on their several quantities and directions, to distinguish the cases in which the forces neutralise each other and mutually equilibrate from those in which motion ensues, to determine the effect which the axis suffers, and, in the cases where motion is produced, to estimate the effects of those centrifugal forces (13'7.) which are created by the mass of the body whirling round the axis. Forces in general have been distinguished by the dura- tion of their action into instantaneous and continued K
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