William Ernest Dalby

Summary

William Ernest Dalby 1911 Encyclopædia Britannica (1911)

The problem involved in the design of a shaft is so to proportion the size that the stress produced by the torque shall not exceed a certain limit, or that the relative angular displacement of two sections at right angles to the axis of the shaft at a given distance apart shall not exceed a certain angle, the particular features of the problem determining which condition shall operate in fixing the size.
Source: Wikisource

William Ernest Dalby 1911 Encyclopædia Britannica (1911)

The assumption tacitly made hitherto that the torque T remains constant is rarely true in practice; it usually varies from instant to instant, often in a periodic manner, and an appropriate value of f must be taken to suit any particular case. Again it rarely happens that a shaft sustains a torque only. There is usually a bending moment associated with it. For a discussion of the proper values of f, to suit cases where the stress is variable, and the way a bending moment of known amount may be combined with a known torque, see Strength of Materials.
Source: Wikisource

William Ernest Dalby 1911 Encyclopædia Britannica (1911)

Assuming for the sake of simplicity that the whole of the power is absorbed by one machine, let T1 be the torque on the first motion shaft of the machine, and let wl be its angular velocity, then the rate at which the machine is absorbing energy is T1ω1 foot-pounds per second. A certain quantity of energy is absorbed by the transmitting mechanism itself for the purpose of overcoming frictional and other resistances, otherwise the rate of absorption of energy by the machine would exactly equal the rate at which it was produced by the prime mover assuming steady conditions of working.
Source: Wikisource

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