Abstract
1. It is well known that every shaft,
however nearly balanced
, when driven at a particular speed, bends, and, unless the amount of deflection be limited, might even break, although at higher speeds the shaft again runs true. The particular or “critical" speed depends on the manner in which the shaft is supported, its size and modulus of elasticity, and the size, weight, and position of any pulleys it carries. The theory for the case of an unloaded shaft first received attention at the hands of Professor Rankine, who obtained numerical formulae for the cases of an unloaded shaft resting freely on a bearing at each end, and for an overhanging shaft working in a shoulder at one end.
Cited by
66 articles.
订阅此论文施引文献
订阅此论文施引文献,注册后可以免费订阅5篇论文的施引文献,订阅后可以查看论文全部施引文献