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The 'two century plus' history of the constant-tension catenary as applied to tall ship sails, paravane and other tows, oil slick catch booms and some buoy moors

机译:恒张力悬链的“两世纪以来”历史,适用于高大的船帆,滑翔伞和其他拖曳物,浮油捕获吊杆和一些浮标

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The best known catenary, caused by gravity acting on a flexible rope, with tension varying and proportional to height above the directix, has been well chronicled historically for three centuries. This has not been the case for the "other" catenary (of constant unvarying tension) of equal oceanic importance, created because of the cross-flow square law when a neutrally-buoyant rope is in a uniform current; even worse, the synthetic history, obtained by tracing back thru referenced sources in the literature, is distorted, omissive and abbreviated. The constant-tension catenary was not first discovered by the aerodynamist Glauert in 1934 as referenced by Pode and many other authors in the nineteen thirties and nineteen forties. Rather it was discovered more than two centuries ago, probably by Leonard Euler, as a mathematical model for the large rectangular sails of tall ships. The simple mathematical relationship between the two catenaries is given.
机译:众所周知,由于重力作用在一根柔性绳索上而引起的悬链线,其张力随方向变化且与高度成正比,因此已经被记录了三个世纪。对于具有同等海洋重要性的(恒定不变的张力)悬链线而言,情况并非如此,这是由于当中性浮力的绳索处于均匀流中时的横流平方定律而产生的。甚至更糟的是,通过追溯文献中的参考资料获得的综合历史被歪曲,遗忘和缩写。恒定张力悬链线并非是波德和其他许多作者在19世纪30年代和40年代引用的1934年航空动力学家格劳特(Glauert)首次发现的。相反,它是在两个多世纪前被伦纳德·欧拉(Leonard Euler)发现的,它是高大船的大型矩形帆的数学模型。给出了两个接触网之间的简单数学关系。

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