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Titlebook: Cryogenic Process Engineering; Klaus D. Timmerhaus,Thomas M. Flynn Book 1989 Springer Science+Business Media New York 1989 cryogenics.desi

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发表于 2025-3-21 17:53:20 | 显示全部楼层 |阅读模式
书目名称Cryogenic Process Engineering
编辑Klaus D. Timmerhaus,Thomas M. Flynn
视频video
丛书名称International Cryogenics Monograph Series
图书封面Titlebook: Cryogenic Process Engineering;  Klaus D. Timmerhaus,Thomas M. Flynn Book 1989 Springer Science+Business Media New York 1989 cryogenics.desi
描述Cryogenics, a term commonly used to refer to very low temperatures, had its beginning in the latter half of the last century when man learned, for the first time, how to cool objects to a temperature lower than had ever existed na tu rally on the face of the earth. The air we breathe was first liquefied in 1883 by a Polish scientist named Olszewski. Ten years later he and a British scientist, Sir James Dewar, liquefied hydrogen. Helium, the last of the so-caBed permanent gases, was finally liquefied by the Dutch physicist Kamerlingh Onnes in 1908. Thus, by the beginning of the twentieth century the door had been opened to astrange new world of experimentation in which aB substances, except liquid helium, are solids and where the absolute temperature is only a few microdegrees away. However, the point on the temperature scale at which refrigeration in the ordinary sense of the term ends and cryogenics begins has ne ver been weB defined. Most workers in the field have chosen to restrict cryogenics to a tem­ perature range below -150°C (123 K). This is a reasonable dividing line since the normal boiling points of the more permanent gases, such as helium, hydrogen, neon, nitrogen, oxyg
出版日期Book 1989
关键词cryogenics; design; development; engine; hydrogen; liquid; process engineering; solid; temperature
版次1
doihttps://doi.org/10.1007/978-1-4684-8756-5
isbn_softcover978-1-4684-8758-9
isbn_ebook978-1-4684-8756-5Series ISSN 0538-7051 Series E-ISSN 2199-3084
issn_series 0538-7051
copyrightSpringer Science+Business Media New York 1989
The information of publication is updating

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发表于 2025-3-21 20:51:07 | 显示全部楼层
Book 1989nd cryogenics begins has ne ver been weB defined. Most workers in the field have chosen to restrict cryogenics to a tem­ perature range below -150°C (123 K). This is a reasonable dividing line since the normal boiling points of the more permanent gases, such as helium, hydrogen, neon, nitrogen, oxyg
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Properties of Cryogenic Fluids,f the “oxygen range” or the “hydrogen range.” Table 2.1 gives the normal (0.101 MPa or 1 atm) boiling temperature, the normal melting temperature, the critical temperature and pressure, and the normal latent heat of vaporization for these five cryogenic fluids and several other common cyrogens. Some
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Properties of Solids,f materials for the construction of cryogenic equipment will be dictated by consideration of mechanical and physical properties such as thermal conductivity (heat transfer along a structural member), thermal expansivity (expansion and contraction during cycling between ambient and low temperatures),
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Equipment Associated with Low-Temperature Systems,ring the influence of heat exchanger effectiveness on the liquid yield for a simple Joule-Thomson liquefaction process. For example, if the working fluid is nitrogen and the lower and upper pressure limits are 0.101 and 20.2 MPa, respectively, the liquid yield under these conditions will be zero for
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Separation and Purification Systems,the major source of commercial oxygen, nitrogen, neon, argon, krytpon, anxenon. The bulk of the commercial helium is currently obtained from helium-bearing natural gas where the separation is effected by a low-temperature process. The low-boiling components of natural gas, such as methane, ethane, a
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