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THE EFFECT OF CONVECTION ON DENDRITIC GROWTH UNDER MICROGRAVITY CONDITIONS

 

作者: M. B. KOSS,   L. T. BUSHNELL,   J. C. LACOMBE,   M. E. GLICKSMAN,  

 

期刊: Chemical Engineering Communications  (Taylor Available online 1996)
卷期: Volume 152-153, issue 1  

页码: 351-363

 

ISSN:0098-6445

 

年代: 1996

 

DOI:10.1080/00986449608936573

 

出版商: Taylor & Francis Group

 

关键词: Dendrite;Microgravity;Convection Ivantsov

 

数据来源: Taylor

 

摘要:

The Isothermal Dendritic Growth Experiment (IDGE) is an orbital space flight experiment, launched by NASA, in March, 1994, as part of the United States Microgravity Payload (USMP-2). The IDGE provided accurately measured dendritic growth rates, tip radii of curvature, and morphological observations of ultra-pure succinontrile obtained at supercoolings in the range 0.05-2.0 K. Data were received in the form of pairs of digitized binary images telemetered to the ground from orbit in near-real-time, and as 35mm photographic film received 3 months after the flight. The IDGE flight data has now been analyzed, permitting a comprehensive comparison between dendritic growth under terrestrial and microgravity conditions. The measured growth kinetics, in the form of velocity versus supercooling, is markedly different from those observed in terrestrial experiments. Above 0.4 K supercooling in microgravity, the process of dendritic growth is diffusion controlled, i.e., thermal conduction is the rate limiting process. Under terrestrial conditions, dendritic growth of SCN remains dominated by convective transport of heat until a supercooling of ca. 1.7 K is exceeded. Beyond a supercooling of 1.7 K, there is excellent agreement between terrestrial dendritic growth measurements, and a theory with one adjustable parameter determined form the microgravity measurements. Surprisingly, however, even under microgravity conditions, dendritic growth of SCN becomes dominated by convective transport at supercoolings of ca. 0.4 K and below. The observations confirm that convection, which depends as a sublinear power of the supercooling, will always dominate at low supercoolings, whereas diffusion, which depends on the superlinear power of the supercooling, will always dominate at high supercoolings.

 

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