Huang Geng, Su Zhengjun, Guan Liyou, et al. Observation and analysis of the aggregation growth among ice-snow crystals. J Appl Meteor Sci, 2007, 18(4): 561-567.
Citation: Huang Geng, Su Zhengjun, Guan Liyou, et al. Observation and analysis of the aggregation growth among ice-snow crystals. J Appl Meteor Sci, 2007, 18(4): 561-567.

Observation and Analysis of the Aggregation Growth Among Ice-snow Crystals

  • Received Date: 2006-03-03
  • Rev Recd Date: 2007-01-11
  • Publish Date: 2007-08-31
  • The process of the ice-snow crystal running together plays an important part in origination of precipitation. It is a focus in cloud physics research. It discusses the cloud and fog that happens in lab and field observations. Result shows that as the droplets coalesce and grow, there is a speed up process also in ice crystals growth, such as snowflake, snow-circular, graupel and hail that coalesce super-cooled droplets and aggregate among ice-snow crystals. Experiments show, in the lab the shapes are fixed basically in temperature of -3.5- -20 ℃. The aggregate among ice-snow crystals only happens in saturated or super-saturated water level vapor pressure in the lab. While in insaturation (no liquid droplets) it does not happen. In 1 m3 chamber their shapes are dendritic and stellar, and their aggregated mechanism is caught by branches appearing in -13- -17.℃ While in 96 m3 chamber the shapes are needle, columnar, dendritic and stellar, the mechanism is adhesion and adhering appearing in -5- -18 ℃. In field observations of natural cloud and fog, the mechanism of the ice-snow crystal running together is adhesion and adhering appearing in -3- -17 ℃, and their shapes are dendritic, stellar, sector, plate, tabular, needle, columnar and columnar bean.The 1 m3 chamber is 1.76 m high and 0.88 m wide, the experiment is made in-3.5- -20 17. The 96 m3 chamber is 14.8 m high, 3.0 m wide, the experiment is made in-5- -18 ℃. The temperature is measure by three Pt resistance thermometers with the difference of 0.1 ℃ to compare with standards one. The sample that burnt for Silver Iodide pyrotechnic is made by deposit method. A great deal ice crystal aggregates into each other appearing in -13- -17 ℃ in 1 m3 chamber when the sample is exposured for 1 minute. But for other temperatures of -3.5- -20 ℃ it does not. While in 96 m3 chamber the aggregation process happens among ice crystals. Their sizes are lager than 1 m3, because the ice crystals could be maintained for a few hours, and there exists torrent and the ice crystal could move with air in 96 m3 chamber. In field observation, the measurement is made by PMS, 2D-C, 2D-P on aircraft in cloud, and by electronic microscope and the samples making for deposit on ground. The shapes of snowflake aggregation vary in cloud in nature because they could exist long in cloud and exhibit convective and torrent features. The ice crystal could interact with them. Another field observation is made by artificial dispersing fog by liquid nitrogen, and samples are measured by electronic microscope for deposit on ground. The ice-snow crystals running into snowflakes by the mechanism of adhering in -3— -8 ℃, and their shapes are hollow columnar, columnar and needle.
  • Fig. 1  Ice cry stals in lab (a, b: aggregated with dendritic and stellar ones; c, d: seldomagg regated)

    Fig. 2  Ice and snow crystals after seeding (a, b: observed with the microscope; c, d: observed with eyes)

    Fig. 3  Snow crystals in natural snowfall

    (a, b: observed with the microscope, c, d: observed with camera)

    Table  1  Shapes of ice crystal and aggregation varied with air conditions in the cloud chamber

  • [1]
    王鹏飞, 李子华.微观云物理学.北京:气象出版社, 1989: 198-199; 311-326; 336.
    [2]
    Mason B J.云物理学∥中国科学院大气物理研究所, 译.北京:科学出版社, 1978: 264-271.
    [3]
    王永生, 盛裴轩, 刘式达, 等.大气物理学.北京:气象出版社, 1987: 320.
    [4]
    江祖藩, 印文建.自然雾中液氮成冰扩散的研究∥曹学成, 王伟民.液氮人工增雨技术.北京:气象出版社, 1997: 42-46.
    [5]
    苏正军, 关立友, 黄庚, 等.一个用于催化剂成冰性能检测的新型等温云室∥中国气象科学研究院.第14次全国云雾降水物理和人工影响天气科学讨论会文集. 2004: 113-118.
    [6]
    王鹏飞, 李子华.微观云物理学.北京:气象出版社, 1989: 214.
    [7]
    苏正军, 王广河, 刘卫国, 等.青海省春季降水云的微物理特征分析.应用气象学报, 2003, 14(增刊): 36-40. http://www.cnki.com.cn/Article/CJFDTOTAL-YYQX2003S1004.htm
    [8]
    苏正军, 刘卫国, 王广河, 等.青海一次春季透雨降水过程的云物理结构特征分析.应用气象学报, 2003, 14 (增刊): 27-35. http://www.cnki.com.cn/Article/CJFDTOTAL-YYQX2003S1003.htm
    [9]
    黄庚, 关立友, 苏正军.液氮消冷雾微结构的演变分析.气象, 2006, 32(3): 27-31. http://www.cnki.com.cn/Article/CJFDTOTAL-QXXX200603004.htm
    [10]
    曹学成, 许晓茂, 朱文治.液氮载体的选择及其播撒装置的研究∥曹学成, 王伟民.液氮人工消过冷雾论文.北京:气象出版社, 1997: 155-159.
    [11]
    Pruppacher H R, Klett J D. Microphysics of Cloud and Precipitation. D Reidel Pub, Co, 1978.
    [12]
    游来光, 王守荣, 王鼎丰, 等.新疆冬季降雪微结构及其增长过程初步研究.气象学报, 1989, 47(1): 73-81. http://www.cnki.com.cn/Article/CJFDTOTAL-QXXB198901008.htm
    [13]
    游来光, 熊光莹, 高明忍, 等.春季吉林地区层状云中冰晶的形成与雪晶增长特点.气象学报, 1965, 35(4): 423-433. http://www.cnki.com.cn/Article/CJFDTOTAL-QXXB196504004.htm
    [14]
    陈万奎. 枝状雪晶碰撞攀附与折裂繁生. 气象科学研究院院刊, 1987, 2 (1): 74-80. http://www.cnki.com.cn/Article/CJFDTOTAL-YYQX198701008.htm
    [15]
    郭金平. 层状云冰雪晶二维图像分析∥游景炎, 段英, 游来光. 云降水物理和人工增雨技术研究. 北京: 气象出版社, 1994: 135-145.
    [16]
    游来光, 李炎辉, 刘玉宝.自然云中冰晶生成的核化过程及雪晶对过冷云滴的撞冻.气象学报, 1992, 50(2): 232-238. http://www.cnki.com.cn/Article/CJFDTOTAL-QXXB199202010.htm
  • 加载中
  • -->

Catalog

    Figures(3)  / Tables(1)

    Article views (3781) PDF downloads(2013) Cited by()
    • Received : 2006-03-03
    • Accepted : 2007-01-11
    • Published : 2007-08-31

    /

    DownLoad:  Full-Size Img  PowerPoint