Luo Ning, Wen Jifen, Zhao Cai, et al. Observation study on properties of cloud and fog in ice accretion areas. J Appl Meteor Sci, 2008, 19(1): 91-95.
Citation: Luo Ning, Wen Jifen, Zhao Cai, et al. Observation study on properties of cloud and fog in ice accretion areas. J Appl Meteor Sci, 2008, 19(1): 91-95.

Observation Study on Properties of Cloud and Fog in Ice Accretion Areas

  • Received Date: 2007-01-24
  • Rev Recd Date: 2007-08-28
  • Publish Date: 2008-02-29
  • Ice accretion on conductors from freezing rain or glaze is a common meteorological disaster in Guizhou mountainous areas, causing serious damages with the warped wire, the collapsed pole and/or tower and broken circuit. For example, the severe ice accretion in 1984 in Guizhou brings the blackout in the local electricity transport network. The security of electricity transport is threatened by ice accretion on conductors. The glaze forms from freezing rain on conductors near surface with the air temperature between 0 ℃ and 6 ℃ in Guizhou. It is found in experiment that ice frozen between 0 ℃ and 6 ℃ is difficult to fall off with its great density, which is a main cause for Guizhou's ice accretion with the extreme danger. In Liupanshui of western Guizhou the site especially for observation of ice accretion on conductors is built by national power company. In this site and two other ice accretion areas in northern and central Guizhou the field observations are conducted with the elevations of 2128 m, 1780 m and 1659 m respectively. The growth rate of conductor ice accretion is closely associated with the cloud-and fog-conditions. The major observation factors include cloud droplet size distribution, water content in cloud and fog, air temperature, wind direction, wind speed, long and short diameters of ice accretion on conductors. The cloud droplets and water content in cloud and fog are colleted with the method of integration suction. The ice accretion is measured in the specific stands in both east-west and north-south directions. In three observation areas there are no significant differences for cloud droplets on both the concentration of 140—312 droplets/cm3 and the average diameters with arithmetic mean diameter of 7.5 μm, cube root diameter of 11.3 μm and median volume diameter of 20 μm; although the number concentration of cloud droplets with the diameter bigger than 14 μg are 12.5% of the total concentration, water content contributed by them is as high as 78% due to the dominant contribution to water content considering the high collision efficient of these large cloud droplets on conductors, the distribution of large droplets is a key factor involving ice accretion; the water content with the average value of 0.20 g·m-3 in cloud and fog decreases with air temperature from 0 ℃ to -6 ℃; more ice accretes on conductors of north-south than east-west direction caused by prevailing northeast wind in the surface levels during the stationary front period in winter; the growth rate of ice accretion is proportional to the water content in cloud and fog and the wind speed, especially of more obvious direct ratio with the wind speed over 3 m·s-1.
  • Fig. 1  Contributing percent of different cloud droplet scale with water content

    (more than 14 μm of integral value for cloud droplet to water content with shaded)

    Fig. 2  Ice accretion process over Maluojing from Feb 2 to 4 in 1991

    Table  1  Micro Characteristics of super-cooling cloud fog in heavy ice region

    Table  2  Cloud and fog droplet formulae

    Table  3  Eigenvalue of water content W in different area

    Table  4  Distribution of water content in different height and temperature (unit:g/m3)

    Table  5  Mean Kd with different wind condition

  • [1]
    Person P, Gaget J F. Ice accretion on wires and anti-icing induced by joule effect. J Appl Meteor, 1988, 27:101-114. doi:  10.1175/1520-0450(1988)027<0101:IAOWAA>2.0.CO;2
    [2]
    Prudi F, Levi L, Levizzani V. Ice accretion on fixed cylinders. Quart J R Met Soc, 1986, 112:1091-1109. doi:  10.1002/(ISSN)1477-870X
    [3]
    谭冠日.电线积冰若干气候特征的探讨.气象学报, 1982, 40 (1):15-22. http://www.cnki.com.cn/Article/CJFDTOTAL-QXXB198201001.htm
    [4]
    Makkonen L. Estimating intensity of atmospheric ice accretion on stationary structures. J Appl Meteor, 1981, 20:595-600. doi:  10.1175/1520-0450(1981)020<0595:EIOAIA>2.0.CO;2
    [5]
    Makkonen L. Modeling of ice accretion on wires. J Climate Appl Meteor, 1984, 23:929-939. doi:  10.1175/1520-0450(1984)023<0929:MOIAOW>2.0.CO;2
    [6]
    Loxowski E P. The icing of an unheated non-rotation cylinder:Icing wind tunnel experiments. J Climate Appl Meteor, 1983, 22:2063-2072. doi:  10.1175/1520-0450(1983)022<2063:TIOAUN>2.0.CO;2
    [7]
    李子华.中国近40年来雾的研究.气象学报, 2000, 59 (5): 616-624. http://www.cnki.com.cn/Article/CJFDTOTAL-QXXB200105011.htm
    [8]
    黄玉生, 黄玉仁, 李子华, 等.西双版纳冬季雾的微物理结构及演变过程.气象学报, 2000, 58 (6):715-725. http://www.cnki.com.cn/Article/CJFDTOTAL-QXXB200006006.htm
    [9]
    吴有训, 陈健武, 杨保桂, 等.黄山冬季气温分类及雪、雨凇和雾凇的气候分析.气象学报, 2000, (58)3:376-384. http://www.cnki.com.cn/Article/CJFDTOTAL-QXXB200003014.htm
    [10]
    何立富, 李峰, 李泽椿.华北平原一次持续性大雾过程的动力和热力特征.应用气象学报, 2006, 17 (2):160-168. http://qikan.camscma.cn/jams/ch/reader/view_abstract.aspx?file_no=20060228&flag=1
    [11]
    刘小宁, 张洪政, 李庆祥, 等.我国大雾的气候特征及变化初步解释.应用气象学报, 2005, 16 (2):221-230. http://qikan.camscma.cn/jams/ch/reader/view_abstract.aspx?file_no=20050227&flag=1
    [12]
    王继志, 徐祥德, 杨元琴.北京能见度及雾特征分析.应用气象学报, 2002, 13 (增刊):160-169. http://www.cnki.com.cn/Article/CJFDTOTAL-YYQX2002S1017.htm
    [13]
    王鹏飞, 李子华.微观云物理学.北京:气象出版社, 1989.
    [14]
    文继芬.雨雾凇天气的滴谱、含水量与积冰.贵州气象, 1994, 18 (6):21-26. http://www.cnki.com.cn/Article/CJFDTOTAL-GZQX199406004.htm
    [15]
    罗宁.气象记录的雨雾凇冰与导线冰害事故的关系.贵州气象, 1994, 18 (6):10-20. http://www.cnki.com.cn/Article/CJFDTOTAL-GZQX199406003.htm
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    • Received : 2007-01-24
    • Accepted : 2007-08-28
    • Published : 2008-02-29

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