气象
氣象
기상
METEOROLOGICAL MONTHLY
2014年
1期
59-65
,共7页
周黎明%王俊%龚佃利%张洪生
週黎明%王俊%龔佃利%張洪生
주려명%왕준%공전리%장홍생
暴雪%微物理参量%粒子谱%速度谱
暴雪%微物理參量%粒子譜%速度譜
폭설%미물리삼량%입자보%속도보
snowstorm%microphysical parameter%particle spectrum%velocity spectrum
为了研究降雪过程中粒子微物理特征,利用架设在济南南部山区的一台THIES激光降水粒子谱仪获取的2009年11月11-12日强降雪过程中降水粒子谱资料,对降雪粒子微物理参量演变特征、粒子谱及速度谱分布特征进行了分析。结果表明,(1)此次降雪天气过程中降水强度与数浓度、最大直径和雷达反射率因子间均具有一定的正相关性;降水强度与最大直径的关系极为密切,粒子的大小直接决定降水强度的大小。(2)降雪过程中谱型分布以单峰型和指数型为主,各粒径档内数浓度分布存在不均匀性,但数浓度峰值直径主要集中在0.5 mm处。(3)粒子速度谱均以单峰结构分布,下落末速基本位于0.375~2 m·s-1之间,随直径的增大几乎没有变化。
為瞭研究降雪過程中粒子微物理特徵,利用架設在濟南南部山區的一檯THIES激光降水粒子譜儀穫取的2009年11月11-12日彊降雪過程中降水粒子譜資料,對降雪粒子微物理參量縯變特徵、粒子譜及速度譜分佈特徵進行瞭分析。結果錶明,(1)此次降雪天氣過程中降水彊度與數濃度、最大直徑和雷達反射率因子間均具有一定的正相關性;降水彊度與最大直徑的關繫極為密切,粒子的大小直接決定降水彊度的大小。(2)降雪過程中譜型分佈以單峰型和指數型為主,各粒徑檔內數濃度分佈存在不均勻性,但數濃度峰值直徑主要集中在0.5 mm處。(3)粒子速度譜均以單峰結構分佈,下落末速基本位于0.375~2 m·s-1之間,隨直徑的增大幾乎沒有變化。
위료연구강설과정중입자미물리특정,이용가설재제남남부산구적일태THIES격광강수입자보의획취적2009년11월11-12일강강설과정중강수입자보자료,대강설입자미물리삼량연변특정、입자보급속도보분포특정진행료분석。결과표명,(1)차차강설천기과정중강수강도여수농도、최대직경화뢰체반사솔인자간균구유일정적정상관성;강수강도여최대직경적관계겁위밀절,입자적대소직접결정강수강도적대소。(2)강설과정중보형분포이단봉형화지수형위주,각립경당내수농도분포존재불균균성,단수농도봉치직경주요집중재0.5 mm처。(3)입자속도보균이단봉결구분포,하락말속기본위우0.375~2 m·s-1지간,수직경적증대궤호몰유변화。
To better study microphysical characteristics during snowfall process,drop size spectra were col-lected with an optical disdrometer during the snowstorm event in 11-12 November 2009 in the southern mountainous area of Jinan.The characteristics of the microphysical parameters,the drop size distribution and speed spectral distribution are investigated.It is found that:(1 )during the snowstorm,precipitation intensity and number concentration,maximum diameter,and the radar reflectivity factor have positive lin-ear correlations;the precipitation intensity and the maximum diameter has a close relationship;precipitati-on intensity is decided by the maximum diameter.(2)In the snow process,the spectrum-type distributions are of unimodal and index distributions,and the peak value of number concentration is focuses around 0.5 mm.The concentration distribution of each particle-size file is inhomogeneous.(3 )The velocity-spectra are mainly single-peak distributions,and the terminal velocity essentially lies in the range of 0.375-2 m·s-1 ,which almost has no change with the increase of diameter.