2008年6月27日
Observation of particle fall velocity in cirriform cloud by VHF and millimeter-wave Doppler radars
Journal of Geophysical Research Atmospheres
- 巻
- 113
- 号
- 12
- 記述言語
- 英語
- 掲載種別
- 研究論文(学術雑誌)
- DOI
- 10.1029/2007JD009125
- 出版者・発行元
- Blackwell Publishing Ltd
In this study, it is demonstrated that a combination of VHF and millimeter-wave Doppler radars is a key tool for observing particle fall velocity in cirriform clouds. VHF (47-MHz) and millimeter-wave (95-GHz) Doppler radars observed cirriform clouds at West Sumatra, Indonesia (0.2°S, 100.32°E) from 2000 LT 14 to 0800 LT 15 November 2005. Radar reflectivity factor (Ze) observed by the 95-GHz radar showed that echoes from cloud particles had tops around 12-14 km and bottoms around 8-10 km. Doppler velocity observed by the vertically pointed beam of the 95-GHz radar (V<
inf>
air+Z<
/inf>
) was compared with vertical air velocity (V<
inf>
air<
/inf>
) observed by the 47-MHz radar to confirm that V<
inf>
air+Z<
/inf>
, a sum of V<
inf>
air<
/inf>
and reflectivity-weighted particle fall velocity (V<
inf>
Z<
/inf>
), showed consistent changes with V<
inf>
air<
/inf>
and hence V<
inf>
Z<
/inf>
is able to be retrieved by subtracting V<
inf>
air<
/inf>
from V<
inf>
air+Z<
/inf>
. The correlation coefficient between V<
inf>
Z<
/inf>
and Z<
inf>
e<
/inf>
in the middle part of clouds (10.5-12.2 km) was -0.81, which was higher than that (-0.47) in the bottom part (7.2-10.5 km). The change of V<
inf>
Z<
/inf>
for Z<
inf>
e<
/inf>
in the middle part was larger (Z<
inf>
e<
/inf>
= -31.9 V<
inf>
Z<
/inf>
- 32.2) than that in the bottom part (Z<
inf>
e<
/inf>
, = -90.2 V<
inf>
Z<
/inf>
- 71.8). These results suggest that particle size was a dominant factor that determined Z<
inf>
e<
/inf>
in the middle part. Using V<
inf>
Z<
/inf>
, median volume diameter (D<
inf>
0<
/inf>
) was estimated to suggest that D<
inf>
0<
/inf>
was larger than ∼70 μm in the bottom part and ranged from ∼40 μm to larger than ∼106 μm in the middle part. Copyright 2008 by the American Geophysical Union.
inf>
air+Z<
/inf>
) was compared with vertical air velocity (V<
inf>
air<
/inf>
) observed by the 47-MHz radar to confirm that V<
inf>
air+Z<
/inf>
, a sum of V<
inf>
air<
/inf>
and reflectivity-weighted particle fall velocity (V<
inf>
Z<
/inf>
), showed consistent changes with V<
inf>
air<
/inf>
and hence V<
inf>
Z<
/inf>
is able to be retrieved by subtracting V<
inf>
air<
/inf>
from V<
inf>
air+Z<
/inf>
. The correlation coefficient between V<
inf>
Z<
/inf>
and Z<
inf>
e<
/inf>
in the middle part of clouds (10.5-12.2 km) was -0.81, which was higher than that (-0.47) in the bottom part (7.2-10.5 km). The change of V<
inf>
Z<
/inf>
for Z<
inf>
e<
/inf>
in the middle part was larger (Z<
inf>
e<
/inf>
= -31.9 V<
inf>
Z<
/inf>
- 32.2) than that in the bottom part (Z<
inf>
e<
/inf>
, = -90.2 V<
inf>
Z<
/inf>
- 71.8). These results suggest that particle size was a dominant factor that determined Z<
inf>
e<
/inf>
in the middle part. Using V<
inf>
Z<
/inf>
, median volume diameter (D<
inf>
0<
/inf>
) was estimated to suggest that D<
inf>
0<
/inf>
was larger than ∼70 μm in the bottom part and ranged from ∼40 μm to larger than ∼106 μm in the middle part. Copyright 2008 by the American Geophysical Union.
- リンク情報
- ID情報
-
- DOI : 10.1029/2007JD009125
- ISSN : 0148-0227
- SCOPUS ID : 50049116036