Automatically locating the typhoon center based on satellite cloud image

2004 ◽  
Author(s):  
Zhengguang Liu ◽  
Juntao Xue ◽  
Yuanfei Yu ◽  
Bing Wu ◽  
Gary Shen
1988 ◽  
Author(s):  
Howard J. Schultz ◽  
Ronald G. Isaacs

2007 ◽  
Author(s):  
Yuan-Xiang Li ◽  
Yan-Bing Li ◽  
Zhong-Liang Jing

2014 ◽  
Vol 22 (7) ◽  
pp. 1886-1895
Author(s):  
金炜 JIN Wei ◽  
王文龙 WANG Wen-long ◽  
符冉迪 FU Ran-di ◽  
田文哲 TIAN Wen-zhe ◽  
尹曹谦 YIN Cao-qian

2020 ◽  
Vol 12 (11) ◽  
pp. 1851
Author(s):  
Mei Du ◽  
Yijun Hou ◽  
Po Hu ◽  
Kai Wang

A coastal inundation simulation system was developed for the coast of the Pearl River estuary (PRE), which consists of an assimilation typhoon model and the coupled ADCIRC (Advanced Circulation) + SWAN (Simulating Waves Nearshore) model. The assimilation typhoon model consists of the Holland model and the analysis products of satellite images. This is the first time an assimilation typhoon model has been implemented and tested for coastal inundation via case studies. The simulation results of the system agree well with the real measurements. Three observed typhoon paths (Hope, Nida, and Hato) were chosen to be the studied paths based on their positions relative to the PRE, China. By comparing the results of experiments with different forcing fields, we determined that the storm surge and the coastal inundation were mainly induced by wind forcing. By simulating coastal inundation for different typhoon center speeds, the Hato3 path most easily causes coastal inundation in the PRE. Moreover, the moving speed of the typhoon’s center significantly affects the coastal inundation in the PRE. The inundation becomes very serious as the movement of the typhoon center was slow down. This study provides a new reference for future predictions of coastal inundations.


1960 ◽  
Vol 41 (3) ◽  
pp. 115-124 ◽  
Author(s):  
Griffith Wang

Based on six years (1950 through 1955) of typhoon data, three equations are formulated for the purpose of forecasting the movement of typhoons. In these equations, the following criteria at the 700-mb level are accounted for:(1) the contour height and its tendency at a point 10 deg of lat north of the typhoon center,(2) the contour height and its tendency at a point 10 deg of lat from the typhoon center and 90 deg to the right of its direction of motion,(3) the contour height and its tendency at a point 10 deg of lat from the typhoon center and 90 deg to the left of its direction of motion, and(4) the intensity and orientation of the major axis of a subtropical high cell which plays the role of steering the movement of the typhoon. Typhoon data collected during the years 1956 through 1958 are used for verification. With use of these equations, results of forecasting a 24-hr typhoon movement are found to be of practical value.


2001 ◽  
Vol 19 (8) ◽  
pp. 925-931 ◽  
Author(s):  
M. Teshiba ◽  
H. Hashiguchi ◽  
S. Fukao ◽  
Y. Shibagaki

Abstract. Typhoon 9707 (Opal) was observed with the VHF-band Middle and Upper atmosphere (MU) radar, an L-band boundary layer radar (BLR), and a vertical-pointing C-band meteorological radar at the Shigaraki MU Observatory in Shiga prefecture, Japan on 20 June 1997. The typhoon center passed about 80 km southeast from the radar site. Mesoscale precipitating clouds developed due to warm-moist airmass transport from the typhoon, and passed over the MU radar site with easterly or southeasterly winds. We primarily present the wind behaviour including the vertical component which a conventional meteorological Doppler radar cannot directly observe, and discuss the relationship between the wind behaviour of the typhoon and the precipitating system. To investigate the dynamic structure of the typhoon, the observed wind was divided into radial and tangential wind components under the assumption that the typhoon had an axi-symmetric structure. Altitude range of outflow ascended from 1–3 km to 2–10 km with increasing distance (within 80–260 km range) from the typhoon center, and in-flow was observed above and below the outflow. Outflow and inflow were associated with updraft and downdraft, respectively. In the tangential wind, the maximum speed of counterclockwise winds was confirmed at 1–2 km altitudes. Based on the vertical velocity and the reflectivity obtained with the MU radar and the C-band meteorological radar, respectively, precipitating clouds, accompanied by the wind behaviour of the typhoon, were classified into stratiform and convective precipitating clouds. In the stratiform precipitating clouds, a vertical shear of radial wind and the maximum speed of counterclockwise wind were observed. There was a strong reflectivity layer called a ‘bright band’ around the 4.2 km altitude. We confirmed strong updrafts and down-drafts below and above it, respectively, and the existence of a relatively dry layer around the bright band level from radiosonde soundings. In the convective precipitating clouds, the regions of strong and weak reflectivities were well associated with those of updraft and downdraft, respectively.Key words. Meteorology and atmospheric dynamics (mesoscale meteorology; precipitation) Radio science (remote sensing)


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