采用美国国家环境预测中心的CFSR(Climate Forecast System Reanalysis)再分析资料和Quick SCAT(Quick Scatterometer)、AVHRR(Advanced Very High Resolution Radiometer)、TRMM(Tropical Rainfall Measuring Mission)高分辨率卫星资料...采用美国国家环境预测中心的CFSR(Climate Forecast System Reanalysis)再分析资料和Quick SCAT(Quick Scatterometer)、AVHRR(Advanced Very High Resolution Radiometer)、TRMM(Tropical Rainfall Measuring Mission)高分辨率卫星资料,研究了大气对春季东海黑潮锋响应的气压调整机制及其年际变化。结果表明,春季东海黑潮锋位于黑潮暖舌的西北侧,呈西南—东北走向,与大尺度气压背景场的等压线走向一致,锋区东南侧暖水与西北侧冷水之间产生的局地气压梯度与大尺度气压梯度形成同向叠加,使得锋区附近西北指向东南的气压梯度达到最大,造成该处的海表面10 m矢量风速也最大,在摩擦作用下形成东北偏北风(NNE)。锋区与其东南侧的NNE风之间沿锋区走向(跨锋区走向)的分量差,会在暖舌附近产生气旋性切变涡度(风速辐合),由此产生上升运动和强降水;而在锋区西北侧的冷水区情况正好相反,有反气旋性切变涡度(风速辐散),并伴有下沉运动和弱降水,从而形成跨锋区的次级环流圈。东海黑潮锋区偏强(弱)年,锋区东南侧暖水与西北侧冷水之间的局地气压梯度也偏强(弱),与大尺度气压梯度同向叠加后形成偏强(弱)的NNE风,造成锋区东南侧暖舌附近的气旋性切变涡度、风速辐合、上升运动和降水均偏强(弱),而锋区西北侧冷水区的反气旋性切变涡度、风速辐散和下沉运动均偏强(弱),跨锋区次级环流圈偏强(弱),这表明在年际时间尺度上气压调整机制仍起作用。展开更多
The Kuroshi’o front eddy’s surface and sectional isothermal distribution characteristics were analyzed on the basis of observation data obtained in April 13-16 of 1989 in the East China Sea. It was found from the si...The Kuroshi’o front eddy’s surface and sectional isothermal distribution characteristics were analyzed on the basis of observation data obtained in April 13-16 of 1989 in the East China Sea. It was found from the similarity between these isothermal distributions with those in January and beginning of June for the years 1986-1990 that the Kuroshio front eddy often occurred from March to the beginning of June. The Kuroshio front eddy movement in the East China Sea in spring was along two routes: the Okinawa Trough route, and the continental shelf slope route. The two moving routes both in the surface layer and in the section are described, their causes are discussed, and differences are compared.展开更多
High spatial resolution sea surface temperature （SST） data from 1993 to 2013 are used to detect the position of the Kuroshio Extension sea surface temperature front （KEF） from 141°E to 158°E, and the sea...High spatial resolution sea surface temperature （SST） data from 1993 to 2013 are used to detect the position of the Kuroshio Extension sea surface temperature front （KEF） from 141°E to 158°E, and the seasonal, monthly and interannual-to-decadal variations of the KEF position are investigated. The latitudinal position of the KEF varies with longitudes： the westernmost part of the KEF from 141°E to 144°E is relatively stable, whereas the easternmost part from 153°E to 158°E exhibits the largest amplitude of its north-south displacement. In the light of the magnitudes of the standard deviations at longitudes, then the KEF is divided into three sections： western part of the KEF （KEFw, 141°-144°E）, central part of the KEF （KEFc, 144°-153°E） and eastern part of the KEF （KEFe, 153°-158°E）. Further analysis reveals that the KEFw position is dominated by the decadal variability, while the KEFc and KEFe positions change significantly both on interannual and decadal time scales. In addition, the KEFw position is well correlated with the KEF path length. The possible mode leading to the decadal oscillation of the KEFw is further discussed. The KEFw position exhibits significant connections with the Pacific decadal oscillation （PDO） index and the north Pacific gyre oscillation （NPGO） index with a time lag of 40 and 33 months, respectively.展开更多
文摘采用美国国家环境预测中心的CFSR(Climate Forecast System Reanalysis)再分析资料和Quick SCAT(Quick Scatterometer)、AVHRR(Advanced Very High Resolution Radiometer)、TRMM(Tropical Rainfall Measuring Mission)高分辨率卫星资料,研究了大气对春季东海黑潮锋响应的气压调整机制及其年际变化。结果表明,春季东海黑潮锋位于黑潮暖舌的西北侧,呈西南—东北走向,与大尺度气压背景场的等压线走向一致,锋区东南侧暖水与西北侧冷水之间产生的局地气压梯度与大尺度气压梯度形成同向叠加,使得锋区附近西北指向东南的气压梯度达到最大,造成该处的海表面10 m矢量风速也最大,在摩擦作用下形成东北偏北风(NNE)。锋区与其东南侧的NNE风之间沿锋区走向(跨锋区走向)的分量差,会在暖舌附近产生气旋性切变涡度(风速辐合),由此产生上升运动和强降水;而在锋区西北侧的冷水区情况正好相反,有反气旋性切变涡度(风速辐散),并伴有下沉运动和弱降水,从而形成跨锋区的次级环流圈。东海黑潮锋区偏强(弱)年,锋区东南侧暖水与西北侧冷水之间的局地气压梯度也偏强(弱),与大尺度气压梯度同向叠加后形成偏强(弱)的NNE风,造成锋区东南侧暖舌附近的气旋性切变涡度、风速辐合、上升运动和降水均偏强(弱),而锋区西北侧冷水区的反气旋性切变涡度、风速辐散和下沉运动均偏强(弱),跨锋区次级环流圈偏强(弱),这表明在年际时间尺度上气压调整机制仍起作用。
文摘The Kuroshi’o front eddy’s surface and sectional isothermal distribution characteristics were analyzed on the basis of observation data obtained in April 13-16 of 1989 in the East China Sea. It was found from the similarity between these isothermal distributions with those in January and beginning of June for the years 1986-1990 that the Kuroshio front eddy often occurred from March to the beginning of June. The Kuroshio front eddy movement in the East China Sea in spring was along two routes: the Okinawa Trough route, and the continental shelf slope route. The two moving routes both in the surface layer and in the section are described, their causes are discussed, and differences are compared.
基金The National Basic Research Program of China under contract Nos 2015CB954004 and 2012CB417402the National Natural Science Foundation of China under contract Nos 41576178 and U1405233
文摘High spatial resolution sea surface temperature （SST） data from 1993 to 2013 are used to detect the position of the Kuroshio Extension sea surface temperature front （KEF） from 141°E to 158°E, and the seasonal, monthly and interannual-to-decadal variations of the KEF position are investigated. The latitudinal position of the KEF varies with longitudes： the westernmost part of the KEF from 141°E to 144°E is relatively stable, whereas the easternmost part from 153°E to 158°E exhibits the largest amplitude of its north-south displacement. In the light of the magnitudes of the standard deviations at longitudes, then the KEF is divided into three sections： western part of the KEF （KEFw, 141°-144°E）, central part of the KEF （KEFc, 144°-153°E） and eastern part of the KEF （KEFe, 153°-158°E）. Further analysis reveals that the KEFw position is dominated by the decadal variability, while the KEFc and KEFe positions change significantly both on interannual and decadal time scales. In addition, the KEFw position is well correlated with the KEF path length. The possible mode leading to the decadal oscillation of the KEFw is further discussed. The KEFw position exhibits significant connections with the Pacific decadal oscillation （PDO） index and the north Pacific gyre oscillation （NPGO） index with a time lag of 40 and 33 months, respectively.
