共查询到18条相似文献，搜索用时 593 毫秒
1.
采用美国国家环境预测中心的CFSR(Climate Forecast System Reanalysis)再分析资料和QuickSCAT(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。 相似文献
2.
采用半地转方程的二维锋生模式，研究了地面暖带附近锋生过程中，大尺度斜压区、地面暧带和潜热释放之间的相互作用，结果表明：变形场中的孤立暖带，当它位于大尺度斜压区暖空气一侧时，可在有限时间内形成强锋区（有潜热加热时锋生速度更快）；当暖带与大尺度斜压区配合时，可出现双锋区结构，强锋区可能先在暖带中出现。在暖带深厚并有潜热释放时表现更明显且有利于双锋区结构的维持，锋生强迫作用和位温扰动是梅雨锋附近两条中－ 相似文献
3.
春季我国东部海洋温度锋区对大气的强迫作用及其机制研究 总被引：6，自引：3，他引：3
首先, 采用高分辨率的卫星资料研究了春季我国东部海区海洋锋区附近的海温与风场之间的关系, 资料分析表明海温与海表面风速之间存在明显的正相关关系, 特别是在海洋锋强的年份, 这种正相关关系更明显。资料分析还表明春季是黄海、 东海海洋锋最强的季节, 海温与海表面风速的对应关系在春季尤为明显。然后, 采用一个高分辨率和先进物理方案的中尺度模式探讨了海洋影响大气的机制。控制试验再现了海洋锋区附近海温与海表面风速之间的正相关关系。模拟的边界层垂直结构说明海温能够明显改变锋区两侧边界层大气的稳定度和垂直混合的强弱, 证明了垂直混合机制的存在。而另一方面, 对控制试验和平滑海温试验的水平动量方程中各收支项的比较分析发现, 由于海洋锋的存在而产生的气压梯度力对穿越锋区的空气的加速也有相当重要的贡献。综合观测和模拟结果说明春季我国东部海区海洋温度锋区的海洋—大气相互作用过程中海洋对大气的影响非常明显, 在海洋影响大气的机理方面, 海平面气压调整机制和垂直混合机制都在起作用。 相似文献
4.
利用NOAA最优插值逐日海表温度资料和AVISO中心的海表高度异常资料,分析了黑潮延伸体区域的海表温度锋的时空变化特征以及导致其年代际变化可能的原因。结果表明,气候平均态的黑潮延伸体区域海表温度锋位于黑潮延伸体区域北部边缘,在143 °E和150 °E附近存在两个弯曲,SST水平梯度最大值出现在142 °E附近,强度超过4.5 ℃/(100 km),其后强度自西向东逐渐递减,在149 °E附近又出现一个较弱的大值中心,在141~153 °E范围内,海表温度锋位置的平均值为36.25 °N,强度的平均值为3.22 ℃/(100 km)。黑潮延伸体区域的海表温度锋南北位置的季节变化很弱,而其强度的季节变化非常显著。相较于较弱的季节变化,海表温度锋位置的年际和年代际的低频变化则要显著得多,其南北变化跨度超过2 °。海表温度锋强度的年际和年代际的低频变化也较强,超过4.5 ℃/(100 km)。黑潮延伸体区域的海表温度锋的变化与太平洋年代际振荡（PDO）以及北太平洋涡旋振荡（NPGO）存在显著的相关关系,NPGO和PDO在中东太平洋区域会强迫产生海表高度异常,随后向西传播,在约3年后到达黑潮延伸体区域,使该区域流场发生变化产生海洋热平流异常,最终导致海表温度锋强度发生变化。 相似文献
5.
蒸发波导是影响海上雷达系统探测性能的主导机制,海表温度（SST）锋带来的蒸发波导非均匀性和突变性具有重要的研究价值。2018年春季航次“海气相互作用观测试验”,曾两次穿越黑潮海域获取了珍贵的观测资料。在此基础上,结合欧洲中期天气预报中心（ECMWF）再分析资料（ERA-Interim）和HYSPLIT（Hybrid Single Particle Lagrangian Integrated Trajectories）气块轨迹溯源,分离出两个重要的走航观测时段。S1段（持续约21 h）气流从暖海水区吹向冷海水区,以稳定层结为主,其间因黑潮海洋锋的存在,气流由黑潮主体的暖水区吹向大陆冷海区时,形成具有强逆温层的海洋边界层,并伴随海雾的生成,导致此处蒸发波导高度突降为0。此后为持续近66 h的S2段,气流由冷海水区吹向暖海水区,以近中性弱不稳定层结为主,蒸发波导高度基本维持在12 m高度。数值模拟结果表明,模拟时段内的黑潮海洋锋区,蒸发波导高度突变性和非均匀性始终存在,且伴随暖海水吹向冷海水的锋区突变性更强。黑潮海洋锋对蒸发波导的这种天气尺度强迫作用的加强与层结稳定度的突变和海雾的生成有关。 相似文献
6.
海表面盛行风背景下大气对黑潮海洋锋的响应特征 总被引：1，自引：0，他引：1
采用一系列高分辨率的卫星资料,应用高通滤波等方法,研究了春季不同海表面盛行风背景下,东海黑潮海洋锋区附近的海气关系。观测分析表明:在东海,春季3种不同海表面盛行风条件下海表面温度与海表面风速之间都存在明显的正相关关系,表现为海洋对大气的强迫作用。大气对海洋锋的响应在3种不同盛行风条件下也存在明显的差异。在西北盛行风和东南盛行风背景下,即当风向垂直于海洋锋由冷侧(暖侧)吹向暖侧(冷侧)时,海表面风的辐散(辐合)出现在海洋锋上空。同时,海洋锋对海平面气压(SLP)、降水和对流活动的影响较弱,表明大气对海洋锋的响应主要局限在大气边界层内。在东北盛行风背景下,即当风平行于海洋锋时,在海洋锋的暖(冷)水侧上空为海表面风的辐合(辐散),并与SLP的异常低(高)值相对应,主要雨带出现在黑潮暖舌上空。无论从总降水还是层云、对流降水频次的空间分布来看,盛行东北风时,海表面温度对其上雨带的影响最为明显。分析结果还表明,在不同盛行风背景下,海洋锋附近的海气关系由不同的物理机制在起主导作用。当盛行平行于海洋锋的东北风时,主要由SLP调整机制起作用;而盛行垂直于海洋锋的西北风时则主要由垂直混合机制起作用。 相似文献
7.
利用英国哈德莱中心（Hadley Center）1949~2014年表层海温资料,将黑潮延伸体海区海温经向梯度的大值区域的平均值定义为黑潮延伸体及其北部海洋锋强度指数（KEFI）,利用数据分析方法研究了各季节KEFI的变化特征及其与北太平洋风暴轴的关系。分析表明,各季节的KEFI存在明显的年际和年代际变化特征,同时在冬季与北太平洋瞬时方差有显著正相关,两者在风暴轴主体位置的相关性最为显著,并且这种相关性在KEFI超前一个月时就所显现,同时对后期风暴轴也有一定影响,即冬季黑潮延伸体海区海洋锋的强度会影响风暴轴区域瞬时方差的变化。之后主要分析了这种影响的可能机制,发现在冬季KEFI高值年,由于海洋锋两侧的热量输送差异更加明显,导致海洋锋附近的近表面气温经向梯度增强,维持了近表面的斜压性,促进涡动热量的向极输送和海洋锋南侧的向上输送,有利于瞬时涡旋的发展。另外大尺度环流场与冬季黑潮延伸体海洋锋也有关系,具体表现为,在海洋锋强年,阿留申低压加深,副热带高压略有加强,对应的对流层低层位势高度场在40°N以北有负变高,以南有正变高,同时高空极锋急流加强,副热带西风急流减弱加宽北抬,海洋锋偏弱年的变化则相反。因此,冬季黑潮延伸体及其北部的海洋锋主要通过两侧海表热量输送差异不断产生气温梯度,进而维持斜压性以促进上层风暴轴的发展。 相似文献
8.
东中国海黑潮海洋锋的季节变化特征及其成因 总被引：1，自引：0，他引：1
利用高分辨率海洋和大气再分析资料研究了东中国海黑潮海洋锋的季节变化特征及其成因。研究表明,东海黑潮海洋锋存在明显的季节变化,从冬季到次年春季逐渐增强,并在春季达到最强,初夏以后强度逐渐减弱,9—10月达到全年最弱。通过诊断混合层热流量方程发现,东海黑潮区一年四季均表现为暖的温度平流,有利于海洋锋的形成和维持,该暖平流也存在季节变化并在春季达到最大,对海洋锋在春季达到最强起了重要作用。海气界面净热通量在秋冬季对海洋锋的形成有促进作用,有利于海洋锋增强,而在春夏季则起抑制作用,促进海洋锋消亡。温度垂直输送全年对海洋锋起一定程度的抑制作用。总之,在海温水平平流和海表净热通量的共同作用下导致海洋锋春季达到最强,而夏秋季海表净热通量和温度垂直输送作用的共同作用致使海洋锋减弱并最后消失。因此,海洋的动力和热力共同作用导致了东海黑潮海洋锋的季节变化,其中海温水平平流和海表净热通量对海洋锋的季节变化起主要作用,而温度垂直输送项对海洋锋的发展起抑制作用,但影响相对较小。 相似文献
9.
春季黑潮延伸体海洋锋区经向位移与东亚大气环流的关系 总被引：6，自引：0，他引：6
采用高分辨率的海表温度资料定义了春季黑潮延伸体北侧海洋锋区的南北位置,并采用EOF分析、相关分析、合成分析、带通滤波等方法,探讨了其南北向位置变动与高空急流、风暴轴以及后期东亚降水之间的关系。结果表明,春季黑潮延伸体北侧海洋锋区位置的南北变动存在明显的年际、年代际变化,其与6月东亚高空急流、太平洋区域风暴轴的南北位置具有很好的对应关系。当春季黑潮延伸体海洋锋区偏北时,6月东亚高空急流、太平洋区域风暴轴偏北,反之亦然。进一步的研究还表明,春季黑潮延伸体海洋锋区经向位置的变动可通过影响东亚大气环流对6月东亚地区的降水产生影响,黑潮延伸体海洋锋区偏北(南)年,6月雨带有显著的北(南)移。 相似文献
10.
2011年江苏梅汛期分为典型和非典型梅雨锋降水两个阶段,针对不同阶段中产生的暴雨,利用常规资料和NCEP/NCAR再分析资料,采用合成平均方法,从天气形势、热力和动力特征方面对其异同进行了分析。结果表明：典型梅雨锋暴雨在500 hPa中纬度低槽和副热带高压的共同作用下产生,暴雨落区在5840 gpm线附近,对流层低层有切变线,近地面梅雨锋特征显著,经向风扰动为深厚的北风,暖湿气流来自于孟加拉湾和南海中北部;非典型梅雨锋暴雨时,中高层江苏处于天气尺度深厚低槽前的西南气流中,冷空气来自东北冷涡后部,低层有倒槽辐合线,近地面锋区较弱,异常强盛的暖湿气流由南海经台湾海峡和东海北上,对流层低层经向风扰动为南风,中高层为北风,暴雨产生在低层南风风速辐合区;两类暴雨的落区均位于锋区暖的一侧以及假相当位温(θse)和比湿(q)大值区的北侧以及强上升运动区。 相似文献
11.
At least two main oceanic fronts (the subarctic and subtropical fronts) exist in the North Pacific. Especially in the subtropical frontal zone (STFZ), the sea subsurface temperature gradient is significantly larger than that of the surface layer in winter. Subseasonal interaction between the subsurface subtropical front and overlaying atmosphere is revealed by using empirical orthogonal function (EOF) analysis of oceanic temperature gradient. The first EOF mode mainly corresponds to the atmosphere-to-ocean influences. With the enhanced westerly wind, a cold sea surface temperature anomaly (SSTA) appears and then passes down to affect the subsurface ocean. However, the second EOF mode indicates the ocean-to-atmosphere forcing. For the second mode, cold oceanic temperature anomaly generates in the subsurface layer and passes up, which makes the SST gradient increasing. Due to the increasing atmospheric baroclinicity, the enhanced westerly wind leads to more heat fluxes from the ocean to the atmosphere, which results in a colder SSTA and a larger SST gradient in the STFZ. Therefore, a positive ocean-atmosphere feedback begins to maintain in the mid-latitude in winter. 相似文献
12.
Mechanisms determining the tropospheric temperature gradient that is related to the intensity of the Asian summer monsoon are examined in an intermediate atmospheric model coupled with a mixed-layer ocean and a simple land surface model with an idealized Afro–Eurasian continent and no physical topography. These include processes involving in the influence of the Eurasian continent, thermal effects of the Tibetan Plateau and effects of sea surface temperature. The mechanical effect on the large-scale flow induced by the Plateau is not included in this study. The idealized land–sea geometry without topography induces a positive meridional tropospheric temperature gradient thus a weak Asian summer monsoon circulation. Higher prescribed heating and weaker surface albedo over Eurasia and the Tibetan Plateau, which mimic effects of different land surface processes and the thermal effect of the uplift of the Tibetan Plateau, strengthens the meridional temperature gradient, and so as cold tropical SST anomalies. The strengthened meridional temperature gradient enhances the Asian summer monsoon circulation and favors the strong convection. The corresponding monsoon rainbelt extends northward and northeastward and creates variations of the monsoon rainfall anomalies in different subregions. The surface albedo over the Tibetan Plateau has a relatively weak inverse relation with the intensity of the Asian summer monsoon. The longitudinal gradient of ENSO-like SST anomalies induces a more complicated pattern of the tropospheric temperature anomalies. First, the positive (negative) longitudinal gradient induced by the El Niño (La Niña)-like SST anomalies weakens (strengthens) the Walker circulation and the circulation between South Asia and northern Africa and therefore the intensity of the Asian summer monsoon, while the corresponding monsoon rainbelt extends northward (southward). The El Niño (La Niña)-like SST anomalies also induces colder (warmer) tropospheric temperature over Eurasia and warmer (colder) tropospheric temperature over the Indian Ocean. The associated negative (positive) meridional gradient of the tropospheric temperature anomalies is consistent with the existence of the weak (strong) Asian summer monsoon. 相似文献
13.
西北太平洋是全球海雾最多的海域,但由于观测资料匮乏,对开阔大洋上海雾形成机理的个例研究很少。2019年9月12—14日,中国北极科考船“向阳红01号”在亲潮延伸体水域捕捉到一次海雾事件。主要利用船载观测数据,分析了海雾形成的物理过程。结果表明,这是一次温带气旋的暖锋和局地海洋锋(海面温度锋)共同影响下的海雾过程。伴随暖锋的偏南气流将暖湿空气向北输送,在亲潮延伸体区,海面空气增湿效应大于增温效应,导致相对湿度不断增加接近饱和。北上暖空气遇到较冷水域上空的冷空气团,向上爬升形成大范围锋面逆温;局地海洋锋强迫出大气边界层内的次级环流,其下沉支使该锋面逆温层底的高度进一步降低,有利于雾滴局限在近海面成雾,雾区出现于暖锋锋面过后局地海洋锋的冷水侧。这项研究明确了海雾形成过程中作为背景环流的大气暖锋与作为局地强迫项的海洋锋的贡献,可为海雾预报提供新的理论支撑。 相似文献
14.
Air–sea interaction over ocean fronts and eddies 总被引：1，自引：0，他引：1
R.J. Small S.P. deSzoeke S.P. Xie L. O&#x;Neill H. Seo Q. Song P. Cornillon M. Spall S. Minobe 《Dynamics of Atmospheres and Oceans》2008,45(3-4):274
Air–sea interaction at ocean fronts and eddies exhibits positive correlation between sea surface temperature (SST), wind speed, and heat fluxes out of the ocean, indicating that the ocean is forcing the atmosphere. This contrasts with larger scale climate modes where the negative correlations suggest that the atmosphere is driving the system. This paper examines the physical processes that lie behind the interaction of sharp SST gradients and the overlying marine atmospheric boundary layer and deeper atmosphere, using high resolution satellite data, field data and numerical models. The importance of different physical mechanisms of atmospheric response to SST gradients, such as the effect of surface stability variations on momentum transfer, pressure gradients, secondary circulations and cloud cover will be assessed. The atmospheric response is known to create small-scale wind stress curl and divergence anomalies, and a discussion of the feedback of these features onto the ocean will also be presented. These processes will be compared and contrasted for different regions such as the Equatorial Front in the Eastern Pacific, and oceanic fronts in mid-latitudes such as the Gulf Stream, Kuroshio, and Agulhas Return Current. 相似文献
15.
Abstract The effects of marine fronts on the local atmospheric surface layer and air‐sea interaction were studied. Several mesoscale fronts were crossed by a research vessel in the Greenland Sea. Air temperature, humidity and stability conditions, and the fluxes of momentum, as well as sensible and latent heat, were investigated. For relatively calm conditions, close air‐sea coupling was observed in the temperature whereas for stronger winds, the air temperature of the surface layer was not markedly modified by the front below. Changes in the moisture content in the frontal area were observed and, in one case, evaporation was observed on the warm water side and condensation on the cold water side of the front. Frontal differences in heating from the sea were assumed to affect the surface‐layer wind field. 相似文献
16.
华西秋雨起止与秋冬季节大气环流转换 总被引：1，自引：0，他引：1
根据1961—2010年平均的逐候NCEP/NCAR再分析资料、1979—2008年平均的逐候CMAP降水资料以及1961—2010年逐候平均的中国553个台站降水资料,讨论了华西秋雨起止日期与秋冬季大气环流转换特征的关系。结果表明,华西地区降水年变化表现为明显的夏、秋双峰特征,8月4—8日(第44候)为双峰间的低谷,10月8—12日(第57候)以后降水降至年平均以下。由此,将华西秋雨建立和结束日期分别确定为8月9—13日(第45候)和10月8—12日(第57候)。华西秋雨的建立对应于东亚夏季风开始向冬季风转变,其标志性环流调整特征是江南地区的西南风转为东南风。东亚经向海平面气压梯度在8月9—13日(第45候)由南高北低转为南低北高,造成850 hPa江南地区的西南风转为东南风,该东南风与来自孟加拉湾的热带西南季风交汇于华西地区,形成风向和水汽的辐合,使得华西地区的降水在夏峰之后再次增强,华西秋雨由此建立。华西秋雨的结束则对应于孟加拉湾热带西南季风结束和东亚冬季风完全建立,其标志性环流调整特征是孟加拉湾地区的西南风转为东北风。随着东亚纬向海平面气压梯度由北向南依次发生东高西低向东低西高的转变,东亚冬季风也逐步向南推进,9月8—12日(第51候)东北冬季风到达江南地区,10月8—12日(第57候)进一步推进到南海地区,此时来自孟加拉湾的热带西南季风消失,造成华西地区完全受大陆冷高压控制,东亚季风经圈环流也转为冬季型哈得来环流,东亚冬季风完全建立,华西秋雨也随之结束。因此,华西秋雨起止可能与东亚夏季风、南亚夏季风向冬季风的转变时间不同步有关,东亚季风与南亚季风的共同作用使得华西秋雨成为亚洲夏季风在中国大陆上的最后一个雨季。 相似文献
17.
Abstract Monthly mean sea‐level pressure (SLP) data from the Northern Hemisphere for the period January 1952‐December 1987 are analysed. Fluctuations in this field over the Arctic on interannual time‐scales and their statistical association with fluctuations farther south are determined. The standard deviation of the interannual variability is largest compared with that of the annual cycle along the seaboards of the major land masses. The SLP anomalies are generally in phase over the entire Arctic Basin and extend south over the northern Russia and Canada, but tend to be out of phase with fluctuations at mid‐latitudes. The anomalies are most closely associated with fluctuations over the North Atlantic and Europe except near the Chukchi Sea to the north of Bering Strait. The associations with the North Pacific fluctuations become increasingly more prominent at most Arctic sites (e.g. the Canadian Arctic Archipelago) as the time‐scale increases. Associations between the SLP fluctuations and atmospheric indices that represent processes affecting sea‐ice drift (wind stress and wind stress curl) are determined. In every case local associations dominate, but some remote ones are also evident. For example, changes in the magnitude of the wind stress curl over the Beaufort Sea are increased if the atmospheric circulation over the North Pacific is intensified; wind stress over the region where sea ice is exchanged between the Beaufort Gyre and the Transpolar Drift Stream is modulated by both the Southern and North Atlantic Oscillations. Severe sea‐ice conditions in the Greenland Sea (as measured by the Koch Ice Index) coincide with a weakened atmospheric circulation over the North Atlantic. 相似文献
18.
To examine the correlation between the sizes of sea breeze fronts and pollutants under the influence of synoptic fields, a numerical simulation was conducted in the southeast coastal area of the Korean Peninsula, where relatively high concentrations of pollutants occur because of the presence of various kinds of industrial developments. Sea breeze and sea breeze front days during the period 2005-09 were identified using wind profiler data and, according to the results, the number of days were 72 and 53, respectively. When synoptic forcing was weak, sea breeze fronts moved fast both in horizontal fields and in terms of wind velocity, while in the case of strong synoptic forcing, sea breeze fronts remained at the coast or moved slowly due to strong opposing flows. In this case, the sea breeze front development function and horizontal potential temperature difference were larger than with weak synoptic forcing. The ozone concentration that moves together with sea breeze fronts was also formed along the frontal surfaces. Ozone advection and diffusion in the case of strong synoptic forcing was suppressed at the frontal surface and the concentration gradient was large. The vertical distribution of ozone was very low due to the Thermal Internal Boundary Layer (TIBL) being low. 相似文献