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1.
New oceanographic observations are used for studying the Kamchatka Current and the Alaskan Stream and its Aleutian eddies in 1990–2017. The Aleutian eddies are mesoscale anticyclonic eddies that are formed within the Alaskan Stream southward of the Aleutian Islands be tween 170° and 180° E and are moving to the southwest. The rapid freshening of the upper layer and the increase in tem-perature and salinity in the Kamchatka Current halocline are detected. In the upper layer of the Kamchatka Current, salinity decreased by 0.2 psu per 27 years. The most rapid variations in salinity and temperature have been observed in recent years. In the halocline (at the isopycnic of 26.75σθ) temperature rose by 1.4°C and salinity in creased by 0.15 psu. The maximum temperature of the warm intermediate layer in the Kamchatka Current exceeded 4°C for the first time. The most likely reason for the temperature and salinity increase in the halocline is the transport of warm and salt water by the Aleu-tian eddies. 相似文献
2.
T. R. Kil’matov 《Russian Meteorology and Hydrology》2008,33(6):383-387
A simple variational model of the zonal region between waters has been developed with a specified density gradient and a convergence zone. An approximate analytical solution has been constructed. The boundary between waters is shown to divide into two fronts, a convergence front and a density front. The density front should be shifted equatorward relative to the convergence axis. Such a structure corresponds to the subarctic/subtropical boundary in the Pacific Ocean: the subarctic front and the Kuroshio Extension front that goes into the North Pacific Current. 相似文献
3.
Seasonal variations of hydrological conditions in the area adjoining the southeastern coast of Sakhalin Island are described based on the analysis of monthly mean temperature and salinity obtained over standard oceanic sections Makarov-Cape Georgii and Cape Svobodny-the sea and from nine oceanic surveys. The Poronai River runoff that promotes the formation of a warm surface layer with low salinity largely influences the water area of Terpeniya Bay in the northern part of the area studied. In spring, these waters primarily spread southward along the coast; in summer, they flow southeastward, forming a weak vortex structure at 144° E. In the fall, major changes occur below 20 m, where waters of the cold intermediate layer are replaced by warmer waters (4–6°C) of low salinity connected with the Amur River runoff. The destruction of the CIL core near the shelf edge at depths of about 100 m resulting from the fall intensification of the East Sakhalin Current is pronounced in the southern, abyssal part of the region. The coastal area is covered by waters with salinity below 32‰ connected with the Amur River runoff. The volume of low-salinity waters coming through the Cape Svobodny-the sea section into the southern part of the Sea of Okhotsk is estimated at 3000 km3 taking into account instrumental measurements of flow rates. 相似文献
4.
Effects of interannual salinity variability on the barrier layer in the western-central equatorial Pacific: A diagnostic analysis from Argo 总被引：4，自引：0，他引：4
ABSTRACT In this paper, interannual variations in the barrier layer thickness （BLT） are analyzed using Argo three-dimensional temperature and salinity data, with a locus on the effects of interannually varying salinity on the evolution of the El Nifio Southern Oscillation （ENSO）. The interannually varying BLT exhibits a zonal seesaw pattern across the equatorial Pacific during ENSO cycles. This phenomenon has been attributed to two different physical processes. During E1 Nifio （La Nifia）, the barrier layer （BL） is anomalously thin （thick） west of about 160°E, and thick （thin） to the east. In the western equatorial Pacific （the western part： 130°-160°E）, interannual variations of the BLT indicate a lead of one year relative to those of the ENSO onset. The interannual variations of the BLT can be largely attributed to the interannual temperature variability, through its dominant effect on the isothermal layer depth （ILD）. However, in the central equatorial Pacific （the eastern part： 160~E- 170~W）, interannual variations of the BL almost synchronously vary with ENSO, with a lead of about two months relative to those of the local SST. In this region, the interannual variations of the BL are significantly affected by the interannually varying salinity, mainly through its modulation effect on the mixed layer depth （MLD）. As evaluated by a onedimensional boundary layer ocean model, the BL around the dateline induced by interannual salinity anomalies can significantly affect the temperature fields in the upper ocean, indicating a positive feedback that acts to enhance ENSO. 相似文献
5.
The Alaskan Stream south of the Blizhnii Strait disintegrates into mesoscale Aleutian eddies, which provide a westward transport
of warm water to the Kamchatka Current and upper Oyashio Current areas. Oceanographic observations from 1949 to 2009 are indicative
of a substantial rise of temperature and salinity in the intermediate waters of the Aleutian and Kamchatka currents. A long-term
temperature trend in the Aleutian Current in the intermediate layer (at isopicnal of 26.75σθ) amounted to ΔT = 0.013°C/year. A positive salinity trend was about 0.0014 psu/year. The ocean upperlayer salinity decreased with a rate
of −0.0021 psu/year simultaneously with the increase in salinity of the intermediate layer. The decreased salinity of the
upper layer and its increase in the intermediate layer result in the intensified halocline. The radius of the Aleutian eddies
significantly increased (by 50–100%), which is equivalent, at least, to twofold increase in the volume of the water transported. 相似文献
6.
A legacy seismic section across the Luzon Strait was reprocessed using the pre-stack depth migration method to reveal thermohaline structures in the water column. Distinct finescale and mesoscale features can be seen from the seismic image. Vertically, reflective patterns are associated with three water layers: upper layer, intermediate layer, and deep layer. The upper layer can be divided into three areas by two opposing weak-to-transparent zones from west to east with individual thicknesses: ～400, 550, and 700 m. They are interpreted as the South China Sea upper water, the Kuroshio water, and the Pacific upper water, respectively, separated by two Kuroshio frontal zones. Internal waves are ubiquitous in the Kuroshio water fluctuating in different amplitudes and wavelengths laterally. The finestructure shows the western Kuroshio front zone is composed of three subparallel blanking zones with an average eastward dipping angle of 2.3°. They are regarded as the well-mixed frontal interfaces developed in and along a multi-frontal frontal zone. The transparent reflection of the intermediate water above the Hengchun is suggestive of a well-mixed layer by the near-bottom turbulence. In the Pacific intermediate water near the eastern mouth of the Bashi Channel, there is an inverted crescent-shaped structure, which is likely associated with the intrusion of the South China Sea intermediate water through the Bashi Channel. These imaged features are consistent with the observed oceanographic phenomena in the region. 相似文献
7.
利用NCEP1°×1°6 h再分析资料,对副热带高压与西风槽典型环流形势配合下发生的一次四川区域性暴雨过程的不同阶段进行对比分析。结果表明,前期暴雨天气过程,其动力条件占到了主导地位,具有明显的经向垂直环流圈和垂直上升运动支,而在副高断裂后较强冷空气作用下,在副高边缘发生的区域性暴雨过程受西风带槽前的能量锋区影响,动力强迫作用和热力强迫作用激发的次级环流,进一步加强了四川盆地垂直运动的发展;冷空气作用前期的暴雨过程和冷空气进入后副高边缘发生的区域性暴雨过程中暴雨区域内的假相当位温均强于高层,大气处于对流性不稳定层结状态,对四川盆地暴雨的增强也起了不可忽视的作用,但由副高控制到副高逐渐断裂,湿位涡的斜压扰动是逐渐增强的过程,导致倾斜垂直涡度发展,激发更为强烈的上升运动;副高与西风槽环流形势相配合的暖区暴雨过程水汽主要来自中低层孟加拉湾;而副高断裂后发生在副高边缘的区域性暴雨过程,水汽主要来自850hPa层南海和孟加拉湾,从对流层中到低层,四川盆地东部恰恰是冷暖气流的交汇处,偏南气流将海上充沛的水汽输送到盆地东部,为暴雨的发生提供充足的水汽条件,并与对流层低层秦岭附近的东北冷气流交汇。 相似文献
8.
利用FNL1°×1°6 h再分析资料及常规资料,对比分析了2010年1月4-8日(简称“过程Ⅰ”)和12月2-6日(简称“过程Ⅱ”)北疆2次罕见暖区暴雪过程机理。结果表明,暴雪区上空θse锋区陡立和条件对称不稳定及垂直环流圈是形成两次暴雪过程的主要动力机制,水汽在西边界为整层输入,对流层低层为水汽强辐合区,暴雪区均具有暖湿结构。不同点:(1)过程Ⅰ的影响系统为低涡型,过程Ⅱ则为短波槽型;过程Ⅰ暴雪持续时间长,过程Ⅱ持续时间短;两个过程的高低空配置不同。(2)大西洋水汽在向东输送过程中,过程Ⅰ有波斯湾及阿拉伯海水汽的补充。(3)条件对称不稳定区形成的时间及中心有所差异,过程Ⅰ形成于暴雪前6 h,中心位于750 hPa,过程Ⅱ形成于暴雪前12 h,中心位于800 hPa及边界层;过程Ⅱθse锋区陡立结构比过程Ⅰ维持的时间长、强度强。 相似文献
9.
利用NCEP1°×1°再分析资料、常规高空及地面资料,对2010年8月12~14日川西高原北部阿坝州东南部的漩映地区出现的连续性暴雨形成机制进行了探讨。结果表明:此次过程发生在副热带高压加强西伸至青藏高原形成一个强大的高压带,此高压带断裂后,在两高之间形成长时间切变,缓慢东移触发不稳定能量的释放;700hPa上西南低空急流为暴雨区输送了源源不断的水汽;地面冷锋受副高阻塞缓慢东移;地形摩擦抬升在盆地西部不断形成气流辐合都是造成此次连续性降水的直接原因。 相似文献
10.
Carried out is the modeling of the process of temperature variations in a droplet and possible ice coating under synoptic conditions observed in the Perm krai on December 14, 2010 that are characterized with the freezing rain fall at the temperature inversion in the atmospheric boundary layer. The phase transition on the moving water-ice interface, the curvature of the phase transition boundary, and variations of heat exchange on the boundary between the ice coating and atmosphere are taken into account. Computed is the thickness of the ice crust formed on fine droplets under conditions that provide the initiation of freezing precipitation. The evolution of the rate of the front of water crystallization on the droplet surface is defined and explained. 相似文献
11.
利用欧洲中期天气预报中心（European Centre for Medium-Range Weather Forecasts， ECMWF）再分析资料，基于大气扰动分解技术，对2012年7月华北东部两次副高边缘大暴雨事件进行扰动分析。结果表明：边界层及对流层低层扰动辐合中心与副高边缘大暴雨中心有较好地对应关系；扰动锋区和扰动比湿大值区（4 g·kg-1）叠加的区域与大暴雨落区相对应，与切变线类暴雨不同，副高边缘暴雨中心并不是出现在冷暖空气対峙扰动（0 ℃线）的位置，而是发生在扰动锋区内的暖区一侧（扰动温度0 ℃以南）；两次过程均存在自南向北的水汽通道，且水汽在输送过程中不断得到抬升，大暴雨落区对应的扰动水汽通量散度中心分别达到-6.8×10-8g·cm-2·hPa-1·s-1和-11.9×10-8g·cm-2·hPa-1·s-1，为大暴雨的形成提供了较好地水汽条件。 相似文献
12.
长江中下游地区暖区暴雨特征分析 总被引：8，自引：6，他引：2
利用2007到2013年5-9月间常规和非常规资料以及6 h一次的NCEP 1°×1°再分析资料,将长江中下游地区暖区暴雨按天气形势划分为冷锋前暖区暴雨、暖切变暖区暴雨以及副热带高压边缘暖区暴雨三种类型。统计表明暖区暴雨一般发生在距离切变线(锋线)100~300 km的暖区内。主要结论包括:(1)冷锋型降水强度偏弱且分布均匀,集中在5、6月;暖切变型发生次数最多且强度大,主要发生在6、7月长江中下游地区的偏南部;副热带高压边缘型发生次数最少但强度较大,发生在7、8月。暖区暴雨的发生次数及强度在大别山、皖南山区较为集中。(2)暖区暴雨中短时强降水贡献大。(3)冷锋背景下的暖区暴雨一般产生在锋前低压槽中,暴雨落区与高低空急流耦合有紧密联系;暖切变型以低层暖切变线为主要天气背景,地面常有弱静止锋,暖区对流活动与中尺度急流结构、地形强迫等因素存在较高的相关性;副热带高压边缘暖区暴雨与局地的水汽积累和对流不稳定条件的发展有密切关系。据此建立三类暖区暴雨的概念模型。 相似文献
13.
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
14.
Michael Frech 《Boundary-Layer Meteorology》1998,87(1):41-68
The impact of mesoscale moisture variability on the vertical energy transfer through a pre-frontal boundary layer is studied with NOPEX aircraft data. The moisture variability relates to a cold front that passed the area 2 1/2 hours after the observations. We find a density front ahead of the cold front. The large vertical divergence of the turbulent moisture flux in the surface layer is partly related to this moisture variability. Large scale horizontal advection contributes to the observed vertical turbulent flux divergence. The estimated horizontal mesoscale advection term in the budget of sensible heat and moisture is on average small but locally it can be large. This term acts to re-distribute moisture in the boundary layer and leads to sub-grid variations of relative humidity, which is an important quantity for boundary-layer cloud models. The distinct spatial variations of specific humidity are mainly related to synoptic forcing and not to heterogeneity in the surface energy balance. 相似文献
15.
应用常规气象观测资料、NCEP 1°×1°再分析资料,选取登陆北上山东地点相近但暴雨落区分别位于台风中心西北侧和东北侧的两个台风,分析暴雨落区相对台风中心非对称分布的成因。结果表明：台风进入中纬度以后,0421号台风“海马”位于高空深槽前,与西风槽相互作用,西风槽携带的冷空气从西北侧侵入台风环流,产生湿斜压锋区强迫抬升、冷暖空气交绥、水汽辐合等因素造成暴雨,暴雨趋于出现在台风中心的西北侧,为高比湿舌前方、较强水汽辐合区与相当位温密集区叠加的区域;而0509号台风“麦莎”与副热带高压相互作用,引起涡度及涡度平流的非对称改变,暴雨区与500 hPa正涡度区或正涡度平流相对应,暴雨趋于出现在台风中心的东北侧,为强正涡度平流区与水汽辐合叠加的区域。 相似文献
16.
应用1971—2016年河西走廊东部代表站的地面观测资料、NCEP 2.5°×2.5°月均地面至300 hPa高空资料,2006—2016年民勤逐日07和19时每隔10 m加密高空资料,分析了近45年河西走廊东部冬季沙尘暴天气的年际变化特征。同时选取2016年11月两次沙尘暴天气过程从天气学成因、物理量场及近地面边界层特征等方面进行了诊断分析。结果表明:近45年河西走廊东部冬季沙尘暴日数呈减少趋势,产生大风沙尘天气的主要原因不仅与大型冷暖空气强度及环流形势有关,还与冷锋过境时间、日变化、近地层风速和干湿程度关系密切。夜间至早晨近地面逆温厚且强,大气层结稳定,削弱沙暴强度,而午后到傍晚,逆温薄而弱,大气层结不稳定性强,加强了动量下传和风速,增强沙暴强度。近地层越干,风速越大,沙暴越强。 相似文献
17.
本文使用常规观测资料、卫星云图、自动气象站降水量以及0.25°×0.25°的NCEP/NCAR再分析资料,对出现在东北地区北部受不同系统影响的连续2d暴雨过程的热力和动力场结构特征展开研究。结果表明:24日为暖锋锋生暴雨,暴雨范围大;25日为台风暴雨,暴雨出现在台风移动路径上,为狭长带状。暴雨是由MCS活动造成的,每次短时强降水均与TBB低值中心相对应,台风倒槽内的MCS强度比暖锋云系内的MCS弱,但是降水强度却更大。台风安比携带大量暖湿空气,其东侧的低空急流向北输送热量和水汽,水汽辐合集中在边界层内,台风暴雨的水汽辐合强度比暖锋暴雨更强烈,所造成的雨强更大。暖锋暴雨期间,小兴安岭迎风坡地形的辐合抬升作用明显;高层强辐散及地形辐合抬升作用对暴雨有较大贡献。台风暴雨期间,低空辐合,特别是水汽辐合作用对暴雨有较大贡献;辐合区位于台风倒槽附近,倒槽表现为冷锋性质。 相似文献
18.
The seasonal variability of oceanographic conditions in the southern part of the Sea of Okhotsk is described based on long-term mean temperature T and salinity S from observations along a standard oceanographic section Cape Aniva-Cape Dokuchaev (May–November). It is shown that the Soya Current is relatively weak in spring, with low temperature and salinity gradients along the section. The Sea of Okhotsk low-salinity water mass is observed in the upper layer. It was formed as a result of melting of a large amount of ice brought here with the East Sakhalin Current from the northwestern part of the Sea of Okhotsk. A cold intermediate layer (CIL) at depths of 50–150 m extends along the entire section. The cold intermediate layer core with a temperature at the edge of the Sakhalin shelf of about ?1.3°C is retained during a period of maximum warming in August; however, in October–November the intensified flow of the East Sakhalin Current (up to 50 cm/s) results in a situation when relatively warm low-salinity waters, connected with the Amur River runoff, dissipate CIL. The results of 12 surveys conducted by the Sakhalin Research Institute for Fisheries and Oceanography in 1998–2004 show significant deviations of T and S [10] in different years from the calculated values. Generally, maximum anomalies (ΔT > 4°C and ΔS > 0.55‰) are observed in the surface layer. Their values and statistical significance decrease with depth. However, the situation is opposite in some cases. The maximum deviation from normal was observed in June 1999, when warm and salt waters were located much further seaward from the Kunashir shelf, which is most likely connected with the Soya Current meandering. 相似文献
19.
20.
The influence of interannual variability of water transport by the East Kamchatka Current, the Oyashio, and the East Sakhalin Current on the dissolved oxygen concentration in the western subarctic Pacific and the Sea of Okhotsk is considered for studying climate change impact on sea water chemical parameters. It is shown that statistically significant relation is observed between the calculated with the Sverdrup equation interannual variations in water transport with the East Kamchatka Current, the Oyashio, and the East Sakhalin Current and changes in mean sea water level at coastal stations in winter. It is found that the main reason of interannual variability of the dissolved oxygen concentration at isopycnic surfaces in the intermediate water layer (100–800 m) of the Sea of Okhotsk and in the western subarctic Pacific is caused by variations in water transport by the East Kamchatka Current, the Oyashio, and the East Sakhalin Current. 相似文献