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1.
中尺度涡旋影响吕宋海峡黑潮变异的动力机制 总被引：5，自引：1，他引：4
使用1.5层约化重力准地转模式,研究了西边界流在西边界缺口处当处于迟滞过程的临界状态时,其路径转变受中尺度涡旋影响的动力机制,初步探讨了中尺度涡旋影响西边界流在缺口处路径变化的几种形式.结果表明,气旋和反气旋中尺度涡旋都可能使西边界流产生由入侵流态到跨隙流态的转变,而只有反气旋式中尺度涡才有可能诱发西边界流由跨隙流态向入侵流态的转变.当西边界流远离其临界状态时,其路径不容易受中尺度涡旋的影响,此时跨隙的西边界流会阻挡中尺度涡旋在缺口处的向西传播,并迫使涡旋在吕宋海峡东侧向北移动.以上结果用来解释了吕宋海峡黑潮变异的某些结构特征. 相似文献
2.
为研究风急流对吕宋海峡处黑潮路径的影响,本文使用1.5层约化重力浅水模式,设置了与吕宋海峡跨度相接近的缺口宽度,考虑西边界流在西边界缺口处当处于迟滞过程的临界状态时,其路径受风急流影响的动力机制,并初步探讨了在实际海陆边界条件下,实际风急流对黑潮路径的影响。结果显示,理想情况下,当西边界流处在由入侵流态到跨隙流态转变的临界状态时,西风、南风以及西南风风急流可以激发西边界流由入侵流态转变为跨隙流态。当西边界流处在由跨隙流态向入侵流态转变的临界状态时,北风、东风以及东北风风急流可以激发西边界流由跨隙流态转变为入侵流态,并且在风急流消失后西边界流不能再恢复到初始流态。实际情况下,冬季风急流有利于黑潮入侵南海,夏季风急流有利于黑潮跨越吕宋海峡,这和理想情况下的模拟结果以及实际观测结果相一致,这对进一步研究南海北部的上层环流以及南海的质量、能量输送有重要意义。 相似文献
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基于日本气象厅长时间序列的温、盐度再分析资料,利用动力计算方法分析了北太平洋西边界的北赤道流及其下游黑潮和棉兰老流流量的年际和年代际变化,并探讨了北赤道流变化的可能原因。结果表明,北赤道流和黑潮具有比较一致的年际和年代际变化,均在1976年前后发生了一次气候跃变,之后有长期偏强的趋势,而棉兰老流的年际和年代际变化则有所不同。特别是,北赤道流1976年之后增加的流量似乎大多进入黑潮,而流入棉兰老流的流量则减少。进一步的分析还表明,西传的Rossby波和棉兰老冷涡的变动可能对北赤道流的年际变化有重要影响。 相似文献
5.
通过最新的高分辨率再分析海洋数据资料,对于东海黑潮以及琉球群岛以东海域的海流进行了研究。结果表明琉球群岛以东西边界流最大流速出现在600~1200 m深度的地形坡度最大处,大小约为0.2 m/s。由于冲绳岛以南庆良间水道的水交换对于东海黑潮流量有重要的影响,东海黑潮的平均流量从南向北逐渐递增,平均流量为28×106~35×106m3/s;琉球群岛以东的西边界流流量则比东海黑潮小一个量级,平均值小于其变化的方差;由于受庆良间水道海流的影响,冲绳岛东侧的流量要远小于奄美大岛东侧的流量。同一纬度大洋中西传的Rossby波对琉球群岛以东的西边界流有较大影响,因此琉球群岛以东西边界流的流量有大约100 d的显著变化周期。庆良间水道以南的东海黑潮由于主要受台湾以东黑潮流量的控制,也有大约100 d的显著变化周期,庆良间水道以北的东海黑潮则没有该特征。 相似文献
6.
印尼贯穿流的诊断计算 总被引：2，自引：0，他引：2
利用全球大洋二维的自由表面诊断模型并采用气候态Levitus(2001)温盐资料及COADS风应力资料估算印尼贯穿流及其季节变化。结果表明,南海的Karimata海峡出流量对印尼贯穿流有显著的贡献,印尼贯穿流的平均流量为16.6Sv,流量在6月最大(18.5Sv),4月最小(12.7Sv)。与其它模式结果和观测结果一致的是,Makas-sar海峡流量在7月最大(13.8Sv),1月最小(0.2Sv),其年平均流量为6.7Sv;Karimata海峡是南海南部最大的出水口,年平均流量为2.6Sv,爪哇海水在5—9月之间流入南海,其它月份南海南部水流入爪哇海;Timor海峡是印尼贯穿流最大的出口;Lombok流量的季节变化表现为半年周期。通过模拟计算结果,结合动力计算,获取了Makassar海峡经向速度的垂向结构,结果显示Makassar海峡的经向速度有明显的垂向切变,100m层次的南向速度为30—35cm.s-1。 相似文献
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本文基于海洋环流模式模拟的高分辨率欧拉场，利用拉格朗日追踪方法，评估了印尼贯穿流（ITF）对印度洋的热量贡献。通过计算ITF水体在印度洋的传输路径及伴随的温度变化来获取ITF水体在印度洋的热量传输过程。模拟结果表明ITF进入印度洋后主要向西流动并在到达马达加斯加后分叉，进入南、北印度洋。热收支分析表明ITF在北印度洋吸收0.41 PW热量，在南印度洋释放0.56 PW热量；这两个过程相互补偿，导致ITF对整个印度洋的净加热贡献并不显著，只有0.15 PW。进一步的检查ITF离开印度洋的出口（跨过34°S），结果表明ITF主要随着位于西边界的奥古拉斯流和位于东边界的利文流离开印度洋。约89%的ITF水体沿着西边界离开印度洋，其余的11%主要沿着东边界离开印度洋；前者对整个印度洋的净加热贡献为0.10 PW，后者的净加热贡献为0.05 PW。 相似文献
8.
西边界流在边界“豁口”的形变及其机制 总被引：1，自引：0，他引：1
大洋西边界流在边界豁口处由于失去边界的支持而发生形变。本文将西边界流视为一种惯性射流，遵循绝对涡度守恒原理，推导了流轴及其两侧流体在西边界豁口处不同形式的弯曲，发现在一定的豁口尺度条件下，西边界流自身的相对涡度分布特点和地球旋转的β效应决定了在失去西侧陆坡支持时，其主体会沿反气旋路径发生一段经向的位移而圈回入射点所在的经度位置。主轴变形的经向尺度与初始速度及西边界流的入射角度有关；主轴西侧可能会出现一小部分分支进入邻近的内海并形成气旋或反气旋式环流；主轴东侧的流体则在豁口以东沿反气旋路径弯曲，从而论证了西边界豁口处形成西边界流弯曲的可能性和原因 相似文献
9.
采用经验正交分解(Empirical Orthogonal Function,EOF)分析方法对印尼贯穿流出流海域卫星测高海面高度异常资料进行了分析,分析结果显示研究海域海面高度异常存在多时间尺度变化特征。1993—2013年期间,研究海域海面高度异常场存在明显的升高趋势,其升高速率为0.6 cm/a;研究海域海面高度异常存在显著的年际变化,其与Niño3.4指数的相关系数超前滞后相关最大可达0.65,且厄尔尼诺年偏高,拉尼娜年偏低;海面高度异常年周期变化显著海域主要受印尼贯穿流、印度洋南赤道流和Eastern Gyral Current(EGC)季节变化的影响,半年周期变化则对应于爪哇沿岸流与南赤道流共同作用下形成的涡旋的半年周期变化;另外,研究海域海面高度异常还存在显著的季节内变化特征。 相似文献
10.
利用高分辨率的OFES数据,通过对中南半岛和海南岛沿岸比较有代表性的几个断面进行流速剖面分析和体积输送量计算,初步探讨了南海西边界流的时空特征.结果显示南海西边界流的季节变化特征明显:夏季向北流,冬季向南流,且冬季强于夏季.在体积输送大小上,越南沿岸流的体积输送量大小为(7.4±7.0)Sv,紧邻海南岛的沿岸流大小仅为(0.57±0.5)Sv,112.0°E以东的海南沿岸西边界流体积输送大小约为(4.8±1.9)Sv,并且常年向南流动.夏季的南海西边界流在北上到达中南半岛的东南部以后偏离岸线向东流动.随着夏季风的盛行,离岸流的流速变大,主轴发生了明显的摆动,由14.0°N移动到了10.0°N.离岸流对西边界流有着显著的影响作用. 相似文献
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Alternating zonal flows in an idealized wind-driven double-gyre ocean circulation have been investigated using a two-layer
shallow-water eddy-permitting numerical model. While the alternating zonal flows are found almost everywhere in the time-mean
zonal velocity field, their meridional scales differ from region to region. In the subpolar western boundary region, where
the energetic eddy activity induces quasi two-dimensional turbulence, the alternating zonal flows are generated by the inverse
energy cascade and its arrest by Rossby waves, and the meridional scale of the flows corresponds well to the Rhines scale.
In the eastern part of the basin, where barotropic basin modes are dominant, the zonal structure is formed through the nonlinear
effect of the basin modes and is wider than the Rhines scale. Both effects are likely to form zonal structure between the
two regions. These results show that Rossby basin modes become an important factor in the formation of alternating zonal flows
in a closed basin in addition to the arrest of the inverse energy cascade by Rossby waves. The wind-driven general circulation
associated with eddy activities plays an essential role in determining which mechanism of the alternating zonal flows is possible
in each region. 相似文献
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The response of the Gulf of Alaska (GOA) circulation to large-scale North Pacific climate variability is explored using three high resolution (15 km) regional ocean model ensembles over the period 1950-2004. On interannual and decadal timescales the mean circulation is strongly modulated by changes in the large scale climate forcing associated with PDO and ENSO. Intensification of the model gyre scale circulation occurs after the 1976-1977 climate shift, as well as during 1965-1970 and 1993-1995. From the model dynamical budgets we find that when the GOA experiences stronger southeasterly winds, typical during the positive phase of the PDO and ENSO, there is net large-scale Ekman convergence in the central and eastern coastal boundary. The geostrophic adjustment to higher sea surface height (SSH) and lower isopycnals lead to stronger cyclonic gyre scale circulation. The opposite situation occurs during stronger northwesterly winds (negative phase of the PDO).Along the eastern side of the GOA basin, interannual changes in the surface winds also modulate the seasonal development of high amplitude anticyclonic eddies (e.g. Haïda and Sitka eddies). Large interannual eddy events during winter-spring, are phase-locked with the seasonal cycle. The initial eddy dynamics are consistent with a quasi-linear Rossby wave response to positive SSH anomalies forced by stronger downwelling favorable winds (e.g. southwesterly during El Niño). However, because of the fast growth rate of baroclinic instability and the geographical focusing associated with the coastal geometry, most of the perturbation energy in the Rossby wave is locally trapped until converted into large scale nonlinear coherent eddies. Coastally trapped waves of tropical origin may also contribute to positive SSH anomalies that lead to higher amplitude eddies. However, their presence does not appear essential. The model ensembles, which do not include the effects of equatorial coastally trapped waves, capture the large Haïda and Sitka eddy events observed during 1982 and 1997 and explain between 40% and 70% of the tidal gauges variance along the GOA coast.In the western side of the GOA basin, interannual eddy variability located south of the Alaskan Stream is not correlated with large scale forcing and appears to be intrinsic. A comparison of the three model ensembles forced by NCEP winds and a multi-century-long integration forced only with the seasonal cycle, shows that the internal variability alone explains most of the eddy variance. The asymmetry between the eddy forced regime in the eastern basin, and the intrinsic regime in the western basin, has important implications for predicting the GOA response to climate change. If future climate change results in stronger wintertime winds and increased downwelling in the eastern basin, then increased mesoscale activity (perhaps more or larger eddies) might occur in this region. Conversely, the changes in the western basin are not predictable based on environmental forcing. Eastern eddies transport important biogeochemical quantities such as iron, oxygen and chlorophyll-a into the gyre interior, therefore having potential upscale effects on the GOA high-nutrient-low-chlorophyll region. 相似文献
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Effect of Taiwan Strait Current on the onshore intrusion of Kuroshio: A geostrophic adjustment model
Young Ho Seung 《Ocean Science Journal》2012,47(1):41-50
The effect of the Taiwan Strait Current on the onshore intrusion of Kuroshio, both contributing to the formation of Tsushima
Warm Current, is addressed theoretically by invoking a geostrophic adjustment model previously proposed. The idealized model
assumes two unbounded basins, shallow and deep, separated by an infinitely long and thin barrier. On either side of the barrier,
a western boundary current in the deep basin and a shelf current in the shallow basin flow along the barrier with the surface
elevation of the former higher than that of the latter. When a part of the barrier is removed and a gap is created, the onshore
part of the western boundary current intrudes onto the shallow basin through the gap while conserving its potential vorticity.
Both the intruding current and the shelf current will later geostrophically adjust themselves to the disturbances created
by the intrusion. Model results show that the transport of onshore intrusion increases with the sea level difference imposed
initially between the deep and shallow basins across the barrier, indicating that the sea level rise associated with the strengthening
of shelf current inhibits the shelf-ward intrusion. The intruding current is in jet mode when its transport is maximized,
which otherwise is in coastal mode. The maximization of transport occurs when the sea level difference between the two basins
is sufficiently large. Although this model greatly idealizes the problem, it explains well the observed fact that the transport
of Tsushima Warm Current is fed mostly by the Taiwan Strait Current in summer when the latter becomes the strongest, and by
the onshore intrusion of Kuroshio in winter when the Taiwan Strait Current nearly vanishes, suggesting that the seasonal variation
of the onshore intrusion of Kuroshio is largely due to the seasonal variation in the strength of the Taiwan Strait Current. 相似文献
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Hideo Nitani 《Journal of Oceanography》1975,31(4):154-173
The variations of the velocity and path of the Kuroshio are investigated by using the data obtained after the World War II. The time scales of these variations are classified into three categories,i.e. long-, medium- and short-terms. Period of the long-term variations seems to be about 7 to 9 years. Large meanders of the Kuroshio off Enshu-nada in 1953–1955 and 1959–1962 are accompanied with the low mean velocity of the Kuroshio. These large meanders are explained as a stationary Rossby wave by applying the equation for the phase velocity of the barotropic Rossby wave with the disturbance of finite width. To obtain the above conclusion, it is assumed that the Kuroshio extends down to the depth of 2,300 db and that the east component of the over-all mean velocity of the meandering Kuroshio should be substituted for the velocity of the eastward basic current in the above equation. As for the medium-term variation of the Kuroshio, there seems to exist variations in the velocity with the periods of 4, 6, 8 and 12 months and those in the position of the Kuroshio axis with the periods of 8 and 12 months. These meanders of the Kuroshio progress towards east with the mean phase velocity of about 5 miles a day, which is nearly the same as the calculated mean phase velocity of a progressive Rossby wave. 相似文献
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1Introduction Planetary waves involve the main processes bywhich perturbation signal in one part of the ocean istransferred to another part.In the1970s,mostof theprevious theoretical studies focus on the local Ekmanpumping and the nondispersive long baroc… 相似文献
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研究海平面上升对河口的影响情况有助于了解输运过程的变化,基于21世纪海平面上升预测研究(陈长霖,2012;张吉,2014),本文选取珠江河口这一径优型与潮优型并存的河口为研究区域,利用数值模拟的方法,研究其在未来海平面上升后可能出现的响应。结果表明,河口的平均盐度、咸潮上溯距离和层化强度都将随着海平面的上升而增加,这些因素的变化有着明显的季节性。伶仃洋平均盐度在4月和10月增加更多;伶仃洋枯水期咸潮上溯距离的增量大于丰水期,磨刀门则相反;伶仃洋丰水期层化强度及其增量都要大于枯水期。海平面上升后的输运过程响应结果显示:(1) 垂向输运时间将增加,虽然海平面上升带来的潮差潮流的增强将加强垂向混合,但是层化的加强会削弱垂向交换。垂向输运时间的增加是由于层化的加强,层化加强抑制了潮汐变化带来的影响,表层水更难交换到底层; (2) 南北向河口环流将加强,表层余流向海加强,底层余流向陆加强,南北向余流整体向海减小。造成这些现象的主要原因是海平面上升后水深增加带来的河道比降的减小和压力梯度力的改变。 相似文献
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In order to fulfill the no-slip condition at the western and eastern boundaries of the ocean basin, introduced ＂effective wind stress＂, which has much larger spatial variations towards the boundaries than in the ocean interior. The effective wind stress can thus be decomposed into spatially slow-varying and fast varying components. Careful scale analysis on the classical Munk winddriven ocean circulation theory, which consists of the interior Sverdrup flow and the western boundary current but of no eastern boundary current, shows that the wind stress curl appearing in the Sverdrup equation must have negligible spatial variations. In the present model the spatially slow-varying component of the wind stress appears in the Sverdrup equation, and the spatially fastvarying component becomes the forcing term of the boundary equations. As a result, in addition to the classical Munk solution the present model has an extra term at the western boundary which （Northern Hemisphere） increases the northward transport as well as the southward return transport, and has a term at the eastern boundary corresponding to the eastern boundary current. 相似文献