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INTRODUCTIONDissolvedorganiccarbon (DOC)makesupthesecondlargestofthebioactivepoolsofcar bonintheocean ,secondtothelargestpoolofdissolvedinorganiccarbon .Theglobaldissolvedorganiccarbonpoolisestimatedtobe 6 85Gt,avaluecomparabletothemassofCO2 intheat mosphere (Hedges,1 992 ) .Thesizeofthereservoir,aswellasitsdynamics ,indicatesthatDOCplaysacentralroleintheoceancarboncycle .AsitrelatestogreenhousegasessuchasCO2 andassociatesclimatecycle ,oceanicDOCbiogeochemicalcycleshavebeenoneoftheh… 相似文献
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Hydrographic observations collected by conductivity-temperature-depth(CTD) and instrumented elephant seals on the Prydz Bay continental shelf during 2012 and 2013 are used to characterize the intrusion of modified circumpolar deep water.As a regular occurrence,modified circumpolar deep water(MCDW) intrudes onto the shelf mainly between 150–300 m layer of 73°–75°E and then turns southeast affected by the cyclonic gyre of the Prydz Bay.The southernmost point of the warm water signal is captured on the east front of Amery Ice Shelf during March 2012.In terms of vertical distribution,MCDW occupies the central layer of 200 m with about 100 m thickness in the austral summer,but when to winter transition,the layer of MCDW deepens with time on the central shelf. 相似文献
3.
4.
内潮对吕宋海峡地转流动力计算的影响 总被引：1，自引：0，他引：1
利用2008年8~9月份吕宋海峡121°E断面上19.5°N~21°N之间4个连续站的CTD资料,讨论了内潮引起的温、盐剖面扰动对地转流诊断计算的影响,指出:在吕宋海峡,内潮引起的温、盐剖面扰动对地转流诊断计算的干扰不可忽略。因此,地转流诊断计算必须剔除温、盐剖面中的"内潮噪声"。另外,本文根据4个连续站时间平均后的温、盐剖面,通过动力计算法得到了吕宋海峡121°E断面上的地转流场,得出结论如下:吕宋海峡地转流速度较大部分多位于350 m以浅,流速最大值出现在表层;黑潮入侵南海主要发生于19.8°N~21°N的上层;在19.5°N~21°N之间,50~1 700 m深度范围内,海水体积通量呈现"上进下出"的垂向结构,350 m以浅为入流,流量约为2.6 Sv(1 Sv=1×106m3.s-1),350 m以深为出流,流量约为3.1 Sv。同期观测所得121°E断面上的盐度分布验证了本文所得地转流场的合理性。 相似文献
5.
应用镭-226解读南极普里兹湾表层水的来源与运移 总被引：1，自引：0，他引：1
中国第22次南极科学考察航次(2005年12月至2006年1月)期间,利用Mn-纤维富集大体积表层海水中的Ra同位素,并通过222Rn直接射气法测量226Ra的比活度,结果表明,普里兹湾表层水的226Ra比活度变化为0.92~2.09 Bq/m3,平均值为1.61 Bq/m3,在深海区域表现出226Ra含量高的特征。从空间分布看,表层水226Ra比活度呈现出由湾内向湾外增加的反常态势,反映出不同Ra含量水团的混合影响2。26Ra比活度与盐度的关系证实研究海域表层水的Ra含量主要受三种端元水体的混合所控制:其一为具有镭含量高、盐度高特征的南极夏季表层水;其二为低镭、低盐特征的冰融水;其三为高盐、中等镭含量的普里兹湾中深层水,该水体的226Ra纯粹由海底沉积物间隙水向上扩散所维持。结合S-226Ra示踪体系及上述三端元混合模型,计算出各组成水体的比例并描绘出它们的空间分布。南极夏季表层水的份额由湾外向湾内逐渐降低,并且在68°E断面向南影响范围较大;冰融水的比例由湾内向湾外降低,并且在湾内东部的高温水体中具有最大贡献;普里兹湾中深层水中受沉积物镭来源影响比较显著的区域出现在湾内西北部,其影响向湾外逐渐降低。冰融水与普里兹湾中深层水份额分别于普里兹湾湾顶东、西部出现高值的分布特征证实埃默里冰架前沿海流东进、西出的运移规律。 相似文献
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普里兹湾水文特征与变化 总被引：2，自引：1，他引：2
根据澳大利亚学者分别在１９８２年１２月和１９８７年２月普里兹湾的调查资料,并结合中国＂极地＂号南极考察船１９９０～１９９１年间的调查资料印证,提出在中国＂中山站＂所在地普里兹湾在初夏与晚夏期间的水文特征。 相似文献
7.
南极普里兹湾及其邻近海域表层水镭同位素的分布及应用 总被引：1，自引：0，他引：1
中国第27次南极科学考察期间(2010年12月30日至2011年1月16日),对普里兹湾及其邻近海域表层海水进行了226Ra和228Ra的分析,结果表明:226Ra和228Ra比活度的变化范围分别为1.47—2.43Bq/m3和0.17—0.45Bq/m3,平均值分别为2.13Bq/m3和0.29Bq/m3,228Ra/226Ra)A.R.(228Ra与226Ra的活度比)的变化范围为0.08—0.20,平均值为0.14。根据盐度和226Ra的质量平衡方程,计算出研究海域表层水中冰融水、南极夏季表层水和普里兹湾中深层水的份额。研究海域表层水中温度、盐度、226Ra、228Ra、228Ra/226Ra)A.R.和冰融水份额的空间分布显示,在埃默里冰架前沿海域,西侧海域较东侧海域具有低温、高盐、高226Ra、低228Ra、低228Ra/226Ra)A.R.、低冰融水份额的特征,证实埃默里冰架下水体东进西出的运动规律。根据埃默里冰架前沿东、西侧水体228Ra/226Ra)A.R.的差异,估算出埃默里冰架下表层水体东进西出所经历的时间为1.85a。此外,在普里兹湾湾口中部海域(66.5—67.5°S,72°—74°E),观察到次表层水的上升通风作用,该区域较高的228Ra含量和228Ra/226Ra)A.R.证明这些表层水体并非来自湾外绕极深层水的上涌,而可能来自湾内埃默里冰架输出水体。 相似文献
8.
自50年代后期以来国际上对普里兹湾区海洋过程的调査研究不断加强(Zverev,1959,1963; Izvekov,1959),尤其是进入80年代后,由于在现场考察中采用了CTD系统和浮标测流系统,人们对该区海洋过程的认识有了长足的进步。但由于该海区的热盐结构有非常显著的时空变化(Kornilov,1971; Smith et al.,1984; Middleton and Hamphries,1989;乐肯堂等,1996,1997),因而对该海区水团和环流中的若干重要问题,例如环流子午向分布向题,底层水形成问题,热盐结构时空变化间题等,仍缺乏足够的了解。
在乐肯堂等(1996,1997)的文章中,我们主要根据中国第六次(CNARE-Ⅵ,1989-1990)和第七次(CNARE-Ⅶ,1990-1991)南极考察中的海洋调查资料,分析了普里兹湾区的热盐结构、环流性质和混合过程。在本文中,我们将着重分析中国第八次(CNARE-Ⅷ,1991-1992)和第九次(CNARE-Ⅸ,1992-1993)南极考察中的CTD资料,并结合CNARE-Ⅵ,Ⅶ的资料,对该区的水团和环流的时空变化问题进行初步探讨。
关于CNARE-Ⅵ和 CNARE-Ⅶ的资料概况可见乐肯堂等(1996),不再重述。CNARE-Ⅷ的CTD断面设置与 CNARE-Ⅶ相同[参见乐肯堂等(1996)];但观测工作分为两个阶段:第一阶段从1991年12月31日至1992年1月5日,完成了从78°E至108°E共6个断面的测站;第二阶段,从1992年1月23日至25日,完成了68°E和73°E两个断面的测站。CNARE-Ⅸ的CTD断面如图1所示;观测工作也分两个阶段:第一阶段从1993年1月11日至1月15日,完成了I、Ⅱ、Ⅲ3个断面的测站;第二阶段从1993年1月29日至2月5日,进行了IV、V、Ⅵ3个断面的观测。这两次考察的CTD观测,每次均分为两个航次,而两个航次之间又都相隔二十余天,因而资料的同步性受到一定的影响。 相似文献
9.
南极普里兹湾及其邻近海域的水文结构特征和底层水的来源 总被引：8，自引：2，他引：8
利用中国第九次南大洋考察中南极普里兹湾及其邻近海域的CTD资料,分析研究了调查海域的水文结构特征及其该区南极底层水(AABW)的来源.研究结果表明,在研究海域,深水洋区近表层流由西向东流,而在普里兹湾内存在一个气旋型涡.水文结构中最明显的海洋学特征是:(1)绕极深层水(CDW)的涌升现象明显,涌升最强的位置是麦克罗伯逊地以北海域,最明显的深度是50～200m层,暖水涌升将冬季冷水分隔成南北两部分,并在其中形成孤立的暖水块;(2)陆缘水边界明显,这是绕极深层水与南极冷水之间形成的锋面,一般处在次表层水中,大致位于64°～66°S之间;(3)存在着双跃层结构.观测期间,普里兹湾以北探水海域存在着南极底层水,其来源可能有二:一为当地形成,二为源于威德尔海和罗斯海. 相似文献
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Variability of the Continental Water Boundary near the Prydz Bay 总被引：2，自引：0，他引：2
Based on the Data Obtained during the 15th Antarctic Expedition of Chian between November 1998 and February 1999,the paper discusses the water masses distributed on both sides of the Continental Water Boundary ( CWB) as well as the spacial variability of the physical characteristics of the central location, the frontal width, the frontal strength, the vertical depth, and the vertical thickness for CWB. The above results are compared with the results from the data obtained during the 9th Antarctic Expedition of China between December 1992 and February 1993, and the temporal variability of those characteristics is discussed. In addition, the inhomogeneity of the kinematic characteristics and the patterns of the dynamic heights for those water masses located on both sides of CWB are illustrated. As it is pointed out in the paper, the trough in the dynamic height field is identified with the frontal location of CWB and the oceanic current shear. Furthermore, the dynamic reason for the upwelling of the circumpolar deep water can be understood by the explanation described in the paper. 相似文献
11.
Sea ice characteristics between the middle Weddell Sea and the Prydz Bay, Antarctica during the austral summer of 2003 总被引：1，自引：0，他引：1
The antarctic sea ice was investigated upon five occasions between January 4 and February 15, 2003. The investigations included: (1) estimation of sea ice distribution by ship-based observations between the middle Weddell Sea and the Prydz Bay; (2) estimation of sea ice distribution by aerial photography in the Prydz Bay; (3) direct measurements of fast ice thickness and snow cover, as well as ice core sampling in Nella Fjord; (4) estimation of melting sea ice distribution near the Zhongshan Station; and (5) observation of sea ice early freeze near the Zhongshan Station. On average, sea ice covered 14.4% of the study area. The highest sea ice concentration (80%) was observed in the Weddell Sea. First-year ice was dominant (99.7%-99.8%). Sea ice distributions in the Prydz Bay were more variable due to complex inshore topography, proximity of the Larsemann Hills, and/or grounded icebergs. The average thickness of landfast ice in NeUa Fjord was 169.5 cm. Wind-blown snow redistribution plays an important role in affecting the ice thickness in Nella Fjord. Preliminary freezing of sea ice near the Zhongshan Station follows the first two phases of the pancake cycle. 相似文献
12.
Takashi Yabuki Toshio Suga Kimio Hanawa Koji Matsuoka Hiroshi Kiwada Tomowo Watanabe 《Journal of Oceanography》2006,62(5):649-655
It has been inferred that the Prydz Bay region is one of the source regions of Antarctic Bottom Water (AABW) based on rather
indirect evidence. In order to examine this inference, we investigate the hydrographic condition of the bay based mainly on
XCTD data obtained during the Japanese Whale Research Program in the Antarctic (JARPA). The JARPA hydrographic data reveal
Circumpolar Deep Water (CDW), which is a salty, warm water mass approaching the shelf break, and capture Modified CDW (MCDW)
intruding into the shelf water. AABW production requires mixing of CDW and cold shelf water saltier than 34.6 psu, which is
a saltier type of Low Salinity Shelf Water (LSSW). Saltier LSSW is observed near the bottom over the shelf, being mixed with
MCDW. We further identify saltier LSSW near the shelf break. This saltier LSSW appears close enough to unmodified CDW to be
mixed with it over the continental slope, indicating a possible source of AABW in Prydz Bay. 相似文献
13.
北黄海冷水团季节变化特征分析 总被引：3，自引：0，他引：3
利用2006—2007年春、夏、秋、冬4个航次的CTD数据,对北黄海冷水团的季节变化及其消长过程进行了分析.结果显示:春季,冷水团特征开始出现,6℃冷水占据了调查区域的1/3,冷水团中心的盐度值大于32 psu.成山头以东的高盐水舌主轴从冬季的124°E西移至123.3°E处;夏季,北黄海冷水团特征最为明显,核心温度约6℃,盐度高于32 psu,盘踞在50 m等深线以深的深槽中,温、盐呈现明显的双峰结构.与前人的结果相比,本文低温中心的位置偏东;秋季,北黄海冷水团强度减弱,但仍存在2个低温中心,并且高盐中心位于38.5°N,122.5°E附近;在垂直方向上,冷水团与上层水之间以温跃层为分界:温跃层春季时形成,位于20～30m;夏季达到最强,跃层在10～20m;秋季减弱,跃层深度降至30～40m;至冬季温跃层完全消失. 相似文献
14.
基于2004—2018年Argo (Array for Real-Time Geostrophic Oceanography)浮标观测的温度、盐度数据, 利用经验正交函数(EOF)分析和小波分析等方法对北印度洋(40°—105°E, 5°S—25°N)障碍层时空分布特征进行分析。结果显示: 北印度洋的东部常年存在障碍层, 而西部障碍层出现的概率相对较低; 较厚的障碍层出现在阿拉伯海东南部(67°—75°E, 3°—12°N)、孟加拉湾(82°—93°E, 11°—20°N)和赤道东印度洋(81°—102°E, 4°S—3°N)。阿拉伯海东南部和孟加拉湾障碍层厚度以年变化为主, 且呈同位相变化, 均为冬季最大, 夏季最小。赤道东印度洋区域则主要呈现半年周期变化, 在夏季和冬季各出现一次峰值。进一步分析表明, 孟加拉湾和赤道东印度洋障碍层厚度主要受等温层深度变化影响, 混合层深度变化对障碍层厚度变化的影响相对较小; 阿拉伯海障碍层厚度同时受等温层深度变化和混合层深度变化影响, 其中等温层深度变化对其影响更大。 相似文献
15.
INTRODUCTIONComparedwithotheroceansintheworld ,thereisrelativelyhigherlevelofnutrients (ni trate ,phosphate ,silicate)intheSouthernOcean .Butprimaryproductivitiesarelow ,andnewproductionisalsoonlyinthemiddlelevelthere .Itiscommonlyconsideredthatthelowerpro ductivitiesintheSouthernOceaniscausedbylowtemperature ,lowlight,lowstabilityofwa ter,scarcityoftraceelementsuchasironandgrazingbyzooplankton (Burkilletal.,1 995) ,etc.ThemostexistedstudiesconcentratedontheAtlanticSectoroftheSouthernO… 相似文献
16.
台湾东北部黑潮次表层水入侵的季节变化规律 总被引：4，自引：1，他引：4
台湾东北部,黑潮次表层水常年入侵东海陆架。但是黑潮次表层水入侵的季节变化规律,尚存在很多不明之处。本文基于2009至2011年间东海4个航次的CTD实测数据,研究了黑潮次表层水入侵东海过程的季节变化规律,发现:黑潮次表层水入侵在春末夏初开始加强,夏季最强,秋季开始减弱,冬季最弱。入侵的黑潮次表层水起源深度也随季节变化有所不同。另外,结果还表明黑潮次表层水入侵存在明显的短期变动。 相似文献
17.
In the summer seasons of 2004–2007, the intensive runoff (cascading) of the Antarctic shelf water (ASW) down the shelf and
continental slope was revealed thanks to the recording of numerous thermohaline profiles across the shelf and continental
slope of the Commonwealth Sea and Prydz Bay. The quickly executed profiles (4–10 h) with submesoscale resolution (near the
shelf’s edge, the scale was even eddy-determinative, i.e., within 1.9–5.6 km), in combination with the fine-structure sounding
and fine vertical resolution of the near-bottom boundary layer, provided a qualitatively new level of understanding the natural
data. The detailed analysis of the temperature, salinity, and density patterns revealed the regularities and peculiarities
of the ASW shelf and slope cascading. The intensive ASW cascading near the shelf break and lower part of the slope can be
forced (appearing as discrete frontal meanders) or free (appearing as discrete plumes) and often has a wave-eddy character.
The field observational data confirmed the obtained representative estimates of the elements of the ASW slope cascading. The
basic area of the ASW formation is near the Amery Shelf Ice, from where the ASW spreads to the northwest, goes around the
Fram Bank, and flows down the continental slope. The evaluative contribution of the ASW slope cascading to the ventilation
of the deep and slope water of the Southern Ocean (near the shelf break 70 km long where the ASW cascading was observed) is
Q
K
= 0.04–0.24 Sv, which agrees well with the analogous estimates obtained in other regions of the Antarctic. 相似文献
18.
The branching of the Tsushima Warm Current (TWC) along the Japanese coast is studied based upon intensive ADCP and CTD measurements
conducted off the Wakasa Bay in every early summer of 1995–1998, the analysis of the temperature distribution at 100 m depth
and the tracks of the surface drifters (Ishii and Michida, 1996; Lee et al., 1997). The first branch of TWC (FBTWC) exists throughout the year. It starts from the eastern channel of the Tsushima Straits,
flows along the isobath shallower than 200 m along the Japanese coast and flows out through the Tsugaru Strait. The current
flowing through the western channel of the Tsushima Straits feeds the second branch of TWC (SBTWC) which develops from spring
to fall. The development of SBTWC propagates from the Tsushima Straits to Noto Peninsula at a speed of about 7 cm sec−1 following the continental shelf break with a strong baroclinicity. However, SBTWC cannot be always found around the shelf
break because its path is influenced by the development of eddies. It is concluded that SBTWC is a topographically steered
current; a current steered by the continental shelf break. Salient features at intermediate depth are the southwestward subsurface
counter current (SWSCC) between 150 m and 300 m depths over the shelf region in 1995–1998 with the velocity exceeding about
5 cm sec−1, although discrepancies of the velocity and its location are observed between the ADCP data and the geostrophic currents.
This revised version was published online in August 2006 with corrections to the Cover Date. 相似文献
19.
南极普里兹湾浮游植物现存量与初级生产力粒级结构和新生产力研究 总被引：9，自引：4，他引：5
报道1998～1999年夏季在南极普里兹湾及其毗邻海域对细胞丰度、优势种类组成、生物量和初级生产力的粒级结构、新生产力及其环境制约机制的研究.结果表明,调查海区具有显著的空间区域化特征.普里兹湾及其毗邻陆架区浮游植物现存生物量和生产力均较高,大陆坡和深海区明显降低;营养盐浓度由于浮游植物的消耗则有相反的分布趋势.浮游植物生物量和生产力受水体的垂直稳定度、浮游动物摄食、水温和光照等环境条件的控制.粒度分级测定结果表明,对调查海区叶绿素a的贡献,小型浮游生物为52.2%,微型为29.4%,微微型为18.4%;对初级生产力的贡献,小型为52.4%,微型为28.7%,微微型为18.9%.研究海区的平均新生产力和f比分别为230.6mg/(m2·d)和0.43. 相似文献
20.
南极普里兹湾及其邻近海域溶解有机碳的分布 总被引：5，自引：0，他引：5
中国南极科学考察第16航次期间(1999年11月～2000年4月),在南极普里兹湾及邻近海域的不同站位与水深采集海水样品用于溶解有机碳测定,通过高温催化氧化法完成样品的分析.结果表明,在调查期间,南极普里兹湾及其邻近海域各测站上层水体(0～100m)溶解有机碳浓度的变化范围为14.3～181.1μmol/dm3,平均为52.5μmol/dm3,该变化幅度比Ross海、太平洋等海域的相应值略大.溶解有机碳垂直分布的特征是0大于25大于50大于100m,即随深度的增加溶解有机碳浓度逐渐减小,与生物活动在垂直方向上的强弱变化相关.根据200m以深水柱溶解有机碳的垂直分布,可确定研究海域难降解溶解有机碳的浓度为40.4μmol/dm3,与其他研究所报道的数值(～42μmol/dm3)相近.上层水体(0～100m)过剩溶解有机碳的空间分布显示,64°S以北海域溶解有机碳过剩较多,而64°S以南海域则过剩溶解有机碳较少.溶解有机碳浓度与分布特征显示,普里兹湾及其邻近海域溶解有机碳浓度与南大洋其他海域相当,具有低溶解有机碳的一般特征.溶解有机碳浓度的空间分布呈现由西南向东北方向逐渐增加的趋势,这可能与南极陆架夏季上层水的北向扩展有关.生物活动及水体运动是研究海域溶解有机碳分布的主要影响因素. 相似文献