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1.
The distributions of partial pressure of carbon dioxide (p CO2 ) in the surface waters of the Changjiang River Estuary and adjacent Hangzhou Bay were examined in the summer of 2010. Surface water p CO2 ranged from 751-2 095 μatm (1 atm=101 325 Pa) in the inner estuary, 177-1 036 μatm in the outer estuary, and 498-1 166 μatm in Hangzhou Bay. Overall, surface p CO2 behaved conservatively during the estuary mixing. In the inner estuary, surface p CO2 was relatively high due to urbanized pollution and a high respiration rate. The lowest p CO2 was observed in the outer estuary, which was apparently induced by a phytoplankton bloom because the dissolved oxygen and chlorophyll a were very high. The Changjiang River Estuary was a significant source of atmospheric CO2 and the degassing fluxes were estimated as 0-230 mmol/(m2 d) [61 mmol/(m2 d) on average] in the inner estuary. In contrast, the outer estuary acted as a CO2 sink.  相似文献   

2.
Dissolved and particulate thorium-234, particulate organic carbon in the upper 150 m of water columns from five stations in the Prydz Bay, the Southern Ocean were determined during the 22nd Chinese National Antarctic Research Expedition (from November 2005 to March 2006 ). The disequilibria between thorium-234 and its parent uranium-238 in upper layer was used to derive the averaged residence time of thorium-234, which decreased along with the latitude to the south and a minimum value, 1 - 8 d for particulate thorium-234 and 29 - 48 d for dissolved thorium-234, appeared at the medium latitude station, and the export fluxes of thorium-234 were calculated too and 'a maximum value, 0. 35 -0. 63 Bq/(m^3 · d) for the particulate thorium-234 and 0. 44 -0. 65 Bq/ (m^3 ·d) for the dissolved thorium-234, appeared at the same station. The export fluxes of particulate organic carbon at different water columns were derived by two methods with irreversible scavenging model, and the averaged values were 104. 7 mmol/ ( m2 · d ) ( E method) and 120. 6 mmol/( m2·d ) ( B method ), respectively, indicating that a relatively high new production would exist in summer in the Prydz Bay where it will play a potential significant role in sequestering the absorption CO2 to deeper ocean.  相似文献   

3.
The global distributions of the air-sea CO2 transfer velocity and flux are retrieved from TOPEX/Poseidon and Jason altimeter data from October 1992 to December 2009 using a combined algorithm. The 17 a average global, area-weighted, Schmidt number-corrected mean gas transfer velocity is 21.26 cm/h, and the full exploration of the uncertainty of this estimate awaits further data. The average total CO2 flux (calculated by carbon) from atmosphere to ocean during the 17 a was 2.58 Pg/a. The highest transfer velocity is in the circumpolar current area, because of constant high wind speeds and currents there. This results in strong CO2 fluxes. CO2 fluxes are strong but opposite direction in the equatorial east Pacific Ocean, because the air-sea CO2 partial pressure difference is the largest in the global cceans. The results differ from the previous studies calculated using the wind speed. It is demonstrated that the air-sea transfer velocity is very important for estimating air-sea CO2 flux. It is critical to have an accurate estimation for improving calculation of CO2 flux within climate change studies.  相似文献   

4.
The 3rd Chinese National Arctic Research Expedition(CHINARE–Arctic III) was carried out from July to September in 2008. The partial pressure of CO2(pCO2) in the atmosphere and in surface seawater were determined in the Bering Sea during July 11–27, 2008, and a large number of seawater samples were taken for total alkalinity(TA) and total dissolved inorganic carbon(DIC) analysis. The distributions of CO2 parameters in the Bering Sea and their controlling factors were discussed. The pCO2 values in surface seawater presented a drastic variation from 148 to 563 μatm(1 μatm = 1.013 25×10-1 Pa). The lowest pCO2 values were observed near the Bering Sea shelf break while the highest pCO2 existed at the western Bering Strait. The Bering Sea generally acts as a net sink for atmospheric CO2 in summer. The air-sea CO2 fluxes in the Bering Sea shelf, slope, and basin were estimated at-9.4,-16.3, and-5.1 mmol/(m2·d), respectively. The annual uptake of CO2 was about 34 Tg C in the Bering Sea.  相似文献   

5.
1Introduction The Prydz Bay has its open water in the northadjacent to the Indian Ocean sector of the SouthernOcean.It borders on the ice shelf to its south,andthe Antarctic Continent to its east and west.It is thelargest water stretching southward into t…  相似文献   

6.
The data were collected during Chinese Arctic and Antarctic Expeditions in the western Arctic Ocean and the marginal sea ice zone (MSIZ) of the Southern Ocean, respectively in the boreal summer from July to September of 1999 and in the austral summer from December of 1999 to January of 2000. The concentrations of CO2 in surface water of the survey regions would mostly present lower than those in the atmosphere. A significant biological driving force could also been observed in summer waters in both of the above oceans. Air to sea CO2 fluxes were also calculated to compare oceanic uptake capacity of CO2 in both oceans with the world oceans using Liss, Wanninkhof, and Jacobs‘s methods. The averaged CO2 fluxes of air to sea in the western Arctic Ocean or in the MSIZ of the Southern Ocean doubled that in the world oceans.  相似文献   

7.
On the basis of data collected in the Jiaozhou Bay in June and July 2003, the DIC distribution in seawater is studied,and an average air-sea flux of CO2 is estimated. The results show that the content of DIC inside the bay is markedly higher than outside the bay in June, but the contem of DIC outside the bay is markedly higher than inside the bay in July. The trend of DIC distribution inside the bay is similar, viz. the content is the maximum in the northeast, then decreases gradually toward the west, and the content is the minimum in the west. The total trend of vertical distribution is to increase gradually from surface to bottom. This characteristic of DIC distribution is determined by Jiaozhou Bay hydrology and there is a close relation between DIC and particulate N.P. Average CO2 flux across the air-sea interface is 0.55 mol/(m^2.a) in June and 0.72 mol/(m^2.a) in July. Jiaozhou Bay is considered as a net annual source for atmospheric CO2 in June and July, and the total CO2 flux from seawater into atmosphere is about 740 t in June and 969 t in July.  相似文献   

8.
A coupled ice-ocean isopycnal numerical model of the Southern Ocean is established tostudy the circulation and its seasonal variability in the region around the Kerguelen Plateau. An analysis of the simulated results shows significant stripe-like structure and non-zonal feature of the Antarctic Cir-cumpolar Current (ACC) in this region. ACC begins to bifurcate and to turn its direction before meeting the plateau. The southernmost branch of ACC is near to the Antarctic coast and displays its strong interaction with the westward Antarctic Slope Current. The northern branch of ACC has a tendency of annual variations while the southern one varies in a semiannual cycle. The variation phases of both branches are coincident with that of the wind stress in this region.  相似文献   

9.
Contrasting decrease and increase trends of sea surface temperature(SST) have been documented in the western Subarctic(WSA) and the rest of the Northwest Pacific(NWP) from 1958 to 2017, respectively. Consequently, more(less) total carbon dioxide(TCO2) due to ocean cooling(warming) is transported to the surface, which leads to increase(decrease) of oceanic surface partial pressure of carbon dioxide(pCO2). With the combined influence of the rising atmospheric carbon dioxide(C...  相似文献   

10.
The primary production and chlorophyll a concentration of picoplankton (0.2 - 2 μm) , nanoplankton (2 - 20μm) and micro- plankton (20 -200 μm) are described in the northeastern Pacific Ocean near the Hawaii Islands during the six survey cruises from 1996 to 2003:DY85-4, DY95-7, DY95-8, DY95-10, DY105-11 and DY105-12.14. The primary production of carbon was in range from 76.8 to 191.9 mg/(m^2 · d) with an average of 116.1 mg/( m^2 · d) in the east region, and from 73.1 to 222.5 mg/( m^2 · d) with an average of 127.1 mg/( m^2 · d) in the west region, similar to the other oligotrophic regions of the Pacific Ocean investigated. The chlorophyll a concentration was about 0.1 mg/m^3 from the surface to the 50 m depth, about 0.2 -0.4 mg/m^3from 50 to 100 m, and gradually decreased below the 100 m depth. The picoplankton accounted for more than 70% of the total chlorophyll a in the upper layer ( surface to 125 m), but it decreased to less than 50% in depth below 125 m. The nanoplankton and microplankton combined only accounted for less than 30% of the total chlorophyll a in the upper layer, but showed a more even vertical distribution.  相似文献   

11.
中国第22次南极科学考察(2005年11月至2006年3月)期间,测定了南极普里兹湾海域5个站位的从表层至150 m水深的不同层位水样中溶解态和颗粒态234Th,238U的放射性比活度以及颗粒有机碳.利用234Th/238U在上层水体中的不平衡,计算了南极普里兹湾上层水体中234Th的平均停留时间和输出通量.结果显示,随着纬度的增加,上层水体中颗粒态和溶解态234Th的平均停留时间总体趋向减小,并在中纬度站位出现了最低值,分别为1~8和29~48 d,而颗粒态和溶解态234Th的输出通量则在中纬度站位出现了最大值,分别为21~38和26~39 dpm/(m3·d).运用箱型清除模式,利用两种不同的方法估算了各水柱中从真光层底部输出的POC通量,平均值分别达到104.7 mmol/(m2·d)(E法)和120.6 mmol/(m2·d)(B法),表明南极普里兹湾夏季存在很高的新生产力,它将会对该海域碳的生物泵过程产生重要作用.  相似文献   

12.
INTRODUCTIONDissolvedorganiccarbon (DOC)makesupthesecondlargestofthebioactivepoolsofcar bonintheocean ,secondtothelargestpoolofdissolvedinorganiccarbon .Theglobaldissolvedorganiccarbonpoolisestimatedtobe 6 85Gt,avaluecomparabletothemassofCO2 intheat mosphere (Hedges,1 992 ) .Thesizeofthereservoir,aswellasitsdynamics ,indicatesthatDOCplaysacentralroleintheoceancarboncycle .AsitrelatestogreenhousegasessuchasCO2 andassociatesclimatecycle ,oceanicDOCbiogeochemicalcycleshavebeenoneoftheh…  相似文献   

13.
厘清河口-陆架连续体的碳源/汇机制是认识海洋在“碳中和”中作用的重要基础。本研究基于2017年春季长江口-东海的走航CO2分压(pCO2)及温、盐等资料,分区域阐述春季长江口-东海连续体pCO2的空间分布格局,半定量解析水团分配、有机质生产及降解等过程对pCO2的控制作用。结果表明:水团来源是决定春季长江口-东海连续体pCO2分布及碳源/汇格局的主要因素,而有机质生产或者降解可强烈影响长江口-东海连续体碳源/汇格局。春季长江口门及浙江沿岸受长江径流影响而具有较高的pCO2,碳源强度可达5.36mmol·m-2·d-1;研究区域北部和东部分别受冲淡水及黑潮表层水的影响,表现为大气碳汇,北部碳汇强度为-15.44mmol·m-2·d-1。2017年春季研究区域平均碳通量为-6.73mmol·m-2·d-1。端元混合模型结果表明陆源有机质降解导致河口pCO2增加了约200μatm,促使春季河口由大气CO2的弱汇转变为碳源;陆架区域在仅考虑水团分配下同样为碳汇,而藻华过程进一步降低了pCO2(下降144μatm),增强了其碳汇能力。  相似文献   

14.
南大洋浮游植物现存量对颗粒有机碳的贡献   总被引:6,自引:1,他引:5  
根据中国第15、16次南极考察观测的颗粒有机碳、叶绿素a浓度的数据,探讨浮游植物现存量对南大洋颗粒有机碳的贡献。结果表明,普里兹湾内浮游植物碳对颗粒有机碳的贡献高于湾北部的大洋区,真光层上部浮游植物碳对颗粒有机碳的贡献高于深层水。同时分析两个航次测区叶绿素a浓度和航程途中叶绿素a浓度的分布,以期了解浮游植物在南大洋颗粒有机碳来源中的作用。  相似文献   

15.
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   

16.
中国南大洋水团、环流和海冰研究进展(1995-2002)   总被引:2,自引:0,他引:2  
总结了1995年以来中国在南大洋物理海洋学研究和南极海冰研究中所取得的成果。普里兹湾海区是中国南大洋研究的重点区域,研究表明,在该海区存在显著的深层水涌升和陆架水北扩现象,某些年份深层水与陆架水混合后产生了较重的水体,但是尚未发现生成南极底层水的直接证据。在普里兹湾所处的印度洋区段,亚热带锋、亚南极锋和极锋表现出显著的时空变化,特别是不同年份的锋面位置存在较大的摆动。该海区的南极绕极流既是风生的,也受到密度场的影响。在凯尔盖朗海台的地形引导作用下,南极绕极流表现出显著的非纬向性特征。南极海冰除了显著的季节变化以外,也表现出长期变化的趋势。此变化与海洋、大气中的其它变化有一定的相关性,表现为两极海冰涛动、南方海洋涛动等多种变化模态,对我国气候也有一定的影响。  相似文献   

17.
采用船载海?气CO2连续观测系统于2011年和2014年夏季在琼州海峡开展了现场观测,分析研究了表层海水二氧化碳分压(pCO2)时空变化及其影响因子。2011年和2014年夏季pCO2分别为(516±29) μatm和(533±15) μatm,海?气CO2交换通量分别为(8.4±1.7) mmol/(m2·d)和(4.5±0.4) mmol/(m2·d),均是大气CO2的强源,高于相邻及相似海域,主要受控于东口海域上升流和海峡中部狭管效应。2011年夏季东口上升流增大pCO2的同时也促进了浮游植物繁殖,光合作用吸收水体CO2,降低了pCO2,而且受其影响,西口口门附近叶绿素a和溶解氧含量陡增,pCO2突降。2014年夏季东口海域上升流较弱,且观测海域垂直混合作用显著,pCO2和溶解氧分布特征与2001年夏季明显不同。海峡中部狭管效应造成水体输运速率大、混合作用强,浮游植物“来不及”生长,pCO2较高。  相似文献   

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