基于浮标观测的春季青岛近岸海水pCO2变化及海-气CO2通量研究

利用海-气界面浮标观测得到的高频数据,分析了春季青岛近岸海域海表二氧化碳分压(pCO₂)的变化规律及驱动因素,并对海-气CO₂通量进行了估算。观测期间该海域由大气的碳汇转变为碳源,主要是由海表pCO₂的不断增长所致。对海表pCO₂控制因素进行分析,发现温度升高是pCO₂增长的主要驱动因素,生物过程起到一定的抑制作用。海表pCO₂呈现出日变化特征,温度和生物因素对海表pCO₂日变化的作用均与太阳辐射相关,但两者的作用相反。此外,分析发现浮标的不同采样频率会对海-气CO₂通量估算产生影响,缩短采样间隔能有效降低海-气CO₂通量估算的偏差,提高估算的准确性。     

北黄海夏季pCO2分布及海-气CO2通量

基于在2006年夏季北黄海收集的的高分辨率的表层CO2分压(pCO2)数据,结合水文和生物地球化学同步观测参数,探讨了夏季北黄海pCO2空间分布的控制因素。结果表明,夏季北黄海与大多数中低纬度陆架海类似,由于水温较高,表层pCO2较高(平均值为(463±41)μatm),整个海域相对大气CO2过饱和。表层pCO2分布具有明显的区域差异,辽南和鲁北近岸海域pCO2明显高于中部区域,辽南近岸的高pCO2主要与河流输入和水产养殖引起的生物好氧呼吸有关,而鲁北沿岸的高pCO2主要与烟台近岸的底层冷水涌升及由混合引起的高碳酸盐含量的黄河泥沙的再悬浮有关;在海区中部大部分水域,pCO2与温度之间有较好的相关性,说明温度是这一区域pCO2分布较为重要的控制因子。另外,采用Wannikhof的海-气气体交换系数估计了北黄海夏季海-气CO2通量,结果表明整个北黄海是大气CO2的源,平均释放速率为(4.00±0.57)mmol.m-2.d-1,高于南黄海夏季海-气CO2通量。     

夏季东海西部表层海水中的pCO2及海-气界面通量

根据2001年夏季长江口及东海西部海域表层海水pCO     

2011年3月胶州湾表层海水pCO2及海-气界面通量

依据2011年3月4日对胶州湾走航连续实测所得pCO2数据,结合水文、化学和生物等要素的同步实测资料,对胶州湾海域pCO2分布及其影响因素进行了初步探讨,并估算了3月海-气CO2通量。结果表明:3月胶州湾表层海水pCO2实测值在191～332μatm之间,平均值为278μatm,海-气CO2通量在-22.76～-7.13mmol·m-2·d-1,平均值为-14.2mmol·m-2·d-1,这一时期胶州湾从大气吸收约1.59×103t C,表现为大气CO2的强汇。生物活动是影响这一时期表层海水pCO2分布的主要原因。     

海-气CO2通量实测数据通量计算中误差传递模拟与敏感性分析

海-气CO₂通量估算模型中参数的可靠性是决定模型可靠性的重要因素, 也决定了模型估算结果的可靠性, 因此开展海-气CO₂通量计算模型中误差传递规律与敏感性分析, 对模型参数端元因子的误差控制, 提高模型预测精度和降低不确定性十分重要。但由于模型中参数众多, 且各种参数间彼此相互影响, 使得误差传递过程与敏感性分析十分复杂困难。本文在海-气界面CO₂通量观测建模过程详细分析的基础上, 以海-气界面CO₂分压差的经典通量计算模型为基础, 以实测数据通量计算过程为例, 针对模型中的参数变量, 在假设参数变量的误差正态分布的前提下, 利用Monte Carlo手段分析各参数变量的误差在模型中的传递规律, 并将单因子扰动试验法用于海-气界面CO₂通量建模的参数敏感性分析。模拟和分析结果表明:CO₂通量计算过程中误差经模型传递后的分布规律存在正态分布、指数分布等多种形式;气体交换系数对通量计算结果的敏感性最大, 通量估算中的风速和表层海水温度是必须进行精度控制的关键参数。     

大洋海区海-气CO_2通量单参数遥感算法的适用性检验

利用卫星遥感技术的优势,基于LDEO数据库的全球海表二氧化碳分压（PCO2）及海表温度（SST）等实测数据,初步建立东太平洋海区PCO2与SST的单参数经验算法,并采用相同区域的独立实测数据检验.结果表明,单参数算法在寡营养大洋海区具有良好的适用性,反演值与实测值之间的均方根误差（RMS）为0.51 Pa（1 Pa=9.869μatm）,由此估算出2003年6月该海域CO2通量为-1.4 mmol/（m2.d）,与实测估算的碳通量基本相符,能够很好地反映出海区CO2源汇特征.将该遥感算法运用到西大西洋海域（15°~25°N,60°~75°W）,反演值与实测值之间均方根误差（RMS）为0.69 Pa.检验结果表明,在寡营养大洋海区,单参数遥感算法具有一定的适用性,在受相似因子调控的同纬度海区可以使用同一遥感算法.     

夏季东海西部表层海水中的pCO_2及海-气界面通量

根据 2 0 0 1年夏季长江口及东海西部海域表层海水pCO2 的实测数据 ,结合水文、化学和生物等要素的同步观测资料 ,对该海域pCO2 分布和变化的重要影响因素进行了探讨。结果表明 ,长江冲淡水是造成东海西部海域表层海水pCO2 分布不均匀的主要原因。利用Wan ninkhof( 1 992 )提出的通量模式计算 ,长江口口门附近海域和浙江近岸海域为CO2 的源区 ,1 2 3°E以东的调查海域表现为大气CO2 的汇 ,尤其是以 1 2 3°E ,32°N为中心 ,存在着一个极强的大气CO2 汇区。就整个东海西部海域而言 ,夏季可从大气净吸收 1 5 3× 1 0 4 tC。     

北部湾东北部春、夏季表层海水CO2分压的24 h变化及其调控机制研究

周日观测对掌握近海碳酸盐体系变化和海-气CO₂交换过程是必要的,有助于降低碳源汇评估的不确定性。针对北部湾东北部的英罗湾-安铺港海域,于2018年4月和8月利用24 h定点逐时采样观测了该区域表层海水碳酸盐体系及相关要素,分析了春、夏季的表层海水CO₂分压(p CO₂)24 h逐时变化规律及其调控因子。观测结果表明,春、夏季p CO₂变化范围分别为530～628μatm和427～748μatm,平均海-气CO2通量分别为(1.7±0.8)mmol/(m²·d)和(1.2±0.8)mmol/(m²·d),均表现为大气CO₂的弱源。其中春季p CO₂ 24 h逐时变化受温度的影响相比夏季更显著,而夏季p CO₂对潮汐作用以及区域内沿岸河流、地下水等淡水汇入引起的生物生产和呼吸代谢过程增强的响应更明显。海水升温主导了春季区域表层高p CO₂的形成,夏季咸淡水的物理混合过程中增...     

春、秋季台湾海峡海-气CO2通量及其影响因素

于2014年的5月(春季)和9月(秋季)在台湾海峡及其邻近南海和东海海域,采用水气平衡法进行了2个航次的海表和大气pCO_2连续走航观测,同时获取了海表温度、海表盐度、风速及气压等数据,并采用海-气CO_2分压差减法估算了海-气CO_2通量.结果显示,春、秋2个航次平均海表pCO_2分别为387±16μatm和408±18μatm.温度是影响台湾海峡及其邻近海域海表pCO_2的主控因子,水团混合和其他因素等也对海表pCO_2有一定影响.2014年春、秋季节,对研究区域的海-气CO_2释放通量的估算结果分别为0.11±1.60 mmol/(m2·d)和2.51±1.10 mmol/(m2·d).台湾海峡海表pCO_2既存在显著的季节变化,又存在较大的空间差异.     

白令海BR断面海-气CO2通量及其参数特征

通过对2008年夏季白令海大气和海水pCO2连续观测资料,结合BR断面上站位水体垂直采样测量,对白令海不同海区pCO2的分布特征及其与理化参数的关系进行了初步研究,结果表明,将白令海划分为4个具有不同CO2吸收能力的海区,其中陆坡流区碳通量高达-18.72 mmol/(m2·d),是海盆北区的近2倍,比海盆南区高一个量...     

东海陆架盆地CO2地质封存适宜性评价

温室气体过量排放引起了明显的全球气候变化及诸多次生灾害,CO2捕集与地质封存技术应运而生。中国东海沿岸CO2排放源众多,但陆上盆地面积狭小,无法满足巨量CO2封存的需求。根据相关学者做出的中国全海域级碳封存适宜性评价,东海陆架盆地在中国近海盆地中碳封存适宜性排名第3,面积宽广且封闭性好,因此,在此基础上对东海陆架盆地开展了盆地级碳封存适宜性评价。结合专家意见和相关学者研究成果,利用模糊综合评价法和层级分析法确立了适宜性评价指标体系及指标权重,再根据盆地内各二级构造单元的相关地质资料,按照评价指标分级赋分表对各单元的每个评价指标进行评分,结合权重计算出综合适宜性评分。综合考虑碳封存容量、封闭性及可操作性的评价结果认为,台北坳陷为盆地中碳封存综合适宜性最好的单元,可作为优先实验性封存区。     

中国南海、东海及黄海海域海气二氧化碳通量与生产力的物理生物地球化学模拟研究

Marginal seas play important roles in regulating the global carbon budget, but there are great uncertainties in estimating carbon sources and sinks in the continental margins. A Pacific basin-wide physical-biogeochemical model is used to estimate primary productivity and air-sea CO_2 flux in the South China Sea(SCS), the East China Sea(ECS), and the Yellow Sea(YS). The model is forced with daily air-sea fluxes which are derived from the NCEP2 reanalysis from 1982 to 2005. During the period of time, the modeled monthly-mean air-sea CO_2 fluxes in these three marginal seas altered from an atmospheric carbon sink in winter to a source in summer. On annualmean basis, the SCS acts as a source of carbon to the atmosphere(16 Tg/a, calculated by carbon, released to the atmosphere), and the ECS and the YS are sinks for atmospheric carbon(–6.73 Tg/a and –5.23 Tg/a, respectively,absorbed by the ocean). The model results suggest that the sea surface temperature(SST) controls the spatial and temporal variations of the oceanic pCO_2 in the SCS and ECS, and biological removal of carbon plays a compensating role in modulating the variability of the oceanic pCO_2 and determining its strength in each sea,especially in the ECS and the SCS. However, the biological activity is the dominating factor for controlling the oceanic pCO_2 in the YS. The modeled depth-integrated primary production(IPP) over the euphotic zone shows seasonal variation features with annual-mean values of 293, 297, and 315 mg/(m~2·d) in the SCS, the ECS, and the YS, respectively. The model-integrated annual-mean new production(uptake of nitrate) values, as in carbon units, are 103, 109, and 139 mg/(m~2·d), which yield the f-ratios of 0.35, 0.37, and 0.45 for the SCS, the ECS, and the YS, respectively. Compared to the productivity in the ECS and the YS, the seasonal variation of biological productivity in the SCS is rather weak. The atmospheric pCO_2 increases from 1982 to 2005, which is consistent with the anthropogenic CO_2 input to the atmosphere. The oceanic pCO_2 increases in responses to the atmospheric pCO_2 that drives air-sea CO_2 flux in the model. The modeled increase rate of oceanic pCO_2 is0.91 μatm/a in the YS, 1.04 μatm/a in the ECS, and 1.66 μatm/a in the SCS, respectively.     

Temperature dependence of CO2 fugacity in seawater

Ideally, the correction of the measured CO₂ fugacity (fCO₂) at temperature T_m to fCO₂ at the in-situ temperature T_in should be made by using at least 2 known parameters (pH-A_T, C_T-A_T,…) and the reliable constants for carbonic acid. In practice however, a measured CO₂ property pair is not always available. When fCO₂ is measured alone, one must make an estimate of the effect of temperature on seawater fCO₂ from the accurate knowledge of seawater salinity and temperature and the approximate knowledge of the carbonate parameters. In this paper we present an empirical relationship that can be used to estimate the effect of temperature on fCO₂. The equation is of the form:

ƒCO_2[t] − ƒCO_2[20]=A + Bt + Ct² + Dt³ + Et⁴

where fCO_2[t] and fCO_2[20] represent fCO₂ at temperatures t°C and 20°C, respectively; the parameters A, B, etc. are functions of the ratio X = C_T/A_T:

E = e₀ + e₁X + e₂X²ln(X) + e₃exp(X) + e₄/ln(X)

where the parameters a_i, b_i, etc. are functions of salinity.The 25-parameter equation is fitted by the values of fCO₂ calculated using the constants of Goyet and Poisson (1989), when X varies from 0.8 to 1.0, t varies from −1dgC to 40°C, and S varies from 30 to 40. For T_m - T_in within ± 10°C, direct measurements of fCO₂ as a function of the temperature (from −I to 30°C verify this equation within less than ±5 μatm.     

Carbonate chemistry and the anthropogenic CO2 in the South China Sea

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南海东北部春季海表pCO_2分布及海-气CO_2通量

2013年南海东北部春季共享航次采用走航观测方式,现场测定了表层海水和大气的二氧化碳分压(pCO2)及相应参数。结合水文、化学等同步观测要素资料,对该海域pCO2的分布变化进行了探讨。结果表明,陆架区受珠江冲淡水、沿岸上升流及生物活动的影响,呈现CO2的强汇特征;吕宋海峡附近及吕宋岛西北附近海域受海表高温、黑潮分支"西伸"、吕宋岛西北海域上升流等因素影响,呈现强源特征。根据Wanninkhof的通量模式,春季整个南海东北部海域共向大气释放约4.25×104 t碳。     

海浪对北太平洋海-气二氧化碳通量的影响

利用4种海-气界面气体传输速率公式对比研究了北太平洋气体传输速率及其CO₂通量的季节变化特征。与单纯依赖风速的算法相比, 考虑波浪影响的气体传输速率和CO₂通量在空间分布和季节变化上具有明显差异。在低纬度地区(0°～30°N), 波浪参数使气体传输速率下降, 海洋对大气CO₂的吸收减少, 而在30°N以北范围内则出现新的气体传输速率高值区, 海洋对大气的吸收增加。进一步研究了黑潮延伸体区域的气候态月平均气体传输速率和CO₂通量。结果表明, 该区域气体传输速率和CO₂通量最大值分别出现于冬季和春季, 引入波浪参数后, 虽然该区域气体传输速率和CO₂通量平均值没有明显差异, 但季节变化强度显著增强。     

CO2 exchange at air-sea interface in the Huanghai Sea

INTRODUCTIONTheroleoftheoceaniscrucialintheoverallcycleofCOZ,withitsspecialpumpingmechanismssuchassolubilitypumpingattheair-seainterfacewithcarbonatechemistry,biologicalpumpinginsurfacewatersandalsointhewatercolumn,anddynamicpumpingassociatedwithoceancirculation(BroeckerandPeng,1982).Inordertounderstandthesevariouspumpingprocessesintheocean,muchresearchhasbeencarriedoutonaglobalscaleasapartofeffortstounderstandtheglobalgeochemicalcycleofCOZ.TheHuanghaiSea,atypicalmid-latitudeepicontine…     

Distributions and air-sea fluxes of CO2 in the summer Bering Sea

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.     

M2 tidal currents near the continental shelf margin in the East China Sea

Time series of velocity and water temperature were measured at three stations on the continental shelf, on the shelf margin and on the slope off the northwest Tokunoshima in December 1980 to study influences of the slope on tides.Tidal currents with semidiurnal periods were dominant at the stations on the shelf and shelf margin. However, semidiurnal components in temperature fluctuations were dominant at the stations on the shelf margin and the slope. We estimated horizontal currents due to semidiurnal internal tides from the vertical distribution of water density and temperature, assuming that the temperature fluctuations were caused by the vertical displacement of water particles due to semidiurnal internal tides. The tidal ellipses at the station on the shelf and the phase relation of the tidal currents between the two stations on the shelf and shelf margin indicated that the M₂ surface tide on the shelf was a Sverdrup wave propagating to the northwest.Semidiurnal tidal currents on the slope were also caused by tides of surface and internal modes. Furthermore, the axis of the tidal ellipse was not perpendicular to the co-tidal line estimated by Ogura (1934) but rather parallel to the isobaths on the slope, which shows a striking effect of the bottom topography on the tidal currents.