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1.
<正>海洋初级生产力是指海洋中初级生产者(主要是浮游植物)通过光合作用或化学合成生产有机物的能力或速率[1-2],它是海洋生态系统中其他异养生物的生存基础,并从根本上影响着全球生物地球化学循环[3]与气候变化[4]。研究表明,海洋浮游植物通过光合作用不仅贡献了生物圈内的一半净初级生产力(以碳计约为5×1013 kg/a)[4],提供了生态系统中其他有机体生长与新陈代谢所需要的初级有机物能源,限制  相似文献   

2.
一株海洋微型硅藻的形态学和分子生物学鉴定   总被引:3,自引:0,他引:3  
1 引言 微型浮游植物(粒径为2~20μm)是海洋环境中主要的初级生产者,在海洋初级生产力中占有很大比重,特别在寡营养水域,微型浮游植物可占初级生产力的80%以上[1],并且在粒级结构上微型浮游植物对初级生产力的贡献要比较大粒级的植物的贡献更大[2].  相似文献   

3.
尽管铁为地壳中丰度位居第4的元素,但它在海水中的浓度却很低,浓度一般为0.05~2.0 nmd/dm3[1]。近年来,国内外的海洋科学家在进行海洋生态系统初级生产力、碳循环等重要生态过程及其对全球气候变化影响的研究中发现,海洋中的铁对浮游植物的生长、初级生产力的水平有着十分重要的影响甚至成为了“限制性因子”,在多个“高营养盐、低叶绿素(HNLC)”海区所实施的富铁实验的结果很好地印证了铁元素在海洋生态系统中的重要作用[2]。最新的研究成果表明近岸海水中的铁可能对浮游植物的种类组成起到决定性的作用,进而对包括氮、磷、硅在内的其他元素的生物地球化学行为产生深远的影响[3]。  相似文献   

4.
海洋中铁的来源,形态和初级生产力的限制作用   总被引:1,自引:0,他引:1  
在海洋中,铁和N,P等主营养盐一样,也是一样限制浮游植物初级生产力的重要因素,由于铁是一种化学活性较高的元素,所以海水中铁的形态,来源及沉降会直接影响其生物可利用性,目前人们一般采用预富集/原子吸收法(AAS)或是借助于电分析技术(如催化极谱)来测定海水中的铁。  相似文献   

5.
河口区水体中磷酸盐的缓冲机制   总被引:8,自引:0,他引:8  
磷酸盐,是海洋自养生物所必需的营养盐之一。浮游植物在进行光合作用时,将海水中营养盐等合成为有机质,成为海洋生物的生活基础。海洋中的磷,又常常是初级生产力的控制因素之一。河流是海洋中磷的来源之一。从大陆岩石风化出来的磷,只有5—10%是  相似文献   

6.
海洋中铁的来源、形态和对初级生产力的限制作用   总被引:6,自引:0,他引:6  
在海洋中,铁和N、P等主营养盐一样,也是一种限制浮游植物初级生产力的重要因素。由于铁是一种化学活性较高的元素,所以海水中铁的存在形态、来源及沉降会直接影响其生物可利用性。目前人们一般采用预富集/原子吸收法(AAS)或是借助于电分析技术(如催化极谱)来测定海水中的铁。  相似文献   

7.
渤海湾浮游植物光合作用强度的测定   总被引:2,自引:0,他引:2  
前言渤海初级生产力的研究,是渤海水产资源增殖计划中的重要研究课题之一。为了估算渤海从初级生产者到渔业捕捞对象各级生物产量和各级营养阶层之间的能量转换关系,首先要研究海洋浮游植物的蕴藏量及其生产能力,即海洋初级生产力。在所有可以用来估算海洋浮游植物蕴藏量的方法中,根据海水中叶绿素含量,来计算海洋浮游植物的蕴藏量的方法,似  相似文献   

8.
长江口、杭州湾水域沉积物对磷吸附行为的研究   总被引:18,自引:0,他引:18  
赤潮发生于沿海一带,尤其是河口海湾水体中的一种生态异常现象,赤潮的发生会对水体生态环境和海水养殖业造成毁灭性打击[1~3].自20世纪70年代以来,赤潮的发展已经成为我国沿海最突出的环境问题之一,目前研究表明,水体的富营养化与赤潮的存在有着某种内在的联系,富营养化的水体可为赤潮生物的生长提供了物质基础.海洋浮游植物对氮、磷的吸收是按一定比例进行的,当N/P>30时,则认为该海域属于磷受限的环境;相反,当N/P<8时,则认为是氮受限的环境[4].我国长江口赤潮多发区氮、磷比的范围为83:1~31:1[5],说明该海域浮游植物的生长均受磷的限制.  相似文献   

9.
悬浮颗粒物中生物硅测定方法的改进与应用   总被引:1,自引:3,他引:1  
硅是河流和海洋中非常重要的营养盐,硅藻、放射虫、硅质海绵、硅鞭毛虫的生长和骨骼形成都离不开硅[1].硅在河流和沿岸海域生态系统中扮演着非常重要的角色,在浮游植物大量繁殖季节,由于硅藻的大量繁殖,使活性硅酸盐含量急剧下降,甚至使硅藻的生长繁殖受到限制.在其他环境条件适宜的情况下,充足的硅又将成为发生硅藻赤潮的物质基础[2].生物硅是用化学方法测定的无定形硅的含量[3],称为生物蛋白石或简称蛋白石,是地球化学、古海洋学研究中非常重要的参数[4].根据世界部分河流生物硅和溶解硅的平均值计算,河流输送入海的硅中有16%的是生物硅,因此河流输送的生物硅的量是全球海洋硅收支中不可忽略的部分[5].  相似文献   

10.
近海港湾浮游植物的春季藻华,初级生产力的分布和变化及其与环境物理化学之间的相互关系已有许多研究,如:潮汐对浮游植物藻华形成的驱动作用[1],垂直稳定或混合对浮游植物生物量粒级分布和初级生产力的影响[2~5],控制港湾浮游植物藻华的过程[6~10],营养盐类对浮游植物生长的限制[11,12]以及浮游植物季节性藻华[13]等.  相似文献   

11.
The generalised gradient approximation based on density functional theory is used to study the structural and electronic properties of the endohedral fullerene dimer (N2@C60)2. Four N atoms sit at the cage centres in the form of two N_2 molecules. The density of states and Mulliken charge analysis explore that the energy levels from -6 to -10 eV are mainly influenced by the N2 molecules.  相似文献   

12.
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   

13.
夏季东海西部表层海水中的pCO2及海-气界面通量   总被引:10,自引:0,他引:10  
根据2001年夏季长江口及东海西部海域表层海水pCO  相似文献   

14.
采用射频磁控溅射方法制备了两种用于相变存储器的Ge1Sb2Te4和Ge2Sb2Te5相变薄膜材料,对其结构、电学输运性质和恒温下电阻随时间的变化关系进行了比较和分析.X射线衍射(XRD)和原子力显微镜(AFM)的结果表明:随着退火温度的升高,Ge1Sb2Te4薄膜逐步晶化,由非晶态转变为多晶态,表面出现均匀的、  相似文献   

15.
The third Chinese National Arctic Research Expedition(CHINARE) was conducted in the summer of 2008.During the survey,the surface seawater partial pressure of CO_2(pCO_2) was measured,and sea water samples were collected for CO_2 measurement in the Canada Basin.The distribution of pCO_2 in the Canada Basin was determined,the influencing factors were addressed,and the air-sea CO_2 flux in the Canada Basin was evaluated.The Canada Basin was divided into three regions:the ice-free zone(south of 77°N),the partially ice-covered zone(77°–80°N),and the heavily ice-covered zone(north of 80°N).In the ice-free zone,pCO_2 was high(320 to 368μatm,1 μatm=0.101 325 Pa),primarily due to rapid equilibration with atmospheric CO_2 over a short time.In the partially ice-covered zone,the surface pCO_2 was relatively low(250 to 270 μatm) due to ice-edge blooms and icemelt water dilution.In the heavily ice-covered zone,the seawater pCO_2 varied between 270 and 300 μatm due to biological CO_2 removal,the transportation of low pCO_2 water northward,and heavy ice cover.The surface seawater pCO_2 during the survey was undersaturated with respect to the atmosphere in the Canada Basin,and it was a net sink for atmospheric CO_2.The summertime net CO_2 uptake of the ice-free zone,the partially ice-covered zone and the heavily ice-covered zone was(4.14±1.08),(1.79±0.19),and(0.57±0.03) Tg/a(calculated by carbon,1Tg=10~(12) g),respectively.Overall,the net CO_2 sink of the Canada Basin in the summer of 2008 was(6.5±1.3) Tg/a,which accounted for 4%–10% of the Arctic Ocean CO_2 sink.  相似文献   

16.
海水中-氧化氮的化学发光法测定   总被引:1,自引:0,他引:1  
基于鲁米诺-H2O2混合溶液作为发光液与海水中NO发生反应产生发光信号的原理,提出了一种测定海水中痕量NO的化学发光法.确定了化学发光法测定NO的最佳条件:pH9.2、浓度1×10-2 mol/dm3的碳酸盐为缓冲体系,鲁米诺浓度为8.4×10-5 mol/dm3,H2O2浓度为1×10-2 mol/dm3,测定温度为...  相似文献   

17.
对长江口泥质区24Z孔的沉积物柱状样进行了粒度和元素分析,根据沉积物的粒度特征可将岩芯从下到上分为3个阶段:A阶段(1931—1964年)粒度参数的波动较小,各层位平均粒度Φ在5.58~7.65;B阶段(1964—1983年)粒度参数波动范围比A阶段更小,整个阶段没有出现明显峰值,Φ在6.51~7.37;C阶段(1983—2003年)粒度参数波动范围明显增大,出现多个峰值,Φ在5.59~7.46。元素Zr和Rb质量比(mZr/mRb)的大小实际上反映了粗粒级矿物与黏土粒级矿物的相对含量的高低,24Z孔的沉积物中mZr/mRb波动范围在1.02~3.59,出现了多个明显的峰值。利用24Z孔沉积物平均粒度和mZr/mRb识别出多个突变层位,结合长江中下游洪水水文记录,发现突变层位年代与20世纪80年代后的水文洪水年份有着较好的对应,这可能与长江主泓的变化有关。对比突变层位与正常层位的粒度特征,突变层位沉积物的粒度频率曲线呈负偏态且峰高而尖,正常层位粒度频率曲线呈正偏态且峰低而宽,同时,概率累积曲线也指示突变层位沉积物在沉积过程中受到了更强的水动力作用。研究长江口泥质区南部24Z孔的沉积物粒度特征和对洪水事件的沉积响应,可以更好地了解长江洪水所携带的粗颗粒物质在长江口泥质区的分布范围,有助于重建长江流域古洪水从而更好的认识长江流域洪水发生的规律。  相似文献   

18.
This paper uses the density functional theory to analyse the stabilities, bond characters, static linear polarisabilities, and aromaticities of the `in-out' isomerism Hn-60@CnH60 (n=70, 72, 74). The binding energies, C--H bond energies, and energy gaps explore that the `in-out' isometric perhydrogenation of Cn (n=70, 72, 74) can remarkably improve the stabilities. The static linear polarisabilies of Hn-60@CnH60 (n=70, 72, 74) are indeed relative to their shapes, while they show almost nonaromatic character. This study can suggest that the `in-out' isometric perhydrogenation of fullerenes could lead to the invention of entirely novel potential hydrogen storage nanomaterials.  相似文献   

19.
We report several biogeochemical parameters (dissolved inorganic carbon (DIC), total alkalinity (TA), dissolved oxygen (DO), phosphate (PO4), nitrate + nitrite (NO3 + NO2), silicate (Si(OH)4)) in a region off Otaru coast in Hokkaido, Japan on a “weekly” basis during the period of April 2002–May 2003. To better understand the long-term temporal variations of the main factors affecting CO2 flux in this coastal region and its role as a sink/source of atmospheric CO2, we constructed an algorithm of DIC and TA using other hydrographic properties. We estimated the CO2 flux across the air–sea interface by using the classical bulk method. During 1998–2003 in our study region, the estimated fCO2sea ranged about 185–335 μatm. The maximum of fCO2sea in the summer was primarily due to the change of water temperature. The minimum of fCO2sea in the early spring can be explained not only by the change of water temperature but also the change of nutrients and chlorophyll-a. To clarify the factors affecting fCO2sea (water temperature, salinity, and biological activity), we carried out a sensitivity analysis of these effects on the variation of fCO2sea. In spring, the biological effect had the largest effect for the minimum of fCO2sea (40%). In summer, the water temperature effect had the largest effect for the maximum of fCO2sea (25%). In fall, the water temperature effect had the largest effect for the minimum of fCO2sea (53%). In winter, the biological effect had the largest effect for the minimum of fCO2sea (35%).We found that our study region was a sink region of CO2 throughout a year (−0.78 mol/m2/yr). Furthermore, we estimated that the increase of fCO2sea was about 0.56 μatm/yr under equilibrium with the atmospheric CO2 content for the period 1998–2003, with the temporal changes in the variables (T, S, PO4) on fCO2sea, thus as the maximum trend of each variable on fCO2sea was 0.22 μatm/yr, and the trend of residual fCO2 including gas exchange was 0.34 μatm/yr. This result suggests that interaction among variables would affect gas exchange between air and sea effects on fCO2sea. We conclude that this study region as a representative coastal region of marginal seas of the North Pacific is special because it was measured, but there is no particular significance in comparison to any other area.  相似文献   

20.
During CREAMS expeditions, fCO2 for surface waters was measured continuously along the cruise tracks. The fCO2 in surface waters in summer varied in the range 320–440 μatm, showing moderate supersaturation with respect to atmospheric CO2. In winter, however, fCO2 showed under-saturation of CO2 in most of the area, while varying in a much wider range from 180 to 520 μatm. Some very high fCO2 values observed in the northern East Sea (Japan Sea) appeared to be associated with the intensive convection system developed in the area. A gas-exchange model was developed for describing the annual variation of fCO2 and for estimating the annual flux of CO2 at the air-sea interface. The model incorporated annual variations in SST, the thickness of the mixed layer, gas exchange associated with wind velocity, biological activity and atmospheric concentration of CO2. The model shows that the East Sea releases CO2 into the atmosphere from June to September, and absorbs CO2 during the rest of the year, from October through May. The net annual CO2 flux at the air-sea interface was estimated to be 0.032 (±0.012) Gt-C per year from the atmosphere into the East Sea. Water column chemistry shows penetration of CO2 into the whole water column, supporting a short turnover time for deep waters in the East Sea. This revised version was published online in August 2006 with corrections to the Cover Date.  相似文献   

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