共查询到19条相似文献，搜索用时 156 毫秒
1.
东太湖水温变化与水-沉积物界面热通量初探 总被引：1，自引：0，他引：1
水温对沉水植被的生长和分布具有重要作用，水-沉积物界面热通量对浅水湖泊水温变化的影响值得关注.东太湖是我国东部典型的草型浅水湖区，采用自2013年11月至2015年10月对东太湖湖心进行的不同深度水体及沉积物温度高频观测数据，结合东太湖表层沉积物的热力学性质计算了水-沉积物界面热通量，分析了东太湖水温和水-沉积物界面热通量的变化特征并探讨了其影响因素.结果表明：东太湖各深度水体日升温过程随水深增加后延，升温过程夏季延长，冬季缩短；表层水温日变幅最大，底层水温日变幅次之，沉积物温度日变幅最小，各深度温度日变幅夏季最小、冬季最大；春季和夏季升温过程中各深度日均温变化沿水深存在约1天的延迟，秋季和冬季无此现象；2015年与2014年东太湖温度变化趋势相同，同比月均温差与气温差呈线性相关.沉积物8：00-19：00向水体放热增加或从水体吸热减少，19：00至次日8：00放热减少或吸热增加；3-9月从水体吸热，为热汇，10月至次年2月向水体放热，为热源，沉积物全年为湖泊热源；逐日水-沉积物界面热通量每月6至15日存在相对年变幅较小幅度的正弦式波动.水温和水-沉积物界面热通量的变化主要受太阳辐射和气温的影响，二者对气象参数的响应具有迟滞现象；水-沉积物界面热通量与水温呈负相关，其变化相对水温迟滞，水-沉积物界面热交换的主要作用为缓冲湖泊水体的热量变化；夏季，沉水植物能降低湖泊各层水温和垂向水温差. 相似文献
2.
滇池流域点源污染控制与存在问题解析 总被引：1，自引：0，他引：1
采用间隙水连续采集法考察滇池和抚仙湖沉积物-水界面营养盐通量,并比较在氧气缺乏及氧气充足条件下界面的氮磷行为.结果表明,滇池草海沉积物-水界面营养盐通量显著高于滇池湖心及抚仙湖.对云南滇池及抚仙湖沉积物进行好氧和厌氧处理对照比较,结果显示,好氧组上覆水pH显著大于厌氧组,而间隙水pH在两处理组之间差异不显著;这可能与厌氧呼吸途径过程中产生酸性物质有关;而在两种处理条件下,间隙水均处于厌氧状态.较好氧条件而言,厌氧条件下间隙水磷和铵氮浓度的增加,与有机质矿化增强有关;而间隙水磷还可能受FeOOH-P模型控制.由分子扩散模型计算获得的界面磷或者铵氮扩散通量均高于表观通量,而且好氧条件下的扩散通量与表观通量之间的差异较厌氧条件下的大;这表明两种营养盐均存在释放潜力,但这种潜力的发挥受氧气的影响,较好氧条件而言,厌氧条件下使用分子扩散模型得到的界面营养盐扩散通量更接近于表观通量. 相似文献
3.
云南滇池和抚仙湖沉积物-水界面营养盐通量及氧气对其的影响 总被引：8，自引：2，他引：6
采用间隙水连续采集法考察滇池和抚仙湖沉积物-水界面营养盐通量,并比较在氧气缺乏及氧气充足条件下界面的氮磷行为.结果表明,滇池草海沉积物-水界面营养盐通量显著高于滇池湖心及抚仙湖.对云南滇池及抚仙湖沉积物进行好氧和厌氧处理对照比较,结果显示,好氧组上覆水pH显著大于厌氧组,而间隙水pH在两处理组之间差异不显著;这可能与厌氧呼吸途径过程中产生酸性物质有关;而在两种处理条件下,间隙水均处于厌氧状态.较好氧条件而言,厌氧条件下间隙水磷和铵氮浓度的增加,与有机质矿化增强有关;而间隙水磷还可能受FeOOH-P模型控制.由分子扩散模型计算获得的界面磷或者铵氮扩散通量均高于表观通量,而且好氧条件下的扩散通量与表观通量之间的差异较厌氧条件下的大;这表明两种营养盐均存在释放潜力,但这种潜力的发挥受氧气的影响.较好氧条件而言,厌氧条件下使用分子扩散模型得到的界面营养盐扩散通量更接近于表观通量. 相似文献
4.
湖泊水底Fe~(2+)和ΣS~(2-)浓度的快速增加是湖泛暴发最早发生于沉积物-水界面的主要前提,缺氧环境下水底扩散层附近Fe~(2+)和ΣS~(2-)的迁移是其在沉积物-水界面处稳定积累的重要原因.以蓝藻聚积水体沉积物-水界面为研究对象,应用湖泊过程模拟装置及间隙水被动采样等技术,重点研究了间隙水和底层上覆水中Fe~(2+)和ΣS~(2-)的垂向分布特征,并定量估算了二者的扩散通量及迁移方向.结果表明:湖泛样品水体沉积物-水界面处于典型的还原性环境,表层沉积物间隙水中Fe~(2+)和ΣS~(2-)浓度显著高于对照样品,二者在表层沉积物中积累趋势明显.湖泛水体沉积物-水界面处Fe~(2+)释放通量较高,表现出较强烈的自沉积物向上覆水方向的释放能力;而湖泛样品ΣS~(2-)在沉积物-水界面处释放通量为负,迁移方向为自上覆水向沉积物扩散.Fe~(2+)和ΣS~(2-)在湖泛水体沉积物-水界面处不同的迁移特征证明:缺氧/厌氧条件下,湖泊水体表层沉积物间隙水中高浓度Fe~(2+)向上覆水的扩散为湖泛致黑物质的形成提供了重要的物质基础;底层上覆水及界面水中SO~(2-)4在表层沉积物中被还原,为终端还原产物ΣS~(2-)为湖泛致黑物质的形成提供了另一重要物质来源. 相似文献
5.
沉积物-水界面污染物迁移扩散的研究进展 总被引：6，自引：0，他引：6
污染物在沉积物-水界面的迁移扩散对研究其环境生物地球化学循环过程和评估水生态系统质量具有重要意义.本文回顾了关于沉积物-水界面的基本研究历程，重点介绍沉积物-水界面的垂向结构以及扩散边界层（DBL）的作用，展示污染物在沉积物-水界面的多维度分布（一维垂向、二维平面和三维立体）及其在沉积物-水界面的扩散过程，详细总结影响污染物在沉积物-水界面迁移扩散的环境因素（包括温度、溶解氧或氧化还原条件、pH值、离子强度或盐度、沉积物组成、共存污染物、溶解性有机质、水动力条件、生物扰动、微生物以及其他因素），讨论当前关于沉积物-水界面污染物扩散通量估算几种方法的优缺点，最后，对沉积物-水界面污染物扩散研究在未来发展需要关注的几个方面进行了展望. 相似文献
6.
动力扰动下太湖梅梁湾水-沉积物界面的营养盐释放通量 总被引：2，自引：2，他引：2
通过波浪水槽试验,研究了不同水动力扰动条件下太湖梅梁湾水-沉积物界面的营养盐通量.结果发现,水动力扰动对该通量的影响很大,在中等扰动强度下(水底波切应力为0.019N·m-2,相当于梅梁湾中部夏季盛行风-东南风风速5～7 m·s-1),TN,DTN和NH4+-N的通量分别为1.92×10-3,-1.81×10-4和5.28×10-4mg·m-2·s-1(向上为正,向下为负),而TP,TDP和SRP的通量分别为5.69×10-4,1.68×10-4和-1.29×10-4mg·m-2·s-1.根据对气象资料的统计,夏季5～7 m·s-1东南风风速的最大持续时间为15h,以上述通量和风速持续时间进行计算,太湖底泥区域按水面积的47.45％,将分别有111tTN,32tNH4+-N,34tTP和10tTDP进入水体,可分别导致整个太湖水体中相应的平均浓度升高约0.025,0.007,0.007和0.002 mg·1-1.当扰动增大时(水底波切应力为0.217 N·m-2,相当于梅梁湾中部东南风速10～11 m·s-1),营养盐通量显著增加,其中TN,DTN和NH4+-N分别达1.16×10-2,6.76×10-3和1.14×10-2 mg·m-2·s-1,而TP通量亦大幅度上升,达到2.14×10-3 mg·m-2·s-1,上述通量的增加幅度均达到一个量级以上.但是,TDP的通量有所减小,其值为9.54×10-5 mg·m-2·s-1,而SRP虽然存在增加趋势,但其通量值却很小(5.42×10-5 mg·m-2·s-1).统计结果显示,太湖地区该风速的持续时间不超过5h.若以5h计,在上述强扰动情况下,营养盐释放量分别为232t TN,134.9t TDN,228t NH4+-N,42.7 t TP,2.0t TDP和1.1tSRP,水体中相应的平均浓度的升高量为0.050,0.029,0.049,0.009,0.0004和0.0002 mg·1-1.由此可见,在浅水湖泊中,动力扰动能造成水体中营养盐浓度的急骤升高,虽然在微扰动情况下,有些指标的释放通量出现负值(如DTN和SRP),水底沉积物表现为上述营养盐成分的汇集场所,但沉积物中大多数营养盐成分会随着底泥悬浮和水体-沉积物界面环境条件的改变而进入水体,给水体生态系统带来严重影响,这也是浅水湖泊所具有的显著特征之一. 相似文献
7.
季节性缺氧导致夏季沉积物内源磷强烈释放，加剧水体富营养化，是我国西南地区深水湖泊（水库）面临的重要挑战.有效增加夏季缺氧期深水沉积物-水界面的含氧量，是减少内源磷释放的关键.现有的深水增氧技术由于缺乏对沉积物-水界面增氧的针对性，因此治理效果有限.近年来，纳米气泡已被证实具有的稳定性好、氧传质速率高和环境风险低等优点，为新型深水增氧技术研发提供了巨大潜力.本文以天然矿物材料白云母、绢云母、硅藻土和沸石为基底，负载纳米气泡，研发纳米气泡改性矿物颗粒技术，开展湖泊沉积物-水界面增氧模拟实验研究，运用平面光电极技术评估其界面增氧效果.结果表明，纳米气泡改性矿物颗粒对沉积物-水界面具有比较明显的增氧效果.其中，改性白云母、绢云母和沸石的界面持续增氧时间可达7天以上，增氧后的界面最大溶解氧（DO）浓度达4.40 mg/L，而改性硅藻土不具有增氧能力.其次，矿物粒度对改性颗粒的增氧效果有一定影响：粒度越细，界面的最大增氧浓度越高，且持续增氧时间越长.纳米气泡改性矿物颗粒技术有望成为夏季缺氧期深水沉积物-水界面精准增氧和内源污染控制的有效技术手段. 相似文献
8.
浅水湖泊生态系统中的沉积物—水界面是湖泊内源氮释放的重要界面,而水动力因素是改变沉积物氮释放的重要因素.三峡大坝修建以后,长江中下游通江湖泊的水动力条件发生了明显的变化.通过采集洞庭湖湖口区域的沉积物和水样,在双向环形水槽动力模拟装置内模拟湖泊水位和流速的变化,探讨湖泊沉积物氮在沉积物和水系统中的二次释放特征.结果表明,随着扰动强度的增加,上覆水悬浮物浓度增大,上覆水中总氮浓度增加,沉积物向上覆水释放氮的强度增强,水动力条件的改变所引起的沉积物内源氮释放不容忽视.在该模拟实验条件下,沉积物存在最适扰动水位(20cm),此水位下上覆水中悬浮物浓度最低,总氮浓度最小.水动力条件的改变对上覆水和沉积物—水界面处铵态氮和硝态氮浓度的影响并不明显,孔隙水中铵态氮与硝态氮之间发生形态的转化. 相似文献
9.
湖泊污染底泥疏浚后新生沉积物-水界面溶解氧的动态响应 总被引：1，自引：1，他引：0
借助微氧电极测试技术对太湖贡湖湾试验区疏浚后的新生界面溶解氧动态进行一年的跟踪调研，分析溶解氧在新生微米级界面的分布特征、扩散通量以及界面附近有机质矿化速率.结果表明疏浚后半年内，溶解氧在表层沉积物的侵蚀深度增大，氧化层明显加厚.氧气在新生界面表层沉积物中呈指数下降，但衰减相对较缓.在连续一年的跟踪调查中发现，仅秋季新生界面附近溶解氧浓度明显高于对照，而在其他月份无差异.污染底泥疏浚后一个月内氧扩散通量及有机碳矿化速率下降最为明显，仅为疏浚前的13%，其他月份沉积物-水界面氧的扩散通量、氧气的消耗速率、有机碳的降解速率均有不同程度下降，疏浚后新生界面氧气交换速率下降以及由此导致的有机碳矿化过程变缓可能深刻影响界面生源要素的迁移过程. 相似文献
10.
东巢湖沉积物水界面氮、磷、氧迁移特征及意义 总被引：2，自引：0，他引：2
以东巢湖近城市湖湾沉积物为研究对象,在沉积物氮、磷营养盐分析的基础上,采用沉积物柱状芯样静态释放模拟法定量评估研究区域沉积物—水界面氨氮、溶解性活性磷酸盐营养盐释放潜力,利用微电极非损伤测定技术获得沉积物—水微界面溶解氧(DO)剖面分布及微界面DO消耗和扩散特征.结果表明:东巢湖近城市湖湾沉积物氮、磷污染物蓄积量较高,受TN、TP污染程度较重.沉积物内源氨氮、磷酸盐释放明显,平均释放速率分别达到32.44 mg/(m~2·d)和1.25mg/(m~2·d),区域内沉积物已成为水柱中氮、磷营养盐的污染源.研究区域上覆水体处于好氧状态,沉积物—水微界面平均DO穿透深度(OPD)达到5.3 mm,平均DO扩散通量为4.56 mmol/(m~2·d),表现出良好的DO扩散能力.沉积物内源氨氮和磷酸盐释放能力与表层沉积物TN/TP物质含量及沉积物—水微界面DO穿透深度有关,在沉积物氮、磷污染较重的情况下,DO穿透深度越低越有利于氮、磷污染物从沉积物向上覆水体释放. 相似文献
11.
湖泊沉积物-水界面营养盐释放是研究湖泊环境行为的重点关注对象,但目前对于湖泊通量的估算方法选择缺乏横向定量比较.以南京莫愁湖为研究对象,在冬春夏3季采用静态释放培养法、机械搅拌培养法、流动培养法和间隙水浓度扩散模型法4种常见的湖泊通量培养方法进行氮磷释放对比实验.结果表明,非扩散模型法（静态释放、机械搅拌、流动培养）在冬季存在负通量,随着气温升高,夏季通量估算值为正,且该3种方法通量数值差异不显著.间隙水扩散模型法在三季实验中结果数值无负值,对比非扩散模型组具有显著差异,约低一个数量级.不同方法在培育过程中溶解氧和pH变化差异显著,流动培养法最为稳定.4种方法的通量结果在不同季节变化趋势具有显著相关性,非扩散模型法估算结果作为表观通量值,适用于计算湖泊沉积物营养盐释放总量,其中静态释放法结果稳定性较差,平行组相对标准偏差最高达70%;流动培养法稳定性最好,平行组相对标准偏差最高仅21%.扩散模型法估算结果作为理论释放值,在估算浅水湖泊通量时低于实际释放通量,适于探究深水湖泊沉积物间隙水动态释放过程,有助于分析湖泊沉积物性质.不同培养方法,有其侧重点,根据不同湖泊状况,应选取合适方法进行通量估算. 相似文献
12.
The hydrodynamics of a system where there is a coupled flow above and below a sediment–water interface (SWI) are not completely understood. We numerically simulate mean two-dimensional, unidirectional, steady, viscous flow in these systems using a sequentially coupled formulation. Simulations were conducted to determine fundamental relationships between bedform geometry, Reynolds number for the water-column flow (Re), interfacial exchange zone depth (dz) in the sediments, and flux through the SWI (qint); the latter two parameters play a significant role in biogeochemical and aquatic-life processes across the SWI. dz and Re are functionally related through an asymptotic growth-curve model while qint and Re follow a power function. These relationships are dynamically explained by the manner in which pressure gradients along the SWI develop due to current–bedform interactions at different Res and by Darcy’s Law. We found that the coupling between water column and exchange zone flow is controlled by the behavior of the water-column eddy. The eddy detaches at or near the point of minimum pressure along the interface, and reattaches near the point of maximum pressure. These two critical points determine the pressure gradient along the bed surface that controls the exchange zone flow field. Moreover, the reattachment point corresponds to flow divides within the sediments. Lastly, pore-water velocities drop with depth below the SWI, and are larger below the bedform crests than below the troughs. 相似文献
13.
The concentrations of222Rn and226Ra in the water column and in the sediments of Santa Barbara and San Nicolas Basins have been measured semi-annually over the last four years. Approximately one-third of excess radon profiles obtained in the water column in these basins can be adequately fit with a one-dimensional eddy diffusion-decay model. Exponential profiles in the center of San Nicolas Basin yield a vertical eddy diffusivity of 26±16 cm2/s and 3.4±1.0 cm2/s for Santa Barbara Basin. The application of a two-dimensional eddy diffusion-decay model to profiles obtained in the center and on the margins of San Nicolas Basin produces a better fit than is found using a one-dimensional vertical eddy diffusivity. The two-dimensional model for San Nicolas Basin predicts a vertical eddy diffusivity of 17 cm2/s and a horizontal eddy diffusivity of 105 cm2/s. These values are in reasonable agreement with those predicted from the vertical buoyancy gradient and the horizontal length scale.The vertically integrated radon excess (standing crop) in the water column of Santa Barbara Basin averages 53±23 atoms/m2 s. This is in good agreement with the flux across the sediment-water interface of 60±15 atoms/m2 s, calculated by measuring radon emanation in the sediments as a function of depth and applying a molecular diffusion-reaction model. Hence, one-dimensional molecular diffusion accurately predicts the flux of radon from the laminated Santa Barbara Basin sediments. In San Nicolas Basin the integrated radon excess in the water column is 376±143 atoms/m2 s, but the diffusive randon flux from San Nicolas Basin sediments averages only 190±53 atoms/m2 s. This descrepancy indicates that a non-diffusive process, probably macrofaunal irrigation, supplies much of the flux of radon from San Nicolas Basin sediments. 相似文献
14.
Darrell F. Strobel 《Pure and Applied Geophysics》1989,130(2-3):533-546
A review of the important constraints on gravity wave induced diffusion of chemical tracers, heat, and momentum is given. Ground-based microwave spectroscopy measurements of H2O and CO and rocket-based mass spectrometer measurements of Ar constrain the eddy diffusion coefficient for constituent transport (K
zz
) to be (1–3)×105 cm2s–1 in the upper mesosphere. Atomic oxygen data also limitsK
zz
to a comparable value at the mesopause. From the energy balance of the upper mesosphere the eddy diffusion coefficient for heat transport (D
H
) is, at most 6×105 cm2s–1 at the mesopause and decreasing substantially with decreasing altitude. The available evidence for mean wind deceleration and the corresponding eddy diffusion coefficient for momentum stresses (D
M
) suggests that it is at least 1×106 cm2s–1, in the upper mesosphere. Consequently the eddy Prandtl number for macroscopic scale lengths is >3. 相似文献
15.
我国南方地区桉树种植区周边水库冬季水体泛黑现象频发,桉树砍伐残体(尤其是叶)浸出液中富含的溶解性有机碳(DOC)、单宁酸与铁、锰、硫化物等一系列反应是其主要致黑原因,然而目前致黑物质对水库泛黑的贡献程度和途径仍不清楚.为了模拟桉树叶浸泡对水库黑水形成的影响机制,研究选取夏季水体未泛黑期(水体热分层稳定)进行室内浸泡实验,测定每6 h上覆水体溶解氧(DO)、氧化还原电位(Eh)、透光度等理化指标,分析DGT有效态铁、锰、硫和DOC、单宁酸浓度分布规律及迁移转化特征,计算沉积物-水界面处Fe2+、Mn2+、S2-表观扩散通量.结果表明:桉树叶浸泡明显消耗水体中的DO,且显著影响水体Eh与透光度.此外,透光度与DO浓度呈显著正相关(相关系数为0.618~0.978).桉树叶浸泡释放大量DOC和单宁酸,其中单宁酸浓度远超有氧马尾松组,其上覆水中浓度分别达到23.9、26.0和34.0 mg/L,说明桉树浸泡为黑水形成提供了重要的DOC和单宁酸来源.桉树叶浸泡后上覆水和表层沉积物中DGT有效态Fe浓度均明显增加,深层沉积物间隙水中DGT有效态Fe浓度明显下降,且其表观扩散通量均为正值,说明深层沉积物中Fe向沉积物-水界面迁移,为黑水形成提供了重要的Fe来源.研究结果可为解决我国南方地区桉树人工林区水库水体突发性泛黑问题提供科学依据. 相似文献
16.
For flux measurement, the eddy covariance technique supplies a possibility to directly measure the exchange between vegetation and atmosphere; and there are two kinds of eddy covariance systems, open-path and close-path systems. For the system error, it may result in difference of flux measurements by two systems. Therefore, it is necessary to compare the measured results from them. ChinaFLUX covers of eight sites applied the micrometeorological method, in which Changbai Mountains (CBS) and Qianyanzhou (QYZ) carried out open-path eddy covariance (OPEC) and close-path eddy covariance (CPEC) measurements synchronously.In this paper the data sets of CBS and QYZ were employed. The delay time of close-path analyzer to the open-path analyzer was calculated; the spectra and cospectra of time-series data of OPEC and CPEC were analyzed; the open-path flux measurement was used as a standard comparison, the close-path flux measurement results were evaluated. The results show that, at two sites the delay time of CO2 density for close-path analyzer was about 7.0-8.0 s, H2O density about 8.0-9.0 s; the spectrum from the open-path, close-path and 3D sonic anemometer was consistent with the expected -2/3 slope (log-log plot), and the cospectra showed the expected slope of -4/3 in the internal subrange; the CO2 flux measured by the close-path sensor was about 84% of that of open-path measurement at QYZ, about 80% at CBS, and the latent heat flux was balanced for two systems at QYZ, 86% at CBS. From the flux difference between open-path and close-path analyzers, it could be inferred that the attenuation of turbulent fluctuations in flow through tube of CPEC affected H2O flux more significantly than CO2 flux. The gap between two systems was bigger at CBS than at QYZ; the diurnal variation in CO2 flux of two measurement systems was very consistent. 相似文献
17.
Shuko Hamada Takeshi Ohta Tetsuya Hiyama Takashi Kuwada Atsuhiro Takahashi Trofim C. Maximov 《水文研究》2004,18(1):23-39
Seasonal changes in the water and energy exchanges over a pine forest in eastern Siberia were investigated and compared with published data from a nearby larch forest. Continuous observations (April to August 2000) were made of the eddy‐correlation sensible heat flux and latent heat flux above the canopy. The energy balance was almost closed, although the sum of the turbulent fluxes sometimes exceeded the available energy flux (Rn ? G) when the latent heat flux was large; this was related to the wind direction. We examined the seasonal variation in energy balance components at this site. The seasonal variation and magnitude of the sensible heat flux (H) was similar to that of the latent heat flux (λE), with maximum values occurring in mid‐June. Consequently, the Bowen ratio was around 1·0 on many days during the study period. On some clear days just after rainfall, λE was very large and the sum of H and λE exceeded Rn ? G. The evapotranspiration rate above the dry canopy from May to August was 2·2 mm day?1. The contributions of understory evapotranspiration (Eu) and overstory transpiration (Eo) to the evapotranspiration of the entire ecosystem (Et) were both from 25 to 50% throughout the period analysed. These results suggest that Eu plays a very important role in the water cycle at this site. From snowmelt through the tree growth season (23 April to 19 August 2000), the total incoming water, comprised of the sum of precipitation and the water equivalent of the snow at the beginning of the melt season, was 228 mm. Total evapotranspiration from the forest, including interception loss and evaporation from the soil when the canopy was wet, was 208–254 mm. The difference between the incoming and outgoing amounts in the water balance was from +20 to ?26 mm. The water and energy exchanges of the pine and larch forest differed in that λE and H increased slowly in the pine forest, whereas λE increased rapidly in the larch forest and H decreased sharply after the melting season. Consequently, the shape of the Bowen ratio curves at the two sites differed over the period analysed, as a result of the differences in the species in each forest and in soil thawing. Copyright © 2003 John Wiley & Sons, Ltd. 相似文献
18.
F. Holwerda R. Burkard W. Eugster F. N. Scatena A. G. C. A. Meesters L. A. Bruijnzeel 《水文研究》2006,20(13):2669-2692
The deposition of fog to a wind‐exposed 3 m tall Puerto Rican cloud forest at 1010 m elevation was studied using the water budget and eddy covariance methods. Fog deposition was calculated from the water budget as throughfall plus stemflow plus interception loss minus rainfall corrected for wind‐induced loss and effect of slope. The eddy covariance method was used to calculate the turbulent liquid cloud water flux from instantaneous turbulent deviations of the surface‐normal wind component and cloud liquid water content as measured at 4 m above the forest canopy. Fog deposition rates according to the water budget under rain‐free conditions (0·11 ± 0·05 mm h?1) and rainy conditions (0·24 ± 0·13 mm h?1) were about three to six times the eddy‐covariance‐based estimate (0·04 ± 0·002 mm h?1). Under rain‐free conditions, water‐budget‐based fog deposition rates were positively correlated with horizontal fluxes of liquid cloud water (as calculated from wind speed and liquid water content data). Under rainy conditions, the correlation became very poor, presumably because of errors in the corrected rainfall amounts and very high spatial variability in throughfall. It was demonstrated that the turbulent liquid cloud water fluxes as measured at 4 m above the forest could be only ～40% of the fluxes at the canopy level itself due to condensation of moisture in air moving upslope. Other factors, which may have contributed to the discrepancy in results obtained with the two methods, were related to effects of footprint mismatch and methodological problems with rainfall measurements under the prevailing windy conditions. Best estimates of annual fog deposition amounted to ～770 mm year?1 for the summit cloud forest just below the ridge top (according to the water budget method) and ～785 mm year?1 for the cloud forest on the lower windward slope (using the eddy‐covariance‐based deposition rate corrected for estimated vertical flux divergence). Copyright © 2006 John Wiley & Sons, Ltd. 相似文献
19.
Modeling gross primary production of a temperate grassland ecosystem in Inner Mongolia,China, using MODIS imagery and climate data 总被引：5，自引：0，他引：5
WeiXing Wu ShaoQiang Wang XiangMing Xiao GuiRui Yu YuLing Fu YanBin Hao 《中国科学D辑(英文版)》2008,51(10):1501-1512
Carbon fluxes in temperate grassland ecosystems are characterized by large inter-annual variations due to fluctuations in precipitation and land water availability. Since an eddy flux tower has been in operation in the Xilin Gol grassland, which belongs to typical temperate grassland in North China, in this study, observed eddy covariance flux data were used to critically evaluate the biophysical per- formance of different remote sensing vegetation indices in relation to carbon fluxes. Furthermore, vegetation photosynthesis model (VPM) was introduced to estimate gross primary production (GPP) of the grassland ecosystem for assessing its dependability. As defined by the input variables of VPM, Moderate Resolution Imaging Spectroradimeter (MODIS) and standard data product MOD09A1 were downloaded for calculating enhanced vegetation index (EVI) and land surface water index (LSWI). Measured air temperature (Ta) and photosynthetically active radiation (PAR) data were also included for model simulating. Field CO2 flux data, during the period from May, 2003 to September, 2005, were used to estimate the "observed" GPP (GPPobs) for validation. The seasonal dynamics of GPP predicted from VPM (GPPVPM) was compared quite well (R2=0.903, N=111, p<0.0001) with the observed GPP. The ag- gregate GPPVPM for the study period was 641.5 g C·m?2, representing a ~6% over-estimation, compared with GPPobs. Additionally, GPP predicted from other two typical production efficiency model (PEM) represents either higher overestimation or lower underestimation to GPPobs. Results of this study demonstrate that VPM has potential for estimating site-level or regional grassland GPP, and might be an effective tool for scaling-up carbon fluxes. 相似文献