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1.
在巢湖西北半湖近岸带设置大型围隔研究秋季连续打捞蓝藻对湖泊温室气体通量的影响，应用YL-1000型大型仿生式水面蓝藻清除设备进行原位打捞蓝藻，通过便携式温室气体分析仪-静态箱法对大型围隔内水-气界面CH4、CO2通量特征及其影响因素进行观测.结果表明：对比未打捞区，蓝藻连续打捞下打捞区水体中叶绿素a（Chl.a）、悬浮物（SS）浓度不断下降，两者削减率分别为72%、85%，Chl.a、SS浓度分别下降到29.6±2.5 μg/L、12.5±1.2 mg/L，打捞对围隔内颗粒态物质去除效果十分明显；打捞过程中水体溶解性有机物（DOM）中微生物代谢类腐殖质（C1）、类蛋白（C3）显著下降趋势，打捞区C1、C3组分（0.18±0.02、0.06±0.01 RU）强度明显低于未打捞区（0.26±0.05、0.12±0.03 RU），打捞能有效控制藻源性溶解性有机质释放.同时，打捞区水-气界面CH4通量呈显著下降趋势，未打捞区CH4通量平均值（17.473±1.514 nmol/（m2·s））为打捞区（7.004±4.163 nmol/（m2·s））近2倍，CH4通量与Chl.a、C1、C3组分均呈显著正相关，水体中藻源性溶解态有机质对CH4通量具有促进作用；打捞区CO2释放通量呈显著上升趋势，打捞区CO2吸收通量（-0.200±0.069 μmol/（m2·s））明显低于未打捞区（-0.344±0.017 μmol/（m2·s）），CO2通量与Chl.a、温度均呈显著负相关.秋季打捞对CH4、CO2综合日平均通量减排量值为0.275±0.076 mol/（m2·d）（以CO2当量计）.研究结果揭示了巢湖秋季连续打捞蓝藻过程对水-气界面温室气体具有显著减排作用，且能在一定程度上减缓蓝藻水华与湖泊富营养化、气候变暖之间的恶性循环，为湖泊碳循环和蓝藻水华灾害防控提供科学数据支撑和理论参考. 相似文献
2.
藏南羊卓雍错湖面大气湍流特征观测分析 总被引：2，自引：1，他引：1
湍流运动是大气边界层的本质特征，是地表与大气之间能量和物质交换的主要方式.本文利用2016和2017年4-10月藏南羊卓雍错湖泊涡动观测资料，分析了湖面大气湍流方差和湍流特征量的统计和变化特征.结果表明：（1）不稳定层结下，三维风速分量和超声虚温、水汽密度、CO2密度的无量纲标准差随稳定度变化符合Monin-Obukhov相似理论的"1/3"或"-1/3"次幂律，垂直风速的拟合效果最好；稳定层结下，除CO2密度无量纲标准差与稳定度无明显关系外，其他量基本上满足相似性规律；中性条件下，以上物理量的无量纲标准差分别趋近常数：3.57、3.93、0.77、20.91、6.35和11.96.（2）水平方向平均湍流强度（0.60和0.58）大于垂直方向（0.13），三维方向湍流强度与平均风速的变化呈显著负相关，相关系数分别为-0.39、-0.42和-0.34.（3）湖面湍流动能随风速呈线性增长，增长率达0.45 m/s；近中性层结时湍流动能最大，层结越稳定或不稳定湍流动能均减小.（4）湖泊下午到傍晚动量输送较强，13：00-22：30时间段平均动量通量达0.091 kg/（m·s2）；热量输送以潜热为主，潜热通量日平均值（77.3 W/m2）是感热通量（14.6 W/m2）的5.3倍，感热和潜热通量日变化峰值分别出现在5：30（22.4 W/m2）和16：00（106.6 W/m2）. 相似文献
3.
以滇池典型生态修复区——大泊口水域为研究对象,研究了富营养化高原湖泊种子库时空特征、种子库与地表覆盖水生植被及水环境的相关关系和恢复潜力.利用高密度样方原位观测与温室控制种子萌发实验相结合,基于2014-2016共3年的长期定位研究,分析湖泊平均种子库密度、分布格局及与覆盖水生植物Sørensen相似性关系,结果显示：年平均种子库形成率在20.35%~34.13%之间,种子库密度2014年为546.67粒/m2,2015年为826粒/m2,2016年为1682粒/m2,眼子菜科的篦齿眼子菜（Potamogeton pectinatus L.）、金鱼藻科的金鱼藻（Ceratophyllum demersum L.）等耐污种属对种子库构成和年增长率贡献较大;垂直方向上种子主要分布于深层底泥（5~30 cm）.随着在时间尺度上的延长,种子库分布更为广泛,且规模越来越大（其中500粒/m2以上规模的分布频率显示增多）.离散系数（V/m）与Lloyd平均拥挤指数（m*）分析显示主要优势群丛（篦齿眼子菜等）为聚集分布,其余为均匀空间分布格局;种子库与水生植被关系评价指标Sørensen相似性系数（SC）研究显示,滇池大泊口平均SC=（0.3628±0.0265）,在湖泊湿地类型和草本群落植被类型属性上处于较低水平,即显示目前植物群落演替过程发生较快,耐污先锋种属在恢复进程上占据优势生态位,而历史优势种和对水环境要求较高的物种却未能规模萌发,一定程度上揭示了高原富营养化湖泊种子库中历史优势植被可恢复性的特征及难点. 相似文献
4.
人为干扰和气候变化会改变湖泊水位状态，明确不同水位条件下湖泊沉积物有机碳矿化特征及其影响因素，对了解内陆水生态系统碳循环具有重要意义.为探究干旱区典型盐湖沉积物有机碳矿化速率对水位变化的响应，以巴里坤湖干涸湖底原状沉积物为研究对象，初步探究了0（T1）、-9（T2）、-23（T3）、-34（T4）和-45 cm（T5）水位处理对沉积物有机碳矿化速率的影响.结果表明，T1、T2和T3处理有机碳矿化速率在试验初期较高（0~10 d），10 d后缓慢下降，T4和T5处理有机碳矿化速率呈先增加后降低趋势；T1（1.718 μmol/（m2·s））与T3（1.784 μmol/（m2·s））处理有机碳矿化速率不存在显著差异，T1处理有机碳矿化速率是T2、T4和T5处理的1.09、3.31和3.57倍，不同处理有机碳累积矿化量表现为T3 > T1 > T2 > T4 > T5.有机碳累积矿化量（Ct）占沉积物有机碳（C0）的比例（Ct/C0）介于0.012~0.044之间，沉积物有机碳潜在排放量（Ci）占C0的比例（Ci/C0）介于0.018~0.045之间；水位降低，沉积物有机碳矿化常数（k值）减小，T1处理k值最大（0.137 d），T4处理最小（0.032 d）.线性方程Cr=0.008x+0.488能较好地模拟有机碳矿化速率（Cr）与水位（x）的关系；不同水位处理有机碳矿化速率与模拟柱中沉积物5 cm温度呈显著的指数函数关系，T4、T5处理有机碳矿化温度敏感系数（Q10）显著高于T1、T2和T3处理，即水位降低增加了巴里坤湖干涸湖底沉积物Q10.因此，就巴里坤湖干涸湖底沉积物而言，水位从0 cm降至-45 cm时有机碳矿化速率降低，Q10增加；反之水位上升则会促进有机碳矿化分解，Q10降低.水位持续下降抑制有机碳矿化可能是维持干旱区盐湖沉积物碳库稳定的机制之一. 相似文献
5.
云南程海浮游植物初级生产力的时空变化及其影响因子 总被引：1，自引：0，他引：1
2016年4月-2017年2月，采用黑白瓶法研究了云南程海单点（码头点位）浮游植物初级生产力的垂直分布及其季节变化，同时基于全湖9个点位的现场调查和生产力垂向归纳模型（VGPM）估算并探讨了程海浮游植物初级生产力的时空变化及其主要影响因子.结果显示，码头点位的年均（均值±标准误）水柱（0~3 m）总初级生产力（GPPC）、净初级生产力（NPPC）和呼吸消耗量（RC）分别为5.40×103±0.64×103、2.36×103±0.63×103和3.06×103±0.82×103 mg O2/（m2·d）；不论春夏季（4-8月）、秋冬季（9月-次年2月）还是全年，码头点位的单位生物量GPP（GPP/Chl.a）和单位生物量NPP（NPP/Chl.a）的最大值和最小值均分别出现在水下0.5 m和3.0 m处.经VPGM估算，程海全湖的初级生产力（PPeu）年均值为6.54×103±0.30×103 mg C/（m2·d）（2.74×103~18.62×103 mg C/（m2·d））.PPeu的时空变化方面，春夏季是PPeu快速上升的时节，秋冬季PPeu的月变化则呈波动状态，春夏季与秋冬季PPeu无显著性差异；PPeu整体空间异质性较弱，仅在降水最为充沛的7、8月表现出南北向的异质性，这与降水条件和流域营养盐输入的空间异质性有关.回归分析发现，虽然程海PPeu的主要影响因子具有季节异质性，但不论春夏季、秋冬季还是全年，浮游植物生物量均是重要的影响因子，水温亦是春夏季的重要影响因子. 相似文献
6.
湖库淡水水域对温室气体排放的贡献不容小觑,然而观测时间的代表性不足以及缺乏对降雨因素的考虑制约了碳排放的准确估计.本研究以湖北宜昌境内官庄水库为例,选取强降雨多发的夏季时段,针对水气界面温室气体通量、水体表层和垂向剖面气体溶存浓度及环境因子开展了为期1周的原位高频观测,以探讨夏季降雨事件对水库温室气体通量变化的影响.结果表明,观测期内官庄水库水气界面CH4通量变化范围为0.007~0.077 mg/（m2·h）,CO2通量范围为5.48~57.57 mg/（m2·h）,白天和夜晚均表现为大气的碳源.小雨、中雨乃至暴雨天气条件下,CH4和CO2日均通量均较低,日通量倾向于受风速和温度调控.CH4和CO2通量变化趋势较为一致,观测期内日间排放量高于夜间排放量出现的次数更多,昼夜差异对降雨天气状况无明显响应,风速是CH4和CO2通量昼夜变化的主导因素.暴雨过程中,CH4-k600和CO2-k600与水气温差存在显著正相关,但水体垂向混合过程十分短暂.在平均雨强为3.8 mm/h的暴雨第I阶段,CH4-k600对风速和降雨的响应明显,而在雨强更大（8.5 mm/h）的第II阶段,CH4-k600与风速、降雨均未表现出相关性,通量箱在强降雨条件下的适用性可能存在雨强阈值. 相似文献
7.
C. O. Oluwafemi 《Pure and Applied Geophysics》1983,121(5-6):1065-1076
Solar, sky, and aureole radiance data from Kensington, Australia, and Lagos, Nigeria, are analysed. The values of the aerosol
optical thickness at Lagos are comparable to measured values elsewhere in the subregion (Abidjan) under light haze. The values
at Kensington are close to those of the “background aerosol.” Identical and anomalous values of aerosol optical thickness
occurred at 1.67 μm at both stations as less than 15% of the values can be accounted for by aerosols. The high optical depths
are therefore explained in terms of absorption, possibly mainly by CO2 (59–65%) and, to a lesser extent, by H2O (20–26%). Following correction for molecular multiple scattering, the aerosol scattering phase function increases substantially
at 0.5 μm in Kensington and decreases considerably at 0.76 μm in Lagos when compared to the uncorrected function, confirming
the relative fineness of the Kensington aerosol. The Lagos aerosol size distribution for moderately dusty air is reasonably
bimodally log-normal with modal radiusr
m=0.49 μm (1.36 μm) for the moder≤1 μm (r>1 μm). The Kensington aerosol resembles one withr
m=0.05 μm forr<1 μm. There the Born approximation appears appropriate, and the weighted mean square radiusp
2=0.13 μm2. In the near forward direction the aerosol scattering phase funciton for Lagos resembles Deirmendjian’s simulations for a
silicate-L haze and, for Kensington, a silicate-H haze. 相似文献
8.
中国松辽盆地商业天然气的非生物成因烷烃气体 总被引：4，自引：0，他引：4
阐述了自然界不同物质来源、不同成烃环境和不同成烃机制, 形成的各类烷烃气体的碳、氢同位素动力学分馏效应及其同位素组成和分布特征. 指出复杂高分子沉积有机质经生物降解作用和热降解作用形成细菌成因气和热成因气. 细菌成因甲烷δ13C1, -110‰~-50‰; 热成因甲烷δ13C1, -50‰~-35‰(或更重). 受同位素动力学分馏效应的制约, 细菌成因和热成因烷烃的碳氢同位素δ13C值和δD值均具有正序分布特征, 即δ13C1< δ13C2< δ13C3< δ13C4和δDCH4< δ DC2H6< δDC3H8< δDC4H10, 且二者之间具正相关关系. 自然界非生物化学过程, 由简单含碳分子(CH4, CO, 和CO2)经聚合反应生成的非生物成因烷烃气体, 甲烷的δ13C1值大于-30‰. 受其同位素动力学分馏效应的制约, 烷烃气体的碳同位素δ13C值具反序分布特征, 氢同位素δD值则具有正序分布特征, 即δ13C1> δ13C2> δ13C3> δ13C4和δDCH4< δDC2H6< δDC3H8< δDC4H10, 且二者之间具负相关关系. 分布于中国松辽盆地徐家围子断陷和莺山-庙台子断陷的26口商业天然气井, 天然气的甲烷碳同位素δ13C1值为-30.5‰~-16.7‰, 氢同位素d D值的变化范围极窄, 为-203‰~-196‰. 烷烃碳同位素δ13C值具反序分布特征, 氢同位素δD值具正序分布特征. 烷烃碳同位素δ13C值和氢同位素δD值之间具负相关关系, 显示了非生物成因特征. 研究表明, 在自然界不仅存在非生物成因甲烷, 而且作为能源气体, 非生物成因烷烃气体还能聚集形成有商业价值的天然气藏. 据估算松辽盆地26口具非生物成因特征的天然气井的储量超过500×108 m3. 松辽盆地勘探实践表明非生物成因天然气具有良好的资源前景, 为在世界范围内研究和寻找非生物成因商业天然气提供了典型实例. 相似文献
9.
内陆水域二氧化碳(CO2)排放是全球碳平衡的重要组成部分,全球CO2排放通量估算通常有很大不确定性,一方面源于CO2排放数据观测的时空离散性,另一方面也是缺少水文情景与CO2排放通量关联性的研究.本文观测了2018年洪泽湖不同水文情景表层水体CO2排放通量特征,并探讨其影响因素.结果表明,洪泽湖CO2排放通量为丰水期((106.9±73.4) mmol/(m2·d))>枯水期((18.7±13.6) mmol/(m2·d))>平水期((5.2±15.5) mmol/(m2·d)),且碳通量由丰(310.2~32.0 mmol/(m2·d))、枯(50.8~2.2 mmol/(m2·d))、平(-17.3~39.8 mmol/(m2·d))3种水文情景的交替表现出湖泊碳源到弱碳汇的转变,空间上CO2排放通量总体呈现北部成子湖区低、南部过水湖区高的分布趋势.洪泽湖CO2排放对水文情景响应敏感,特别是上游淮河流域来水量的改变,是主导该湖CO2排放时空分异的重要因子.丰水期湖泊接纳了淮河更多有机和无机碳的输入,外源碳基质的降解和矿化显著促进了水体CO2的生产与排放,同时氮、磷等营养物质的大量输入,加剧了水体营养化程度,进一步提高CO2排放量,间接反映出人类活动对洪泽湖CO2变化的深刻影响.平、枯水期随着上游淮河来水量的减少,驱动水体CO2排放的因素逐渐由外源输入转变为水体有机质的呼吸降解.此外,上游河口区DOM中陆源类腐殖质的累积与矿化能够促进CO2的排放,而内源有机质组分似乎并没有直接参与CO2的排放过程.研究结果揭示了水文情景交替对湖库CO2排放的重要影响,同时有必要进行高频观测以进一步明晰湖泊的碳通量变化及其控制因素. 相似文献
10.
模型估算法是水-气界面甲烷（CH4）通量监测的主要方法.本研究选择6种不同的参数化模型方法估算了2015年6、8和10月两个亚热带河口养殖塘水-气界面CH4传输速率（kx）及其扩散通量，探讨了河口养殖塘kx及CH4扩散通量的变化特征和影响因子.结果表明：研究期间，不同模型估算下的kx及其扩散通量均值在闽江河口养殖塘变化范围分别为1.60±0.75~6.29±1.30 cm/h和9.19±2.67~30.64±6.28 μmol/（m2·h），在九龙江河口养殖塘的变化范围分别为0.89±0.19~6.07±0.61 cm/h和3.18±0.48~21.03±2.13 μmol/（m2·h）；kx及其扩散通量在两个河口区均呈现随时间推移而升高的特征；整个养殖期间，养殖塘水-气界面平均CH4传输速率kx呈现闽江河口略高于九龙江河口（P>0.05），但水-气界面平均CH4扩散通量呈现闽江河口显著高于九龙江河口的特征（P<0.05）；风速、水体溶解CH4浓度和盐度是调控河口区养殖塘水-气界面CH4扩散通量变化的重要因子；不同模型估算出的河口养殖塘水-气界面CH4传输速率kx存在差异，表明模型估算法获得的水-气界面CH4扩散通量存在一定的不确定性. 相似文献
11.
The eddy covariance and energy balance method was employed to determine evapotranspiration (LE) over a wet temperate C3–C4 co‐existing grassland in Japan. After sensible heat flux (H) was estimated via the eddy covariance technique, LE was calculated as the residual of the energy budget with calibration against the direct measurements of LE by a lysimeter. Daily mean LE varied from 0·8 to 10·5 MJ d−1, with a peak at 16·5 MJ d−1 in late July to early August. Day‐to‐day and seasonal variability in LE was affected appreciably by net radiation (Rn), atmospheric vapour pressure deficit (VPD), canopy surface conductance (gc) and leaf area index (LAI). Before the canopy closure, LE responded to LAI in a linear manner. However, LE decreased with increasing LAI later in summer. Daytime variation in the decoupling coefficient (Ω) demonstrates that the canopy decoupled from the atmosphere in the morning and LE was primarily driven by the available energy, while in the afternoon the canopy partially coupled to the atmosphere so that LE was sensitive to VPD and gc. Throughout the whole measurement period, Ω was generally larger than 0·5, suggesting that the available energy contributes more to LE than VPD. Copyright © 2004 John Wiley & Sons, Ltd. 相似文献
12.
源区划分和质量过滤提高湖面涡动相关通量数据可靠性的同时,却降低了通量时间序列的连续性.为此,本文基于TensorFlow机器学习框架构建了一种超宽人工神经网络(ANN)模型.在选择输入ANN模型的特征变量信息时,我们采取了尽可能获取湍流输送过程中热力、动力学同步观测背景强迫信息的原则.通过ANN模型模拟通量的插补,本文实现了通量时间序列连续性的优化,插补后的羊卓雍错湖面通量数据的时间覆盖率从不足0.40提升至超过0.98.基于10次折叠交叉验证的ANN模型通量模拟性能检验则表明,各个检验组之间ANN模型的模拟误差波动较小,这显示出了较好的稳健性.具体地讲,感热通量、潜热通量和水汽通量原始观测平均值分别约为18.8 W/m~2、81.5 W/m~2和1.84 mmol/(s·m~2),10组交叉验证的插补感热通量、潜热通量和水汽通量平均绝对误差分别为5.4 W/m~2、15.7 W/m~2和0.35 mmol/(s·m~2).这表明本文所探索的ANN建模结构和同步观测变量筛选原则可更充分地利用观测点局地同步观测信息估算通量强度,有效地优化湍流通量数据的时间连续性,从而提升通量数据的可分析性. 相似文献
13.
Jiabing Wu Dexin Guan Shijie Han Tingting Shi Changjie Jin Tiefan Pei Guirui Yu 《水文研究》2007,21(18):2425-2434
Components of the energy budget were measured continuously above a 300‐year‐old temperate mixed forest at the Changbaishan site, northeastern China, from 1 January to 31 December 2003, as a part of the ChinaFlux programme. The albedo values above the canopy were lower than most temperate forests, and the values for snow‐covered canopy were over 50% higher than for the snow‐free canopy. In winter, net radiation Rn was generally less than 5% of the summer value due to high albedo and low incoming solar radiation. The annual mean latent heat LE was 37·5 W m?2, accounting for 52% of Rn. The maximum daily evaporation was about 4·6 mm day?1 in summer. Over the year, the accumulated precipitation was 578 mm; this compares with 493 mm of evapotranspiration, which shows that more than 85% of water was returned to the atmosphere through evapotranspiration. The LE was strongly affected by the transpiration activity and increased quickly as the broadleaved trees began to foliate. The sensible heat H dropped at that time, although Rn increased. Consequently, the seasonal variation in the Bowen ratio β was clearly U‐shaped, and the minimum value (0·1) occurred on a sunny day just after rain, when most of the available energy was used for evapotranspiration. Negative β values occurred occasionally in the non‐growing season as a result of intensive radiative cooling and the presence of water on the surface. The β was very high (up to 13·0) in snow‐covered winter, when evapotranspiration was small due to low surface temperature and available soil water. Vegetation phenology and soil moisture were the key variables controlling the available energy partitioning between H and LE. Energy budget closure averaged better than 86% on a half‐hourly basis, with slightly greater closure on a daily basis. The degree of closure showed a dependence on friction velocity u*. Copyright © 2006 John Wiley & Sons, Ltd. 相似文献
14.
River supercooling and ice formation is a regular occurrence throughout the winter in northern countries. The resulting frazil ice production can obstruct the flow through intakes along the river, causing major problems for hydropower and water treatment facilities, among others. Therefore, river ice modellers attempt to calculate the river energy budget and predict when supercooling will occur in order to anticipate and mitigate the effects of potential intake blockages. Despite this, very few energy budget studies have taken place during freeze-up, and none have specifically analysed individual supercooling events. To improve our understanding of the freeze-up energy budget detailed measurements of air temperature, relative humidity, barometric pressure, wind speed and direction, short- and longwave radiation, and water temperature were made on the Dauphin River in Manitoba. During the river freeze-up period of late October to early November 2019, a total of six supercooling events were recorded. Analysis of the energy budget throughout the supercooling period revealed that the most significant heat source was net shortwave radiation, reaching up to 298 W/m2, while the most significant heat loss was net longwave radiation, accounting for losses of up to 135 W/m2. Longwave radiation was also the most significant heat flux overall during the individual supercooling events, accounting for up to 84% of the total heat flux irrespective of flux direction, highlighting the importance of properly quantifying this flux during energy budget calculations. Five different sensible (Qh) and latent (Qe) heat flux calculations were also compared, using the bulk aerodynamic method as the baseline. It was found that the Priestley and Taylor method most-closely matched the bulk aerodynamic method on a daily timescale with an average offset of 8.5 W/m2 for Qh and 10.1 W/m2 for Qe, while a Dalton-type equation provided by Webb and Zhang was the most similar on a sub-daily timescale with average offsets of 20.0 and 14.7 W/m2 for Qh and Qe, respectively. 相似文献
15.
16.
The complementary relationship (CR) between potential evaporation (LEp) and actual evaporation (LE) is widely used to explain the evaporation paradox and to estimate LE, in which wet environment evaporation (LEw) is usually calculated using the Priestley–Taylor equation. However, in many studies on the CR, it has been found that the Priestley–Taylor parameter α is not a constant. Through seasonal variation of α for estimating LEw in the CR, this paper analyses its seasonal variability. Based on flux observation data at two flux experiment sites (Kogma in Thailand and Weishan in China) in the Asian monsoon region, seasonal variability of the CR is detected, i.e. the α value is larger in winter than in summer. This seasonal variability might be caused by seasonal variability in the transport of water vapor and sensible heat between oceans and continent. The monsoon increases air humidity and lowers air temperature in summer, which leads to a decrease in α; it increases atmospheric air temperature and vapor content in winter, increasing α. Nevertheless, during May–September, α has a range of 1.06–1.16 at the Kogma site and 1.00–1.36 at the Weishan site, which is approximate to the typical range 1.1–1.4. Copyright © 2012 John Wiley & Sons, Ltd. 相似文献
17.
Groundwater circulation is known to be one of the agents responsible for the redistribution of geothermal energy by acting as a source or sink in the course of its movement through porous media. Heat transport in groundwater systems is considered to be a coupled process and the theory based on this was used to analyse temperature profiles of 30 thermally stable observation wells in a deep, semi-confined aquifer system in the Tokyo Metropolitan area. Vertical water fluxes in the semi-confined aquifers and the associated upward heat fluxes were estimated from a heat flux equation that describes convection and conduction processes of heat transport in one dimension. The vertical downward water fluxes in Shitamachi lowland, Musashino and Tachikawa terraces were 0.69.26.91 × 10?9, 1.46-70.92 × 10?9 and 2.61.2204 × 10?9 m/s, respectively. A vertical upward water flux of 1.80-33.60 × 10?9 m/s was estimated in Shitamachi lowland. The water flux generally decreased with increasing depth for observation wells which intercepted more than one semi-confining layer. The estimated upward heat fluxes for Shitamachi lowland, Musashino and Tachikawa terraces were 0.32-1.12, 0.49-1.21 and 1.00-11.62 W/m2, respectively. The heat flux was highest in Tachikawa terrace where a major fault, the Tachikawa fault, is located. Generally, the estimated heat flux was higher in the semi-confining layers than in the aquifers. Areas with heat sources and sinks as well as groundwater flow patterns in the semi-confined aquifers were revealed by heat flux and temperature distributions in the study area. 相似文献
18.
The sorption of Eu species onto nano-size silica-water interfaces is investigated at pH range of 1―8.5 and the initial Eu
concentrations (CEu) of 2×10−5, 2×10−4 and 2×10−3 M using fluorescence spectroscopy. The sorption rate of Eu is initially low, but significantly increases at pH > 4. For the
initial CEu of 2×10−5, 2×10−4 and 2×10−3 M, the dissolved Eu species are completely sorbed onto silica-water interfaces at pH = 4.75, −5.8 and 6.6, respectively,
with the respective sorption densities of −1.58×10−8, 1.58×10−7 and 1.58×10−6 mol/m2. The sorbed Eu species at pH < 6 is aquo Eu3+, which is sorbed onto silica-water interfaces as an outer-sphere complex at pH < 5, but may be sorbed as an inner-sphere
bidentate complex at 5 < pH < 6, due to the decrease of the NH2O to −6 at pH = 6. At pH = 6 – 8, Eu(OH)2+, Eu(CO3)+and Eu(CO3)2
− form in the solutions, and Eu(CO3)+is dominant at pH = −7.5. These ions may be sorbed onto silica-water interfaces as inner-sphere bidentate complexes or multi-nuclear
pre-cipitates. 相似文献
19.
Using data from the National Center for Environmental Prediction (NCEP), the paper analyzed the surface latent heat flux (SLHF) variations for five inland earthquakes occurred in some lake area, moist area and arid area of China during recent years. We used the SLHF daily and monthly data to differentiate the global and seasonal variability from the transient local anomalies. The temporal scale of the observed variations is 1-2 months before and after the earthquakes, and spatial scale is about 10°×10°. The result suggests that the SLHFs adjacent the epicenters all are anomalous high value (>μ+2σ) 8-30 days before the shocks as compared with past several years of data. Different from the abnormal meteorological phenomenon, the distribution of the anomalies was isolated and local, which usually occurred in the epicenter and its adjacent area, or along the fault lines. The increase of SLHF was tightly related with the season which the earthquake occurs in; the maximal (125 W/m2, Pu'er earthquake) and minimal (25 W/m2, Gaize earthquake) anomalies were in summer and winter, respectively. The abundant surface water and groundwater in the epicenter and its adjacent region can provide necessary condition for the change of SLHF. To further confirm the reliability of SLHF anomaly, it is necessary to explore its physical mechanism in depth by more earthquake cases. 相似文献
20.
基于2019—2020期间在盘锦市含章湖利用浮式观测平台开展湖冰原型观测试验,分析不同因素对湖冰变化造成的影响.结果表明:99 d冰期内湖冰的生消过程可概述为:湖泊封冻(3 d)—稳定生长(62 d)—冰厚稳定(7 d)—加速消融(24 d)—破碎分解(3d).生长期冰厚的平均增长速率为0.4 cm/d,最大冰厚为30.7 cm;不同深度(5～17 cm)冰温对气温变化的响应存在滞后性,滞后时间为70～158 min,冰温与气温的最大相关系数为0.52～0.89;降雨过程造成冰面反照率由0.22降至0.09,影响了冰内温度以及冰下40 cm以内的浅层水温,但14 mm的降雨量并未引起表面冰厚增加;降雪过程造成冰面反照率由0.25升至0.90,同时阻碍了 5 cm以内的浅层冰温对气温变化的响应,但风速长时间大于8 m/s时会导致冰面积雪被吹散,冰面重新裸露;消融期冰厚的衰减过程呈抛物线趋势,存在显著的加速过程,融化速率由0.3 cm/d逐渐增加到2.7 cm/d;湖冰生长期的冰底热通量均值为4.8 W/m~2;到消融期增加至8.1 W/m~2,为生长期的1.7倍;太阳辐射与湖冰边界侧向融化是导致湖冰加速融化的关键因素.本研究填补了国内湖冰冻融全过程实测资料的空缺,为湖冰热力学模型的改进提供了科学支撑. 相似文献