共查询到20条相似文献，搜索用时 140 毫秒
1.
为分析水流交汇区污染物输移扩散规律,开展了交汇区污染物浓度分布规律的实验和数值模拟研究。建立了交汇区污染物扩散的水气两相流数学模型,并采用实验结果进行验证,对交汇区不同流量、动量和交汇角情况进行实验和数值模拟研究。结果表明:含高浓度污染物的支流汇入干流后,在交汇口下游支流侧形成较长的污染带,且支流与干流的交汇角和流量比(动量比)越小,污染带越狭长;在污染带范围内,污染物浓度梯度较大;污染物分布主要受随流输移和扩散的综合作用影响,其中在交汇区污染物的扩散作用明显。 相似文献
2.
基于卸荷岩体力学基本理论,运用三维有限差分软件,提出以塑性体积应变增量变化区间与不同卸荷区域岩体力学参数相对应的卸荷模拟方法,模拟了不同侧压系数条件下开挖洞周附近围岩最大体积应变增量以及围岩损伤范围的变化情况。数值模拟结果表明：当侧压系数较低时,洞周附近围岩的塑性体积应变增量区域的外边界近似为竖向椭圆形,随着侧压系数的增大,其外边界逐渐向圆形变化,最后变为横向椭圆形。侧压系数越大,围岩的卸载效应越显著,洞周附近围岩的塑性体积应变增量就越大,其所产生的围岩损伤范围也相应越大。利用所获得的结果,可以为深埋隧洞的稳定性分析以及支护设计提供依据。 相似文献
3.
包气带水分入渗过程受多种因素的影响。定量研究层状非均质岩性结构和入渗速率对其影响,有助于解决根据不同条件选择单相流模型或水气二相流模型模拟包气带水分入渗过程的问题。结合填埋场等场地地层条件及污废水入渗特征,分别建立了“上细下粗”和“上粗下细”包气带层状非均质岩性结构水分入渗单相流和水气二相流模型,探讨不同层状非均质岩性结构条件下模型的适用性。在“上粗下细”岩性结构模型基础上,进一步探究入渗速率对水气两相运移结果的影响。基于论文模型研究表明:（1）在包气带岩性结构为“上细下粗”的条件下,气相的影响基本可以忽略,可直接采用单相流模型对包气带水分运移进行模拟;在“上粗下细”岩性结构和本次模型设定的底部压力保持不变及污废水泄漏前场地未接受降水入渗补给等条件下,当包气带上下层介质渗透率比值大于16倍时,气相会对水相运移产生明显影响,且下层介质渗透率越小、上下层介质渗透率比值越大,单相流与两相流的运移结果差别越大,需要采用水气二相流模型模拟包气带水分运移。（2）在包气带“上粗下细”岩性结构条件下,入渗速率越大,气相对水流入渗的阻滞作用越明显,此时包气带水分运移模拟应采用水气二相流模型。 相似文献
4.
渐缩渐扩洞塞消能和空化特性 总被引：1，自引：0，他引：1
建立了三维RNG k-ε紊流数学模型和突缩突扩洞塞泄流的物理模型试验,利用实验结果对数学模型进行了验证,利用验证后的数学模型对突缩突扩洞塞和渐缩渐扩洞塞的水头损失系数和空化数进行了计算。结果表明,洞塞渐缩(或渐扩)段相对长度一定时,随着渐扩(或渐缩)段相对长度的增加,水头损失系数减小,最小空化数增加。当渐缩段和渐扩段几何尺寸互换时,水头损失系数和最小空化数的变化不大;其他几何参数一定的情况下,随着横断面半径收缩比的减小,水头损失系数增加,最小空化数降低。圆弧连接情况下,随着圆弧夹角的增加,水头损失系数呈现先降低后增加的趋势;而最小空化数呈现先增加后降低的趋势。其他几何参数一定的情况下,圆弧连接的水头损失系数小于斜线连接的对应值,最小空化数则相反。在水头损失系数和最小空化数权重相等的假定条件下,初步探讨了渐缩渐扩洞塞几何体型参数的优化方法,给出了渐缩渐扩洞塞的最优几何体型参数。 相似文献
5.
井底流压对煤层气的开采至关重要。在考虑煤层产水量与井底流压的耦合作用下,基于质量和能量守恒定律建立了计算井底流压的数学模型。采用压力增量迭代法,利用matlab7.11编写了求解程序,分析了排采参数相互间的关系。研究结果表明:产水量与井底流压两者的关系呈非线性关系;储层渗透率越好、煤层厚度越厚,产水量与井底流压的耦合关系会更显著些;气液两相流阶段中,高产气量不仅能降低环空中气体流动的压降损失,还利于煤层气在地面管汇的运输。 相似文献
6.
减饱和法是一种通过减小饱和砂土地基中水的饱和度来处置可液化砂土地基的方法。基于单相流-固耦合理论,将减饱和砂中水-气两相流体等效为单相流体,提出一种可以考虑加载过程中孔隙流体体积模量变化的减饱和砂土静态液化的单相流改进算法,用其进行单调荷载作用下三轴不排水压缩试验数值模拟研究,分析了不同饱和度条件下的减饱和砂土的不排水反应并与饱和砂土三轴不排水试验结果进行对比。研究结果表明,单相流改进算法能够很好地反映减饱和法的抗液化特性。此外,对比不同数值分析方法模拟结果,得出以下结论：采用单相流简化算法分析减饱和砂土的不排水反应时,因为不考虑加载过程中的孔隙流体体积模量变化,所以初始的流体体积模量取值会影响减饱和砂土的强度,初始围压为100 kPa、饱和度为96%的减饱和砂土在单调荷载作用下,气体体积模量取值从100 kPa增加至200 kPa时,减饱和砂试样的峰值偏应力会减小约30%,孔隙压力会增加约40%;通过对比同等条件下的单相流改进算法和两相流算法的应力-应变关系曲线以及饱和度和体积应变变化曲线,两者结果相近,误差在5%以内。综上所述,单相流改进算法是一种较为合理而简洁地模拟减饱和砂土静态液化的计算方法。 相似文献
7.
在河流排污引起的污染物扩散计算中,不同河流宽度类别对应不同的移流扩散解析解算式,但缺少具体的河流宽度分类判别准则,给实际应用带来很大困难。按照河流污染物扩散受边界反射影响程度的不同,从移流扩散解析解算式的简化条件出发,提出了宽阔、中宽、窄小的分类方法和定义;根据二维可忽略边界反射的条件和达到全断面均匀混合距离小于等于河流宽度的条件,分别求解了河流宽阔与中宽窄小的分区临界关系线和中宽与窄小的分区临界关系线,提出了相应判据的数学表达式;给出了河流宽阔、中宽、窄小的分类判别准则以及各类别河流移流扩散解析解算式的对应关系。最后指出基于环境扩散条件的河流宽阔、中宽、窄小分区是相对的,对于同一河流在不同水力要素、扩散系数、排污强度和允许浓度升高值等条件下,可以得到不同的分区结果。 相似文献
8.
探究斑块尾流中多尺度紊流结构对理解植被群落影响下的泥沙输移规律和河床演化过程有着重要意义。通过室内水槽试验,分析不同高径比及植被体积分数影响下的斑块后水流特性,得到时均流速及雷诺应力分布规律;通过谱本征正交分解对其脉动场进行分析,探究不同尺度涡的空间模态及能量分布规律。研究结果表明：(1)冠层垂向剪切层内剪切强度及其最大量纲一剪切层垂向厚度随着植被体积分数增大而增大,随着高径比增大而减小。(2)斑块尾流中,大尺度涡旋对应频率集中在0.15～0.29 Hz,对应斯特劳哈尔数为0.16～0.32,垂向分布介于0.2～1.3倍植被高度,纵向分布介于2～6倍斑块直径,横向关于植被中心线呈现出非对称分布。(3)纵向出流流速及剪切层内紊动强度是影响稳定尾流区长度的重要因素。剪切层纵向输运速度随着纵向出流流速增大而增大,剪切层垂向扩散速度随着紊动强度的增大而增大。 相似文献
9.
为研究淤泥质河口的水沙运动规律,建立了用于模拟淤泥质河口水沙运动的二维数学模型。该模型采用基于无结构三角网格下的有限体积法对方程组进行离散,结合Roe-MUSCL方法及时间方向的预测-校正格式,使模型在时空方向具有二阶计算精度。模型中分别采用不同方法计算粘性和非粘性泥沙的输移源项,并引入粘性泥沙的起动流速和冲刷率计算公式。采用已有的概化水槽试验数据对模型进行了初步验证。然后模拟了1995年10月小潮及大潮期间海河口的潮流运动与泥沙输移过程,计算得到的潮位、潮流速及含沙量过程与实测过程符合较好,结果表明模型能够用来模拟淤泥质河口粘性和非粘性泥沙的不平衡输移过程。同时还比较了泥沙输移源项的不同处理方式对计算结果的影响,计算表明在淤泥质河口水沙运动数学模型中必须同时考虑粘性和非粘性泥沙的输移。 相似文献
10.
为了研究浅水湖泊水上煤田钻探工程中可能发生的钻井液泄漏对水体的污染情况,以淮南顾北矿港河水上勘探为例,实测分析了不同浓度钻井液对污染指标和鲫鱼存活的影响,其中污染指标包括pH值、悬浮物、CODcr、总Cr和Cd。采用保守物质的对流扩散方程,对钻井液输移扩散进行了数值模拟。研究发现,当钻井液浓度小于1 000mg/L时,所测试的污染指标基本上能够达到二级排放标准;当钻井液浓度达到5000mg/L时,鲫鱼死亡率约为原水中养殖的正常死亡率的2倍;钻井液在扩散初期其浓度迅速减少,且水流整体流速越大,则钻井液扩散越快,在扩散后期钻井液会形成高浓度聚集区,钻井液浓度的衰减变慢。 相似文献
11.
坡体地下水位上升是诱发滑坡的重要因素,实时排出地下水是防治边坡地质灾害的有效手段。虹吸排水具有免动力和流动过程由液位变化自动控制的物理特性,可满足实时排出坡体地下水的需要,但虹吸管中空气积累会导致虹吸过程中断,制约了边坡虹吸排水技术的推广应用。溶解于水的空气因虹吸管内压力降低而释出是形成气泡的物理基础。实验结果表明,虹吸进水口水面以上垂直高度3.5 m以上就会出现大量气泡,经过虹吸顶点后,气泡发生强烈的兼并形成大气泡。当虹吸管的进出水口的水头差较大时,气泡间的水弹容易推动气泡从出水口排出。当虹吸管直径大于5 mm时,缓慢的虹吸流动,会发生管内气泡的积累,最终破坏虹吸过程;虹吸管的直径小于4 mm时,可以形成基本稳定的弹状流。因此,为保持边坡虹吸过程长期有效,经常性降雨并且坡体地下水丰富的地区可选用直径为5 mm的虹吸管,非经常性降雨的地区应选择小于等于4 mm的虹吸管。 相似文献
12.
地下水曝气工程技术研究——以德州胜利油田地下水石油污染治理为例 总被引：5，自引：0，他引：5
为了研究地下水石油污染现场曝气治理效果,在胜利油田石油开采区进行了地下水现场曝气治理技术研究。采用溶解氧浓度法研究了曝气操作条件(曝气深度、曝气压力和曝气流量)对地下水石油污染曝气治理技术的影响。实验结果表明:在相同曝气压力和流量下,曝气深度越大,影响半径越大,但影响区内的气流分布越稀疏;相反,曝气深度越小,则曝气影响半径越小,但在影响区内空气流线分布越密。气流分布密度和曝气影响半径随曝气压力和流量增大而增大,但存在一个最佳限值;现场曝气存在气流分布不对称现象,是由于土壤介质的渗透性不均匀所致。地下水曝气技术对地下水石油污染治理效果显著,但曝气操作条件对该技术影响较大,需根据地质条件通过现场曝气试验确定。 相似文献
13.
根据三峡工程坝区水域实测数据,分析了水库蓄水以后大坝上、下游断面溶解氧浓度和溶解氧饱和度的变化特性,探讨了水位、流量因素对大坝下游水体溶解氧量的影响。结果表明,坝身孔口过流水体大量掺气后进入下游河道导致下游水体溶解氧浓度和饱和度显著增加,甚至达到超饱和状态。由于电站过流基本不改变水体溶解氧量,在电站和坝身孔口同时过流时,两种水体掺混后,下游溶解氧量主要受流量比的影响。此外,下游溶解氧量随流量的增加和下游水位的升高而增大。过坝总流量超过35 000 m3/s,下游水位超过68 m以及坝身孔口过流流量占总流量的绝大部分时,需特别重视溶解氧超饱和现象对水生生物可能造成的影响。 相似文献
14.
基于青藏高速公路试验工程的实测资料,利用数值模拟系统分析了通风路基通风管内的空气流动特性和变化规律.研究表明,当外界环境风速一定时,通风管内不同区域流动特征显著不同,表现为较为明显的三段性：在入口扰动区段,管内空气紊流强度最大;中部为完全湍流区,紊流强度最弱;出口射流影响区的紊流强度介于入口扰动区和完全湍流区之间.随着外界环境风速的增加,管内空气流速相对环境风速增加的量值随之增加,总体呈现非线性快速增加的趋势;入口扰动响应的长度和紊流强度增加最显著;尾部射流影响区由于受到空气流动惯性等因素影响,其长度以非线性加速减小,其空气运动轨迹的振动幅度以非线性加速提高.管内各区域空气流动特性的不同是造成通风管不同部位局部换热量差异的根本原因,这些流动特性的存在进一步叠加,或是导致通风管路基阴阳坡效应的重要因素之一. 相似文献
15.
长距离无压引水洞岔洞是影响水流流态和分流量的关键水工建筑物之一,充水阶段流态复杂。通过Fluent软件对不同入口流量、岔洞夹角下的无压卜型岔洞充水阶段进行了数值仿真研究,并通过模型试验对不同入口流量下水流平稳后的岔洞段各监测断面水深及支洞分流比进行了验证。结果显示,充水阶段支洞分流比对入口流量敏感性小,岔洞夹角在15°～45°范围内变化时,分流比变化较大。另外,岔洞夹角增至60°时,侧支洞外侧上部水流出现回流区。岔洞夹角对总干水面线影响较小,岔洞段各断面水位随入口流量增加而升高。 相似文献
16.
Diving and aerial flight place conflicting physiological constraints on diving birds depending on their typical dive depths. The amount by which air volumes in the respiratory system and plumage are reduced by hydrostatic pressure decreases rapidly with depth. Thus, birds diving shallowly, and ascending passively by means of positive buoyancy, content with greater work against buoyancy as well as more unstable buoyancy as they move vertically in the water column. The buoyancy of air far exceeds that of tissues or blood, whose buoyancy does not change appreciably with depth. Accordingly, experiments on ducks suggest that birds adapt to shallow diving by increasing blood volume and thus blood oxygen stores while decreasing respiratory volume. During dives, increased inertia from greater mass of blood and associated muscle lowers the costs of foraging at the bottom by resisting the upward buoyant force, but raises the costs of descent because of higher inertial work in accelerating the body with each stroke. Thus, average dive depth (compression of buoyant air spaces), stroke kinematics (inertial effects), and the relative time spent descending versus bottom foraging will determine the appropriate balance between buoyancy and inertia for diving. Greater blood volume also increases wing loading, so elements of dive costs must be balanced against flight costs in optimizing allocation of oxygen stores to blood versus the respiratory system. For example, biomechanical models for ducks suggest that increasing blood volume while decreasing respiratory volume lowers dive costs only for dives to depths <5 m or for dives with extended time at constant depth. If flight costs are also considered, these anti-buoyancy mechanisms reduce daily energy expenditure only if average dive depth is <2 m. High wing-loading in many foot-propelled divers is probably not an adaptation to diving but rather a result of modifications in wing size and shape for high flight-speed. These wing modifications appear possible because competing demands on wing morphology (maneuverability, takeoff ability) are relaxed in open aquatic environments. 相似文献
17.
南海北部琼东南海域HQ-48PC站位地球化学特征及对天然气水合物的指示意义 总被引：2，自引：0，他引：2
南海北部陆坡琼东南海域是中国天然气水合物勘探最具潜力的区域之一。对该海域的HQ-48PC站位沉积物样品的顶空气甲烷含量、孔隙水阴、阳离子及微量元素含量等地球化学特征进行综合分析,结果显示:在硫酸盐-甲烷界面(SMI,Sulfate-Methane Interface)(推算深度约为6.05 mbsf)发生了强烈的甲烷厌氧氧化反应(AMO,Anaerobic Meth-ane Oxidation),主要表现为SO24-含量线性降低接近于0、CH4含量发生骤增、有机碳和黄铁矿含量达到最大值及形成一个"钡锋"等特征。在SMI之上,HCO3-浓度随深度的增加呈明显上升的趋势,Ca2+、Mg2+、Sr2+等离子浓度随深度的增加呈降低的趋势,Mg2+/Ca2+比值随深度的增加呈明显增加的趋势,自生碳酸盐矿物以方解石为主;在SMI之下,HCO3-浓度随深度的增加呈缓慢下降的趋势,Ca2+浓度变化不大,Mg2+、Sr2+浓度和Mg2+/Ca2+比值随深度的增加呈降低的趋势,自生碳酸盐矿物以白云石为主。沉积物孔隙水的PO34-和NH4+含量较高,它们随深度的增加呈明显升高的趋势,且这种变化趋势与SO42-含量的下降趋势大致呈镜像关系。这些地球化学异常特征与国际上已发现有天然气水合物地区的地球化学特征相类似,暗示该采样站位深部沉积物中可能赋存有天然气水合物藏。 相似文献
18.
Ben K. Greenfield Geoffrey S. Siemering Joy C. Andrews Michael Rajan Stephen P. Andrews David F. Spencer 《Estuaries and Coasts》2007,30(4):627-640
Management actions to control invasive aquatic species can have significant ecosystem-scale effects. We evaluated the water
chemistry and nutrient effects of mechanical shredding to control water hyacinth (Eichhornia crassipes) in an agricultural slough and a tidal wetland on the Sacramento-San Joaquin River Delta, California. Shredding was conducted
with two types of shredder boats in fall of 2003 and another boat in spring of 2004. Shredding measurably affected water quality,
but specific effects varied as a function of shredding site and season. Significant increases were observed for total Kjeldahl
nitrogen and total phosphorus for all experiments. Dissolved oxygen effects varied by site, decreasing after shredding at
the agricultural slough but increasing at the tidal wetland. The increase in dissolved oxygen likely resulted from tidal incursions
from the adjacent river. A year-long time series of dissolved oxygen data indicated a negative relationship between hyacinth
abundance and dissolved oxygen concentrations. Hyacinth contained similar tissue concentrations of mercury to underlying sediments,
suggesting that plant harvesting could aid mercury remediation efforts. Simple mass calculations indicated that Delta-wide
shredding operations could cause between 0.1% and 9.6% increases in the overall abundance of carbon, nitrogen, and phosphorus
in the Delta water column. Results suggest that local effects of management actions to control invasive aquatic plants will
vary widely as a function of site-specific hydrology, but that estuary-wide effects would be limited. 相似文献
19.
构建起双向耦合的液固两相流动旋涡动力学模型与数值方法;应用离散涡方法,计算非定常不稳定水流场;采用Lagrange方法模拟颗粒运动,颗粒对流体的反作用通过修正涡泡运动速度来实现。利用所建模型,计算了两种St数的泥沙粒子在圆柱绕流场中的运动。结果证明了液固两相流动中颗粒运动与旋涡存在着明确的相关结构:(1)当水沙混合物中的泥沙颗粒碰上旋涡时,泥沙颗粒被卷入旋涡中,被卷入旋涡中的泥沙颗粒在运动过程中始终分布于旋涡区;(2)均匀水沙混合物绕圆柱流动,由于流体流过圆柱时产生剧烈分离流动,使得在尾迹流内中等St数 (St～o (1))的泥沙颗粒从均匀水沙混合物中分离出来而往旋涡区聚集。 相似文献
20.
Flows with high suspended sediment concentrations are common in many sedimentary environments, and their flow properties may show a transitional behaviour between fully turbulent and quasi‐laminar plug flows. The characteristics of these transitional flows are known to be a function of both clay concentration and type, as well as the applied fluid stress, but so far the interaction of these transitional flows with a loose sediment bed has received little attention. Information on this type of interaction is essential for the recognition and prediction of sedimentary structures formed by cohesive transitional flows in, for example, fluvial, estuarine and deep‐marine deposits. This paper investigates the behaviour of rapidly decelerated to steady flows that contain a mixture of sand, silt and clay, and explores the effect of different clay (kaolin) concentrations on the dynamics of flow over a mobile bed, and the bedforms and stratification produced. Experiments were conducted in a recirculating slurry flume capable of transporting high clay concentrations. Ultrasonic Doppler velocity profiling was used to measure the flow velocity within these concentrated suspension flows. The development of current ripples under decelerated flows of differing kaolin concentration was documented and evolution of their height, wavelength and migration rate quantified. This work confirms past work over smooth, fixed beds which showed that, as clay concentration rises, a distinct sequence of flow types is generated: turbulent flow, turbulence‐enhanced transitional flow, lower transitional plug flow, upper transitional plug flow and a quasi‐laminar plug flow. Each of these flow types produces an initial flat bed upon rapid flow deceleration, followed by reworking of these deposits through the development of current ripples during the subsequent steady flow in turbulent flow, turbulence‐enhanced transitional flow and lower transitional plug flow. The initial flat beds are structureless, but have diagnostic textural properties, caused by differential settling of sand, silt and cohesive mud, which forms characteristic bipartite beds that initially consist of sand overlain by silt or clay. As clay concentration in the formative flow increases, ripples first increase in mean height and wavelength under turbulence‐enhanced transitional flow and lower transitional plug‐flow regimes, which is attributed to the additional turbulence generated under these flows that subsequently causes greater lee side erosion. As clay concentration increases further from a lower transitional plug flow, ripples cease to exist under the upper transitional plug flow and quasi‐laminar plug flow conditions investigated herein. This disappearance of ripples appears due to both turbulence suppression at higher clay concentrations, as well as the increasing shear strength of the bed sediment that becomes more difficult to erode as clay concentration increases. The stratification within the ripples formed after rapid deceleration of the transitional flows reflects the availability of sediment from the bipartite bed. The exact nature of the ripple cross‐stratification in these flows is a direct function of the duration of the formative flow and the texture of the initial flat bed, and ripples do not form in cohesive flows with a Reynolds number smaller than ca 12 000. Examples are given of how the unique properties of the current ripples and plane beds, developing below decelerated transitional flows, could aid in the interpretation of depositional processes in modern and ancient sediments. This interpretation includes a new model for hybrid beds that explains their formation in terms of a combination of vertical grain‐size segregation and longitudinal flow transformation. 相似文献