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Level Set方法

Level Set方法的相关文献在1998年到2022年内共计129篇,主要集中在力学、自动化技术、计算机技术、水利工程 等领域,其中期刊论文105篇、会议论文24篇、专利文献10217117篇;相关期刊72种,包括科学技术与工程、西安交通大学学报、铸造等; 相关会议21种,包括2013年中国工程热物理学会传热传质学学术年会、第十五届全国流体力学数值方法研讨会、中国工程热物理学会传热传质学2009年学术会议等;Level Set方法的相关文献由278位作者贡献,包括赵宁、廖斌、张斌等。

Level Set方法—发文量

期刊论文>

论文:105 占比:0.00%

会议论文>

论文:24 占比:0.00%

专利文献>

论文:10217117 占比:100.00%

总计:10217246篇

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Level Set方法

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    • 纪佑军; 王力龙; 韩海水; 蒋国斌; 王泽根
    • 摘要: 泡沫在孔隙中的流动行为影响波及范围和驱油效率,对提高采收率起到重要作用。首先,建立单毛管模型,利用Level-set方法研究了泡沫在单毛管内流动的影响因素,分析了泡沫通孔隙介质中运移产生的贾敏效应、聚并机理和微观选择性运移机理,评价了不同类型泡沫的封堵性能;然后,通过XB油田岩芯的CT图像构建了真实的孔隙介质微观数值模型,研究了泡沫在其中的运移特点。结果表明,泡沫变形程度随管径比的增大而减小,润湿壁接触角对毛细管内泡沫的流变性无影响,半径1.2μm的N_(2)泡沫破裂时的液相流速临界值为64 mm/s;泡沫通过孔道时所受压力与其表面张力成正比,泡沫具有优先通过大孔道的微观运移特征;N_(2)泡沫稳定性强,封堵性能好,较适合高含水期的低渗油田进行调驱,为现场采用气液分散体系进行调驱并提高采收率提供有益启示。
    • 高翔宇; 杨伟东; 王媛媛; 屠熹远; 张争艳
    • 摘要: 以微滴喷射的增材制造技术为研究对象,采用守恒水平集方法建立了液滴喷射过程的数值仿真的物理数学模型.通过仿真实验分析了液滴喷射的流场分布,采用曲面响应法的中心复合设计建立了拟合模型并进行了修正,提出了液滴喷射过中液滴成球距离和断裂高度分别与入口处压强脉冲的幅值与脉宽的拟合关系式.模拟结果表明:在液滴喷射过程中喷嘴入处的压强脉冲的幅值与脉宽和液滴形态之间有密切的关系,压强幅值与脉宽之间存在一个临界关系,当不满足这个关系时液滴无法从喷嘴口喷出,只有当压强幅值与脉宽满足这个临界条件时,液滴才能够克服喷嘴口处的表面张力顺利喷出;在满足喷射条件的情况下压强幅值与脉宽时间越大,喷出的液滴成球距离越远;压强幅值与脉宽时间越小,喷出的液滴成球距离越近.
    • 吴昊; 朱际休; 廖斌; 陈善群
    • 摘要: 基于雷诺时均Navier-Stokes方程(RANS)和连续方程,结合k-ω 湍流模型,建立波浪与非淹没竖直圆柱相互作用的三维数值模型.在验证波浪对单个竖直圆柱波浪力和自由液面高程的基础上,着重研究圆柱间距S对两串联竖直圆柱波浪力与自由液面高程的影响.计算结果表明,圆柱间距S较大时(S=4D),两串联圆柱中上游圆柱波浪力与单圆柱波浪力的演化曲线较为吻合;圆柱间距S较小(S=0.5D)时,上游圆柱背风面自由液面高程明显抬升,使得上游圆柱波浪力较单圆柱大,同时上游圆柱侧方自由液面高程受反射波的影响较大.
    • 吴昊1; 朱际休2; 廖斌1; 陈善群1
    • 摘要: 基于雷诺时均Navier-Stokes方程(RANS)和连续方程,结合k-ω湍流模型,建立波浪与非淹没竖直圆柱相互作用的三维数值模型.在验证波浪对单个竖直圆柱波浪力和自由液面高程的基础上,着重研究圆柱间距S对两串联竖直圆柱波浪力与自由液面高程的影响.计算结果表明,圆柱间距S较大时(S=4D),两串联圆柱中上游圆柱波浪力与单圆柱波浪力的演化曲线较为吻合;圆柱间距S较小(S=0.5D)时,上游圆柱背风面自由液面高程明显抬升,使得上游圆柱波浪力较单圆柱大,同时上游圆柱侧方自由液面高程受反射波的影响较大.
    • 廖斌; 陈善群; 任超洋
    • 摘要: In this study,a computational model is established for solving wave propagation over a submerged dike based on RANS equations combined with Level-Set method.The fifth-order finite difference WENO scheme is used for spatial discretization,and a TVD third-order Runge-Kutta explicit time scheme is employed for time discretization in the model.The Level-Set method is used for tracking the free interface between the air and water phases,and a relaxation method is employed for wave generation and absorption.In order to validate the accuracy and applicability of the model,numerical investigation of the wave propagation over a submerged dike is conducted.The numerical results show a good agreement with experimental data.Further studies are carried out to investigate the influence of physical parameters,such as wave height,submerged depth,seaward and leeward slope gradients,on the process of wave propagation over a submerged dike.Results reveal that when the wave height is higher,submerged depth smaller,and seaward slope flatter,the effect of shoaling is more obvious;when leeward slope is flatter,the effect of shoaling on wave is slightly larger,but not obvious.%以RANS方程结合Level-Set方法为研究基础,采用五阶.WENO有限差分格式进行空间离散、三阶TVDRunge-Kutta格式进行时间推进、Level-Set方法追踪波浪与空气间自由面以及解析松弛法来实现数值水槽中的造波消波,建立了一种求解潜堤上波浪传播问题的数值计算模型.选取经典的潜堤上波浪传播物理试验模型对数值模型进行了验证,水位计算结果与试验值吻合较好.进一步研究了波高、潜堤顶部淹没深度以及潜堤坡度等参数对潜堤上波浪传播过程的影响.结果表明:波高越高、淹没深度越浅、潜堤向波坡度越小,波浪受浅水作用越明显;潜堤背波坡度越小,波浪受反浅水作用稍大,但并不明显.
    • 高亚军; 姜汉桥; 李俊键; 常元昊; 陈文滨
    • 摘要: 达西定律渗流理论以对油水运移规律的研究仍停留在宏观尺度上,很多微观机理无法考虑,窜流形成时的微观孔道中油水运移特征未能体现清楚.本文建立二维微观孔隙模型,引入Level Set方法对油水两相界面进行追踪,采用有限元方法对两相数值模型进行求解.在玻璃刻蚀平面驱替实验的基础上,建立并联毛细管束模型.通过模拟不同驱替压差、润湿性以及界面张力等情况下的流动状态,结合二维孔隙数值模拟结果,给出了发生微观窜流的临界条件:在入口压力恒定时,水驱油速度逐渐变大;驱替压力增大时,大孔道中的两相流速增加比例更大;油水两相界面张力越大,壁面越亲油,越容易发生微观窜流.%Both study of the seepage theory of Darcy's law and the flow regularity oil-water are on a large scale,many microscopic mechanism cannot be taken into consideration.Also,at present,the oil-water flow characteristics of the pore throat is failure to present clear when the flow channel is formed.Two-dimensional micro two-phase displacement model is set up in this article,which level set method is introduced to trace the oil-water two phase fluid interface,and finite element method is adopted to solve the numerical model.Parallel waney capillary bundle model is set up based on the glass etching areal water flooding experiment.The critical channel diameter ratio in microscopic fluid channeling is obtained by numerically calculated the various displacement pressure,various contact angel and the various interface tension,which combined the simulation result of two-dimensional pore scale model.The flow velocity in the pore throat is increasing gradually at a displacement constant pressure.On the other hand,the velocity increase with the displacement pressure,but the increase rate of velocity is bigger in the bigger capillary.What's more,the increase of oil-water interface tension in oil-wet reservoir and wall contact angel are not conducive to small pore throat oil displacement,which can be more easily to cause channel flow.
    • 高亚军; 姜汉桥; 李俊键; 赵玉云; 胡锦川; 常元昊
    • 摘要: The flow characteristic of the droplets impacting on solid surface is extremely significant for practical engineering applications.The problem is also very complicated since there are many parameters that may influence the process of droplets impacting on a solid surface.Therefore the numerical study of behaviors of droplets impacting on a solid surface is performed in this work.With a given impact velocity,two two-dimensional axisymmetric droplets subsequently interact on the solid surface.To conduct numerical simulations,a mass conserved level set method is adopted,and the gravity and surface tension are taken into consideration in the process of droplet development on the solid surface.The effects of Weber number,surface contact angle,the horizontal distance between the two droplets,and droplet arrangement on the dynamic behaviors of droplet impact are systematically investigated.It is found that two droplets vertically impacting on solid surface simultaneously can produce a columnar liquid jet column,and the horizontally spreading liquid on the solid surface will break up in several segments as time goes by.With the increase of Weber number,the secondary droplets are generated from liquid jet,and the columnar liquid jet rebounds away from the surface subsequently.If the Reynolds number,surface contact angle and the horizontal distance are set to be,respectively,2000,90°and 2,in particular,the non-dimensional length of liquid spread is unrelated to Weber number when the non-dimensional time T < 2,and it increases as the Weber number increases when T > 2.Meanwhile,the dynamic change characteristics of the non-dimensional liquid jet height are about the same during the jet rising,but the jet falling time becomes shorter as the Weber number decreases.Obviously,the bigger the Weber number,the bigger the biggest non-dimensional height of liquid jet and length of liquid spread are.On the other hand,with the increase of surface contact angle,the columnar liquid jet rebounds away from the surface and the spreading liquid breaks up much earlier on the surface.Also,the non-dimensional height of liquid jet and length of liquid spread grow with the increase of surface contact angle.In addition,in the case that the Weber number,Reynolds number and surface contact angle are set to be 32,2000 and 90° respectively,we also find that the correlation between the biggest non-dimensional jet height and horizontal distance is not monotonic.Under the circumstances,the biggest non-dimensional height of liquid jet is achieved when the distance is set to be 2,and the phenomenon of liquid jet rebound occurs subsequently,whether the rebound phenomenon of the jet liquid column is related to the horizontal distance of the droplet or not.And finally,as the horizontal distance between the two droplets increases from 1.5 to 3,the non-dimensional length of liquid spread gradually increases.%采用质量守恒的level set方法对双液滴同时垂直撞击干壁面后的流动过程进行了模拟研究,主要讨论了韦伯数(We)、壁面接触角(θ)以及双液滴水平间距(S)等物理参数对相界面流动过程的影响,分析了不同参数下射流高度和水平铺展半长随时间的变化规律.研究表明:We数较大时,中心射流液柱将产生二次液滴,随后液柱反弹至空中,且We数越大,中心射流产生的二次液滴次数越多,最大无量纲射流高度和最大无量纲铺展半长越大;随壁面接触角的增大,中心射流液柱出现反弹现象,水平铺展液流出现断裂的时间越早,最大无量纲射流高度和最大无量纲铺展半长越小;最大无量纲射流高度值与液滴水平间距的相关性不单调,铺展半长随水平间距的增大而增大.
    • 张屹; 刘西霞; 史如坤; 王霞; 杨雄
    • 摘要: 构建了激光深熔焊接三维混合态连续模型,模拟了固液界面过渡层的固、液态共存和熔池高于焊接表面的特征,并采用Level-Set方法追踪了气液界面的移动,计算得到了小孔和熔池的动态形成过程。结果表明,熔池在小孔前沿薄后沿厚,温度梯度在小孔前沿大后沿小,小孔及熔池前沿和后沿存在明显的非对称性;孔壁上蒸发的金属蒸气由孔壁流向小孔中轴线,且向孔外喷射;孔底吸收的激光功率密度最大,最高温度3700 K位于孔底,高于汽化温度567 K;小孔形成的初期阶段孔深的变化较快,但随着小孔深度的增加,孔深变化速率逐渐下降。
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