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Solving first-order hyperbolic problems for wave motion in nearly incompressible fluids, two-phase fluids, and viscoelastic media by the CESE method.

机译:用CESE方法解决几乎不可压缩的流体,两相流体和粘弹性介质中波动的一阶双曲问题。

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摘要

This dissertation reports the development of generic first-order, hyperbolic partial differential equations and the associated numerical method for modeling wave motion in complex media, including propagating waves in liquids, in two-phase fluids, and in viscoelastic media. The model equations are cast into a set of first-order, fully coupled, hyperbolic, partial differential equations (pde's) with or without the dissipation terms. In this dissertation, the dissipation terms can be found with viscous terms and stiff source. For different types of dissipation terms, their treatment in the setting of the space-time Conservation Element and Solution Element (CESE) method is illustrated in this dissertation.;First, acoustic waves in low-speed, nearly incompressible flows are of interest. The Bulk modulus is employed to unify the constitutive equation for different media. As that in the most of the incompressible fluid flows, the energy equation is not included in the model equations, and thus the current model is suitable for isothermal flows only. The dependence of the Bulk modulus on the temperature of the medium is out of the scope of the present development.;Next, the constitutive model developed for the incompressible fluids is extended to that for wave motion in two-phase flows. Similar to that of incompressible fluids, the two-phase flow model assumes the fluid is nearly isothermal but is compressible to accommodate the disparity in density of the gas phase and the liquid phase where phase change is involved. To test the capabilities of the model, cavitation associated with the water hammer effect is modeled.;As the last example, a set of first-order, fully coupled, hyperbolic pde's have been derived for wave motion in viscoelastic media. In particular, wave propagation in soft tissues for biomedical applications is of interest. The model equations have been developed based on the fundamental description of the material, including linear theory of relaxation functions, the standard linear solid model, and the use of the internal variables. Small deformation and constant temperature are assumed in the present model.;For the hydro-acoustics model and for the wave in two-phase flow model, the Riemann invariants have been explicitly derived. Moreover, the Riemann invariants were obtained by using the three-dimensional equations instead of the usual one-dimensional approach. The Riemann invariants of the two-phase flow model are further analyzed to derive the Rankine-Hugoniot shock jump relationship for the water hammer effect in the two-phase flow. With the derived shock-jump condition, the required pressure ratio for creating the shock wave in two-phase flow has been obtained. The derived shock relation has also been used as the analytical solution to verify the numerical simulation.;The numerical solutions of all above three models have been obtained by using the space-time CESE method. The numerical results have been compared with the available experimental data and/or theoretical solutions. In this dissertation, the open-sourced software SOLVCON for generic hyperbolic pde's solver, developed at OSU, has been used. The CESE method is the default CFD method for SOLVCON although other solver kernel could be easily implemented.;For the hydro-acoustics model for wave motion in nearly incompressible flows, two sets of the numerical simulations have been performed. The first set involves air and water flows over a circular cylinder. The calculated Strouhal number was derived based on the numerical results and compared with the experimental data. The second case is an air flow over a rectangular cavity. The acoustic pressure is measured in the numerical simulation and is compared with the experimental data and the analytical solution.;Finally, the newly derived viscoelastic model for wave propagation in soft tissues has been solved. In particular, the ultrasound longitudinal waves in a soft tissue have been simulated. The focused longitudinal waves would cause a local shear deformation at the focal point.;This dissertation demonstrates that a wide range of wave phenomena can be accurately modeled by a set of coupled, first-order, hyperbolic pde's. Traditionally, wave motion in complex solids have been routinely modeled by second-order wave equations. The present dissertation shows that the first-order pde's represent a much more versatile and open theoretical platform to accommodate complex modeling requirements. The analyses of the first-order pde's are shown to be based on the eigen-structure of the Jacobian matrices. In the analyses, we strive to achieve genuine three-dimensional analyses instead of conventional one-dimensional approaches. Moreover, the present work also shows that SOLVCON is indeed a versatile solver for easy implementation for time accurate solutions of wave motion by using unstructured meshes and hybrid parallel computation. (Abstract shortened by UMI.).
机译:本文报道了一般的一阶双曲偏微分方程的发展以及相关的数值方法,用于对复杂介质中的波运动建模,包括在液体,两相流体和粘弹性介质中的传播波。将模型方程式转换为一组带或不带耗散项的一阶全耦合双曲偏微分方程(pde)。本文可以用粘性项和刚性源来找到耗散项。对于不同类型的耗散项,本文阐述了它们在时空守恒元和解元(CESE)方法中的处理。首先,低速,近不可压缩流中的声波引起了人们的关注。体积模量用于统一不同介质的本构方程。由于在大多数不可压缩流体中,能量方程不包括在模型方程中,因此当前模型仅适用于等温流动。体积模量对介质温度的依赖性超出了本研究的范围。接下来,针对不可压缩流体开发的本构模型扩展到了两相流中的波动模型。与不可压缩流体相似,两相流模型假设流体几乎是等温的,但可压缩以适应涉及相变的气相和液相密度的差异。为了测试模型的功能,对与水锤效应相关的气蚀进行了建模。作为最后一个示例,已经导出了一组一阶完全耦合的双曲pde,用于粘弹性介质中的波动。特别地,用于生物医学应用的软组织中的波传播是令人关注的。模型方程是基于材料的基本描述而开发的,包括松弛函数的线性理论,标准线性实体模型以及内部变量的使用。在该模型中假设了小变形和恒定温度。对于水声模型和两相流模型中的波,已经明确导出了黎曼不变量。此外,通过使用三维方程而不是通常的一维方法来获得黎曼不变量。进一步分析了两相流模型的黎曼不变量,得出了两相流中水锤效应的兰金-休格尼奥特激跳关系。利用导出的冲击跳跃条件,已经获得了在两相流中产生冲击波所需的压力比。推导的冲击关系也被用作解析解来验证数值模拟。;通过时空CESE方法获得了以上三个模型的数值解。数值结果已与可用的实验数据和/或理论解进行了比较。本文使用了OSU开发的通用双曲pde解算器开源软件SOLVCON。尽管可以轻松实现其他求解器内核,但CESE方法是SOLVCON的默认CFD方法。;对于几乎不可压缩的流动中的波动的水声模型,已进行了两组数值模拟。第一组涉及空气和水流过圆柱体。根据数值结果推导计算出的斯特劳哈尔数,并与实验数据进行比较。第二种情况是矩形腔上方的气流。在数值模拟中测量了声压,并将其与实验数据和解析解进行了比较。最后,解决了新推导的用于软组织中波传播的粘弹性模型。特别地,已经模拟了软组织中的超声纵波。聚焦的纵波将在焦点处引起局部剪切变形。;本论文表明,可以通过一组耦合的一阶双曲pde精确地建模各种波现象。传统上,通常使用二阶波动方程对复杂固体中的波动进行建模。本论文表明,一阶pde代表了一个更加通用和开放的理论平台,可以满足复杂的建模需求。一阶pde的分析显示为基于Jacobian矩阵的本征结构。在分析中,我们努力实现真正的三维分析,而不是传统的一维分析。此外,当前的工作还表明,SOLVCON确实是通用的求解器,可通过使用非结构化网格和混合并行计算轻松实现时间精确的波动运动求解。 (摘要由UMI缩短。)。

著录项

  • 作者

    Lin, Po-Hsien.;

  • 作者单位

    The Ohio State University.;

  • 授予单位 The Ohio State University.;
  • 学科 Mechanical engineering.
  • 学位 Ph.D.
  • 年度 2015
  • 页码 214 p.
  • 总页数 214
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

  • 入库时间 2022-08-17 11:53:07

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