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Construction of a multi-dimensional Lagrangian hydrodynamics model of a plasma using the Lie group theory of point transformations

机译:利用点变换的李群理论建立等离子体的多维拉格朗日流体力学模型

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摘要

Conservative macroscopic governing equations for a plasma in the magnetohydrodynamic (MHD) approximation were derived from the symmetry properties of the microscopic action integral. Invariance of the action integral under translation and rotation symmetries was verified. Noether's Theorem was used to express the invariance equations as two sets of microscopic equations that represent the Euler-Lagrange (E-L) equations for the plasma and an equation in divergence form, called a conservation law, that is the first integral of the Euler-Lagrange equations. The specific forms of the conservation laws were determined from the invariance properties admitted by the action integral. Invariance under translations gave the conservation law for the translational momentum balance while invariance under rotations gave the conservation law for the angular momentum balance. The ensemble average of the microscopic equations was taken to give the kinetic representation of the equations. The momentum integrals in the kinetic equation were evaluated to give the fluid representation of the system. The fluid representation was then expressed in the MHD limit to give the one-fluid representation for the plasma. The total derivatives in the conservation laws were evaluated for the kinetic and fluid representations to verify that the expressions are first integrals of the respective E-L equations. The symmetry properties of the conservation laws in auxiliary form were determined to test the system, of equations for mapping properties that may allow the nonlinear conservation laws to be expressed as nonlinear or linear expressions. The results showed that no nonlinear to linear mapping was possible for the governing equations with charge distributions. The quasi-neutral governing equations admitted a scaling group that allows mapping from the source nonlinear equations to nonlinear target equations that contain one less independent variable.;The translation conservation laws were used in a two-dimensional computer simulation of the confined eddy problem to demonstrate an application of the equations. Comparison of the results produced by the code using the conservation law governing equations with previous work is limited to qualitative comparison since differences in the numerical input and graphics software make direct quantitative comparison impossible. Qualitative comparison with previous work show the results to be consistent.
机译:磁流体动力学(MHD)近似中的等离子体的守恒宏观控制方程是从微观作用积分的对称性质导出的。验证了在平移和旋转对称下动作积分的不变性。用Noether定理将不变性方程表示为两组微观方程,分别代表等离子体的Euler-Lagrange(EL)方程和发散形式的方程(称为守恒定律),这是Euler-Lagrange的第一个积分方程。守恒定律的具体形式是根据动作积分所接受的不变性来确定的。平移下的不变性给出了平动动量平衡的守恒律,而旋转下的不变性给出了角动量平衡的守恒律。取微观方程的整体平均值,以给出方程的动力学表示。对动力学方程中的动量积分进行了评估,以给出系统的流体表示。然后以MHD极限表示流体表示,以给出血浆的单流体表示。对守恒律中的总导数进行了动力学和流体表示评估,以验证表达式是各个E-L方程的第一积分。确定了辅助形式的守恒定律的对称性质以测试系统,用于映射属性的方程式可以使非线性守恒定律表示为非线性或线性表达式。结果表明,对于带电荷分布的控制方程,非线性到线性映射是不可能的。拟中性控制方程接纳一个比例组,该比例组允许从源非线性方程映射到包含一个较少独立变量的非线性目标方程。;平移守恒定律被用于二维涡旋问题的计算机模拟中,以证明方程的应用。由于使用数字输入法和图形软件的差异使得不可能直接进行定量比较,因此使用守恒定律的控制方程将代码产生的结果与以前的工作进行比较仅限于定性比较。与先前工作的定性比较表明结果是一致的。

著录项

  • 作者

    Temple, Brian Allen.;

  • 作者单位

    University of Illinois at Urbana-Champaign.;

  • 授予单位 University of Illinois at Urbana-Champaign.;
  • 学科 Plasma physics.;Nuclear engineering.
  • 学位 Ph.D.
  • 年度 1999
  • 页码 322 p.
  • 总页数 322
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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