The force/work differencing of exceptional points in the discrete, compatible formulation of Lagrangian hydrodynamics

This study presents the force and mass discretization of exceptional points in the compatible formulation of Lagrangian hydrodynamics. It concludes a series of papers that develop various aspects of the theoretical exposition and the operational implementation of this numerical algorithm. Exceptional points are grid points at the termination of lines internal to the computational domain, and where boundary conditions are therefore not applied. These points occur naturally in most applications in order to ameliorate spatial grid anisotropy, and the consequent timestep reduction, that will otherwise arise for grids with highly tapered regions or a center of convergence. They have their velocity enslaved to that of neighboring points in order to prevent large excursions of the numerical solution about them. How this problem is treated is given herein for the aforementioned numerical algorithm such that its salient conservation properties are retained. In doing so the subtle aspects of this algorithm that are due to the interleaving of spatial contours that occur with the use of a spatially-staggered-grid mesh are illuminated. These contours are utilized to define both forces and the work done by them, and are the central construct of this type of finite-volume differencing. Additionally, difficulties that occur due to uncertainties in the specification of the artificial viscosity are explored, and point to the need for further research in this area.

[1]  M. Shashkov,et al.  Elimination of Artificial Grid Distortion and Hourglass-Type Motions by Means of Lagrangian Subzonal Masses and Pressures , 1998 .

[2]  Mikhail Shashkov,et al.  A tensor artificial viscosity using a mimetic finite difference algorithm , 2001 .

[3]  Donald E. Burton,et al.  Exact conservation of energy and momentum in staggered-grid hydrodynamics with arbitrary connectivity , 1991 .

[4]  J. Gillis,et al.  Methods in Computational Physics , 1964 .

[5]  E. J. Caramana,et al.  Numerical Preservation of Symmetry Properties of Continuum Problems , 1998 .

[6]  Mikhail Shashkov,et al.  Formulations of Artificial Viscosity for Multi-dimensional Shock Wave Computations , 1998 .

[7]  C. Lanczos The variational principles of mechanics , 1949 .

[8]  John K. Dukowicz,et al.  Vorticity errors in multidimensional Lagrangian codes , 1992 .

[9]  A. J. Ayer,et al.  Language, Truth, and Logic , 1936 .

[10]  W. F. Noh Errors for calculations of strong shocks using an artificial viscosity and artificial heat flux , 1985 .

[11]  C. L. Rousculp,et al.  A Compatible, Energy and Symmetry Preserving Lagrangian Hydrodynamics Algorithm in Three-Dimensional Cartesian Geometry , 2000 .

[12]  E. J. Caramana Timestep relaxation with symmetry preservation on high aspect-ratio angular or tapered grids , 2001 .

[13]  Mikhail J. Shashkov,et al.  A Compatible Lagrangian Hydrodynamics Algorithm for Unstructured Grids , 2003 .

[14]  Mark L. Wilkins,et al.  Use of artificial viscosity in multidimensional fluid dynamic calculations , 1980 .

[15]  Roger B. Lazarus,et al.  Self-Similar Solutions for Converging Shocks and Collapsing Cavities , 1981 .

[16]  M. Shashkov,et al.  The Construction of Compatible Hydrodynamics Algorithms Utilizing Conservation of Total Energy , 1998 .

[17]  C. Habel,et al.  Language , 1931, NeuroImage.

[18]  R. D. Richtmyer,et al.  A Method for the Numerical Calculation of Hydrodynamic Shocks , 1950 .