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Titlebook: Computer Simulation of Dynamic Phenomena; Mark L. Wilkins Book 1999 Springer-Verlag Berlin Heidelberg 1999 Computer.Maxwell‘s equations.Si

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11#
發(fā)表于 2025-3-23 12:32:44 | 只看該作者
Book 1999s points. The numerical procedures described in the text permit the exact con- servation of physical properties in the solutions of the fundamental laws of mechanics: (1) conservation of mass, (2) conservation of momentum, (3) con- servation of energy. The laws of mechanics are universal in their ap
12#
發(fā)表于 2025-3-23 17:23:57 | 只看該作者
1434-8322 the solutions of the fundamental laws of mechanics: (1) conservation of mass, (2) conservation of momentum, (3) con- servation of energy. The laws of mechanics are universal in their ap978-3-642-08315-0978-3-662-03885-7Series ISSN 1434-8322 Series E-ISSN 2198-2589
13#
發(fā)表于 2025-3-23 19:52:38 | 只看該作者
Elements of Fluid Mechanics,s different particles, and may be compressible or incompressible. The material may totally or partially take the shape of its container. The concept of a continuum is also implied. This means that the pressure, temperature, and density vary continuously from point to point. Hydrodynamics is the stud
14#
發(fā)表于 2025-3-23 23:59:44 | 只看該作者
Numerical Techniques,s that describe fluid dynamics in one space dimension. The material is divided into a Lagrange grid that moves with the flow. The space between consecutive grid lines is referred to as a zone. For multidimensional problems a zone is defined as the interior space of intersecting grid lines. The inter
15#
發(fā)表于 2025-3-24 03:49:06 | 只看該作者
16#
發(fā)表于 2025-3-24 08:46:32 | 只看該作者
Sliding Interfaces in Two Dimensions, provided to allow slippage of one grid on the other. A sliding interface is a line or a surface defined by a set of Lagrange coordinates. In two dimensions the interface is a line defined by . coordinates and in three dimensions the interface is a plane defined by . coordinates. In the method emplo
17#
發(fā)表于 2025-3-24 13:09:04 | 只看該作者
Magnetohydrodynamics of HEMP,problem considers cylindrical symmetry, in that only the .. component of a magnetic field is present. The problem is formulated so that the stress contributions resulting from a magnetic field are incorporated into the stress tensor of an elastic-plastic computer program. In addition to the Lorentz
18#
發(fā)表于 2025-3-24 18:51:43 | 只看該作者
19#
發(fā)表于 2025-3-24 21:20:00 | 只看該作者
978-3-642-08315-0Springer-Verlag Berlin Heidelberg 1999
20#
發(fā)表于 2025-3-25 02:18:47 | 只看該作者
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