Titlebook: Computational Science and High Performance Computing; Russian-German Advan Egon Krause,Yurii I. Shokin,Nina Shokina Conference proceedings

spinal-stenosis

Offensive

Completely splitting method for the Navier-Stokes problem,ical level, this problem is splitted into two processes: convection-diffusion and action of pressure. The convection-diffusion step is further splitted in two geometric directions. To implement the finite element method, we use the approach with uniform square grids which are staggered relative to o

DEFER

Methods of shock wave calculation,-conducting medium, give a corollary saying about entropy conservation along the particle trajectory..Conservation laws on the surface of a strong shock are algebraic equations showing that entropy grows across the shock wave. This is the fundamental difference between a shock wave and a continuous

Militia

Distributed and collaborative visualization of simulation results,ualize simulation results either on a desktop computer or on stereo projection environments. It supports the coupling of ongoing simulations with visualization thus enabling simulation steering. In addition it is possible for multiple engineers or scientists at different locations to discuss the sam

Anguish

聾子

可觸知

災(zāi)難

Computer simulation at VNIIEF,tational institutions. The team passed a way of 50 years long from manual calculations to numerical simulation of various physical phenomena and processes in real, i.e. 2d and 3D, geometries. The paper presents the basic research fields and challenges, describes the generation and development steps

不自然

多節(jié)

Method of particles for incompressible flows with free surface,ree-Lagrange one and is a kind of special Galerkin method, where convective transport is being calculated by means of material particle motion. As a result, the material derivative is calculated in Lagrange variables, while the mass forces, inner and surface stresses — in Eulerian variables. The mai