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A nonlinear registration algorithm (fluid) was used to calculate atrophy rates in six regions: frontal, medial temporal, temporal (extramedial), parietal, occipital lobes and insular cortex.
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Secondly, by utilizing the multi-material Arbitrary Lagrange-Euler (ALE) algorithm, Fluid-Structure Interaction (FSI) method and erosion algorithm implemented in the finite element (FE) code LS-DYNA, and describing the concrete targets with the original and modified HJC models, the formation and impact processes of EFP are well reproduced.
Figure 11 shows the algorithm for fluid flow calculation.
Open image in new window Fig. 11 Algorithm of fluid flow calculation.
Turbulent pipe flow controlled by the opposition control algorithm [J. Fluid Mech. 262 (1994) 75 110] is studied by means of direct numerical simulation.
A one-dimensional algorithm for fluid simulation of interpenetrating multi-component plasmas, developed earlier for the collisionless case [1], is extended to include collisions between species.
The numerical simulation was performed in various in-situ stress conditions with the consideration of a transient flow algorithm for fluid flow.
In our current algorithm, the fluid motion is solved by LBM, the deformation of the solid body is solved by the finite element method, and the Lagrange multiplier is solved on the low-order mesh.
No specific algorithm for fluid administration was used.
The algorithm for fluid replacement during the first 12 hours after ICU admission in the Doppler group was similar to that used by Sinclair and colleagues [ 23].
With the improvement of computer power and numerical algorithms, computational fluid dynamics (CFD) has become a useful tool for studying the hydrodynamics in complex multiphase systems.
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