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A partitioned strategy with load transfer method is selected for achieving successful fluid structure interaction (FSI) simulations with strong two-way coupling.
This paper presents an advanced CAD integrated approach for 3D simulations with strong non-linear boundary conditions including reaction efficiency and moving cathode tools.
When using larger computer systems of up to 256 nodes the scalability of simulations with strong convergence toward specific geometries is less sensitive to overheads due to the shuffling of metadata information.
The only exception to this was in sensitive period simulations with strong exposure correlation, where there was less distinction between accumulation and critical period hypotheses.
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Simulations with stronger (purple: 0.4 mM) or weaker (light green, 18 mM) longitudinal interactions show higher or lower maximal polymerase activity.
In simulations with a strong electric field (0.1 V/nm or above) and positional restraints on the S1 and S2 helices, S4 movement was observed consisting of displacement along the S4 helix axis and a screwlike axial rotation.
Photosynthetic capacities (Jmax25) and CO2 assimilation rates (Ag) increased with Ca in all simulations, with a stronger increase in Ag for seasonal vegetation in the medium term, but a stronger increase for perennial vegetation in the long term.
Table 5 and Fig. 3A and B show the following additional trends: Photosynthetic capacities (J max25) and CO2 assimilation rates (A g) increased with C a in all simulations, with a stronger increase in A g for seasonal vegetation in the medium term, but a stronger increase for perennial vegetation in the long term.
Simulations with progressively stronger (dark green: 1.7 mM; light green, 0.35 mM) longitudinal interactions show higher maximal polymerase activity.
Several simulations of flows with strong shocks, including the forward-facing step test, double Mach reflection test, and a strong shock of Mach number 5.09 diffracting around a corner, were carried out on hexagonal lattices, showing the model's capability of simulating the propagation of strong shock waves.
The discrepancies between the mathematical analysis and computer simulations arise because with strong repressors the approximation that leads to Michaelis-Menten-like hyperbolic repression terms ceases to be valid.
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