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During the main simulation run, the animal movement was simulated for 600 s.
Thereafter, a three-dimensional paleotectonic stress field during the Late Himalayan movement was simulated by the finite element method.
Thigh calf contact force characteristics from an earlier study were included and a squatting movement was simulated.
The movement was simulated by moving the crank axis, or modifying the distance between the two cranks (±10 cm).
As introduced by Galle et al. (2005) for monolayers, and Drasdo et al. (2007) for multi-cellular spheroids, cell movement was simulated by a stochastic equation of motion for the position of each cell.
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Large amplitudes of rapid movement are simulated in order to investigate how the original vortex wake re-establishes itself after a sudden movement has occurred.
The dynamic effect of traffic vehicles are modeled as a row of equidistant moving forces, while the earthquake movement is simulated as the vertical oscillation of boundary supports.
Peristaltic movement is simulated by a V-shaped grate, pressed down on the bags, which rocks from side to side, driven by compressed air.
The impact of inter- and intra-molecular movements was simulated for polyurethane reactions to better understand the impact of mass transfer on polymerization reactions.
The specimens were mounted into a specially designed simulator in which isokinetic flexion-extension movements were simulated.
Drug movements were simulated with a finite element computer model of the inner ear fluids.
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