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Fluid motion is calculated by directly solving the Navier Stokes equations by a SIMPLE approach.
N-Decane (C10H22) is used as the liquid fuel, and the droplet motion is calculated by the Lagrangian method.
The motion is calculated based on feedback data of angular position via an encoder connected to the secondary axis of the motor.
The structure motion is calculated with six degrees of freedom in terms of the ice contact force, the buoyancy, the drag force of current, and the mooring force.
In the simulation model, particle motion is calculated by solving Newton's equations and the flow field of air is predicted by the Navier Stokes equations.
The free field wave motion is calculated using the 1D time-domain finite element method and is then extended to 3D.
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The underwater drag for the range of motion was calculated by using the general fluid equation.
For dynamic analysis, the time responses for accelerating motion and torque-driven motion are calculated.
The amplitude and frequency of transverse motion are calculated for various Keulegan-Carpenter numbers and reduced velocities.
These forces were given to the musculoskeletal simulation as the external forces, and muscle activity required for any given physical exercise (e.g. swimming motion) was calculated.
T50G was found to correlate with the Tg of PMMA, and the volume of polymer segments undergoing glass transitional motion was calculated to be 1.7 nm3.
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