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The fluid interface motion is computed using a highly accurate boundary integral method.
The continuous phase is described in an Eulerian framework and liquid droplet motion is computed by the Lagrange approach.
Phase boundaries are considered sharp and their motion is computed using the coupled level set/volume-of-fluid (CLSVOF) method.
Comparison of such responses to those that arise in response to conventional laboratory stimuli (i.e. moving bars) should provide insight as to the effectiveness with which motion is computed during natural viewing.
Since our algorithm is cell-centered, the final mesh motion is computed by using a suitable node solver algorithm.
The blade vibration is modeled with an aeroelasticity model in which blade motion is computed by linear combination of responses of each mode under unsteady loads.
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Exact mode shapes and natural frequencies associated with the flexural motion are computed for various piezoceramic distributed actuator arrangements.
In particular, we focus on large eddy simulation (LES) in which the large scales of motion are computed explicitly while the small or subgrid-scale motions are modeled.
The maps of the mean amplitudes of seasonal oscillations of atmospheric excitation functions of polar motion are computed for the fifty years period in 108 equal-weight sectors.
In addition, to verify the stability results, the time responses of flapwise motion are computed by the generalized-α time integration method.
Although the method is general, here it is applied to the description of two, however diverse, robot behaviours, in which the induced motion was computed on the basis of information retrieved from different cameras: a camera integrated with the robot gripper and a camera statically mounted above the scene.
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