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Motion is modeled by means of optical flow, computed for different directions and scales.
The bending motion is modeled in this section using this prototype.
Therefore, the target motion is modeled as the RFS Sk|k-1 xk-1).
The spatial variation of ground motion is modeled by an empirical coherency loss function.
This is possible, if the target motion is modeled as a Markov random walk of first order.
The fluid response from the solid motion is modeled through specifying the cell-face velocity with partial-cell treatment (PCT).
Similar(48)
Missile motion is modelled to be nonlinear with unknown parameters and uncertainties.
The indicated motion is modelled as a band-limited Gaussian white noise process.
The fluid motion is modelled as a potential flow and computed using a boundary element method.
The surface ground motion is modelled with the Kanai–Tajimi power spectral density, i.e. as an "ideal white noise" at the bedrock filtered through the soil deposit.
Contact/impact in flexible multibody systems that undergo pre-contact free motion, contact/impact and post-impact constraint motion is modelled.
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