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Fluid motion is assumed to be irrotational, incompressible and inviscid.
The motion is assumed to be two-dimensional.
When grain boundaries come into contact with particles, boundary motion is assumed to be pinned.
Motion is assumed to be slow, in such a way that any inertial effects are negligible.
Small amplitude motion is assumed, such that linear system theory is valid.
The blade motion is assumed to be a linear combination of modes shapes with the modal coefficients depending on time.
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Slip of 30 cm in the direction of N115°E, opposite to the relative plate motion, was assumed with a ~100-km-wide checkerboard pattern.
Inertial terms in the equation of motion are assumed to be negligibly small because of the high viscosity of magma in our model, so we obtain: (3)where a is the conduit radius, η f is the melt viscosity, p is the melt pressure, and g is the gravitational acceleration.
The vocal fold shape and its motion are assumed to be symmetrical with respect to the medial axis.
That is, early sensory feature detection mechanisms (e.g., for color, orientation, motion) are assumed to compute feature contrast (i.e., dimensional saliency) signals for all locations across the visual field.
The molecular motion was assumed to be isotropic.
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