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The details of the posture adjustment motion are described in the next section.
In this section the proposed methods to compute (Section 2.1) and analyze (Section 2.2) the left ventricle motion are described.
The torsional vibrations of crankshafts, input and output shafts of mechanisms having variable inertia characteristics are generally modelled as discrete systems, and the governing equations of the motion are described by ordinary differential equations.
Similar(57)
Defect motion is described by two transport equations.
The motion is described by the Stokes equations driven by the input pressure and gravity force.
The relative orbital motion is described by the Hill Clohessy Wiltshire equation.
First, a mass-spring model was applied and the equation of motion was described.
The stochastic ground motion is described by fully non-stationary sigma-oscillatory model.
The details of the resultant fluid motion is described using the material stretching coordinate technique.
The beam motion is described by the transverse displacement and the slope.
The Nosé-Hoover style non-Hamiltonian NPT equations of motion were described in detail by Shinoda et al. [32].
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