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Then, a more detailed description of each motion is given.
The law of motion is given by a fuzzy algorithm which optimizes the parameters of movement.
The law of the Brownian motion is given formally as the Gaussian measure (1.2).
The pitching motion is given by α = Am sin ωpt) + αm.
The equation of motion is given as a nonlinear partial differential equation with periodically variable coefficients.
Evidence for chaotic motion is given through Poincaré sections, frequency spectres and Lyapunov exponents.
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The equations of motion are given by.
The conditions for existence of a sliding manifold guaranteeing a stable sliding motion are given.
In cylindrical coordinates the equations of motion are given by (2.1).
The Hopf and subharmonic bifurcation conditions of period n 1 motion are given.
The individual translational and rotational components of the motion are given in the Additional file 1 (part 2).
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