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The motion of such systems is described by partial differential equations complemented by suitable boundary conditions.
In general, the motion of such a beam can be very complex.
For the first time equations of motion of such system in the mechanically resistive medium are derived and numerically solved.
The global results are finally interpreted in terms of the physical traveling wave motion of such gyroscopic continua.
Therefore, multibody dynamic techniques are used to form and solve the equations of motion of such coarse-grained systems.
The aim of a simulation is to solve the equations of motion of such a model, which is designed to represent the time-evolution of its target system.
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If so, the motions of such an outflow would be detectable in the radio emissions.
1. Descartes held that all other properties arise from the configurations and motions of such bodies — from geometric complexes.
The symmetry for the stable, asymmetrical, periodic motions of such a system is observed.
The periodic motions of such an oscillator are predicted analytically through the corresponding mapping structure.
Den Hartog [1] gave an exact solution for the symmetric steady state motions of such a system in 1930.
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