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The axial speed is characterized as a simple harmonic variation about the constant mean speed.
Numerical simulation demonstrates the effects of the stiffness, the viscosity and constant mean speed of beam.
When the axial speed is a constant mean speed with small harmonic variations, the governing equation can be treated as a continuous gyroscopic system with small periodically parametric excitations and a damping term.
When the axial speed is a constant mean speed with small harmonic variations, the governing equation can be regarded as a continuous gyroscopic system under small periodically parametric excitations and a damping term.
The relatively constant mean speed of the beam during the valve opening pulse for the NPV results in a phase-space distribution with a position spread that is approximately given by v 0 τ.
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With this model, the highway could be of multiple unidirectional lanes and the vehicles are allowed to have variable speed, but move with constant mean velocity.
The velocity function is assumed to be a harmonically varying function about a constant low mean speed.
Searchers using different strategies were compared: Amoeboid motions were parameterized using our experimental data, random walks were simulated using the average speed for Dictyostelium, and straight-line movement at a constant speed used the mean speed of these amoebae.
Using analytical and numerical methods, this paper investigates the stochastic dynamic response of a rotating simply supported beam subjected to a random force with constant mean value moving with a constant speed along the beam.
The axial speed is assumed to be comprised of a constant mean value along with harmonic fluctuations.
with constant mean power.
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