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The lift coefficient Cl(t) is assumed to be a zero mean, narrow band process and the velocity V0, composed of a uniform, constant velocity current plus oscillating wave, a broad band process.
Theoretical calculations at different pressures, performed within the density functional theory, are provided to confirm that the D band process involves iTO phonons along the K Γ direction.
In this paper it is shown that the extremes of a Gaussian, non-narrow band process are asymptotically equal to the extremes calculated according to the narrow band formula.
The 60-yarn CNT wire resulted in a stake and socket fibre fracture when loaded to failure in constant tension; however, in the cyclic loading condition, the wire failed by kink band process.
The background response was regarded as a broad band process, while the resonant response was a narrow band process.
As α1 tends to unity, X t) becomes a very narrow band process.
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The thickness dependence of yielding and fracture of metallic glass plates subjected to bending is considered in terms of the shear band processes responsible for these properties.
Then the original narrow band processes emerge in the relevant Ito system only as a couple of input process spectral density values in significant points of the system resonance curves.
The method has the attraction of converging to the same results as the well known Rayleigh distribution for narrow band processes, if either of the spectral peaks is small.
The Poisson approximation may result in serious errors for very narrow band processes [3].
While the Poisson approximation is generally valid for broad band processes, it may fall short for very narrow band processes, and lower threshold levels of practical interest, due to the tendency of crossings to occur in cluster [2, 3].
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