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The small correction term h x1, x3) describes the oscillation structure in higher orders of the perturbation theory.
While examining the SMS oscillation structure described by Eq. (27) one may put φ = 0 in its right-hand part.
Therefore, a solution to (30) may be sought using the method of different scales, representing the potential ψS as (32 where the function U (x1) describes, in the main order, the small-scale transverse structure of oscillations along the x1 coordinate, whereas the function S x1, x3) describes the oscillation structure along magnetic field lines.
However, (1) the higher accuracy and lower variability of the bare ground measurements from the dipole when compared with the geodetic antenna and (2) the continued clear and distinct oscillation structure in the SNR for the dipole antenna in the presence of snow show the superiority of the design.
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At these scales the frequency of oscillation for structures increases (from megahertz up to gigahertz frequencies), offering new design possibilities (such as for noise filters); however, the devices become increasingly sensitive to any defects arising from their fabrication.
The numerical tests show successfully that the quality solutions can be obtained smoothly with the proposed algorithm, i.e., the expected convergence order of the numerical solution with the mesh refinement can be reached, while the non-oscillation shock structure can be obtained.
The interaction between galloping and Kármán-vortex resonance for long rectangular cylinders is a crucial issue in flow-induced vibration, since this type of instability can cause catastrophic oscillations of structures or structural elements exposed to wind.
Vortex-induced vibrations cause in-line and cross-flow oscillations on the structure; however, in-line oscillations are significantly larger.
As demonstrated in Fig. 11, for (alpha = 0.997), the amplitude of the structure oscillation is highly reduced when the TMD is used.
In practical applications, many vibration absorbers are used to absorb oscillation of a structure, one of which is pendulum-type vibration absorbers.
The ICC consists of multiple parallel first-order lossy integrators, with the goal of targeting all major participating resonant modes in the oscillation of the structure.
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