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A mode matching method based on the characteristics of accurate mode shape estimates is then proposed to ensure the correctness of the estimates.
Accurate mode profiles and confinement factors are calculated by Finite Difference mode solver, OptiWave [19, 20], in order to avoid ripples due to Gibbs phenomenon inherent to FMM.
A mode matching method based on the characteristics of accurate mode shape estimates is proposed to ensure the correctness of the estimates.
Cells were sorted at the most accurate mode (single cell, one drop) with a sorting speed of 4,000 s−1 and a sample chamber cooled to 4°C.
For the physically accurate mode, it is shown analytically that the numerical dispersion relation is accurate to order 2p+2, where p is the highest order of the basis polynomials.
Frequency responses for six different mode expansions are studied and compared with that for single mode to find the more contracted and accurate mode expansion investigating traveling wave vibration.
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An inverse problem of cohesive zone modeling is performed to obtain accurate mode-I cohesive zone laws from experimentally measured deformation fields.
It has a more accurate mode-splitting due to redefined barotropic pressure-gradient terms to account for the local variations in density field, while maintaining the computational efficiency of a split model.
The results show that the trapezoidal Fourier p-element produces much higher accurate modes than the conventional finite elements with the same number of d.o.f.s.s
The results show that the finite strip Fourier p-element can obtain much higher accurate modes than the Fourier p-element, the finite strip and the conventional finite elements.
The computed natural frequencies of cantilever and simply supported square plates show that the convergence rate of the present element is very fast with respect to the number of hierarchical terms and it can predict very accurate modes.
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