Exact(3)
Variations between operation modes are larger for the foaming liquid than for the other liquid solutions employed.
It is also shown that the damping factors in torsionally coupled modes are larger than those in translational modes.
If the taken modes are larger then one, it comes under the category of higher order azimuthally polarized mode beams at the same time β should be take >1 under the high NA focusing condition.
Similar(57)
Numerical simulations demonstrate that the results from Rayleigh Quotation iteration with the asymptotic solutions are better than ones from Lapack solver when the norms of modes are large enough.
Both the contact forces and maximum bending moments in the intra-helical buckling mode are larger than that in the inter-helical buckling mode, so intra-helical buckling should be avoided in the optimal design of connectors on tubular strings.
The results show that the Richardson number and the Fill efficiency of the equalizer mode are larger than those of the other two modes and that the MIX number for the equalizer mode is smaller than those of the other two modes.
Hence, the time delay between modes is large resulting in a wide pulse width and a low BER of 4.65 × 10−2.
Hence, the time delay between highly coupled modes is large, resulting in large differential mode delays and high BERs of 6.15 × 10−7 when Δl = 1 for Fig. 4(a) and 7.87 × 10−8 for Δl = 2 in Fig. 4(b).
The loss of these fundamental modes is negligibly small and the separation of adjacent transverse modes is large enough to discriminate the fundamental mode from the higher-order modes.
If the number of modes is large enough, the base can be considered complete and imaging can be approximated as being partially coherent [ 15].
The difference of these two Raman spectra is that the intensity ratio of ZnSe to MnSe mode is larger in the ZnSe Mn ( CH 3 COO ) 2 nanobelt.
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