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It is found that the first two modes are the flexural motion and the third mode is the coupled flexural torsional motion.
It is found that when the forcing frequency is very close to the third natural frequency of free vibration, the motion is similar to that for a linear material and the third mode dominates the motion.
T 2 J, KI and T 3 K, JI is the matrix of size I × K J (resp. J × K I and K × J I) obtained by unfolding the array of size I × J × K in the first mode (resp. the second mode and the third mode), and Λ is the R × R diagonal matrix defined as Λ= D i a g{λ1,…, λ R }; see [5] for further details on matrix unfoldings.
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When the rotational component is considered the effects of the first and the third modes which relate to H θ in Eq. 14a, 14b would appear.
H y is related to the first and the third modes in all three cases in Fig. 10b, but the effect of the third mode increases by increasing the effect of the rotational component.
However, the first and the third modes of model B were not so similar to any of the five modes of model A. This result indicates that the new types of motions emerged once the interactions of Arg with other residues were eliminated.
The voltage frequency was 288.0 kHz for the first mode and 576.0 kHz for the third mode, which was twice that of the first mode.
The strain dataset is arranged as a three-way array with strains in the first mode, spoligotype deletions in the second mode, and MIRU patterns in the third mode.
The second mode is a twist mode at 2059 Hz, the third mode is the second bending at 4334 Hz, and the fourth mode is the second twist at 5831 Hz, and the fifth mode is the third bending mode at 6651 Hz.
Correspondingly, in the case of bimodal distribution, the following rule was applied: The first mode in the distribution is within dbh classes from 10 − 20 cm, and the second mode in the distribution is after the 25 30-cm 25 30-cms.
According to the analysis, as expected each mode has a different sensitivity and the first mode is the most sensitive mode of flexural and axial vibration for the SNOM probe.
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