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The direction and the amplitude of such changes have however remained controversial because of a lack of quantitative approaches.
Moreover, it is also noticed that the amplitude of such solitons remain larger in the case of positively charged dust grains in comparison with negatively charged dust grains.
The direction and amplitude of such a slowness vector were regarded as the incident azimuth and apparent slowness of the incoming IG waves, respectively.
Moreover, the amplitude of such a soliton remains larger in the case of positively charged dust grains in comparison with the negatively charged dust grains.
A geometrically exact mechanical formulation is proposed to describe three-dimensional motions of flexible cables without any restriction on the amplitude of such motions.
It is shown how one can use the amplitude of such excitations to change the way in which oscillators behave, making them respond as free oscillators of the same or different type.
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The amplitudes of such signals are distributed according to the Gutenberg Richter (GR) law and characterised through the b-value which decreases systematically with damage growth.
The coupled nonlinear matrix amplitude equation (in-plane motion is coupled with flexural motion) is solved to obtain (1) nonlinear free flexural vibration frequencies of isotropic and composite plates with different in-plane boundary conditions, (2) flexural vibration amplitudes of such plates under transverse harmonic pressure or periodic in-plane load.
The amplitudes of such evoked Ca2+ transients then initially remained close to control values, at 5.14 ± 1.46 (P > 0.05; n = 50 peaks from four cells).
Hence, avoiding the occurrence of large amplitude vibration of such systems is of great importance.
We have embarked on a program to quantify the amplitude effects of such spontaneous-evoked interactions both within and across sensory modalities, under varying states of the cortical network.
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