To be more specific, the deteriorative degree of dielectric relaxation is shown to be consistent with the beta value from the CD modeling by quantization, which is due to the beta-dominating exponent part in CD modeling (Equation 2).
For "shorter" waiting times, the distribution is dominated by the exponent α∼0.7, implying that consecutive avalanches are correlated (like in the Omori law for earthquakes [45], which has recently been observed for neuronal avalanches [46]).
For "longer" waiting times, the distribution is dominated by the much larger exponent β∼3, a regime in which consecutive avalanches would be independent.
Many of the finest sections were dominated by the virtuoso Malian n'goni exponent Bassekou Kouyate.
However, while using (10), the exponent of palm oil fraction dominated the correlation.
However in practice, only the largest exponent is calculated as this dominates the trajectory divergence [ 21].
When gravity dominates, the oil recovery scales as a power law with time with an exponent that depends on the oil mobility, whereas when capillary forces dominate, the oil recovery has an exponential variation with time and the ultimate recovery is poorer.
Linear stability analysis can indicate when nonlinearities can be expected to dominate the dynamics, and local finite-time Lyapunov exponents can indicate regions on an attractor where these nonlinearities will cause all uncertainties to decrease cause trajectories to converge rather than diverge so long as trajectories remain in those regions.
For rocks with good pore structure, the proportion of macropore components is dominant, high cementation exponents and low saturation exponents can be obtained, and on the contrary, rocks with poor pore structure will be dominated by the proportion of small pore components, and they will contain low cementation exponents and high saturation exponents.
The evidence of the chaotic advection in these SAW-driven flows is further verified through a pixel intensity analysis, in which mixing times, quantified through a normalised mixing index, were observed to be inversely proportional to the Lyapunov exponent, characteristic of processes in which transport is dominated by chaotic advection.
As an exponent of the yank-and-pull school that has dominated the Ailey company's recent novelties, Mr. Rhoden is not interested in a sustained equivalent of a melodic line.
