At the microscopic level, each particle undergoes Brownian motion, leading to a diffusion field governed by (1) when a large number of these particles are considered.
By applying a diffusion gradient field of high b values, the biexponential model can differentiate the diffusion in extracellular from that in intracellular, which are defined as fast diffusion coefficient D∗ and slow diffusion coefficient D, respectively.
Then, by properly extending this scheme to our sensor network setting, we design and propose an effective diffusion field sensing strategy.
We conducted an open diffusion field experiment with 13 groups of wild common marmosets, Callithrix jacchus.
The thermal stabilization of the microstructure by the occurrence of diffusion field impingement allows for the observation of the glass transition of the remaining amorphous phase in the matrix by modulated differntial scanning calorimetry (DSC).
This phenomenon is explained by temporary changes in the diffusion field and the reaction zone.
The termination of the nucleation process by the expansion of diffusion fields is considered, as well as the deviations from randomness observed in the distribution of nuclei on the electrode surface.
For alloy compositions further inside the limit, there was no such stop, except by the action of impingement of diffusion fields for carbon.
In this paper, we will consider diffusion fields induced by spatially localized and temporally instantaneous sources, with the following distribution: f(mathbf{x}, t) = sum_{m=1}^{M} c_{m} {deltaleft(mathbf{x}-boldsymbol{xi}_{m}, t - tau_{m}right)}, (3).
Diffusion coefficients of both the cation [C2mim]+ and anion [OAc]− were determined by a pulsed-field gradient H NMR technique using a widebore Avance II NMR Spectrometer (Bruker Biospin) operating at a H resonant frequency of 400 MHz.
