The separation from the nanoparticle to achieve bulk behavior of the accessible volume depends also weakly on the size of the probe particle.
The line crack-like damage generated within a small material volume may change the material behavior of the material volume from initially isotropic to effectively orthotropic, depending on damage orientation.
PALS measurements were performed in order to determine contents and sizes of free volume on the 'standard' and 'phase-separation' polymers; important differences in the behavior of the free volume composition curves were found, which are explained in terms of the formation of microregions in the phase separation material.
A phenomenological model was proposed to rationalize the scaling behavior of the activation volume with the external sample size and to highlight the effect of the internal feature size on the rate-limiting behavior of conventional bulk nanostructured metals (Cu).
According to the TFA, the behavior of the representative volume element (RVE) is studied accounting for the nonlinear effects by means of the presence of a uniform inelastic strain distribution in the nonlinear constituent of the heterogeneous material.
Replacing the rates by their corresponding expressions and dividing both members by C T we obtain: Equations (1) and (2) form a system of differential equations whose solution gives the temporal behavior of the cell volume, v, and the number of molecules of nutrient inside the cell, n.
Given the design-dependent characteristic of body-forces, three main difficulties are encountered when dealing with topology optimization problems under this load condition, namely, the non-monotonous behavior of the compliance, inactive volume constraint of the optimum, and parasitic effect in low-density regions.
To further verify the improved behavior of the morphology and volume changes of metal-coated nb-Si, particularly the Cu-coated samples, we performed SEM analysis of the metal-coated nb-Si at a full delithiation after 50 cycles compared to a pristine one (as shown in Figure 6).
As expected, the projected area increases with sequence length, reflecting the behavior of the total conformational volume.
We showed that the data projected on to the first eigenvector follows the spatial and temporal behavior of blood volume and the projection on to the second eigenvector of oxygenation.
We used the corrected model to describe the swelling behavior of the hydrogel and the volume transition temperature.
