It assumes that the in-plane displacements have a piece-wise linear shape across the thickness depending on the shear stiffness of each composite layer.
To briefly summarize, we have demonstrated that the Drosophila trajectories are scale-free by showing that (1) displacements have a power-law dependency upon time of flight, (2) the time series of saccade intervals has a long-range power-law correlation, and (3) trajectories are fractal.
The expected and observed actual displacements had a high level of correlation with coefficients of determination of 1.0 for all axes.
The Michelson contrast of the vessel changed as indicated by the black arrow in Fig. 2A, with larger displacements having a higher contrast 62%, 61%, 76%, and 77% for the 0, 2×, 6× and 8× the Airy disk diameter offset, respectively.
Even though the observed vertical displacement has a large error, our model roughly explains the data distribution and the profile pattern.
In this model, the in-plane displacements take cubic polynomial distributions and the transverse displacement has a quadratic one thorough the core thickness.
Simulations show that the magnetic flux variation in response to vertical displacement has a negative exponential shape (Figure 10), in accord to previous works [26, 27, 35]. Figure 10 Simulation of the magnetic flux against vertical displacement.
The displacement filed accounts for an in-plane displacements varying linearly through the layer thickness; and the out-of-plane displacement has a parabolic variation through the layer thickness.
The results show that the passive ankle joint angular displacement has a considerable influence on the elongation of the tendinous and architectural structures of the GM muscle tendon unit.
In contrast, for a dielectrically highly conducting interface the electric potential is continuous across the interface whereas the normal electric displacement has a discontinuity across the interface which is proportional to a certain differential expression of the electric potential.
