DOI: http://dx.doi.org/10.7554/eLife.09206.015 The cell cortical layer of actomyosin is modeled as a thin axisymmetric layer of length L with principal axis z = − L / 2 (anterior side)… L / 2 (posterior side).
Profiles, taken from the HAADF-STEM images in Fig. 1a, b, point out a similar behaviour in both samples: roughly abrupt interfaces, GaAsBi layers of similar length (~ 140 nm).
Consider a simply supported beam of span (L) with plastic layer material (e.g. concrete) strengthened mechanically with upper and lower elastic layer materials, of length (l up and l lp), respectively, and subjected to a uniformly distributed load (p).
Compared to a single graphene layer of shorter length, the double graphene layer with longer length presents stronger absorption and higher modulation depth.
The model assumes the turbulence viscosity as a function of velocity deformation rate and the length scale in the inner layer and function of length scale and local mean velocity in the outer layer.
The longer layers give the illusion of length and the shorter layers create volume.
The thickness of all intestinal layers, the length of the villi and the depth of the crypts were measured under a light microscope using the AxioVision program 4.5 (Carl Zeiss MicroImaging GmbH, Jena, Germany).
For each member of the hierarchy, boundary conditions for layers of the finite length are formulated.
In addition, a study of the effect of layer length on the behaviour of the sandwich beam is submitted.
Here, we investigate metastable SiNy solid solubility in TiN and probe the effects of surface segregation during the growth of TiSiN films onto substrates that are either flat TiN 001)/MgO(001) epitaxial buffer layers or TiN 001) facets of length 1 5 nm terminating epitaxial TiN(111) nanocolumns, separated by voids, deposited on epitaxial TiN(111)/MgO(111) buffer layers.
