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This justifies the greater resistance and also the gentle drop in bearing capacity of the 3D sub-assemblage in comparison to the planar specimen.
To achieve these goals, a 3D RC sub-assemblage including a transverse beam was exposed to monotonic downward displacement of the middle joint and the results are compared to a corresponding planar specimen.
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For planar specimens, such ion-induced surface modifications have been studied quite extensively in the past for a large variety of (binary) systems [1, 2].
In addition, comparison of the 3D and planar specimens demonstrated that the transverse beam helps to achieve a more symmetric and ductile behavior within the main beams.
A rather different and innovative experimental approach has been instead described by Romo et al. [ 19] and Kim et al. [ 20], involving bulge inflation test on planar specimens, the use of stereo-digital image correlation to investigate the strain field, and the application of the virtual fields methods for material characterization purposes.
We were, however, able to estimate CI on the basis of two independent sources: 1) www.skullsite.co.uk – an amateur collection of various different animal skulls, including a wolf skull picture and corresponding morphological measurements, and 2) Multi-planar specimen pictures of a gray wolf skull archived by the University of Michigan's Museum of Zoology [18].
Point-to-point compensation for the bending of the optical path and laser wavelength changes accounted for the majority of the correction, while the addition of geometric compensation for the non-planar specimen shape conferred relatively little additional error reduction.
This work establishes guidelines for SVET use and the potential issues that must be taken into account when using SVET to examine the corrosion behaviour of non-planar specimens.
This method is then used to evaluate Lewis relation in the case of the flow of free air stream over a flat planar test specimen.
An analysis of moiré fringes in planar view specimens, corroborated by high resolution TEM (HRTEM), shows that that the strain in the InN QDs is almost fully accommodated by a MD network at the InN/GaN interface.
With the increase of σ2, the temperature change area is planar of rock specimen which proofs that the failure mode of rock specimen turns into slabbing.
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