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This deviation is more for the lower specimen size and seems to be converging at higher specimen size.
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Firstly, certain numbers of convex particles are generated based on a grading curve, and then the particles are randomly placed into a higher space than the required specimen size in height.
Therefore, differences in ϕ'cs of different specimen sizes can lead to different bearing capacity factors, with the smaller specimen size producing a higher Nγ value.
Also the specimen size seems of importance since large-sized (50 – 70 mm) surgical specimens exhibits higher resistance (31 – 312 Ω·cm) [ 25- 28] compared to small-sized (0.65 – 5 mm) biopsy specimens (12 – 30 Ω·cm) in this study and others [ 16, 24, 29].
A marked specimen size effect was noticed, with micropillars exhibiting significantly higher flow stress than bulk samples.
These virtual specimens can be much larger than the real specimens from which the data were originally gathered, a necessary feature when real specimen size is limited by the nature of high resolution computed tomography.
Experimental results indicate that despite the increase of specimen size, no explosive spalling occurred in any of the specimens during the high temperature exposure.
High constraint conditions near the crack tip are ensured and this corresponds to lower-bound toughness values independent of specimen size and geometry.
The final geometries of the coated APT specimens were characterized with high-resolution scanning electron microscopy and transmission electron microscopy, and an empirical model was proposed to determine the optimal coating thickness for a given specimen size.
The phenomenon is dependent on specimen size and shape.
The estimated ultimate shrinkage did not depend on specimen size.
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