A second-order multiscale approach for viscoelastic analysis of statistically inhomogeneous materials

2019 ◽  
Vol 220 ◽  
pp. 550-565
Author(s):  
Zhiqiang Yang ◽  
Yi Sun ◽  
Yizhi Liu ◽  
Qiang Ma
Keyword(s):  
Second Order ◽  
Multiscale Approach ◽  
Inhomogeneous Materials ◽  
Viscoelastic Analysis

Dynamic thermo-mechanical coupled simulation of statistically inhomogeneous materials by statistical second-order two-scale method

2015 ◽  
Vol 31 (5) ◽  
pp. 762-776 ◽  
Author(s):  
Zihao Yang ◽  
Junzhi Cui ◽  
Yufeng Nie ◽  
Zhiqiang Huang ◽  
Meizhen Xiang
Keyword(s):  
Second Order ◽  
Inhomogeneous Materials ◽  
Coupled Simulation ◽  
Scale Method

Disappearance Voltage Determinations Using a Convergent Beam

1971 ◽  
Vol 29 ◽  
pp. 184-185
Author(s):  
W. L. Bell
Keyword(s):  
Second Order ◽  
Objective Method ◽  
Uniform Thickness ◽  
Rocking Curve ◽  
Crystal Perfection ◽  
Kikuchi Line ◽  
Central Maximum ◽  
Diffraction Patterns ◽  
Convergent Beam ◽  
Beam Technique

Disappearance voltages for second order reflections can be determined experimentally in a variety of ways. The more subjective methods, such as Kikuchi line disappearance and bend contour imaging, involve comparing a series of diffraction patterns or micrographs taken at intervals throughout the disappearance range and selecting that voltage which gives the strongest disappearance effect. The estimated accuracies of these methods are both to within 10 kV, or about 2-4%, of the true disappearance voltage, which is quite sufficient for using these voltages in further calculations. However, it is the necessity of determining this information by comparisons of exposed plates rather than while operating the microscope that detracts from the immediate usefulness of these methods if there is reason to perform experiments at an unknown disappearance voltage.The convergent beam technique for determining the disappearance voltage has been found to be a highly objective method when it is applicable, i.e. when reasonable crystal perfection exists and an area of uniform thickness can be found. The criterion for determining this voltage is that the central maximum disappear from the rocking curve for the second order spot.

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