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Until recently, numerical implementations of cohesive-zone models have suffered from a certain mesh bias.
Numerical representations of cohesive-zone models suffer from a certain mesh bias.
The CNTs grown with a mesh bias of + 300 V show a density of ∼ 1.5 μm− 2 and a height of ∼ 5 μm.
A proper representation of the discrete character of cohesive-zone formulations which avoids any mesh bias can be obtained elegantly when exploiting the partition-of-unity property of finite element shape functions.
A proper representation of the discrete character of cohesive-zone formulations which avoids any mesh bias is obtained by exploiting the partition-of-unity property of finite element shape functions.
Similar(54)
The growth of CNTs can be controlled by the mesh electrode bias which in turn controls the plasma density and ion flux on the sample.
We apply this method to several two- and three-dimensional problems in statics and dynamics and show through several numerical examples that the method does not show any "mesh" orientation bias.
However, CNTs do not grow when the mesh electrode is biased to − 300 V.
The anode was electrically grounded while the cathode and the mesh were both negatively biased, causing no plasma to occur below the mesh.
The deposition reactor was designed in order to allow the intermediate mesh electrode to be biased independently from the ground and power electrodes.
Numerical finite element studies document the avoidance of spurious mesh sensitivity and mesh orientation bias, and demonstrate objectivity and size effect.
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