Molecular basis for coke strength: Stacking-fault structure of wrinkled carbon layers

Carbon ◽  
2020 ◽  
Vol 162 ◽  
pp. 56-65 ◽  
Author(s):  
Yan Tian ◽  
Guang-Yue Li ◽  
Hang Zhang ◽  
Jie-Ping Wang ◽  
Zi-Zhao Ding ◽  
...  
2006 ◽  
Vol 124 (13) ◽  
pp. 134905 ◽  
Author(s):  
Tesfu Solomon ◽  
Michael J. Solomon

2009 ◽  
Vol 94 (4) ◽  
pp. 041914 ◽  
Author(s):  
H. Tanei ◽  
K. Tanigaki ◽  
K. Kusakabe ◽  
H. Ogi ◽  
N. Nakamura ◽  
...  

2016 ◽  
Vol 365 ◽  
pp. 280-290 ◽  
Author(s):  
Beini Gong ◽  
Yonghong Lu ◽  
Pingxiao Wu ◽  
Zhujian Huang ◽  
Yajie Zhu ◽  
...  

1991 ◽  
Vol 39 (5) ◽  
pp. 825-831 ◽  
Author(s):  
K.H. Hwang ◽  
W.S. Yang ◽  
T.B. Wu ◽  
C.M. Wan ◽  
J.G. Byrne

1998 ◽  
Vol 05 (01) ◽  
pp. 21-25
Author(s):  
Z. Zhang ◽  
M. A. Kulakov ◽  
B. Bullemer

Large unit cells of dimer-adatom-stacking-fault structure and related 2 × 2 and c(4 × 2) reconstructions have been prepared by low-temperature solid-phase epitaxy and observed by scanning tunneling microscopy. The size-different unit cells of the DAS structure are considered to be a structure evolution in which more electron charge transfers in a larger unit cell from the adatom dangling bonds to the rest-atom dangling bonds. In some cases the DAS structure can degenerate into triangular 2 × 2 domains and bundlinke c(4 × 2) domains. The rest atoms are always fully filled by electrons due to the charge transfer. The adatom dangling bonds are partially filled in a c(4 × 2) symmetry and essentially empty in a 2 × 2 symmetry. As a result, the rest atoms in 2 × 2 domains can be imaged without the adatom protrusions while in the c(4 × 2) domains the protrusions of the adatoms and the rest atoms appear in zigzag chains, when the sample is negatively biased.


1996 ◽  
Vol 12 (08) ◽  
pp. 727-734
Author(s):  
Meng Xian-Ping ◽  
◽  
Wang Ying-Xia ◽  
Wei Cheng-Qian ◽  
Zhang Wan-Jing ◽  
...  

1999 ◽  
Vol 433-435 ◽  
pp. 401-404 ◽  
Author(s):  
T. Ishimaru ◽  
K. Shimada ◽  
T. Hoshino ◽  
I. Ohdomari

Nanomaterials ◽  
2021 ◽  
Vol 11 (10) ◽  
pp. 2603
Author(s):  
Dong-Dong Jiang ◽  
Peng-Yu Chen ◽  
Pei Wang ◽  
An-Min He

In this study, the effects of Cu nanoparticle inclusion on the dynamic responses of single crystal Al during shockwave loading and subsequent spallation processes have been explored by molecular dynamics simulations. At specific impact velocities, the ideal single crystal Al will not produce dislocation and stacking fault structure during shock compression, while Cu inclusion in an Al–Cu nanocomposite will lead to the formation of a regular stacking fault structure. The significant difference of a shock-induced microstructure makes the spall strength of the Al–Cu nanocomposite lower than that of ideal single crystal Al at these specific impact velocities. The analysis of the damage evolution process shows that when piston velocity up ≤ 2.0 km/s, due to the dense defects and high potential energy at the interface between inclusions and matrix, voids will nucleate preferentially at the inclusion interface, and then grow along the interface at a rate of five times faster than other voids in the Al matrix. When up ≥ 2.5 km/s, the Al matrix will shock melt or unloading melt, and micro-spallation occurs; Cu inclusions have no effect on spallation strength, but when Cu inclusions and the Al matrix are not fully diffused, the voids tend to grow and coalescence along the inclusion interface to form a large void.


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