Unit cell block including dielectric cube wrapped with metallic wire mesh for 3-D isotropic CRLH metamaterials

Author(s):  
Takumi Ishiyama ◽  
Tetsuya Ueda ◽  
Yoshiaki Sato ◽  
Tatsuo Itoh
Keyword(s):  
2007 ◽  
Vol 76 (24) ◽  
Author(s):  
J. Bravo-Abad ◽  
L. Martín-Moreno ◽  
F. J. García-Vidal ◽  
E. Hendry ◽  
J. Gómez Rivas

1986 ◽  
Vol 108 (3) ◽  
pp. 446-449 ◽  
Author(s):  
G. A. Karim ◽  
M. G. Kibrya

The combustion of a homogeneous lean methane-air stream was investigated in a vertical, cylindrical combustor of 150 mm diameter in the presence of a metallic wire mesh. Eight metallic materials were deposited in turn onto a stainless steel wire mesh by electroplating. The potential improvement in the lean blowout limit due to catalytic effects was established separately from those due to the thermal and aerodynamic contributions of the wire mesh and its holder ring. The effectiveness of the various metallic surfaces tested in the lean combustion of methane was in the following descending order: Pt → Cu → Ag → brass → Cr → Cd → Ni → stainless steel. Moreover, it was confirmed that hydrogen was more sensitive to catalytic effects extending to relatively lower temperatures than methane.


2022 ◽  
Vol 170 ◽  
pp. 108599
Author(s):  
Xin Xue ◽  
Yuhan Wei ◽  
Fang Wu ◽  
Hongbai Bai ◽  
Chunhong Lu ◽  
...  

2013 ◽  
Vol 57 (2) ◽  
pp. 690-697 ◽  
Author(s):  
Zenghui Zhao ◽  
Yoav Peles ◽  
Michael K. Jensen
Keyword(s):  

2007 ◽  
Vol 253 (6) ◽  
pp. 3303-3310 ◽  
Author(s):  
Hong Sun ◽  
Xie Quan ◽  
Shuo Chen ◽  
Huimin Zhao ◽  
Yazhi Zhao

Author(s):  
Peter G. Self ◽  
Peter R. Buseck

ALCHEMI (Atom Location by CHanneling Enhanced Microanalysis) enables the site occupancy of atoms in single crystals to be determined. In this article the fundamentals of the method for both EDS and EELS will be discussed. Unlike HRTEM, ALCHEMI does not place stringent resolution requirements on the microscope and, because EDS clearly distinguishes between elements of similar atomic number, it can offer some advantages over HRTEM. It does however, place certain constraints on the crystal. These constraints are: a) the sites of interest must lie on alternate crystallographic planes, b) the projected charge density on the alternate planes must be significantly different, and c) there must be at least one atomic species that lies solely on one of the planes.An electron beam incident on a crystal undergoes elastic scattering; in reciprocal space this is seen as a diffraction pattern and in real space this is a modulation of the electron current across the unit cell. When diffraction is strong (i.e., when the crystal is oriented near to the Bragg angle of a low-order reflection) the electron current at one point in the unit cell will differ significantly from that at another point.


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