General Integral Formulation of the Diffraction of an Electromagnetic Wave by an Infinitely Conducting, Biaxial Periodic Surface

1979 ◽  
Vol 26 (6) ◽  
pp. 801-808 ◽  
Author(s):  
A. Wirgin
Keyword(s):  
Electromagnetic Wave ◽  
Integral Formulation ◽  
Periodic Surface ◽  
General Integral

A General Integral Formulation for Rotational Flows in Aerodynamics

1991 ◽  
pp. 85-94 ◽  
Author(s):  
P. Bassanini ◽  
M. R. Lancia ◽  
R. Piva ◽  
C. M. Casciola
Keyword(s):  
Integral Formulation ◽  
General Integral ◽  
Rotational Flows

scholarly journals General Integral Formulation for the 3D Thin Shell Modeling

2013 ◽  
Vol 49 (5) ◽  
pp. 1989-1992 ◽  
Author(s):  
Tung Le-Duc ◽  
Gerard Meunier ◽  
Olivier Chadebec ◽  
Jean-Michel Guichon ◽  
Joao Pedro A. Bastos
Keyword(s):  
Thin Shell ◽  
Integral Formulation ◽  
General Integral

scholarly journals General Integral Formulation of Magnetic Flux Computation and Its Application to Inductive Power Transfer System

2017 ◽  
Vol 53 (6) ◽  
pp. 1-4 ◽  
Author(s):  
Limin Huang ◽  
Gerard Meunier ◽  
Olivier Chadebec ◽  
Jean-Michel Guichon ◽  
Yanling Li ◽  
...  
Keyword(s):  
Magnetic Flux ◽  
Integral Formulation ◽  
Transfer System ◽  
Power Transfer ◽  
Inductive Power Transfer ◽  
General Integral ◽  
Inductive Power

A Stationary Solution of High-Energy Electron Reflection (HEER) for An Arbitrary Surface

1990 ◽  
Vol 48 (2) ◽  
pp. 374-375
Author(s):  
YIQUN MA
Keyword(s):  
Stationary Solution ◽  
High Energy ◽  
Bloch Wave ◽  
Dynamical Theory ◽  
High Energy Electron ◽  
Bulk Materials ◽  
Periodic Surface ◽  
Electron Transmission ◽  
Electron Reflection ◽  
Long Time

For a long time, the development of dynamical theory for HEER has been stagnated for several reasons. Although the Bloch wave method is powerful for the understanding of physical insights of electron diffraction, particularly electron transmission diffraction, it is not readily available for the simulation of various surface imperfection in electron reflection diffraction since it is basically a method for bulk materials and perfect surface. When the multislice method due to Cowley & Moodie is used for electron reflection, the “edge effects” stand firmly in the way of reaching a stationary solution for HEER. The multislice method due to Maksym & Beeby is valid only for an 2-D periodic surface.Now, a method for solving stationary solution of HEER for an arbitrary surface is available, which is called the Edge Patching method in Multislice-Only mode (the EPMO method). The analytical basis for this method can be attributed to two important characters of HEER: 1) 2-D dependence of the wave fields and 2) the Picard iteractionlike character of multislice calculation due to Cowley and Moodie in the Bragg case.

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