The Electrostatic Field About a Thin Oblate Dielectric Body of Revolution

1992 ◽  
Vol 52 (3) ◽  
pp. 651-675 ◽  
Author(s):  
Richard Barshinger
Keyword(s):  
Electrostatic Field ◽  
Body Of Revolution ◽  
Dielectric Body

Nystrom method for the Muller boundary integral equations on a dielectric body of revolution: axially symmetric problem

2015 ◽  
Vol 9 (11) ◽  
pp. 1186-1192 ◽  
Author(s):  
Vitaliy S. Bulygin ◽  
Yuriy V. Gandel ◽  
Ana Vukovic ◽  
Trevor M. Benson ◽  
Phillip Sewell ◽  
...  
Keyword(s):  
Integral Equations ◽  
Boundary Integral Equations ◽  
Boundary Integral ◽  
Body Of Revolution ◽  
Symmetric Problem ◽  
Axially Symmetric ◽  
Dielectric Body ◽  
Nyström Method ◽  
Nystrom Method

The Electrostatic Field Around a Slender Conducting Body of Revolution

1967 ◽  
Vol 15 (4) ◽  
pp. 824-841 ◽  
Author(s):  
Richard A. Handelsman ◽  
Joseph B. Keller
Keyword(s):  
Electrostatic Field ◽  
Body Of Revolution ◽  
Conducting Body

The Electrostatic Field about a Slender Dielectric Body

1987 ◽  
Vol 47 (3) ◽  
pp. 605-623 ◽  
Author(s):  
Richard Barshinger ◽  
James Geer
Keyword(s):  
Electrostatic Field ◽  
Dielectric Body

scholarly journals Решение задачи дифракции на теле вращения, расположенном в диэлектрическом слое

2019 ◽  
Vol 127 (12) ◽  
pp. 942
Author(s):  
С.А. Маненков
Keyword(s):  
Circular Cylinder ◽  
Plane Wave ◽  
Dielectric Layer ◽  
Layered Medium ◽  
Body Of Revolution ◽  
Dielectric Body ◽  
Material Characteristics ◽  
Homogeneous Spheroid

Two methods for solving the problem of diffraction of the plane wave by the dielectric body of revolution located in the homogeneous dielectric layer are proposed. Two methods are compared using the example of the scattering of the plane wave by the homogeneous spheroid and the circular cylinder of finite dimensions located in the layer. The results of calculating the pattern for the case of diffraction by the finite circular cylinder which is immersed in the layer and has variable material characteristics are presented. The wavelength dependences of the pattern for plasmon particles located in the layered medium are obtained.

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