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Page 296
The power radiated per unit solid angle in the scalar Kirchhoff approximation is 2 Cosa + cos 0 dP ( ka ) - Pi COS O. dΩ 477 2J ( kaş ) kaξ ( 9.112 ) 2 cos a where P , is given by ( 9.104 ) . If we compare the vector Kirchhoff result ...
The power radiated per unit solid angle in the scalar Kirchhoff approximation is 2 Cosa + cos 0 dP ( ka ) - Pi COS O. dΩ 477 2J ( kaş ) kaξ ( 9.112 ) 2 cos a where P , is given by ( 9.104 ) . If we compare the vector Kirchhoff result ...
Page 297
Then both scalar and vector approximations reduce to the common expression , dp ( ka ) | J ( ka sin 0 ) 2 ( 9.113 ) d12 ka sin 0 The vector and ... The solid ( dotted ) curve gives the vector ( scalar ) approximation in each case .
Then both scalar and vector approximations reduce to the common expression , dp ( ka ) | J ( ka sin 0 ) 2 ( 9.113 ) d12 ka sin 0 The vector and ... The solid ( dotted ) curve gives the vector ( scalar ) approximation in each case .
Page 307
( 6 ) Compare your result in part ( a ) with the standard scalar Kirchhoff approximation and with the result in Section 9.8 for the polarization vector in the plane of incidence . 9.8 A rectangular opening with sides of length a and b ...
( 6 ) Compare your result in part ( a ) with the standard scalar Kirchhoff approximation and with the result in Section 9.8 for the polarization vector in the plane of incidence . 9.8 A rectangular opening with sides of length a and b ...
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Contents
Introduction to Electrostatics | 1 |
References and suggested reading | 23 |
Multipoles Electrostatics of Macroscopic Media | 98 |
Copyright | |
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