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Page 296
The power radiated per unit solid angle in the scalar Kirchhoff approximation is dp ( ka ) cos a + cos 0 2J ( kaş ) CP ( 9.112 ) dΩ 40T 2 cos a ka 2 i COS O. 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 dp ( ka ) cos a + cos 0 2J ( kaş ) CP ( 9.112 ) dΩ 40T 2 cos a ka 2 i COS O. 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 ) ? ... The solid ( dotted ) curve gives the vector ( scalar ) approximation in each case . We see that for ka = 7 there is a considerable disagreement ...
Then both scalar and vector approximations reduce to the common expression , dp ( ka ) ? ... The solid ( dotted ) curve gives the vector ( scalar ) approximation in each case . We see that for ka = 7 there is a considerable disagreement ...
Page 628
... 308 by sphere in short wavelength limit , 299 comparison of scalar and vector approximations , 296 Fresnel and Fraunhofer , 292 Kirchhoff approximation in , 282 scalar Huygens - Kirchhoff theory of , 280 Smythe's vector theorem for ...
... 308 by sphere in short wavelength limit , 299 comparison of scalar and vector approximations , 296 Fresnel and Fraunhofer , 292 Kirchhoff approximation in , 282 scalar Huygens - Kirchhoff theory of , 280 Smythe's vector theorem for ...
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Contents
Introduction to Electrostatics | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
TimeVarying Fields Maxwells Equations Con | 169 |
Copyright | |
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