Classical Electrodynamics |
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Page 258
This expression for Q has an intuitive physical interpretation when written in the
form : e = ” ) ( Geometrical factor ) ( 8 . 92 ) * u . 158 ) ^ where V is the volume of
the cavity , and Sits total surface area . The Q of a cavity is evidently , apart from a
...
This expression for Q has an intuitive physical interpretation when written in the
form : e = ” ) ( Geometrical factor ) ( 8 . 92 ) * u . 158 ) ^ where V is the volume of
the cavity , and Sits total surface area . The Q of a cavity is evidently , apart from a
...
Page 559
Apart from factors of the order of unity , the transition probability for magnetic
multipoles is , according to ( 16 . 102 ) , I għ 2 1 ( 16 . 105 ) TM ( 1 ) \ mcal Te ( 1 )
The presence of the factor ( ka ) 22 in the transition probability ( 16 . 104 ) means
...
Apart from factors of the order of unity , the transition probability for magnetic
multipoles is , according to ( 16 . 102 ) , I għ 2 1 ( 16 . 105 ) TM ( 1 ) \ mcal Te ( 1 )
The presence of the factor ( ka ) 22 in the transition probability ( 16 . 104 ) means
...
Page 606
We see that near the resonant frequency w , the absorption cross section has the
same Lorentz shape as the scattering cross section , but is larger by a factor T / .
At high frequencies I ' , → wot , so that the absorption cross section approaches ...
We see that near the resonant frequency w , the absorption cross section has the
same Lorentz shape as the scattering cross section , but is larger by a factor T / .
At high frequencies I ' , → wot , so that the absorption cross section approaches ...
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Contents
Introduction to Electrostatics | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
RelativisticParticle Kinematics and Dynamics | 391 |
Copyright | |
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