v.Ẽ = 0, (7.6a) V xẾ = - jøµÃ, V.à = 0, (7.6b) (7.6c) V xà = jwe,Ẽ. (7.6d) CHAPTER 7 PLANE-WAVE PROPAGAT n view of Eq. (7.6a), the use of Eq. (7.11) in Eq. (7.10) g v³Ẽ + w³µe‚Ẽ = 0,

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start from maxwell equations.(7.6a) (7.6b) (7.6c)
(7.6d) to derive equation(7.13) in differential form
v.Ẽ = 0,
(7.6a)
%3D
V × Ẽ = - jøµñ,
(7.6b)
%3D
V.Ã = 0,
(7.6c)
%3D
V × Ã = jwe̟Ẽ.
(7.6d)
%3D
CHAPTER 7 PLANE-WAVE PROPAGATION
In view of Eq. (7.6a), the use of Eq. (7.11) in Eq. (7.10) gives
v³Ẽ +w³µe‚Ẽ = 0,
(7.13
which is known as the homogeneous wave equation for E. B.
defining the propagation constant y as
Transcribed Image Text:start from maxwell equations.(7.6a) (7.6b) (7.6c) (7.6d) to derive equation(7.13) in differential form v.Ẽ = 0, (7.6a) %3D V × Ẽ = - jøµñ, (7.6b) %3D V.à = 0, (7.6c) %3D V × Ã = jwe̟Ẽ. (7.6d) %3D CHAPTER 7 PLANE-WAVE PROPAGATION In view of Eq. (7.6a), the use of Eq. (7.11) in Eq. (7.10) gives v³Ẽ +w³µe‚Ẽ = 0, (7.13 which is known as the homogeneous wave equation for E. B. defining the propagation constant y as
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