start from maxwell equations.(7.6a) (7.6b) (7.6c) (7.6d) to derive equation(7.13) in differential form V.Ế = 0, (7.6a) V xẼ = - jwµĤ, (7.6b) v.Ñ = 0, (7.6c) V x à = jwe,Ẽ. (7.6d) CHAPTER 7 PLANE-WAVE PROPAGATION In view of Eq. (7.6a), the use of Eq. (7.11) in Eq. (7.10) gives v²Ẽ +o³µe‚Ẽ = 0, (7.13 which is known as the homogeneous wave equation for E. Bị defining the propagation constant y as
start from maxwell equations.(7.6a) (7.6b) (7.6c) (7.6d) to derive equation(7.13) in differential form V.Ế = 0, (7.6a) V xẼ = - jwµĤ, (7.6b) v.Ñ = 0, (7.6c) V x à = jwe,Ẽ. (7.6d) CHAPTER 7 PLANE-WAVE PROPAGATION In view of Eq. (7.6a), the use of Eq. (7.11) in Eq. (7.10) gives v²Ẽ +o³µe‚Ẽ = 0, (7.13 which is known as the homogeneous wave equation for E. Bị defining the propagation constant y as
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Transcribed Image Text:start from maxwell equations.(7.6a) (7.6b) (7.6c)
(7.6d) to derive equation(7.13) in differential form
v.Ế = 0,
V × Ẽ = - jwµñ,
(7.6a)
%3D
(7.6b)
%3D
V.Ã = 0,
(7.6c)
V × Ĥ = jwe̟Ẽ.
(7.6d)
CHAPTER 7 PLANE-WAVE PROPAGATION
In view of Eq. (7.6a), the use of Eq. (7.11) in Eq. (7.10) gives
v³Ẽ +w³µ€‚Ẽ = 0,
(7.13
which is known as the homogeneous wave equation for E. BỊ
defining the propagation constant y as
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