Engineering ElectromagneticsThe Uniform Plane Wave Nguy ễ n Công Ph ươ ng... Wave Propagation in Free Space 2.. Wave Propagation in Free Space 2... Wave Propagation in Free Space 3... Wa
Trang 1Engineering Electromagnetics
The Uniform Plane Wave
Nguy ễ n Công Ph ươ ng
Trang 2I Introduction
II Vector Analysis
III Coulomb’s Law & Electric Field Intensity
IV Electric Flux Density, Gauss’ Law & Divergence
V Energy & Potential
VI Current & Conductors
VII Dielectrics & Capacitance
VIII Poisson’s & Laplace’s Equations
IX The Steady Magnetic Field
X Magnetic Forces & Inductance
XI Time – Varying Fields & Maxwell’s Equations
XII The Uniform Plane Wave
XIII Transmission Lines
XIV Plane Wave Reflection & Dispersion
XV Guided Waves & Radiation
Trang 3The Uniform Plane Wave
1 Wave Propagation in Free Space
2 Wave Propagation in Dielectrics
3 The Poynting Vector
4 Skin Effect
5 Wave Polarization
Trang 4Wave Propagation in Free Space (1)
0
∇ .H =
0
∇ = .E
Trang 5Wave Propagation in Free Space (2)
Trang 6Wave Propagation in Free Space (3)
Trang 7Wave Propagation in Free Space (3)
Trang 8Wave Propagation in Free Space (4)
Trang 9Wave Propagation in Free Space (5)
xs
xs
d E
k E dz
Trang 10Wave Propagation in Free Space (6)
Trang 11Wave Propagation in Free Space (7)
0 0
x y
E H
µ ε
Trang 12The Uniform Plane Wave
1 Wave Propagation in Free Space
2 Wave Propagation in Dielectrics
3 The Poynting Vector
4 Skin Effect
5 Wave Polarization
Trang 13Wave Propagation in Dielectrics (1)
Trang 14Wave Propagation in Dielectrics (2)
1/ 2 2
Trang 15Wave Propagation in Dielectrics (3)
1/ 2 2
Trang 16Wave Propagation in Dielectrics (4)
0 0
x y
Trang 17Wave Propagation in Dielectrics (5)
Find the attenuation of a 2.5 GHz wave propagating in fresh water,
given ε’r = 78, ε’’r = 7, μr = 1.
Ex.
1/ 2 2
9 8
Trang 18Wave Propagation in Dielectrics (6)
Trang 19Wave Propagation in Dielectrics (7)
1/ 2 2
Trang 20Wave Propagation in Dielectrics (8)
1
ε ε
Trang 21Wave Propagation in Dielectrics (9)
Trang 22The Uniform Plane Wave
1 Wave Propagation in Free Space
2 Wave Propagation in Dielectrics
3 The Poynting Vector
4 Skin Effect
5 Wave Polarization
Trang 23The Poynting Vector (1)
Trang 24The Poynting Vector (2)
Trang 25The Poynting Vector (3)
1
[1 cos(2 )] 2
T x
Trang 26The Poynting Vector (4)
[cos(2 2 2 ) cos ] 2
z x
,
1
cos 2
z x
Trang 27The Uniform Plane Wave
1 Wave Propagation in Free Space
2 Wave Propagation in Dielectrics
3 The Poynting Vector
4 Skin Effect
5 Wave Polarization
Trang 29Skin Effect (2)
Dielectrics
Conductor 0
Trang 32H = η
Trang 33z x
S = E × H
2
2 / 0
2 2 / 0
1
cos
1 4
z x
av
z x
E
E e
δ δ
Trang 34Skin Effect (7)
/ / 0
(1 ) / 0
z jz
xs x
j z x
Conductor
Trang 35Skin Effect (8)
2
2
2 0
1 ( )
Conductor
Trang 37The Uniform Plane Wave
1 Wave Propagation in Free Space
2 Wave Propagation in Dielectrics
3 The Poynting Vector
4 Skin Effect
5 Wave Polarization
Trang 38Wave Polarization (1)
• In the previous sections, E & H are supposed to lie in
fix directions
• However, the directions of E & H within the plane
perpendicular to a z may change as functions of time and position
• λ, v p , S, …
• The instantaneous orientation of field vectors
• Wave polarization: its electric field vector orientation as
a function of time, at a fixed point in space
• H can be found from E
Trang 40Wave travel Observer
location