Chapter 7: Plane-Wave Propagation
[Pages:33]317
Chapter 7: Plane-Wave Propagation
Lesson #43
Chapter -- Section: 7-1 Topics: Time-harmonic fields
Highlights: ? Phasors ? Complex permittivity ? Wave equations
Special Illustrations:
318
Lesson #44
Chapter -- Section: 7-2 Topics: Waves in lossless media
Highlights: ? Uniform plane waves ? Intrinsic impedance ? Wave properties
Special Illustrations: ? Example 7-1 ? CD-ROM Modules 7.3 and 7.4
319
Lesson #45 and 46
Chapter -- Section: 7-3 Topics: Wave polarization
Highlights: ? Definition of polarization ? Linear, circular, elliptical
Special Illustrations: ? CD-ROM Demos 7.1-7.5 ? Liquid Crystal Display
Liquid Crystal Display (LCD)
LCDs are used in digital clocks, cellular phones, desktop and laptop computers, and some televisions and other electronic systems. They offer a decided advantage over other display technologies, such as cathode ray tubes, in that they are much lighter and thinner and consume a lot less power to operate. LCD technology relies on special electrical and optical properties of a class of materials known as liquid crystals, first discovered in the 1880s by botanist Friedrich Reinitzer.
Physical Principle
Liquid crystals are neither a pure solid nor a pure liquid, but rather a hybrid of both. One particular variety of interest is the twisted nematic liquid crystal whose molecules have a natural tendency to assume a twisted spiral structure when the material is sandwiched between finely grooved glass substrates with orthogonal orientations (A). Note that the molecules in contact with the grooved surfaces align themselves in parallel along the grooves. The molecular spiral causes the crystal to behave like a wave polarizer; unpolarized light incident upon the entrance substrate follows the orientation of the spiral, emerging through the exit substrate with its polarization (direction of electric field) parallel to the groove's direction.
320
Lesson #47
Chapter -- Section: 7-4 Topics: Waves in lossy media
Highlights: ? Attenuation and skin depth ? Low loss medium ? Good conductor
Special Illustrations: ? CD-ROM Demos 7.6-7.8
321
Lesson #48
Chapter -- Section: 7-5 Topics: Current flow in conductors
Highlights: ? Skin depth dependence on frequency ? Surface impedance
Special Illustrations:
322
Lesson #49
Chapter -- Section: 7-6 Topics: EM power density
Highlights: ? Power density in a lossless medium ? Power density in a lossy medium ? Time-average power
Special Illustrations: ? CD-ROM Module 7.5
CHAPTER 7
323
Chapter 7
Section 7-2: Propagation in Lossless Media
Problem 7.1 The magnetic field of a wave propagating through a certain nonmagnetic material is given by
H ? z^ 30 cos 108t ? 0 5y? (mA/m)
Find (a) the direction of wave propagation, (b) the phase velocity, (c) the wavelength in the material, (d) the relative permittivity of the material, and (e) the electric field phasor.
Solution:
(a) Positive y-direction.
(b) ? 108 rad/s, k ? 0 5 rad/m.
up ?
?
k
108
0 5
?
2 108 m/s
(c) ? (d) r ?
2? k ?
c up
2
2
?
?0 5
3
?
2
12 6 m.
108 108
2
?
2 25.
(e) From Eq. (7.39b),
E ? ? k^ H?
?
?
? ?
?
120 ?
r
120
1 5
?
251 33
()?
k^ ? y^ ?
and
H?
z^30e
j0 5y ?
10 3
(A/m)
Hence, and
E?
?
251 33y^
z^30e
j0 5y ?
10 3 ?
?
x^7 54e
j0 5y ?
(V/m)?
??? E y? t???
Ee jt ??? ? x^7 54 cos 108t ? 0 5y? (V/m)
Problem 7.2 Write general expressions for the electric and magnetic fields of a
1-GHz sinusoidal plane wave traveling
medium with relative permittivity r ?
in9.theTh? ey-edleircetcritciofineilndaislopsoslleasrsizneodnamloanggnetthice
x-direction, its peak value is 6 V/m and its intensity is 4 V/m at t ? 0 and y ? 2 cm.
324
CHAPTER 7
Solution: For f ? 1 GHz, ?r ? 1, and r ? 9,
? 2 f ? 2 109 rad/s?
k? E y? t???
? ? ? 2
?
2 0
r ?
2 f c
r ?
2 109 3 108
9?
x^6 cos 2 109t ? 20y ? 0? (V/m)
20 rad/m?
At t ? 0 and y ? 2 cm, E ? 4 V/m:
Hence,
4?
6cos ? 20
2
10
2
?
0 ???
6cos ? 0 4 ?
0?
?
0 ?
0 4 ?
cos 1
4 6
?
0 84 rad ?
which gives
0 ? 2 1 rad ? 120 19?
and
E y? t ??? x^ 6cos 2 109t ? 20y ? 120 19? ? (V/m)
Problem 7.3 The electric field phasor of a uniform plane wave is given by
E?
y^
10e
j0 ?
2z
(V/m).
If
the
phase
velocity
of
the
wave
is
1
5
108 m/s and the relative
permeability of the medium is ?r ? 2 4, find (a) the wavelength, (b) the frequency f
of the wave, (c) the relative permittivity of the medium, and (d) the magnetic field
H z? t? .
Solution:
(a) From E ? y^10e j0? 2z (V/m), we deduce that k ? 0 2 rad/m. Hence,
?
2 ?
k
2
0 2
?
10 ?
31 42 m
(b)
f?
up
?
1 5 108 31 42
?
4 77 106 Hz ?
4 77 MHz
(c) From
? up ?
c ?rr
?
r ?
?
1 ?r
c up
2
?
?
1
2 4
3
1 5
2
?
1 67
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