microwave 04 [相容模式] -...
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![Page 1: Microwave 04 [相容模式] - 國立中興大學web.nchu.edu.tw/~ycchiang/MicroWave/Microwave_04.pdf · 2013-09-24 · Fields and Waves in Communication E lectronics, Ramo et a ,](https://reader030.vdocuments.mx/reader030/viewer/2022040216/5f272fc07c57a42e4362facc/html5/thumbnails/1.jpg)
Waveguides
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General Solutions for TEM,Ge e a So ut o s o ,TE and TM Waves
Figure 3.1 (p. 92)(a) General two-conductor transmission line and (b) closed waveguide.
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General Solutions for TEM,Ge e a So ut o s o ,TE and TM Waves
ikhFi dB CA l2
0,equation sLaplace' from , Solve 1.
:line0),(TEMaanalyzingfor Procedure 2
yxyx
HE
t
zz
,,ˆ1, ,,, .3
,in constantsunknown theFind B.C.Apply .2
TEM
HEZyxez
Zyxhyxyxe
yx
xt
,,, ,,,, 2
TEM
eyxhzyxHeyxezyxE
HZzjzj
y
, , .5
, .4
0
121
CLIVZcv
ldHIldEV
rp
C
caseTE:0,equationHelmholtzfrom,Solve1
:s waveguide0)( TMor 0)( TE analyzingfor Procedure
222
yxhkyxh
HE zz
caseTM :0,equation Helmholtz from ,Solve
caseTE :0,
equation Helmholtz from ,Solve 1.
22
2
2
2
22
yxekyxe
yxhkyx
yxh
zcz
zcz
3
,
q, 22
yyx
y zcz
![Page 4: Microwave 04 [相容模式] - 國立中興大學web.nchu.edu.tw/~ycchiang/MicroWave/Microwave_04.pdf · 2013-09-24 · Fields and Waves in Communication E lectronics, Ramo et a ,](https://reader030.vdocuments.mx/reader030/viewer/2022040216/5f272fc07c57a42e4362facc/html5/thumbnails/4.jpg)
General Solutions for TEM,Ge e a So ut o s o ,TE and TM Waves
, , ,
,,,:case TE .2
HjEHjEHjHHjH
eyxhzyxH
zzzz
zjzz
,,,:case TM
, , ,
2222
eyxezyxE
xkE
ykE
ykH
xkH
zjzz
cy
cx
cy
cx
constantunknowntheFindB CApply3
,
,
, 2222
ky
EkjE
xE
kjE
xE
kjH
yE
kjH z
cy
z
cx
z
cy
z
cx
, , .4
constant unknown theFind B.C.Apply .3
TMTE22
kHEZk
HEZkk
k
y
x
y
xc
c
waves)TMor(TENp/mtanLoss Dielectric toDuen Attenuatio
2
kj
yy
waves)(TEM Np/m tan
waves)TMor (TE Np/m2
k
j
d
dd
4
)(p2d
![Page 5: Microwave 04 [相容模式] - 國立中興大學web.nchu.edu.tw/~ycchiang/MicroWave/Microwave_04.pdf · 2013-09-24 · Fields and Waves in Communication E lectronics, Ramo et a ,](https://reader030.vdocuments.mx/reader030/viewer/2022040216/5f272fc07c57a42e4362facc/html5/thumbnails/5.jpg)
Parallel Plate Waveguidea a e ate Wavegu de
Figure 3.2 (p. 98) Geometry ofFigure 3.2 (p. 98) Geometry of a parallel plate waveguide.
Figure 3.3 (p. 102) Bouncing plane wave interpretation of the TM1 parallel plate
id d
Figure 3.5 (p. 106) Field lines for the (a) TEM, (b) TM1, and (c) TE1 modes of a parallel plate waveguide. There is no variation across the width
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waveguide mode. of the waveguide.
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Rectangular Waveguideecta gu a Wavegu de
Figure 3.7 (p. 107)Geometry of a rectangular waveguide
Figure 3.6 (p. 107) Photograph of Ka-band (WR-28) rectangular waveguide components. Clockwise from top: a variable attenuator, and E-H (magic) tee junction, a directional coupler, an adaptor to ridge waveguide, an E-plane swept bend an adjustable short and a sliding matched load Courtesy of Agilent
Geometry of a rectangular waveguide.
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bend, an adjustable short, and a sliding matched load. Courtesy of Agilent Technologies, Santa Rosa, CA
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Rectangular Waveguideecta gu a Wavegu de
Figure 3.9 (p. 114) Field lines for some of the lower order modes of a rectangular waveguide. Reprinted from ld d l l © il )
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Fields and Waves in Communication Electronics, Ramo et al, © Wiley, 1965)
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Circular WaveguideC cu a Wavegu de
Figure 3.11 (p. 117)f i l idGeometry of a circular waveguide.
Figure 3.14 (p. 125) Field lines for some of the lower order modes of a circular waveguide.i d f ld d l l © il )
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Reprinted from Fields and Waves in Communication Electronics, Ramo et al, © Wiley, 1965)
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Coaxial LineCoa a e
0,1,1
ModesTEM2
bVa 0, ,,
0,,
0
22
ab
bVlnln, 0
e
abVzE jkz ˆ
ln,, 0
e
abVzH jkz
ˆ
ln,, 0
Figure 3.15 (p. 126)Coaxial line geometry.
k
ababZ
r
,ln602ln 0
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Coaxial LineCoa a e
bkff cc
2 1
ModesOrder Hihger
max
baba
ff ccmax
Figure 3.17 (p. 129) Field lines for the
Figure 3.16 (p. 129) Normalized cutoff frequency of
Figure 3.17 (p. 129) Field lines for the (a) TEM and (b) TE11 modes of a coaxial line.
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g (p ) q ythe dominant TE11 waveguide mode for a coaxial line.
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Coaxial Line (optional)Coa a e (opt o a )
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Coaxial LineCoa a e
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Coaxial LineCoa a eFigure coaxial connectors
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StriplineSt p e
Figure 3.22 (p. 137)Stripline transmission line. (a) Geometry. (b) Electric and magnetic field lines.
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Stripline transmission line. (a) Geometry. (b) Electric and magnetic field lines.
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Stripline (Analysis Formula)St p e ( a ys s o u a)
441.030
0
bWbZ
er
0 35for0
of width effective the:
WWWe
0.35for 3.0
0.35for 02
bW
bW
bb
Wb
We
0 isconductor of thickness
t
bb
0forFormula t
2768841ln30 2tbtbtbZ0for Formula t
27.61ln0 wwwZ
r
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Stripline (Synthesis Formula)St p e (Sy t es s o u a)
120for 6.085.0120for
0
0
ZεxZεx
bW
r
r
tan3.27tan
:nAttenuatio Loss Dielectric
k r
441.030 where0
0
Zεx
r
r
2 0d
107.2
:nAttenuatioConductor
03
0
ZR
r
mode)order high lewest theis (TE modeorder higher for Cutoff
120for16.0
120for 30
107.20
0
ZεBR
ZεAtb
ZR
s
rrs
c
GHz)(in 4//
115bwb
fr
c
120for 00
ZεBbZ r
tb
btb
bWA ,2ln121with
cmin and bw
tW
Wt
tWbB
ttbtb
4ln
21414.05.0
70501
16
tWtW 27.05.0
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Stripline (Graphic Analysis)St p e (G ap c a ys s)
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Microtrip Linec ot p e
If:supported mode TEM No
d mode TEM-quasi
cv
eff0
eff
p
k
v
01
pCvC
LZ
Figure 3.25 (p. 143) Microstrip transmission line. (a) Geometry. (b) Electric and magnetic field lines.
eff
0g
p
2
eff
eff
vc
CC
18
air
pvC
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Microtrip Linec ot p e
• Advantages1. Low cost, small size2. Absence of critical matching & cutoff freq.3. Easy integrated with active device4 Good repeatability and reproducibility mass production4. Good repeatability and reproducibility, mass production5. Compatibility with monolithic circuits
• Disadvantages ( cf waveguide, coaxial circuits)1. Higher loss2 Lower power handling capability2. Lower power handling capability3. Greater temperature instability
• The synthesis & analysis formula are well documented• Many discontinuities have been characterized• Commercial programs are available for optimization & prediction
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Commercial programs are available for optimization & prediction
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Microtrip Linec ot p e
r rr r
r eff 121
eff r2
rr eff121
ff 2
: factor filling q
eff
r
11111eff
q
qqq rr
121
r12
q
dW /
2
20
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Microtrip Linec ot p e
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Microtrip Line (Analysis Formula)c ot p e ( a ys s o u a)
:1For
2
dW
104.01211
21
21
2
eff dW
Wdrr
48ln60
eff0 d
WWdZ
111
:1For dW
1201211
21
21 eff Wd
rr
444.1ln667.0393.1
120
eff
0
dW
dW
Z
22
dd
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Microtrip Line (Synthesis Formula)c ot p e (Sy t es s o u a)
A
A
dW
ee
W2 2for
28
r WBBB
de
dW
2for61.03901ln112ln12
2
rr
rr
ZA
dBBB
0 11.023011where
2for 39.01ln2
12ln1
rr
rr
B
A
0
377
23.01260
where
rZB
02
:nAttenuatio LossDielectric :factorFilling :nAttenuatioConductor
Np/m 12
tan1
eff
eff0
r
rd
k
1
1g
eff
eff
r
r
Np/m
0WZRs
c
23
eff r e 0
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Microtrip Line p(Further Considerations)
• Finite Conductor Thickness Effect of Dispersion
2
0
Wt
Wfd
Ff r
2
eff5.1eff
eff
14
041
0
rW d
f
dW
cfd
F r 1ln215.014
dW
tW
dt
dW
W 21 4ln1
25.1
f
fZfZeff
eff
eff
eff00
01010
dW
td
dt
dWd
212ln1
25.1
dWdtr /
6.41
effeff
24
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Other types of LinesOt e types o es
Figure 3.33 (p. 156)Geometry of a printed slotline.
Figure 3.35 (p. 157)Covered microstrip line.
1 Easy fabrication1. Easy fabrication2. quasi-TEM operation3. radiation problem gap width ~/2
Figure 3.34 (p. 156)Coplanar waveguide geometry.
3. radiation problem gap width /24. monolithic application5. surface wave mode coupling
25
p g