Upload
kiveti
View
63
Download
2
Embed Size (px)
DESCRIPTION
Impedance matching
Citation preview
Advanced Impedance Matching - Dr. Ray Kwok
Advanced Impedance MatchingSo far….
• 2-elements tuning• Lumped Elements (L,C)
• Transmission Lines
• Stubs (single & double)• 1-port network
• single frequency
Now:
• are all tuning the same?
• wideband matching – multiple sections• multi-ports (simultaneously tuned)
Advanced Impedance Matching - Dr. Ray Kwok
Let’s compare our 2-element tuning examples over frequency…
• Lumped Elements (L,C)
• Transmission Lines
• Stubs (Single and Double)• Quarter-Wave transformer
Advanced Impedance Matching - Dr. Ray Kwok
LumpedElements
R=1G=1
If ZL is inside the G=1 circle,
first element cannot be shunt
ZL (0.4, 1)YL (0.34, -0.87)
Z (0.4, 0.48)Y (1, -1.24)
=0.4+j1ZL
jB = +j1.24 = jZoωC
jX = -j0.52 = -j/ωCZo
Z (0.4, -0.48)Y (1, 1.24)
=0.4+j1ZL
jB = -j1.24 = -jZo/ωL
jX = -j1.48 = -j/ωCZo
Z (1, 1.4)Y (0.34, -0.48)
jB = +j0.39 = jZoωC
=0.4+j1ZL
jX = -j1.4 = -j/ωCZo
Z (1, -1.4)Y (0.34, 0.48)
jB = +j1.35 = jZoωC
=0.4+j1ZL
jX = j1.4 = jωL/Zo
If ZL is inside the R=1 circle,
first element cannot be in series
Advanced Impedance Matching - Dr. Ray Kwok
Return Loss
0.01 0.11 0.21 0.31 0.41 0.5
Frequency (GHz)
Lump
-50
-40
-30
-20
-10
0
DB(|S[1,1]|)
Lump1
DB(|S[1,1]|)
Lump2
DB(|S[1,1]|)
Lump3
DB(|S[1,1]|)
Lump4
Advanced Impedance Matching - Dr. Ray Kwok
Using Stubs
ZL (0.4, 1)YL (0.34, -0.87)
Z (0.4, -0.48)Y (1, 1.24)
=0.4+j1ZL
short shunt stub
jB = -j1.24 = -jcotβl
open series stub
jX = -j1.48 = -jcotβl
Z (1, 1.4)Y (0.34, -0.48)
open shunt stub
jB = +j0.39 = jtanβl
=0.4+j1ZL
open series stub
jX = -j1.4 = -jcotβl
l
l
l
l
β=
β−=
β−=
β=
tanjYY
cotjYY
cotjZZ
tanjZZ
oop
osh
oop
osh
One way, simply replace lumped elements with stubs
Zo can be
anything here
previous example
Advanced Impedance Matching - Dr. Ray Kwok
Open – Short Stubs
0.01 0.11 0.21 0.31 0.41 0.5
Frequency (GHz)
Stubs
-50
-40
-30
-20
-10
0
DB(|S[1,1]|)
Stub1
DB(|S[1,1]|)
Stub2
Advanced Impedance Matching - Dr. Ray Kwok
ZL (0.4, 1)YL (0.34, -0.87)
=0.4+j1ZL
Transmission Line Matching
usually requires 1 more element
previous example
0.130λλλλ
0.185λλλλ
0.055λ
50 Ω
jX = -j1.85 = -j/ωCZo
=0.4+j1ZL
0.435λλλλ
0.305λ
50 Ω
Y (1, 1.9)
short shunt stub
jB = -j1.9 = -jcotβl
Z (1, 1.85)
Advanced Impedance Matching - Dr. Ray Kwok
Single Stub Tuningrefers to sliding a stub (any kind)
along a transmission line.
previous example
0.130λλλλ
0.064λλλλ
=0.4+j1ZL
0.435λλλλ
0.305λ
50 Ω
Y (1, 1.9)
short shunt stub
jB = -j1.9 = -jcotβl
In practice, usually shunt stubs,
short stub for waveguides,
open stub for microstrip.
=0.4+j1ZL
0.434λ
50 Ω
open shunt stub
jB = j1.9 = jtanβl
ZL (0.4, 1)YL (0.34, -0.87)
Y (1, -1.9)
Advanced Impedance Matching - Dr. Ray Kwok
Any Stubtanβl can be “+” or “-”
previous example
0.130λλλλ
0.064λλλλ
=0.4+j1ZL
0.435λλλλ
0.305λ
50 Ω
Y (1, 1.9)
open shunt stub
jB = - j1.9 = jtanβlβl = -1.086 + π = 2.055length = 0.327λ > λ/4
can use any type depends on realization.
e.g. use shunt open stub only…
=0.4+j1ZL
0.434λ
50 Ω
open shunt stub
jB = j1.9 = jtanβlβl = 1.086length = 0.173λ
ZL (0.4, 1)YL (0.34, -0.87)
Y (1, -1.9)
Advanced Impedance Matching - Dr. Ray Kwok
Transmission Line + Stub
0.01 0.11 0.21 0.31 0.41 0.5
Frequency (GHz)
xline_stub
-50
-40
-30
-20
-10
0
DB(|S[1,1]|)
single_stub1
DB(|S[1,1]|)single_stub2
DB(|S[1,1]|)
single_stub3
DB(|S[1,1]|)single_stub4
DB(|S[1,1]|)
single_stub5
Advanced Impedance Matching - Dr. Ray Kwok
Double Stub Tuninge.g. 2 shunt short stubs (50Ω)
separated by a 50Ω line of 0.2λ
0.3λλλλ
0.5λλλλ
– 0.2λλλλ
• rotate the 1-circle by line length
• adjust d1 along constant-G circle
• stop at the rotated blue-circle
• xline will bring it to the green circle
• adjust d2 along the green circle to Zo
• not for all ZL !! Forbidden zone.
d1d2
ZL
0.2λ
50 Ω =0.4+j1
ZL(0.4,1)
YL(0.34,-0.87)
Y (0.34,-0.2)
Y (1,1.22)
-cotβd1 = +0.67βd1 = -0.98 +π = 2.16
d1 = 0.344λ
-cotβd2 = −1.22βd2 = 0.687
d2 = 0.109λ
50 Ω50 Ω
Advanced Impedance Matching - Dr. Ray Kwok
e.g. Quarter-Wavee.g. shunt stub (100Ω) then λ/4
ZL = 20 + j 50 Ω
• move Z to the real axis
• normalized Zc = √Z = √3.1; Zc = 1.76
• Zc = 50(1.76) = 88 Ω
ZL(0.4,1)
YL(0.34, -0.87)
Z (3.1,0)
Y(0.34,0)
(1/100) tanβd= (0.87)(1/50)βd = 1.05
d = 0.167λ
d
ZL
λ/4
Zc =0.4+j150 Ω
100Ω
Advanced Impedance Matching - Dr. Ray Kwok
Double Stub / Quarter-wave
0.01 0.11 0.21 0.31 0.41 0.5
Frequency (GHz)
double_n_quarter
-30
-20
-10
0
DB(|S[1,1]|)
double_stub
DB(|S[1,1]|)
quarter_wave
Advanced Impedance Matching - Dr. Ray Kwok
Mixed matching samples
0.01 0.11 0.21 0.31 0.41 0.5
Frequency (G Hz)
Mixed
-40
-30
-20
-10
0
DB(|S[1,1]|)
double_s tub
DB(|S[1,1]|)
Lump1
DB(|S[1,1]|)
quarter_wave
DB(|S[1,1]|)
single_stub2
DB(|S[1,1]|)
Stub 1
Advanced Impedance Matching - Dr. Ray Kwok
2-port tuning
2 – port
network
MatchingNetwork ?
Especially useful for active component design : amplifier (transistor)or inserting devices into a system (such as SAW filter…)
for matched load
11in S=Γ
Advanced Impedance Matching - Dr. Ray Kwok
Unmatched load (from previous lecture)
2 – port
networkb1
b2
a1a2 = ΓLb2
ZL
This is what we measure.
How does that affect our matching process?L22
21L1211in
1
1
L22
121L121111
L22
1212
2L221212221212
2L121112121111
2
1
2221
1211
2
1
S1
SSS
a
b
S1
aSSaSb
S1
aSb
bSaSaSaSb
bSaSaSaSb
a
a
SS
SS
b
b
Γ−
Γ+=Γ≡
Γ−Γ+=
Γ−=⇒
Γ+=+=
Γ+=+=
=
Advanced Impedance Matching - Dr. Ray Kwok
To what we match? (from previous lecture)
( ) ( ) ( )22
g
2
g
2
g
2
g
g
2
g
ininlossLoad
gg
2
XR4
RV
2
1
X2R2
RV
2
1RI
2
1PP
+=
+=== −
( ) 2
g
2
go
o
2
g
o
2
total
g
oLineLoadXRZ
ZV
2
1Z
Z
V
2
1ZI
2
1PP
2
++====
Case 1: match ZL = Zo = real → ΓL = 0, VSWR = 1 on the line
Zin lZo ZL
Zg=Rg + jXgVg
Zin
Zg
Vg
Case 2: match Zin = Zg → Γin = 0, VSWR > 1
g
2
g
2
g
g
2
g
LoadR
V
8
1
R4
RV
2
1P ===
Case 3: match Zin = Z*g → Xin = -Xg
= max power available
conjugate matching
Ideally, match all Zo = Zg = ZL = real, then all 3 PLoad are the same = Pmax.
Advanced Impedance Matching - Dr. Ray Kwok
Conjugate Match
Zo
Output
matching
Input
matching
Device
to be
matched
Zo
Γin
Γout
ΓL
ΓS
L22
21L1211in
S1
SSS
Γ−
Γ+=Γ
S11
21S1222out
S1
SSS
Γ−
Γ+=Γ
*
inS Γ=Γwant *
outL Γ=Γand
Advanced Impedance Matching - Dr. Ray Kwok
Simultaneous Conjugate Match G. Gonzales: Microwave Transistor Amplifiers
21122211
*
11222
*
22111
22
11
2
222
22
22
2
111
2
2
2
2
22
L
1
2
1
2
11
S
SSSSS
SSC
SSC
SS1B
SS1B
C2
C4BB
C2
C4BB
−==∆
∆−=
∆−=
∆−−+=
∆−−+=
−±=Γ
−±=Γ
Advanced Impedance Matching - Dr. Ray Kwok
Example
0 1.0
1.0
-1.0
10.0
10.0
-10.0
5.0
5.0
-5.0
2.0
2.0
-2.0
3.0
3.0
-3.0
4.0
4.0
-4.0
0.2
0.2
-0.2
0.4
0.4
-0.4
0.6
0.6
-0.6
0.8
0.8
-0.8
S_ParametersSwp Max
6GHz
Swp Min
6GHz
S[1,1]
ex1_raw_spara
S[2,2]
ex1_raw_spara
Match this FET at 6 GHz
o
2
2
2
2
22
L
o
1
2
1
2
11
S
o*
11222
o*
22111
22
11
2
222
22
22
2
111
o
21122211
9.103718.0C2
C4BB
3.177762.0C2
C4BB
9.1033911.0SSC
3.1774786.0SSC
8255.0SS1B
9928.0SS1B
1103015.0SSSSS
∠=−−
=Γ
∠=−−
=Γ
−∠=∆−=
−∠=∆−=
=∆−−+=
=∆−−+=
∠=−==∆
( )
−∠∠
∠−∠=
oo
oo
7.95572.05.28058.2
3.16057.03.171641.0S
Non-reciprocal, non-symmetrical
0 1.0
1.0
-1.0
10.0
10.0
-10.0
5.0
5.0
-5.0
2.0
2.0
-2.0
3.0
3.0
-3.0
4.0
4.0
-4.0
0.2
0.2
-0.2
0.4
0.4
-0.4
0.6
0.6
-0.6
0.8
0.8
-0.8
simulate_conjugateSwp Max
6GHz
Swp Min
6GHz
S[1,1]
ex1_conjugate_s11
S[1,1]
ex1_conjugate_s22
ΓS & ΓL
S11 & S22
Advanced Impedance Matching - Dr. Ray Kwok
What does that mean?Zo
Output
matching
Input
matching
Device
to be
matched
Zo
Γin
Γout
ΓL
ΓS
NEED ΓΓΓΓin & ΓΓΓΓout for matching, which are just ΓΓΓΓ*S & ΓΓΓΓ*L
0 1.0
1.0
-1.0
10.0
10.0
-10.0
5.0
5.0
-5.0
2.0
2.0
-2.0
3.0
3.0
-3.0
4.0
4.0
-4.0
0.2
0.2
-0.2
0.4
0.4
-0.4
0.6
0.6
-0.6
0.8
0.8
-0.8
S_ParametersSwp Max
6GHz
Swp Min
6GHz
S[1,1]
ex1_raw_spara
S[2,2]
ex1_raw_spara
0 1.0
1.0
-1.0
10.0
10.0
-10.0
5.0
5.0
-5.0
2.0
2.0
-2.0
3.0
3.0
-3.0
4.0
4.0
-4.0
0.2
0.2
-0.2
0.4
0.4
-0.4
0.6
0.6
-0.6
0.8
0.8
-0.8
simulate_conjugateSwp Max
6GHz
Swp Min
6GHz
S[1,1]
ex1_conjugate_s11
S[1,1]
ex1_conjugate_s22
0 1.0
1.0
-1.0
10.0
10.0
-10.0
5.0
5.0
-5.0
2.0
2.0
-2.0
3.0
3.0
-3.0
4.0
4.0
-4.0
0.2
0.2
-0.2
0.4
0.4
-0.4
0.6
0.6
-0.6
0.8
0.8
-0.8
para_4matchSwp Max
6GHz
Swp Min
6GHz
S[1,1]
ex1_s11_4match
S[1,1]
ex1_s22_4match
S11 & S22ΓΓΓΓin & ΓΓΓΓout
ΓΓΓΓS & ΓΓΓΓL
Advanced Impedance Matching - Dr. Ray Kwok
Match 1-port at a timeIND
L=ID=
0.4827 nHL1
CAP
C=ID=
1.345 pFC1
1
SUBCKT
NET=ID=
"ex1_s11_4match" S2 PORT
Z=P=
50 Ohm1
CAP
C=ID=
0.899 pFC2
IND
L=ID=
1.572 nHL1
1
SUBCKT
NET=ID=
"ex1_s22_4match" S1
PORT
Z=P=
50 Ohm1
CAP
C=ID=
0.899 pFC2 CAP
C=ID=
1.345 pFC3
IND
L=ID=
0.4827 nHL1
IND
L=ID=
1.572 nHL2
1 2
SUBCKT
NET=ID=
"ex1_raw_spara" S1
PORT
Z=P=
50 Ohm1 PORT
Z=P=
50 Ohm2
Advanced Impedance Matching - Dr. Ray Kwok
Wide-Band Matching
Without using Resistor...
Use Multiple-sectionsGetting into Microwave Filter Design…….
Advanced Impedance Matching - Dr. Ray Kwok
0 0.1 0.2 0.3 0.4 0.5
Frequency (Hz)
2_poles
-50
-40
-30
-20
-10
0
DB(|S[1,1]|)
2_sections
LOAD
Z=ID=
1.355 OhmZ1
CAP
C=ID=
0.622 FC1
IND
L=ID=
0.843 HL1
PORT
Z=P=
1 Ohm1
0 1.0
1.0
-1.0
10.0
10.0
-10.0
5.0
5.0
-5.0
2.0
2.0
-2.0
3.0
3.0
-3.0
4.0
4.0
-4.0
0.2
0.2
-0.2
0.4
0.4
-0.4
0.6
0.6
-0.6
0.8
0.8
-0.8
SmithSwp Max
0.5Hz
Swp Min0.01Hz
S[1,1]
2_sections
Example: 1.355ΩΩΩΩ at 0.159Hz
Advanced Impedance Matching - Dr. Ray Kwok
6-sections: 1.355ΩΩΩΩ at 0.159Hz
CAP
C=ID=
0.8618 FC1
IND
L=ID=
1.903 HL1
LOAD
Z=ID=
1.355 OhmZ1
CAP
C=ID=
1.517 FC2
IND
L=ID=
2.056 HL2
CAP
C=ID=
1.404 FC3
IND
L=ID=
1.168 HL3
PORT
Z=P=
1 Ohm1
0 1.0
1.0
-1.0
10.0
10.0
-10.0
5.0
5.0
-5.0
2.0
2.0
-2.0
3.0
3.0
-3.0
4.0
4.0
-4.0
0.2
0.2
-0.2
0.4
0.4
-0.4
0.6
0.6
-0.6
0.8
0.8
-0.8
Smith_6Swp Max
0.5Hz
Swp Min0.01Hz
S[1,1]
6_sections
0.01 0.11 0.21 0.31 0.41 0.5
Frequency (Hz)
6_poles
-50
-40
-30
-20
-10
0
DB(|S[1,1]|)
6_sections
Loops around the center…
More frequency points can be matched
Many choices (combinations)
Choice of filter topologies.
Advanced Impedance Matching - Dr. Ray Kwok
Example: 1:2 quarter-wave
LOAD
Z=ID=
2 OhmZ1
TLIN
F0=EL=Z0=ID=
1 GHz90 Deg1.414 OhmTL1
PORT
Z=P=
1 Ohm1
1.0
1.0
-1.0
2.0
0.2
-0.2
0.4
-0.4
0.6
0.6
-0.6
0.8
0.8
-0.8
1.2
1.2
1.4
1.6
1.8
0.1
-0.1
0.3
-0.3
0.5
0.5
-0.5
0.7
0.7
-0.7
0.9
0.9
-0.9
N1
Swp Max
2GHz
Swp Min
0.1GHz
S[1,1]
1_section
0.1 0.6 1.1 1.6 2
Frequency (GHz)
N1_RL
-60
-40
-20
0
DB(|S[1,1]|)
1_section
Advanced Impedance Matching - Dr. Ray Kwok
2-sections 1:2 quarter-waveTLIN
F0=EL=Z0=ID=
1 GHz90 Deg1.64 OhmTL1
LOAD
Z=ID=
2 OhmZ1
TLIN
F0=EL=Z0=ID=
1 GHz90 Deg1.219 OhmTL2
PORT
Z=P=
1 Ohm1
1.0
1.0
2.0
0.2
-0.2
0.4
-0.4
0.6
0.6
-0.6
0.8
0.8
-0.8
1.2
1.2
1.4
1.6
1.8
0.1
-0.1
0.3
-0.3
0.5
0.5
-0.5
0.7
0.7
-0.7
0.9
0.9
-0.9
N2
Swp Max
2GHz
Swp Min
0.1GHz
S[1,1]
2_sections
0.1 0.6 1.1 1.6 2
Frequency (GHz)
N2_RL
-50
-40
-30
-20
-10
0
DB(|S[1,1]|)
2_sections
Again, many choices of
the intermediate Z’s
Advanced Impedance Matching - Dr. Ray Kwok
4-sections: 1:2 quarter-waveTLIN
F0=EL=Z0=ID=
1 GHz90 Deg1.785 OhmTL1
TLIN
F0=EL=Z0=ID=
1 GHz90 Deg1.541 OhmTL2
LOAD
Z=ID=
2 OhmZ1
TLIN
F0=EL=Z0=ID=
1 GHz90 Deg1.298 OhmTL3
TLIN
F0=EL=Z0=ID=
1 GHz90 Deg1.12 OhmTL4
PORT
Z=P=
1 Ohm1
1.0
1.0
2.0
0.2
-0.2
0.4
-0.4
0.6
0.6
-0.6
0.8
0.8
-0.8
1.2
1.2
1.4
1.6
1.8
0.1
-0.1
0.3
-0.3
0.5
0.5
-0.5
0.7
0.7
-0.7
0.9
0.9
-0.9
N4
Swp Max
2GHz
Swp Min
0.1GHz
S[1,1]
4_sections
0.1 0.6 1.1 1.6 2
Frequency (GHz)
N4_RL
-60
-50
-40
-30
-20
-10
0
DB(|S[1,1]|)
4_sections
Advanced Impedance Matching - Dr. Ray Kwok
Compare bandwidth
0.1 0.6 1.1 1.6 2
Frequency (GHz)
Return Loss
-60
-40
-20
0
DB(|S[1,1]|)
1_section
DB(|S[1,1]|)
2_sections
DB(|S[1,1]|)
4_sections