A Planar Reconfigurable Yagi-Uda Antenna With End-fire Beam Scan
The Yagi-Uda Antenna - WordPress.com · 2020. 12. 16. · •The Yagi Array: –an be designed...
Transcript of The Yagi-Uda Antenna - WordPress.com · 2020. 12. 16. · •The Yagi Array: –an be designed...
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Part 2
Presenter-Tom Kihm, KJ6PST
12/15/2020 1
The Yagi-Uda Antenna
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Part 2 Agenda
• Empirical design NBS TN
• Computer-aided design examples
• Mutual coupling effects on input impedance
• Matching approaches
• Conclusions
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Yagi Antenna Design
• Historically Empirical Design
– Uda’s Original Research
– National Bureau of Standards (NBS) Technical Note
• Recently, Computer-aided designs
– Method of Moments
– Induced EMF method
– Plus others
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Several on-line calculators use NBS rules of thumb for
reflector, DE and director lengths and spacings
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NBS Design Curves
The following design curves were derived from experimental data taken at 400 MHz that explains data plotted over 10l
array lengths: focus is on gain , not F/B ratio
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This photo shows a NBS 4l test array
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Gain Effect of the Reflector Element-NBS TN
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Optimum reflector spacing SR (for maximum directivity) is between 0.10 and 0.20 wavelengths
Measured gain in dBd
of a dipole and reflector
element for different
spacings SR.
Spacing SR (l) of reflector behind driven element
3
2
1
0.05 0.10 0.15 0.20 0.25 0.30 0.35
Reflector Driver
SR
Typicallyused spacing
Dipole gaindBd= 2.15dBi
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Yagi Gain vs Number of Directors- NBS TN
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These curves cover long arrays. For HF, focus on data for < 1l
array length. 0.2l element spacing provides slightly more directive gain than 0.3l spacing
Note: the reflector is included
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An Interesting Comparison
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0
2
4
6
8
10
12
0 1 2 3 4
Gai
n, d
Bd
Number of directors
Yagi Gain, Directors spaced 0.2l& 0.3l
from DE
0.2l spacing, l=.382l
0.2l spacing, l=.411l
0.3l spacing, l=.382l
0.3l spacing, l=.411l
2 3 4 5 6
Equivalent number of elements
From NBS Tech Note
Note the approximate gain agreement for 3-5 elements
0
1
2
3
4
5
6
7
8
9
10
11
12
0 1 2 3 4 5 6 7 8
Gai
n, d
Bd
Number of Elements
Commercial Yagi Gain vs # Elements
Gain, dBd, Hy-gain Gain, dBd, Long John
Gain, dBd, Cushcraft
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3 Element 20,15 &10 meter Design Examples
Note: Pattern gain, F/B, Zin, change with frequency and Rin < 50 Ohms
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Zin
Freq.Dir. GainF/BZinSWR
Zin
Freq.Dir. GainF/BZinSWR
Zin
Freq.Dir. GainF/BZinSWR
These results are from computer-aided design software
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Yagi Input Impedance
• The driven element is often a dipole; some designs use a folded dipole to raise the impedance
• Expect ~ 73 Ohms resistive for free-space, half-wave dipole driving impedance
• However, the reflector and director(s) generally reduce that impedance due to mutual impedance
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The Yagi input impedance commonly requires matching
to a 50 Ohm transmission line by various techniques.
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Driven Element Free-space Feed Impedance
Note: the DE self impedance is often tuned for slightly
capacitive reactance when a Beta match is used.
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These theoretical values are half those of the driven dipole element.
Note: At resonant length, the reactance is not =0.Below resonance, the reactance is capacitiveAbove resonance, the reactance is inductive
ind
uct
ive
cap
acit
ive
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Mutual Impedance Alters Input Impedance
The element 1 E field induces a current I2 in element 2. That element current radiates an E field inducing a port voltage in element 1,
altering port 1 input impedance. Examples shown later.12/15/2020 11
V1I1
Port 1
Isc=I2V2=0
Element 1 Element 2
Z11 Z12
Z21 Z22
V1V2=0I2=Isc
2 port network
Port 2
Mutual impedance = Z12=Z21Z12=Z21 reciprocity
V1=Z11*I1+Z12*I2V2=Z21*I1+Z22*I2
V2=0, I2=-(Z21*I1)/Z22
So V1/I1=Zin= Z11-(Z12)2/Z22
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Mutual Impedance vs Element Spacing
As element spacing increases mutual impedance decreases.Generally 0.2-0.3 l spacing is used.
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V1
Port 1 Port 2
E1
Driven element parasitic element
I2=IscZ12=V1/Isc
V1
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Simplest Yagi-Uda Array Impedance Examples
Za = 92.47 + 104.19j , 75.68 + 11.63j
75.68 + 11.63j , 73.07 + 41.37j
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Zb= 73.07 + 41.37j , 59.77 + 4.35j59.77 + 4.35j , 57.65 − 17.01j
V V
DE DE DirRefl
d dd=0.1 l
L1=0.54 lL2=l/2L3=0.46 l
L1 L2 L3
Note: the reflector self impedance is inductive while the director self impedance is capacitive. The mutual impedance values are
needed to calculate the DE driving point impedance.
Mutual impedance
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Matching The Yagi
• From the 20, 15 & 10 meter design examples, Re(Zin) generally is less than 50 Ohms
• Matching Choices
– Impedance transformer; N:1 balun
– Gamma match
– T match and
– Beta match
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The choice is generally between the Gamma and Beta match
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2019 Nov. QST Dipole Matching Methods
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Notice balanced vs unbalanced techniques, preference
is gamma match for a coax feed line
Delta T-match
Gammamatch
SymmetricalGammamatch
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DX Engineering Quote
• “There are various ways to match the driven element to the feed-line successfully; Gamma Match, T-Match, and the Hairpin (aka Beta Match) are favorites. The Gamma match is an outdated, unbalanced system that typically distorts the antenna radiation pattern. The T-match is basically two Gamma Match systems on either side of the boom, which may correct the imbalance, but is a mechanical nightmare and is difficult to tune correctly.”
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The Beta or Hairpin Match
Used in MARC Yagis suitable for “balanced” driven element, it raises the Zin to minimize SWR to a 50 Ohm transmission line,
the driven element is isolated from the boom
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Unbalanced transmission line
Could be attached to boomAt neutral point
ChokeDX EngineeringHairpin match; DXE-HMS-1P
DXE-HMS-1P
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The Hairpin Effect
Shunt inductance, Xl, increases
the resistive part of Za=R, to match Rin.
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Xl= (Rin x R1/2)/(Rin-R)1/2
Xl
Rin=Re(Zin)
0.0
20.0
40.0
60.0
80.0
100.0
120.0
140.0
160.0
180.0
200.0
0.0 20.0 40.0 60.0
Hai
rpin
Re
acta
nce
, Xl,
Oh
ms
Antenna Driving Point Resistance Re(Za)=R, Ohms
Hairpin Inductance Vs. Driving Point Resistance, At Resonance
Transmission Line Zo=50 Ohms
Transmission Line Zo=70 Ohms
Set Rin=Zo
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Conclusions- Part 2
• The Yagi Array:– Can be designed using empirical data; “rules of thumb” or
computer-aided design SW
– Exhibits less than 50 Ohms driving point impedance due to mutual impedance
– Is compatible with several matching techniques
• The Yagi performance:– Increases directive gain with more directors (longer array)
– Varies with frequency; especially directive gain and F/B ratio
– Uses hairpin match; a simple and effective technique
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Bottom line : It is a winner
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References1. Wikipedia, “Yagi-Uda Antenna”
2. Thiele, Gary A., Analysis of Yagi-Uda Type Antennas” IEEE Trans. On antennas & Propagation, Vol. AP-17, No.1, Jan., 1969
3. “Yagi Antenna/ Yagi-Uda Aerial”
4. Viezbricke, Peter, “Yagi Antenna Design”, Nat. Bur. Standards TN688, December, 1976
5. Ch25, “Coupled Antennas “ , http://eceweb1.rutgers.edu/~orfanidi/ewa/ch25.pdf
6. Steyer, Martin, DK7ZB, “ 3 Element-Yagi, 20m/15m/10m, 28Ohm Design”, www.qsl.net/dk7zb
7. Magliacane, John, KD2BD, “Thoughts on Perfect Impedance Matching of a Yagi”
8. Wortman, Bill, N6MW, “ The Hairpin Match”
9. vu2nsb.com/antenna/yagi-antennas/
10. ARRL Antenna Handbook
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