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Part 2 Presenter-Tom Kihm, KJ6PST 12/15/2020 1 The Yagi-Uda Antenna

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

Page 2: The Yagi-Uda Antenna - WordPress.com · 2020. 12. 16. · •The Yagi Array: –an be designed using empirical data; “rules of thumb” or computer-aided design SW –Exhibits less

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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