11
Two Bands from One Dipole Marc C. Tarplee Ph.D., N4UFP ARRL South Carolina Section Technical Coordinator

Two Bands from One Dipole Marc C. Tarplee Ph.D., N4UFP ARRL South Carolina Section Technical Coordinator

Embed Size (px)

Citation preview

Page 1: Two Bands from One Dipole Marc C. Tarplee Ph.D., N4UFP ARRL South Carolina Section Technical Coordinator

Two Bands from One Dipole

Marc C. Tarplee Ph.D., N4UFP

ARRL South Carolina Section

Technical Coordinator

Page 2: Two Bands from One Dipole Marc C. Tarplee Ph.D., N4UFP ARRL South Carolina Section Technical Coordinator

Drawbacks of Existing Two-Band Dipoles• Multiple dipoles on a common feed.

– Spreaders are required to separate the two sets of wires

– Proximity of the dipoles makes tuning difficult

– The additional weight of the spreaders makes the antenna heavy and cumbersome to erect

• Addition of a second parasitic radiator.– Spreaders are required to maintain proper

spacing– No simple design rule exists for this antenna;

much experimentation is necessary to get a workable design

– Tuning can be difficult

• Trapped dipoles.– Weather resistant, high-Q traps are not easy

to construct.– Traps add weight to the antenna.– Traps increase losses in the antenna.

Page 3: Two Bands from One Dipole Marc C. Tarplee Ph.D., N4UFP ARRL South Carolina Section Technical Coordinator

Transmission Line Transformers

• When a transmission line in terminated in an impedance not equal to its characteristic impedance, the impedance at the input to the line depends on the line’s electrical length

• A transmission line can be used to transform a load impedance into a more desirable value.

• Example: quarter-wave sections used to match loops.

• The input impedance, load impedance and line length are related by the following equation:

Page 4: Two Bands from One Dipole Marc C. Tarplee Ph.D., N4UFP ARRL South Carolina Section Technical Coordinator

Transmission Line Transformers

• The input impedance, load impedance and line length are related by the following equations:

• Where– Z0 is the line impedance

– ZA is the antenna impedance, which depends on the antenna length

– f is the frequency

– x is the length of the transmission line

– fv is the velocity factor of the line

Page 5: Two Bands from One Dipole Marc C. Tarplee Ph.D., N4UFP ARRL South Carolina Section Technical Coordinator

A Two-Band Dipole Using a Transmission Line Transformer

• An antenna system made up of dipole antenna of length l, fed with a transmission line of impedance Z0 and length x, will have a resistive input impedance when the following condition is satisfied:

• The SWR will be less than 2.0 if the next condition is also satisfied:

• Although the function ψ(x) is known, there is no closed form functional representation for ZA(l), so these equations must be solved numerically.

• The problem can be solved by using antenna simulation tools to create a table of values for ZA(l) which is put into mathematics software such as MathCAD® along with the transmission line equations. Variables x and l are varied until the antenna has a low SWR at the two design frequencies.

100Re))(sin()())(cos(

))(sin())(cos()(Re25

0

00

IN

A

A ZxljZxZ

xjZxlZZ

0Im))(sin()())(cos(

))(sin())(cos()(Im

0

00

IN

A

A ZxljZxZ

xjZxlZZ

Page 6: Two Bands from One Dipole Marc C. Tarplee Ph.D., N4UFP ARRL South Carolina Section Technical Coordinator

Two-Band Dipole Designs

• These designs are made from #14 copper wire and 450 ohm ladder line with a 0.9 velocity factor

Bands Dipole Length

Ladder Line Length

Lower Resonant Frequency

Lower Frequency Input Z

Higher Resonant Frequency

Higher Frequency Input Z

75/40 144 ft 10 in 89 ft 6 in 3.87 MHz 89 Ω 7.25 MHz 32 Ω

30/17 54 ft 9 in 36 ft 2 in 10.12 MHz 88 Ω 18.12 MHz 39 Ω

20/17 77 ft 8 in 76 ft 2 in 14.13 MHz 33 Ω 18.11 MHz 83 Ω

20/15 51 ft 0 in 50 ft 8 in 14.17 MHz 53 Ω 21.27 MHz 41 Ω

20/12 68 ft 0 in 46 ft 8 in 14.15 MHz 33 Ω 24.92 MHz 82 Ω

20/10 48 ft 3 in 50 ft 6 in 14.08 MHz 34 Ω 28.40 MHz 50 Ω

17/12 28 ft 7 in 46 ft 8 in 18.11 MHz 77 Ω 24.95 MHz 75 Ω

17/10 33 ft 4 in 62ft 6 in 18.08 MHz 88 Ω 28.42 MHz 87 Ω

15/10 102 ft 0 in 70 ft 6 in 21.25 MHz 48 Ω 28.32 MHz 64 Ω

10/6 16 ft 6 in 33 ft 5 in 28.40 MHz 69 Ω 50.10 MHz 64 Ω

Page 7: Two Bands from One Dipole Marc C. Tarplee Ph.D., N4UFP ARRL South Carolina Section Technical Coordinator

Design Comments

• 450 ohm ladder line (vf = 0.9) was used for these designs because of its low cost, low loss, and wide availability. It is possible to redesign the antenna systems to use other parallel lines.

• As the ratio of the two design frequencies approaches an odd multiple of 1/2 , the length of the dipole is a minimum. For example:

• In general, as the ratio of the design frequencies becomes close to 1.0, the electrical length of the antenna and matching section becomes very long.

• In general, the dipole portion of the antenna system will not be resonant on either band (even though the system as a whole is)

Bands Freq. Ratio Dipole Length Line Length

20/17 1.28 77 ft 8 in 76 ft 2 in

20/15 1.50 51 ft 0 in 50 ft 8 in

20/12 1.76 68 ft 0 in 46 ft 8 in

Page 8: Two Bands from One Dipole Marc C. Tarplee Ph.D., N4UFP ARRL South Carolina Section Technical Coordinator

Design Comments

• These designs have less bandwidth on a given band than a single band dipole.

• All designs except the 75/40 m design have been tested. The resonant frequencies and SWR were close to that predicted by simulation of the design.

• For antenna systems whose ratio of resonant frequencies is less than 2.0, the radiation pattern will be similar on both bands.

• The antenna system is fed with 50 ohm coaxial cable that is connected to the input of the antenna system (the ladder line) through a choke balun.

Page 9: Two Bands from One Dipole Marc C. Tarplee Ph.D., N4UFP ARRL South Carolina Section Technical Coordinator

Use of Other Types of Feed Lines as Matching Sections

• Coaxial cable is not used because it is relatively lossy when used at high SWR.

• Other types of ladder line could be used (300 ohm, 600 ohm, etc.), but the design of the dipole must be reworked.

• Certain frequency ratios cannot be matched when 450 ohm line is used, necessitating the use of a different type of ladder line.

• 440 ohm ladder line may be used in place of 450 ohm ladder line without problem

Page 10: Two Bands from One Dipole Marc C. Tarplee Ph.D., N4UFP ARRL South Carolina Section Technical Coordinator

Putting up a Dipole

• A dipole may be erected between 2 supports or with one support.

• A dipole antenna using a single support is known as an “inverted-V”

• The legs of a dipole may also be bent to form an inverted U. The bend should be at least half way to the end of the wire

Page 11: Two Bands from One Dipole Marc C. Tarplee Ph.D., N4UFP ARRL South Carolina Section Technical Coordinator

Closing Comments

• This is about the simplest and least expensive multi-band antenna that one could construct.

• There is room for further experimentation:– Is it possible to vary l, x, and ZB so that there is a good match on 3

frequencies?

– Is there any advantage to using thicker elements?

– Can this technique be adapted to vertical antennas?