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Antennas with Loads and Traps – What are these things and why are they used in our antennas? By: Dave Brown K3CTN.

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Presentation on theme: "Antennas with Loads and Traps – What are these things and why are they used in our antennas? By: Dave Brown K3CTN."— Presentation transcript:

1 Antennas with Loads and Traps – What are these things and why are they used in our antennas?
By: Dave Brown K3CTN

2 Impedance – The ohmic value of an antenna
feed point, matching section or transmission line. An impedance may contain a reactance as well as a resistance component. (ARRL Antenna Book, 23rd Edition) R Resistance j XL - j XC or Reactance Antenna Impedance X is Positive for Inductive Reactance, R + j X Negative for Capacitive Reactance

3 Today's transmitters are designed to deliver
power to a resistive 50 ohm antenna. Less than maximum power is transferred to the antenna when the antenna impedance varies from 50 ohms resistive. Some sort of impedance matching mechanism is used to “match” the transmitter to an antenna.

4 Impedance Matching – The Antenna Tuner

5 Concepts discussed here apply to both
Horizontal and Vertical Antennas

6 Antenna Engineering Handbook – Jasik

7 Antenna Engineering Handbook – Jasik

8 Move part of the Antenna Tuner “into” the Antenna
Transmission Line Load Antenna RANT j XLOAD - j XANT Load Inductor

9 A Dipole or Vertical (with Ground image) shorter, or longer, than a half wavelength (λ/2) can:
Have a reactive “load” built into the antenna to remove or minimize the antenna's reactance. But where should this “load” be placed in the antenna? (λ / 4) (< λ / 4) (> λ / 4) Transmission Line Connection

10 Designing a Shortened Antenna – Lopes
Design a shortened half wave dipole with loading coils due to limited available space: Where do you put the loading coils? How do you determine the loading coil inductance? Lopes solution: You specify the antenna length and loading coil locations Use transmission line theory to calculate the loading coil inductance

11 Calculate the line's characteristic impedance
Determine the reactance at points X1 and X2, the piece of wire that will be replaced by a coil Determine the inductance of the coil

12 A “Trapped” Dipole (or Vertical)

13 Example: 40 / 20 meter Trap Dipole
Target Frequencies: 7.05 mHz and mHz Trap Parallel Resonant Frequency: ~ mHz 3.3 uHy 39 pF 0 ft, Transmission Line Connection 16.8 ft 29.7 ft

14 Example: 40 / 20 meter Trap Dipole
SWR < 3:1 6.90 – 7.28 mHz 13.86 – mHz

15 When a Trap is Parallel Resonant between two amateur bands, the Trap will effectively provide loading where: At a lower amateur band frequency, the Trap has an inductive reactance At a higher amateur band frequency, the Trap has a capacitive reactance In other words, inductive loading will electrically lengthen an antenna and capacitive loading will electrically shorten an antenna Design of a two-band dipole with a Parallel Resonant Trap between two bands is a challenge

16 Design of a Two-band Loaded Dipole Antenna – Birnbaum
David Birnbaum, K2LYV described an innovative solution to this problem in a recent QEX article Birnbaum's solution uses an out of band Parallel Resonant Trap where: You choose an antenna length that will fit into your available physical space The dipole feedline-to-Trap length must be shorter than λ/4 at the higher frequency Continued

17 Birnbaum continued: Using Lopes' method, calculate the value of inductive reactance for the lower frequency Also, using a modified method of Lopes, calculate the value of the capacitive reactance for the higher frequency Use these two reactance values in additional calculations described by Birnbaum to identify the Trap's Parallel Resonant frequency along with the Trap's L and C values

18 Birnbaum Clarification
Total Length Trap Inner Length Low Freq, Total Length < λ / Trap = j XL High Freq, Total Length > λ / Trap = - j XC

19 Example: 30 / 20 meter Trap Dipole
Dipole length = 40 ft fLOW = mHz, fHIGH = mHz 3.0 uHy 53 pF 0 ft, Transmission Line Connection 14 ft 20 ft Trap Parallel Resonance ≈ 12.6 mHz

20 Example: 30 / 20 meter Trap Dipole
SWR < 3:1 9.95 – mHz 13.93 – mHz

21 Notes “The ARRL Antenna Book,” 23rd Edition, 2015.
Jasik, “Antenna Engineering Handbook”, 2nd Edition, 1984, Figs. 4-3 and 4-4. Luiz Duarte Lopes, CT1EOJ “Designing a Shortened Antenna,” QST, Oct. 2003, pp David Birnbaum, K2LYV, “Design of a Two-Band Loaded Dipole Antenna,” QEX, Sept./Oct. 2017, pp Ward Silver, N0AX, “Antenna Modeling for Beginners,” ARRL, 2012.


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