Detuning Towers

Detuning Towers

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Detuning Towers

The goal of detuning is not to avoid resonance, but rather to
minimize re-radiation and/or current in the interfering structure.

When large enough, structures can re-radiate and cause severe
pattern distortion even when they are NOT resonant. Consider, for example, how
effective a large non-resonant screen or solid disk is at reflecting signals
even when it is nowhere near resonance.

We can minimize re-radiation by making an area or areas of the
structure “electrically vanish”. We often call this
“de-tuning”, even though it is more correctly electrical trapping or
sectionalizing of a structure.  

Most structures or towers, when detuned, have a section adjusted to represent
parallel tuned circuit.

Section A and B carry out-of-phase currents. Picture the current flowing
upwards in A. It must then flow downwards in B.  Since it is a closed loop,
these out-of-phase currents are equal and flow in opposite directions at
resonance. The result is radiation from sections A and B cancel each other. When section A and B are exactly resonant, sections D and C are isolated by
a high impedance. The high impedance is caused by or related to the high current
though the capacitor and the inductance of section A. When current is maximum,
voltage drop is maximum.

This results in the electrical structure on the right, with section A
and B removed!!

In effect, we have created a trap much like the trap in a dipole. As in the
trap dipole, current is maximum in the trap at the trap’s resonant frequency.

NOTE: The condition of  proper tuning occurs with MAXIMUM current
in section B, NOT minimum current!! To electrically sectionalize the tower and isolate
C and D (and minimize radiation from A) section B must be tuned for MAXIMUM

As either section C or D approach resonance by themselves, the tuning
condition will change. This would occur when D is grounded and near 1/4wl or an
odd multiple of 1/4wl long, or when C (with whatever is mounted on it) is
self-resonant with section A removed!!

Under this condition, you would either need to sectionalize and detune C or D
with additional detuning, or move the location of sections A and B to a new
point that (when  isolated) prevents resonance in C and/or D.

A few general rules apply. Pay attention to these guidelines to insure best

  • Never parallel-tune a large area. Certainly not an area over
    3/16th wavelength long
  • The detuning “loop” must have a good solid connection to the
    structure being detuned. Don’t connect the detuning wire out to a separate
    object or earth stake
  • We want to adjust for MAXIMUM current in section B, the exception being
    when that would cause resonance in C or D
  • We can not have any electrically large structures or wires hanging from
    the tower in the area being detuned.
  • Ideally any cables passing the detuning area  should be grounded to
    the tower at the top and bottom of the detuning area, or pass through that
    area in the center of the tower or mast. At the very least, cable shields
    should be bonded to the tower at the top and bottom of the cable run and
    unshielded cables placed inside the tower.  
  • Tuning is fairly narrow. ~5% total BW is about all that can be expected in
    most cases, but this varies greatly with the system including distances to
    the other affected antennas and the amount of pattern distortion

Note: I added the section about cables on Feb 17,2003. I’m
surprised cables are often not grounded at the top and bottom of tall towers,
and that unshielded control cables are not passed through the inside of towers.
Cables should always be treated that way for lightning protection if for no
other reason! 

Capacitor Size

The amount of capacitance and the voltage rating of the capacitor is not easy
to predict. The size depends on unwanted power levels that excite the detuned
structure, the electrical characteristics of the detuned structure, and the Q of
the detuning section. Capacitance values will be fairly high with short sections on lower
bands like 160, almost certainly in the range of a few thousand pF for ~20 foot
long sections. The exact value would depend heavily on dimensions of the A to B

Voltages across the capacitor are generally not high, although they can be at
times. The “loop Q” of A and B affects voltage, as does the amount of
excitation and load presented by the impedances of C and D.

MFJ sells a clamp-on calibrated current meter that will not perturb the
system. It is a cheap version of a current meter I designed. This is a
calibrated meter with internal amplifier that measures current from a few mA to
3 amperes, not the uncalibrated RF-sniffer commonly sold. Some RF-sniffers,
including those by MFJ, actually change the impedance and resonant frequency of
the system because the pick-up transformers are not properly designed and
terminated current transformers. Avoid
loop-stick type current meters, since they measure ANY external field and can
provide misleading results. Use a current meter that is directly inserted in line B, or clamps
around line B with the closed core of a terminated current transformer. Use a
meter that does NOT perturb the system when removed!  

Lacking a current meter, it is possible to tune this system with a grid dip
meter, by forming a small one or two turn coupling loop. As an alternative, the
loop can can be broken at any point near the capacitor and a MFJ-259 or similar
antenna analyzer connected in series. Proper adjustment is at the point were
minimum impedance occurs. If that impedance is not low, you probably are not
effectively detuning the structure.

Multiple Stacked Antennas or Tall Structures

When multiple stacked antennas are used, especially on a fairly tall tower,
it may be necessary to sectionalize multiple points. Individual sections between
antennas can be resonant, or appear electrically long.  

If the tower or structure or any part of the structure or tower becomes
resonant when section A is tuned to present a high impedance, then we need to
move section A or tune it to some  condition other than maximum current
(resonance). Adjustments under this condition can only be made two ways:

  • A sampling loop can be mounted on the structure 1/10th wl or more above or
    below section B and adjusted for minimum terminal voltage
  • Field strength of the pattern can be plotted, and the structure tuned for
    minimum pattern distortion
  • Never detune an area that contains large yagis or other electrically large
    objects, like long conductive guy lines, dipoles, or cables leaving the