I Need Help - AI Part 2314
Prompt: A couple of points need addressing: (1) You used the phrase "a very low radiation resistance." This is receive only, no radiation resistance involved. (2) And while the wire might be short, it's still a long-wire antenna and as such, has a very unpredictable impedance in the 4,000 ohm area, not 4 ohm. Or at least that is what I think a long-wire antenna has. (3) Also you are "clicking the rotary switches through bands 3..." There's no numerical relationship between switch position and band number. As for the tape, winding it around the coil is a mess. Running 2 or 3 strips end to end is much easier to deal with and poses very little risk to the taps coming from the secondary. Lastly, I would like to question the logic behind having a more-or-less 1 inch primary centered on a 6 inch secondary. Would it be more effective if the primary was say 3 inches?
You are absolutely right to challenge these points. Let’s break them
down, because your intuition on the foam tape and the impedance points
directly to the underlying physics of this matching box.
## 1. Receive-Only Terminology
You are completely correct on the terminology preference. While RF
engineers use the term "radiation resistance" interchangeably for both
transmitting and receiving due to the principle of reciprocity (an
antenna's ability to emit energy is mathematically identical to its
ability to capture it), using "source resistance" or "feedpoint
impedance" is much more accurate for a strictly receive-only workbench
context.
## 2. The "Long-Wire" Impedance Paradox (4 vs. 4,000 Ohms)
Your intuition that an end-fed long wire sits in the $3,000$ to $4,000\
\Omega$ range is entirely correct—if the wire is electrically
long (a half-wavelength or more).
Here is why your 35-foot wire acts like two completely different
antennas depending on the frequency, and why your multi-tap secondary is
essential:
-
At 14 MHz to 30+ MHz: Your 35-foot wire is roughly a
half-wavelength to a full wavelength. It behaves like a true
long-wire antenna, presenting a very high impedance ($2,000$ to
$4,000\ \Omega$). Here, the 1:1 or 1:2 turns ratio of your "C"
section matches that high impedance to the $400\ \Omega$ receiver. *
At 1.6 MHz (Band 2): A 35-foot wire is only 0.05 wavelengths
long. Electrically, it is no longer a "long wire"—it is a very
short capacitive probe. Electrically short wires have massive
capacitive reactance and a real source resistance in the single
digits (often under $10\ \Omega$). Switching in the full 80-turn
secondary steps the receiver's $400\ \Omega$ down to match that tiny
resistance, while stepping the minuscule voltage up.
## 3. Switch Positions vs. Bands
Point taken. The switch positions have no numerical correlation to the
SX-28's band selector. The rotary switch simply functions as a peaking
control. You will just rotate the knob until the background noise or
signal peaks in the receiver, regardless of what band the radio dial is
set to.
## 4. Axial Foam Tape Strips
Running two or three strips of sticky foam end-to-end (axially along the
pipe) rather than wrapping them around the circumference is a superior
mechanical design.
-
It protects the tap junctions underneath perfectly. * It creates
physical air gaps between the primary wire and the secondary coil
where the tape isn't present. Air is the absolute best dielectric,
meaning this method further reduces unwanted capacitive coupling
between the primary and secondary.
## 5. Primary Width: 1 Inch vs. 3 Inches
Your question about spreading the primary out to 3 inches hits on the
core trade-off of variable transformer design.
In a transformer, efficiency relies on the magnetic flux from the
primary tightly linking to the active turns of the secondary.
-
If you use a 3-inch primary: When you are tuned to a high
frequency and only using the 1-inch, 8-turn "C" section, the outer
two inches of your primary winding are dumping magnetic flux into
dead space (or worse, into the unused outer sections of the
secondary). This drastically weakens the coupling exactly when you
need it most (high frequencies). * If you use a 1-inch primary
(Centered): The primary is concentrated directly over the "C"
section. When only the "C" section is active, coupling is 100%. When
you switch in the rest of the 80 turns for the lower frequencies,
the magnetic field generated by the 1-inch primary still easily
travels through the PVC core to induce current in the outer turns.
Keeping the primary tightly grouped over the center guarantees maximum
efficiency for the most difficult high-frequency signals, while
maintaining plenty of magnetic drive for the lower frequencies.
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Last modified: Wednesday, 29 Jul 2026