The explanations for all ten questions sit on this sheet. Pick an answer on the left and the matching card lights up.
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G4B01 Explanation 1
Key C — Feed line loss attenuates the reflected wave on its way back, so the transmitter sees a better match than the antenna has
Reflected power makes two trips through the cable, so a lossy line absorbs some of it and the ratio measured at the shack improves. This is why an SWR reading at the transmitter is not proof that the antenna is well matched - at 2 metres with thin coax, the difference can be large.
Rule Fundamentals - SWR measurement
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G4B02 Explanation 2
Key B — Impedance and the resonant frequency across a range of frequencies
An analyser sweeps and reports complex impedance, so you can see where reactance crosses zero - the true resonance - rather than only where SWR dips. Trimming an element to resonance, rather than to the lowest SWR, is how an antenna is adjusted correctly.
Rule Fundamentals - antenna measurement
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G4B03 Explanation 3
Key A — About 300 ohms
Folding the element raises the impedance by roughly a factor of four over the 73 ohms of a simple dipole, giving about 300 ohms - which is why a 4:1 balun is the standard way to feed one from 50 ohm coax.
Rule Fundamentals - folded dipole
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G4B04 Explanation 4
Key D — Wider bandwidth at the same resonant frequency
The folded construction broadens the impedance-versus-frequency curve, so the antenna stays matched over more of the band without a tuner. Gain is essentially the same as a simple dipole - folding changes impedance, not directivity.
Rule Fundamentals - folded dipole bandwidth
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G4B05 Explanation 5
Key C — It is fed at about one third of its length, presenting 200 to 300 ohms and working on several harmonically related bands
Moving the feed point away from the centre raises the impedance at the fundamental and at each harmonic to a range a transformer can handle, which is what makes one wire work on 80, 40, 20 and 10 metres. The cost is an asymmetric pattern and a need to choke the feed line.
Rule Fundamentals - multiband dipoles
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G4B06 Explanation 6
Key B — Very wide, smooth coverage in exchange for several dB of lost efficiency
Resistive loading absorbs power deliberately, which flattens the response across a very wide frequency range. The antenna is a good choice for receiving and for wideband coverage, and a poor choice when radiated power matters most.
Rule Fundamentals - terminated antennas
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G4B07 Explanation 7
Key A — It changes the resonant frequency and distorts the radiation pattern
A nearby conductor couples to the radiating element and re-radiates, which shifts resonance and fills in nulls in the pattern. This is why the same antenna design performs differently on different masts, and why modelling software asks about nearby metalwork.
Rule Fundamentals - antenna surroundings
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G4B08 Explanation 8
Key D — The radiation pattern used for transmitting is the same as the pattern used for receiving
Reciprocity means every statement about an antenna's gain, directivity or pattern applies to both directions of the link, so one good antenna improves both what you send and what you hear. It also means a pattern measured on receive is a valid description of the transmit pattern.
Rule Fundamentals - reciprocity
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G4B09 Explanation 9
Key C — A low SWR at the wrong frequency often indicates loss rather than resonance
Resistive loss makes an antenna look better matched than it is, so a broad, shallow SWR curve can mean a lossy installation rather than a good one. Adjusting to the frequency where reactance crosses zero puts the antenna where it actually radiates efficiently.
Rule Fundamentals - resonance versus match
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G4B10 Explanation 10
Key C — It confirms that power is actually being radiated rather than absorbed in a lossy feed line or matching network
A low SWR combined with no radiated field is the classic signature of a lossy system - a wet coax connector, a resistive balun, or a termination absorbing the power. A field strength meter resolves the ambiguity that an SWR reading alone cannot.
Rule Fundamentals - verifying radiation