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Ham Radio Cubical Quad Antennas — Complete Guide

The cubical quad is one of the most debated antennas in amateur radio — its proponents claim it consistently outperforms a Yagi of the same element count, while skeptics question the real-world advantage. What is not in debate: a well-built quad delivers genuine high gain with lower takeoff angle, quieter receive characteristics, and a radiation pattern that many HF operators find superior for DX work. This guide covers quad theory, element dimensions for all HF bands, spreader design, multi-band construction, feed systems, and the honest performance comparison with Yagis.

8–12 dBdTypical gain (2-el)
+1.5 dBdOver equiv. Yagi
20m–10mTypical coverage
~50–100ΩFeed impedance
⊞⊳

2-Element Cubical Quad

One driven loop and one reflector loop on a single boom. Delivers approximately 7–8 dBd — slightly more than a 3-element Yagi on a comparable boom length. The entry-level quad beam for HF DX and contesting.

7–8 dBd~50–100ΩSingle bandAdvanced
⊞⊳⊳

3-Element Cubical Quad

Driven loop, reflector, and one director. Delivers approximately 9–10 dBd with improved front-to-back ratio over the 2-element design. Comparable to a 5-element Yagi on similar boom length. A serious DX and contest antenna.

9–10 dBdHigh F/BSingle bandExpert
⊞⊞⊳

Multi-Band Quad

Multiple sets of loops on the same spreader arms — one set per band. Typically covers 20m, 15m, and 10m from one antenna structure. The outer (longer) loops are for the lowest band; inner (shorter) loops for higher bands, all sharing the same four spreader arms.

20m · 15m · 10mShared spreadersMulti-bandExpert
△⊳

Delta Loop Beam

Two or more delta (triangular) loops in a driven/reflector arrangement. Delivers ~5 dBd gain with excellent low-angle radiation. Easier to support than a square quad — the apex at the top and base at the bottom fits naturally on a single tall mast with two lower side supports.

~5 dBd40m · 20mWire loopsAdvanced
□⊳

Moxon Rectangle

A 2-element Yagi variant with folded-back element tips forming a compact rectangle. Approximately 30% shorter footprint than a full-size 2-element Yagi with similar gain (~5 dBd) and excellent front-to-back ratio. Wire construction on a simple PVC or fiberglass frame.

~5 dBdHigh F/BCompactIntermediate

Spider Quad

A multi-band quad using a central hub with spreader arms radiating outward like a spider's legs. Multiple bands of loops are mounted on the same set of spreaders. Compact and mechanically elegant — the spreaders support all bands simultaneously from a single center mounting point.

Multi-bandSingle hubCompactExpert

Full-Wave Loop Elements vs Half-Wave Dipole Elements

The fundamental difference between a quad and a Yagi is the element type. A Yagi uses half-wave dipole elements — straight conductors. A quad uses full-wave loop elements — closed wire squares (or other loop shapes). This difference in element type produces several performance advantages:

  • A full-wave loop has approximately 2 dBd gain over a half-wave dipole — it is inherently a stronger radiator per element
  • The loop element produces lower-angle radiation at a given antenna height compared to a dipole at the same height — better for DX
  • The loop geometry reduces sensitivity to nearby conducting objects — quads are less detuned by rain, ice, and wet foliage than Yagi dipole elements
  • Loop elements are less susceptible to static charge buildup — quads are somewhat self-draining via the closed loop conductor
  • The closed loop provides DC continuity between all parts of the element — simplifying lightning protection

The quad's gain advantage over a Yagi comes entirely from the superior efficiency of loop elements versus dipole elements. A 2-element quad (driven + reflector) delivers approximately the same gain as a 3-element Yagi on a comparable boom length — the extra element in the Yagi compensates for the dipole's inherently lower gain per element.

The Quad vs Yagi Debate — What the Measurements Say

Few topics generate more discussion in amateur radio than whether a quad outperforms a Yagi. The honest answer, based on NEC2 modeling and practical measurements:

  • A 2-element quad delivers approximately 7–8 dBd — slightly more than a 3-element Yagi (~7 dBd) on similar boom length
  • A 3-element quad delivers approximately 9–10 dBd — comparable to a 5-element Yagi
  • The gain advantage of the quad is real but modest — typically 0.5 to 1.5 dBd over a comparable Yagi
  • The quad's lower takeoff angle at the same physical height is a genuine advantage for DX propagation
  • The quad's quieter receive characteristic is real — fewer operators report the noise increase when switching to a quad that they do when switching to a Yagi
  • The quad's mechanical disadvantage — fiberglass spreaders, heavier wire loops, more complex construction — is also real

Bottom line: the quad is a genuinely superior HF DX antenna when built well. The mechanical challenge is the real barrier to wider adoption — not any theoretical performance limitation.

Element Dimensions — The Loop Formula

Quad loop elements use a different length formula from dipoles. A full-wave loop is approximately 2–3% longer than the theoretical full wavelength — the loop conductor's end-effect is opposite to a dipole's, adding electrical length rather than subtracting it:

Full-wave loop circumference: Driven element: 1005 / f(MHz) = total wire (ft) Reflector: 1030 / f(MHz) = total wire (ft) (+2.5%) Director: 975 / f(MHz) = total wire (ft) (−3%) Each side of square loop = total wire / 4 Spreader arm length = side length × √2 / 2 Element spacing (driven to reflector): 0.14–0.20 × λ Element spacing (driven to director): 0.12–0.18 × λ

The reflector is longer than the driven element — opposite to a Yagi where the reflector is longer than a dipole but the comparison is to the driven element. For a quad, the driven element is already a full-wave loop; the reflector needs to be slightly longer to provide the correct phase relationship for the reflector action.

Antenna calculators →

Feed Systems and Impedance

The feedpoint impedance of a quad loop depends on the feed position. A square loop fed at the bottom center presents approximately 100–130Ω. This requires a matching network for direct 50Ω coax connection:

  • λ/4 coax matching section — a quarter-wave section of 75Ω coax transforms 100Ω to 56Ω (close to 50Ω). The simplest matching approach for a single-band quad.
  • 2:1 current balun — a 2:1 (or 1.5:1) current balun at the feedpoint steps the impedance down to 50Ω. More expensive but frequency-independent.
  • Corner feed — feeding at a corner of the square loop rather than the bottom center changes the impedance toward 50–75Ω depending on the exact position, potentially eliminating the need for a matching transformer.
  • Delta loop feed — feeding a triangular loop at the apex typically presents ~50Ω, simplifying the match.

A current choke (1:1 current balun) at the feedpoint is always recommended to prevent common-mode current from flowing on the coax shield — the quad's geometry makes it slightly more prone to this issue than a center-fed dipole in a Yagi.

Band Frequency Driven loop (ft) Each side (ft) Reflector loop (ft) Director loop (ft) Spreader arm (ft) Refl spacing Dir spacing
40m7.150 MHz140.6 ft35.1 ft144.1 ft136.3 ft24.8 ft19.6 ft16.8 ft
30m10.125 MHz99.3 ft24.8 ft101.8 ft96.3 ft17.5 ft13.9 ft11.9 ft
20m14.200 MHz70.8 ft17.7 ft72.5 ft68.6 ft12.5 ft9.9 ft8.5 ft
17m18.120 MHz55.5 ft13.9 ft56.9 ft53.8 ft9.8 ft7.7 ft6.6 ft
15m21.200 MHz47.4 ft11.9 ft48.6 ft46.0 ft8.4 ft6.6 ft5.6 ft
12m24.940 MHz40.3 ft10.1 ft41.3 ft39.1 ft7.1 ft5.6 ft4.8 ft
10m28.500 MHz35.3 ft8.8 ft36.2 ft34.2 ft6.2 ft4.9 ft4.2 ft

Driven loop = 1005/f(MHz). Reflector = driven × 1.025. Director = driven × 0.970. Spreader arm = side × 0.707. Element spacings: reflector at 0.20λ, director at 0.17λ. Cut loops 2–3% long and trim to resonance after installation using a NanoVNA at the feedpoint.

Adding a Director to the Quad

A 3-element quad — driven element, reflector, and one director — delivers approximately 9–10 dBd of gain with a front-to-back ratio of 25–30 dB. This is comparable to a 5-element Yagi on a similar boom length and represents a serious DX and contest antenna for the operator who can manage the mechanical challenge of quad construction.

The director loop is shorter than the driven element — approximately 3% shorter in circumference. Its spacing from the driven element is typically 0.12–0.18 wavelengths in the forward direction. The interaction between reflector, driven, and director in a quad is similar to a Yagi but the loop elements produce lower mutual coupling, which means the element spacings and lengths are somewhat less critical than in a tightly-coupled Yagi design.

  • 3-element quad boom length: approximately 0.35–0.40λ total
  • For 20m at 14.2 MHz: boom length approximately 24–28 feet
  • Gain advantage over 2-element: approximately 2 dBd additional
  • F/B improvement: from ~20 dB (2-element) to ~28 dB (3-element)
  • Adding more directors continues to increase gain — each additional director adds ~1 dBd
Model your quad in NEC2 before building →

3-Element Quad Dimensions — 20m Example

A complete 3-element quad for 14.200 MHz using the standard design ratios:

Frequency: 14.200 MHz Wavelength: 984 / 14.2 = 69.3 ft Reflector loop: 1030 / 14.2 = 72.5 ft Each side = 18.1 ft Spacing behind driven: 13.9 ft (0.20λ) Driven element: 1005 / 14.2 = 70.8 ft Each side = 17.7 ft Director loop: 975 / 14.2 = 68.7 ft Each side = 17.2 ft Spacing forward of driven: 11.8 ft (0.17λ) Total boom: 13.9 + 11.8 = 25.7 ft Spreader arm (driven): 17.7 × 0.707 = 12.5 ft Spreader arm (reflector): 18.1 × 0.707 = 12.8 ft Spreader arm (director): 17.2 × 0.707 = 12.2 ft Estimated gain: ~9.5 dBd Estimated F/B: ~27 dB

Spreader Materials and Construction

The spreader arms that hold the quad loop wire in its square shape are the most mechanically demanding aspect of quad construction. They must be non-conductive (so they don't detune the loops), strong enough to support the wire tension and wind loading, and light enough not to overload the rotator and mast. The main material options:

  • Fiberglass tubing (most common) — available from kite shops, antenna suppliers, and composites dealers. UV-resistant fiberglass is the standard choice. Hollow tube is lighter than solid rod but less rigid over long spans. Typical OD: 3/4" to 1" for HF quads.
  • Bamboo — historically popular, still used by homebrewers. Lightweight, strong, readily available. Must be sealed against moisture absorption (varnish or epoxy). Degrades over 3–5 years outdoors — needs periodic replacement.
  • PVC pipe (schedule 40) — heavy and UV-degrades over time (becomes brittle). Acceptable for shorter spreader arms on higher bands (15m, 10m) but not ideal for 20m where arms exceed 12 feet.
  • Carbon fiber — strongest and lightest option. Excellent mechanical properties. One significant caveat: carbon fiber is electrically conductive — it will significantly detune the loops if the spreaders contact the wire. Require careful electrical isolation at all contact points.
  • HDPE or polycarbonate rod — excellent UV resistance, low weight, easy to machine. More expensive than fiberglass but very clean to work with.

Hub Design and Spreader Mounting

The central hub connects the spreader arms to the boom and mast. Four spreader arms radiate outward at 90° to each other, angled downward at approximately 5–10° from horizontal to create a slight droop that helps the wire loops maintain their shape. Hub construction options:

  • Commercial fiberglass quad hubs are available from several antenna suppliers — these are the most reliable option for a permanent installation
  • PVC pipe fittings (cross tee) provide a simple homebrew hub — drill holes for the spreader arms and secure with set screws or bolts through the PVC wall
  • Aluminum plate hub — a piece of aluminum flat bar or plate with holes drilled for each spreader arm. Strong and durable but heavier than PVC or fiberglass options
  • Each spreader arm connects to the hub with a set screw, clamping bolt, or through-bolt plus epoxy for permanent installations
  • The wire loop attaches to the spreader arm tips via small insulators — commercial end caps or homemade holes through the fiberglass tip
  • The corner where the wire reaches each spreader tip should be supported by a small loop of UV-resistant cord through the insulator — the wire tension should be borne by the cord, not by a sharp corner that could cut the wire over time

How Multi-Band Quads Work

A multi-band quad uses multiple sets of loops on the same spreader structure — one set of loops (driven + reflector) per band, all mounted on the same four spreader arms. The outer loops (larger circumference) resonate on the lowest frequency band; progressively smaller inner loops resonate on higher frequency bands. At any given operating frequency, only the loops for that band are resonant — the other loops present a high impedance and do not significantly load or detune the active band's loops.

The most common commercial configuration covers 20m, 15m, and 10m from one set of spreader arms:

  • Outermost loops: 20m driven and reflector (~17.7 ft each side)
  • Middle loops: 15m driven and reflector (~11.9 ft each side)
  • Innermost loops: 10m driven and reflector (~8.8 ft each side)
  • All six loops share the same four spreader arms — the 20m loop runs near the spreader tips, 15m at mid-arm, 10m near the hub
  • Each band has its own feedline — three separate coax runs to the operating position, or a relay box for remote band selection

Multi-Band Quad Challenges

Multi-band quad construction is significantly more complex than a single-band quad. The additional loops interact with each other electromagnetically, and the mechanical challenge of routing multiple wire loops on the same spreader arms while maintaining proper spacing and tension is considerable. Key issues to manage:

  • Loop interaction — the 15m and 10m loops affect the 20m loop's resonance slightly and vice versa. Final tuning requires iteration — adjusting one band's loop affects adjacent bands. Model the complete multi-band structure in 4NEC2 before cutting wire.
  • Wire routing — six loops of wire on four spreader arms creates a complex web that must be organized to prevent tangling, chafing, and electrical contact between loops of different bands.
  • Feedline routing — three separate feedlines must run from the three driven element feedpoints down the boom to the mast without coupling to each other or to the other antenna loops.
  • Weight and wind loading — three sets of loops plus three feedlines adds significant weight and wind area compared to a single-band quad. Verify the rotator and mast load ratings before finalizing the design.
4NEC2 modeling guide →

What Is a Moxon Rectangle?

The Moxon rectangle (developed by Les Moxon G6XN) is a 2-element beam antenna where the element tips are folded back toward each other, forming a compact rectangular shape. It is essentially a 2-element Yagi with the element ends bent inward to reduce the antenna's footprint by approximately 30% compared to a full-size 2-element Yagi on the same band.

The folded tips create a capacitive coupling between the driven element and reflector that improves the front-to-back ratio beyond what a conventional 2-element Yagi achieves — typically 25–35 dB F/B at the design frequency. Forward gain is approximately 4.5–5.5 dBd — slightly less than a full-size 2-element Yagi but with a dramatically smaller footprint.

  • Footprint: approximately 70% of a full-size 2-element Yagi width
  • Forward gain: 4.5–5.5 dBd (less than standard 2-element Yagi's ~5.5 dBd)
  • F/B ratio: 25–35 dB at design frequency (significantly better than standard 2-element)
  • Feed impedance: ~50Ω — direct coax feed with a 1:1 current choke
  • Construction: wire on a simple PVC or fiberglass cross frame — no aluminum tubing required
  • Popular for: 10m, 15m, 20m portable and stealth installations, balcony beams

Moxon Dimensions — 10m and 20m

The Moxon rectangle dimensions are more complex than a simple dipole or loop because the tip gap and element spacing are critical to the F/B ratio and impedance. The Moxon Antenna Project calculator (moxonantennaproject.com) provides precise dimensions for any frequency and wire diameter — always use a calculator or NEC2 model rather than estimating.

10m Moxon at 28.500 MHz: Overall width (A): 11.4 ft Element length (B): 4.65 ft (each side of driven) Tip section (C): 0.56 ft (folded tip, each side) Gap between tips (D): 0.47 ft Overall depth (E): 4.66 ft 20m Moxon at 14.200 MHz: Overall width (A): 22.8 ft Element length (B): 9.30 ft (each side of driven) Tip section (C): 1.12 ft (folded tip, each side) Gap between tips (D): 0.94 ft Overall depth (E): 9.32 ft Feed impedance: ~50Ω Use 1:1 current choke at feedpoint
Build: 10m Moxon guide →

Building a 2-Element 20m Cubical Quad

Fiberglass spreader arms, wire loops, and a λ/4 matching section — approximately 7.5 dBd on 14 MHz.

1

Calculate All Dimensions

For 14.200 MHz: Driven loop = 1005 ÷ 14.2 = 70.8 ft (each side 17.7 ft). Reflector = 1030 ÷ 14.2 = 72.5 ft (each side 18.1 ft). Spreader arm length for driven element = 17.7 × 0.707 = 12.5 ft. Element spacing (driven to reflector) = 0.20 × (984 ÷ 14.2) = 13.9 ft. Total boom: 13.9 ft. Cut all wire 3% long for trimming.

Tip: Run the design through MMANA-GAL or 4NEC2 before cutting wire — verify the modeled feedpoint impedance and confirm the element spacing produces the expected gain and F/B ratio at your design frequency.
2

Build the Boom and Hubs

Cut a 1.5" aluminum tube boom to 13.9 feet. Fabricate or purchase two quad hubs — one for the driven element position, one for the reflector. Mount the hubs on the boom at the calculated positions. Insert four fiberglass spreader arms into each hub at 90° intervals, angling them approximately 5° downward from horizontal. Secure each arm with set screws and epoxy for permanent installation.

3

String the Reflector Loop

Start with the reflector — errors here are easier to correct before the driven element is in place. Cut 74.7 feet of wire (72.5 ft calculated + 3% extra). Starting at the bottom center, run the wire up to the top of one spreader arm, across to the next arm tip, down to the bottom opposite corner, and back to the starting point. Secure at each spreader arm tip with a small UV-resistant cord loop through the fiberglass tip. The wire should be taut but not under extreme tension — moderate tension is correct.

Tip: Tape the wire to the spreader arm along its length using self-amalgamating tape at the mid-point — this prevents the loop from shifting position in wind while not creating a rigid bond that stresses the spreader.
4

String the Driven Element Loop

Cut 72.9 feet of wire (70.8 ft + 3%). Run the loop in the same pattern as the reflector. Leave a gap at the bottom center for the feedpoint — approximately 2 inches between the wire ends. Connect both wire ends to an SO-239 feedpoint plate or a commercial quad feedpoint assembly. Leave the feedpoint accessible — you will need to access it for the matching section connection and any trimming.

5

Install the Matching Section

Cut a quarter-wave section of 75Ω coax for the matching section. At 14.200 MHz, the electrical quarter-wave in 75Ω coax (VF = 0.66 for solid PE): 234 ÷ 14.2 = 16.5 ft × 0.66 = 10.9 ft. Connect one end to the driven element feedpoint and the other end to the main 50Ω coax run. This matching section transforms the loop's ~100Ω impedance to approximately 56Ω — close enough to 50Ω for SWR below 1.3:1.

Tip: Wind 8 turns of the 50Ω feedline coax through an FT-240-31 toroid immediately after the matching section junction — this current choke prevents common-mode current from flowing back down the main feedline.
6

Raise and Initial SWR Sweep

Raise the antenna to its final operating height on the mast or tower. Connect the NanoVNA and sweep 13.5–15 MHz. The SWR minimum should fall near 14.200 MHz. If it is above 14.200 MHz, the driven element is too short — splice additional wire at the feedpoint gap. If below, trim equal amounts from both sides of the driven element. The reflector does not need to be trimmed — it sets the gain and F/B, not the SWR.

7

Optimize Reflector for F/B

The reflector length controls front-to-back ratio. With the antenna pointed at a known station or using the Reverse Beacon Network, adjust the reflector length for maximum F/B — lengthen the reflector (splice in wire) if F/B is low, or shorten slightly if the SWR minimum has drifted. The optimum reflector length produces a clear null off the back — typically 20+ dB below the forward gain. Document the final loop lengths for future reference.

Tip: The Reverse Beacon Network is ideal for optimizing a beam's F/B ratio — transmit CW on 20m and compare spot strength from stations in the forward direction versus stations directly behind the antenna. The ratio is your real-world F/B.

Does a quad really outperform a Yagi?

Yes, by a modest but real margin. A 2-element quad delivers approximately 7.5 dBd — comparable to a 3-element Yagi (~7 dBd) on similar boom length. The quad's additional advantage is a lower takeoff angle at the same physical height, which benefits DX propagation, and slightly quieter receive characteristics. The performance edge over a Yagi is real but not dramatic — typically 0.5 to 1.5 dBd. The mechanical complexity of building a quality quad is the main practical trade-off compared to an aluminum Yagi.

Why are fiberglass spreaders used instead of aluminum?

Aluminum is a conductor — if the spreader arms were aluminum, they would interact electromagnetically with the wire loops and significantly alter the antenna's resonant frequency, gain, and pattern. Non-conductive spreaders (fiberglass, bamboo, PVC) are transparent to RF and allow the wire loops to function as designed. Carbon fiber spreaders are sometimes used but require careful electrical isolation at all contact points because carbon fiber is also conductive — a carbon fiber spreader touching the loop wire creates a short circuit that destroys the loop resonance.

What is the feed impedance of a cubical quad loop?

A square quad loop fed at the bottom center presents approximately 100–130Ω in free space. Over real ground at typical operating heights, the impedance varies from 90 to 140Ω depending on height and surroundings. The most common matching approach for direct 50Ω coax connection is a quarter-wave section of 75Ω coax as an impedance transformer. Feeding at a corner rather than the center of a side changes the impedance toward 50–75Ω for some configurations — this varies enough with height that it requires measurement rather than calculation for precise matching.

How do I tune a quad antenna for maximum performance?

Tune in two steps. First, adjust the driven element length for minimum SWR at the target frequency — this sets the resonant point. Second, adjust the reflector length for maximum front-to-back ratio using the Reverse Beacon Network — longer reflector increases F/B up to an optimum, then decreasing. These two adjustments are somewhat independent: changing the driven element length shifts the SWR curve without much effect on F/B; changing the reflector length changes F/B and gain without much effect on SWR. Make small changes (1 inch at a time on 20m) and document each step.

Can I build a quad antenna for 40m?

Yes, but the physical size is a significant challenge. A 2-element 40m quad requires spreader arms of approximately 24.8 feet — nearly 25 feet long. This creates a structure approximately 35 feet wide and 14 feet deep, weighing considerably more than a comparable Yagi due to the wire loops and long spreader arms. Some operators have built 40m quads successfully with commercial-grade fiberglass spreaders and heavy-duty hubs, but it requires careful structural engineering and a substantial tower and rotator. Most operators building a 40m beam choose a Yagi over a quad for mechanical practicality.

What is the difference between a quad and a Moxon rectangle?

A standard 2-element quad uses two separate full-wave square loops — one driven, one parasitic reflector or director. A Moxon rectangle is also a 2-element beam but with a different geometry: the elements are folded dipoles where the tips bend back toward each other, creating a compact rectangle. The Moxon is smaller than a quad of the same band and feeds at ~50Ω directly without a matching transformer. Its forward gain is slightly less than a quad (~5 dBd vs ~7.5 dBd) but its front-to-back ratio is exceptional — typically 25–35 dB — making it excellent for interference reduction. Wire construction on a simple PVC frame makes the Moxon more accessible to beginners than a full quad build.

Moxon build guide →

How does rain and ice affect a quad antenna?

Quads are generally less affected by rain and ice than Yagis for an important reason: the loop element's resonance is less sensitive to its immediate dielectric environment than a dipole element's resonance. Rain wetting a dipole element changes its effective electrical length noticeably because water is a lossy dielectric directly on the conductor. On a quad loop, rain runoff tends to collect and drip from the bottom of the loop rather than wetting the entire conductor surface uniformly, reducing the detuning effect. Ice loading on the wire is a structural concern for both types — heavy ice can break wire loops — but the DC continuity of the quad loop allows simple drip discharge of static charges that would build up on isolated Yagi elements.

Is a multi-band quad better than separate antennas for each band?

A multi-band quad is more mechanically complex than separate antennas but offers the practical advantage of a single installation covering 20m, 15m, and 10m from one tower position. The multi-band design does slightly compromise performance on each individual band — the presence of the other bands' loops introduces some mutual coupling that affects gain and F/B compared to a dedicated single-band quad. For most operators the compromise is acceptable: a multi-band quad on 20m performs perhaps 0.5 dB less well than a dedicated 20m quad, which is a reasonable trade for covering three bands from one antenna.

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