Now in Beta: 160+80+40 on One inverted L. To add the 40m third band to the dual-band project, see . Particulars of a one year evaluation are now included in the article.
Without any change to the aerial wire, there is a way to use an already installed and working 160 meters Inverted L over FCP with Isolation Transformer (160 L/IsoT/FCP) as an excellent 80 meter end-fed halfwave L (80EFHWL).
We are not tacking on a compromise antenna just so we can say it covers 80 meters. Rather we enhance near-the-ground components of an existing efficient 160 inverted L to add an efficient omnidirectional 80m operation. Then a multiband solution for higher bands can use shorter 40m ½ λ wires without the need for longer 80m ½ λ wires.
The 80m EFHWL is a single wire antenna without the pattern null points of a vertical, dipole or inverted vee. The EFHWL has an essentially omnidirectional, roughly hemispherical 3D pattern that works well for both local and DX.
From 2011 until his passing, W0UCE worked 80m by feeding his 160m L/FCP as an 80EFHWL, using an early equivalent to the circuit below. The 80EFHWL was always his best performing antenna on 80m.
For local coverage, the 80EFHWL lacks the skip zone weaknesses of the vertical, having no doughnut hole in the high angle pattern. The horizontal wire fills in the doughnut hole without taking power from the EFHWL low angle pattern. The EFHWL has reduced RF ground fields in front of the L reducing ground loss versus a ¼ λ vertical. This supplies recovered loss to fill in the doughnut hole.
For DX, the 80EFHWL has a better vertical polarization component than a ¼ λ vertical with near or in-ground radials/counterpoise. A ¼ λ vertical has it's highest RF current down at the bottom of the vertical radiator where nearness to ground subjects it to maximum ground induction loss.
In contrast the 80EFHWL has its lowest RF current near the ground. It has its highest RF current at the top around the bend. This improves efficiency by keeping the bulk of RF current well away from ground and its radiation not obstructed by ground clutter and trees to low DX takeoff angles.
For DX, an 80EFHWL will defeat an 80m dipole or inverted V with supports in the 50-60-70 foot (15-20m) neighborhood. An 80m dipole or V needs at least ½ λ elevation, the 130 foot (40m) neighborhood, for it's best low angle DX.
Correctly done, the 80EFHWL is a proven strong performer. Some argue that the EFHWL is the best all-around single wire antenna for 80m.
The aspect of a low-band EFHWL keeping its performance from making it wildly popular has always been the need for a remote tuning device at the base of the halfwave wire. With a feed Z sometimes more than 2000 ohms, the EFHWL cannot directly match 50 ohm coax. It has no commercial off-the-shelf remote tuning product designed for it.
The existing 160L/IsoT/FCP feed configuration has already established the point of opportunity for 80 meter adaptation, with at least an IsoT. A relay at the center of the FCP easily flips the FCP to an effective and efficient counterpoise for 80m.
If you do not already have an existing 160 meter L/IsoT/FCP, you begin the 160/80 project by putting up a 160 meter L/IsoT/FCP and making all adjustments to get 160 working well. You do not tune the 80 meter matching circuitry until 160 operation is satisfactory.
The 80 meter tuning circuitry is switched out of line during 160 operation. Adding or changing the 80 meter operation will not materially affect 160m. Changing the aerial wire, the FCP, or the isolation transformer for the 160 meter operation will detune 80 meters.
For 80 meters:
1) The 160 meter L aerial wire is used as is, no changes. No traps or coils or double wires are needed in the aerial wire.
2) The 160 meter isolation transformer is used as is, no changes.
3) the 160 meter FCP has one item added, otherwise physically unchanged: A knife switch or high voltage relay is added shorting between the FCP feed point and the middle of the third wire to "flip" the FCP to 80M operation. See the red connection in the following diagram:
With the red wire connection open (not shorted), the FCP is on 160 meters. Closed (shorted), it's on 80 meters. The relay and shorting wire's physical layout needs to be brief. Otherwise they will detune the FCP's 160 operation and increase loss by undoing the net zero sum of fields. To avoid this:
3a) Keep the distance between the center of the FCP's third folded wire and the relay points or switch as short as possible.
3b) After 3a), keep the connection from the relay to the FCP feed as direct as possible. The relay or switch will need to be up on the FCP center support.
At K2AV this means the relay is mounted in the usual 4x4 sealable plastic electrical box affixed to the center spreader.
3c) At a site where the works are contained in a project box at the center of the FCP, 3a), 3b) requirements bear on wiring layout inside the box. When picking wire and insulation and routing these wires, remember the 8kV p-p RF running around. For these connections do not use wire with unknown insulation characteristics. Some lengths of wire/sleeving left over from trimming the isolation transformer leads may be a good choice. Or use #14 AWG (2.5 mmsq) bare solid copper wire in standard wall #12 PTFE tubing.
The shorting connection points are an RF high voltage point when open. The modeled RF voltage for 160 meter 1500 watt operation at the switching point is 8kV peak to peak, requiring attention to a shorting relay or switch able to tolerate 12 kV DC or better. Satisfying this need is discussed below.
4) For 80 meters, a DPDT knife switch or DPDT relay switches in a tapped parallel LC tuning network to tune the now high feed impedance of the unchanged aerial wire.
5) A later addition will extend this scheme to two ranges in 1.8-2 MHz and up to five ranges in 3.5-4 MHz. Each desired range on 80 will require a separate additional DPDT relay and pair of taps. This will require a switch box in the shack and multi-conductor cable to the switch.
Here is the diagram for a single tuned range on 160 and a single tuned range on 80. For those who only operate CW on 160 and 80, this simple circuit may be enough.
A single, separate twisted pair of wires should transport the relay energizing voltage for this single range per band setup. This wire pair will need a common mode choke at the tuning network to be prevent the wire pair becoming a source of noise to the antenna and a ground shunt to the antenna system.
There should be a second choke on the wire pair between the tuning network and the station entry ground, either just on the antenna side of the station entry ground or approximately 65 feet (20m) from the tuning network, whichever is closest to the tuning network. Place a common mode choke on the feed coax at this same point.
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It is clear from field experience there are no one-size-fits-all values for the coil and capacitor. You may have to experiment with values. Our original and work-most-of-the-time starting values are below.
Please advise us of changes in supply and/or new sources of supply for identical or equivalent material.
We currently estimate a fixed 500 ρF high voltage, high current (fully derated 5 kV, rated 10 amps RF at 3.5 MHz) transmitting doorknob or vacuum capacitor. It is easy enough to find fixed caps with the voltage rating. But other parameters are just as important.
The RF current rating at frequency must be known and is not always available. Do not use capacitors without a known, adequate current rating. Other than being destroyed by heat from I²×R loss, capacity change with heat will cause the tuning to wander. Unfortunately, the physical size of a doorknob cap does not guarantee its current carrying ability.
500 ρF, with adequate voltage and amperage ratings, can be provided in a number of ways.
♦ Vacuum capacitors are the most stable, generally with high voltage and current ratings, if one owns or wishes to procure them.
♦ Russian surplus transmitting doorknob caps are available that show a kVA reactive rating. Some of these Russian caps appear heavy duty, but we have scattered, verified reports of destroying "large" Russian caps with 1500 watts in this application.
Russian KVA lettering looks like kBAp or KBAP. Caps with these labels usually include a kB rating which is kV. Divide the kBAp by kB which will give you its most conservative maximum current rating. One such 470 ρF cap has 15kB and 40kBAp or 2.7 amps. That might be OK, depending on its dielectric material and physical surface area. It can certainly be tried, but without frequency derating curves can't be confidently engineered, and therefore gets no unqualified recommendation. You will know a particular cap is not going to make it if under full power the SWR starts to drift, indicating heat-induced change to the capacitor value.
See the HEC documentation below for an example of derating curves.
♦ Probably the least price, fully rated, made from currently produced, stock store-bought components, a 500 ρF transmitting capacitor can be made with three paralleled High Energy Corp (HEC) HT50 "barrel" style ceramic transmitting caps. Three 7.5 kV 170 ρF (HT50V171KA) in parallel will produce 510 ρF.
HEC HT50 transmitting caps actually manufactured by HEC are fully specified with derating curves on HEC's web site. See pp 10, 11 of the document. Three 7.5 kV 170 ρF in parallel will be rated 30 kVA, with a 3.5 MHz derated current of 5 amps each for a robust total 15 amps at 7.5 kV. See page 11 rating curve graph HT50V101KA, which applies to the 170 ρF's N750 material.
Three 170 ρF in parallel was deliberately chosen over a single HEC HT50 500 ρF for a number of reasons:
At this writing these 170 ρF caps, apparently three different brands including HEC, are available from Surplus Sales of Nebraska as their part (CFC)HT580170-75 , Look down the page under HT-50/58 Series. MFJ sells them as their 290-0170-7, two used as load capacitor padding on 160 in their AL-82, AL-1200 and AL-1500 QRO amps. You will have to order them verbally via Ameritron technical support, they (and most of their parts now) are no longer listed in their catalog or web site. RF Parts sells them as their 580170-7 . See links or inquire for prices. At this writing, the RF Parts illustration shows the HEC branding on the capacitor. So we have a source for the documented brand, with comparable price.
As of (V.2019.03.15), the bargain-priced JCSL-500-5S fixed value vacuum cap previously mentioned here is no longer for sale at MaxGain. From time to time such items will appear on Ebay or the sources above with limited quantities. The only way to find these bargains is to keep a lookout.
We currently estimate a one-size-fits-all coil at 10 to 12 bare turns, 4 turns per inch, of solid bare AWG 12 (IEC 4 sqmm) or larger copper wound on a 3 inch (75 mm) diameter form. This can be any sufficiently rigid high current coil format providing about 3 µH overall inductance. The coil will need enough space between windings to allow placing and soldering taps to vary µH and ratios for tuning. To reduce loss the winding form should be removed from the coil for actual operation. Support the coil at each end. However, do not remove the four polystyrene bars that support manufactured coil stock. 3/16 or 1/4 inch copper tubing hand wound on a 3 inch form and mounted without the form to insulators at the ends may be the least expensive and most efficient winding.
3 inch diameter 4 TPI bare #10 tinned copper is available as "coil stock" (see left) from MFJ, their part 404-0024, used in the output networks of their Ameritron AL-82,-1200,-1500 amplifiers, and repairs of same. You will have to order the coil stock verbally via Ameritron technical support. It and most of their parts now are no longer listed in their catalog or web site. This coil stock is a good choice for the 160-80 dual-banding project, with just enough space between turns to support taps. It is supplied in 11 inch lengths at far less than Barker and Williamson charges for the same diameter/wire size product.
A number of important information points apply to use of the MFJ coil stock. Please read all five below:
(A) There can be a back-order interval on coil stock until a manufacturing run. You should order this item far in advance of your need and be thankful we have a reasonably priced source at all.
(B) This project will only use three of the eleven inches stock length. MFJ only sells the eleven inch manufactured length. You may wish to share part of the length with others to save on cost. However, this writer is forever needing coil stock for something or another, and bought two 11 inch lengths the last time, just for himself. Once treated per (C) it has a near infinite shelf life.
(C) The coil stock itself is a bit fragile as manufactured. For this strengthening task only use Krazy Glue™ or an exact equivalent very thin consistency cyanoacrylate glue. Put a tiny drop of glue on both sides of the wire at all points where the wire is melted into the support rods. The very thin glue will soak into the tiny air bubble spaces where the wire embeds the plastic. Do not use a "regular" or "thick" glue. It will not soak into the bubble spaces.
Start on the 11 inch coil with a brand-new, unopened bottle of Krazy Glue. You will use most of the bottle placing 178 drops for the 11 inches. Previously opened Krazy Glue does not store well, suffering loss of ingredients to the air even with a tightly closed cap.
Allow the full 24 hours for full curing before handling or cutting the coil into smaller pieces. When you have done this, the coil will have a distinct rigid solid "feel" to it.
(D) When you are cutting a piece of the coil stock to use, leave extra length for forming mounting wires. To do this, leave an extra entire ¼ turn for connection on either end. Do not attempt to use the short ⅛ turn piece for connection. For three inches count 12 full turns plus two additional full ¼ turn sections, a total of 50 ¼ turn sections. In the middle of the 51st ¼ turn section cut the wire with a Dremel tool. Keep the angle of the cutting disk to the wire very small, almost parallel to the wire, to keep from scoring the adjacent turns. You can clean up the coil after you separate the 12 turn section.
Cut the wire before you cut the clear support rods. Otherwise you risk separating the wire from the support rods, which you will find amazingly difficult to repair.
Before cutting the support rods, twice carefully recount the ¼ turns, and twice carefully verify the cutting points. Mark the verified cutting points with a sharp tipped marker. It is very easy to get the cutting points mixed up if they are not marked.
Once the coil section has been separated, free the outside ends of the ¼ turn end wires from the support rods, cutting with the Dremel tool right next to the outer wire. You can then clean up the outer end of the ¼ turn worth of end wire with the Dremel tool.
Important: When forming the bends for the connecting ends of the coil, do not use the clear support rods as the rigid clamp for bending the wire. Use an end tip of a bench vise or vise-grip pliers to solidly grab the ¼ turn end wire right next to the clear support rod. Then make your bends, cuts, etc, with the vise protecting the fragile wire/support rod junction from any twisting or bending moment. Later on, if adjusting the mounting leads, always protect the wire/support rod junction.
(E) Until you have performed (C) on the coil stock, do not store or use this coil stock anywhere the air can be damp (including outdoors in an enclosure). Where the wire melts into the support rods, if the tiny bubbles get filled with water, carbon arc paths can develop under high power. The Krazy Glue fills the pockets where the tiny bubbles touch the wire. For that reason it is a good idea to do (C) when you first get the coil stock.
For the main relay that switches in the 80M circuitry, a single 12 volt DPDT Deltrol 20852-81 suffices well. You can find these at Allied Electronics . These are also stocked at Array Solutions at a markup, but may get you one in time when Allied is back ordered.
These Deltrol relays need to be protected from dampness in a weatherproof enclosure. See the first four bullet points at Balun Design's Installation Notes PDF for useful time-tested advice on weather-proofing an enclosure.
We had also been evaluating the Deltrol relay for shorting the FCP to flip it to 80M operation.
To understand the voltage requirements for the FCP shorting relay, in EZNEC Pro running the NEC4 engine on an L over FCP model, we inserted an EZNEC "load" in the FCP shorting wire, and set R and L to 0 (short) and set C to values up to 20 ρF to represent misc capacitances across an open relay. Clicking LOAD DAT on the main EZNEC window, NEC4 calculated as much as 3540 volts RF RMS across the open circuit. RMS voltage is needed to calculate power, etc.
To calculate the DC breakdown voltage most often quoted in relay specifications, we have to convert the RF RMS voltage to RF peak-to-peak. RF PP = RF RMS × 2.88. 3540 × 2.88 = 10195 VPP. That means that we could expect a relay with a DC breakdown voltage of 8 kV to arc if 1500 watts makes it to the FCP feed point. A minimum 12 kV, or better 15 kV DC breakdown gives a rounded figure plus a safety factor.
Modifications to the Deltrol DPDT relay produces an SPST normally open shorting relay with .160 inch (4 mm) of total contact gap space. Both Normally Closed contacts are bent outward to increase the gap between the armature leaf contact and the Normally Open contact. The new gap is 80 mils (2 mm). The connection between the armature leaf and the base connection pin is removed on both poles. The two armature leafs are then wired together, placing the two normally open contacts in series.
The 3.0 kV/mm dry air gap breakdown rule says each gap provides 6 kV isolation.
When measured with a Hi-Pot, either gap tested by itself breaks down at approximately 6 kV DC, according to the rule. However, when the two gaps are wired in series, the combined gap breaks down at only 9 kV DC. This is less than the possible 10 kV calculated operating voltage at the shorting point, as indicated in the NEC4 model. So 9 kV is inadequate at 1500 watts, but is enough to handle 500 watts (6 kV at the shorting point), easily handling a barefoot transceiver.
It is clear from measured results that one cannot add the individual breakdowns when gaps are put in series. So to handle 1500 watts, this application would take a pair of modified Deltrols, their coils in parallel, and their four contacts in series to handle QRO with 6+3+3+3 = 15 kV. This makes vacuum relays less expensive relatively, and intuitively far longer-lived in this actual use.
An installer may have a suitable 12+ kV vacuum relay on hand or reasonably available. Several stations originally considering Deltrol for the FCP shorting relay have managed to obtain 12+ kV vacuum relays from various sources.
Before purchasing a vacuum relay verify the manufacturer specs for the model of vacuum relay. Being called "HV" by the seller may mean anything. The most common vacuum relays, RJ-1A, HC-1, etc, at 2.5 or 3 kV DC are woefully short of the needed 12 kV. There are many vacuum relays with 5, 8, 10 kV DC ratings inadequate to this purpose.
Another source of confusion on voltage specs is some suppliers listing load switching voltage instead of voltage rating between contacts. When you see a vacuum relay with a 1000 or 1200 VAC rating it is probably the maximum under-load switching voltage that can be frequently exercised without a huge decrease in operational life.
SPST single throw vacuum relays may require making modification to the dual band circuit above to accommodate NC or NO contacts. Many available suitable 12+ kV vacuum relays have 24-26 VDC windings and so will require a power supply other than the common shack 12 VDC to power the switching.
At times, we have seen Jennings RD6A vacuum relays at Max-Gain at a very decent price. 15 kV DC, 24 volt coil, SPST Normally Closed. Potential users of the circuit will need to keep their eyes on the various sources for vacuum relays. They come and they go. K2AV bought an RD5A from Surplus Sales for his FCP shorting relay. The RD5A is SPST, 15 kV normally open contacts, and will allow his preferred power-off-selects-160M.
The vacuum relays above are most often used pulls from equipment, sometimes NOS. The only ham price new manufacture vacuum relay we are aware of is the Taylor brand VC2T-13-2 sold by RF Parts . This is an SPDT vacuum relay rated 15 kVDC, with a 12 volt coil and threaded mount. It will support power-off selects 160m using the NO contact or selects 80m using the NC contact.
The RD6A's normally closed contacts will require that power-off-selects-80M, and 24 volts applied selects 160. The Deltrol 20852-82 is the 24 volt version of the 20852-81, and if used for the tuning circuit switch will allow a single selection voltage for operation. Note that several contacts of the diagram above need to be reversed for power-off selects 80M.<== you are here
Do not tune the 80 meter addition until 160 operation is satisfactory.
80 meter tuning is done by alternately moving the 50 ohm tap, and a resonating tap which sets the electrical base of the coil. You will probably need to set the base and 50 ohm taps by moving clip leads while watching an RF analyzer. The tuning points can be marked and then soldered to for connection to the relay(s).
Switching from the shack is accomplished by supplying relay voltage for the band assigned the normally open contacts on the relays. Using Deltrol relays for the FCP short, coil voltage is supplied for 80 meters.