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Observations, analysis and modifications of the JPC-12 vertical antenna

By: KA7OEI
29 May 2024 at 17:34

The JPC-12 antenna (possibly made by BD7JPC) is relatively inexpensive a portable vertical antenna - made in China, of course - that may be found for sale at quite a few places  under a few different brand names (including "Chelegance"). The price varies very widely - sometimes well over $200 - but I got mine via AliExpress for about $120, shipped, about a year and a half ago.

Note: 

I analyzed the JPC-7 loaded dipole antenna - which is made by the same company and uses many of the same components - and reported on it in previous article, and you may find that discussion HERE.
Stay tuned for a future article about rewinding/testing the loading coils of the JPC-12 and JPC-7 for better performance and lower loss.

Figure 1:
All of the standard components of the JPC-12 kit.
Click on the image for a larger version.
As for a vertical antenna, there are only so many variations on a theme.  The JPC-12 is intended to be used as resonant vertical, and with its included coil, it is capable of operation down to 40 meters - but it can be operated sans loading coil at higher bands, adjusting the length of the telescoping section to resonance.

"The perfect is the enemy of the good"

The above statement should be kept in mind when doing any temporary, portable installation.  The idea is to have an antenna that will work "well enough" to do the job.  It's also likely that in the situation where you are portable, you will not (and cannot!) spend an inordinate amount of time tweaking things to eke out the last decibel.

This is not to say that one should not be mindful of good practices as too much corner-cutting can excessively impact performance and potentially replacing enjoyment with frustration.  One should achieve a balance between that which works well and something that will allow more operation than fussing about.

Remember:  The more time you spend trying to get that last bit of performance out of your system is less time that you are spending operating - and I'm presuming that operating is your goal.

What is included with the JPC-12

As shipped and as depicted in Figure 1, the antenna comes with these components:

  • Aluminum ground stake.  This is a pointed stake 9-5/8" (24.5cm) long end-to-end about 1/2" (1.3cm) diameter.  This stake has M10-1.5 (coarse) threads on the end - the same as all other male and female threads used on the other mast/coil components of this antenna.
This stake is intended to be pushed into the ground and be capable of holding it vertically - which works fine in fairly compact soil, but it may be inadequate for looser soil or sand requiring, instead, a longer stake or a bit of guying.  Faced with the situation where putting the stake in the ground was not an option (the soil was way too rocky) I have also clamped it to existing supports, such as a metal "T" stake using locking pliers.
 
While the antenna is ostensibly "grounded" with the stake, solely stabbing metal into lossy dirt is never going to result in an effective vertical antenna so its being "grounded" by the stake is incidental and not important to its overall performance:  It's going to be the system of radial and/or counterpoise wires that you set up that will form other "half" of any 1/4 wave vertical (which is really a form of dipole with the other half "mirrored" by the ground plane) antenna to make it work effectively.
  • Four aluminum mast sections.  These are hollow tubes with (pressed in?) screw fittings on the ends - one male and the other female, both with M10-1.5 coarse threads that may be assembled piece-by-piece into a mast/extension.  End-to-end these measure 13-3/16" (33.5cm) each, including the protruding screw - 12-3/4" (32.4cm) from flat to flat and are 3/4" (1.9cm) diameter.
    Figure 2:
    The feedpoint for the JPC-12.  The upper half (right)
    is insulating while the bottom portion is machined aluminum.
    Click on the image for a larger version.

  • Feedpoint assembly.  This has a (correctly-machined!) SO-239 (female UHF connector) - the shield of which connects to the bottom half while the top - which is isolated by a section of fiberglass tubing - is connected to the center pin.  On both ends are female M10-1.5 threads to receive the screw from the ground stake (on the bottom) and the "hot" portion of the antenna on top.  This piece appears to be well built and is 6-9/16" (16.7cm) long.
  • Adjustable coil.  This is a piece of what appears to be thermoplastic or possibly nylon with molded grooves for the wire.  This unit is connected to the others via a male threaded stud on the bottom and female threads on the top, both being M10-1.5 like everything else.

Figure 3: 
The adjustable resonator coil, wound with 1mm stainless-
steel wire.  (The markings are mine.)
Click on the image for a larger version.

The form itself is 4-1/2" (11.4cm) long not including the stud and 1-11/16" (4.3cm) diameter - wound with 34 turns of 18 AWG (1mm) stainless steel wire.  The coil has an inside diameter of approximately 1.66" (4.21cm) over a length of about 2.725" (6.92cm) and it has a slider with a notched spring that makes contact with the coil and this moves along a stainless steel rod about 0.12" (3mm) diameter that is insulated at the top, meaning that as the slider is moved down, the inductance of the coil is increased.
 
The coil has painted markings indicating "approximate" locations of the tap for both 20 and 40 meters when the telescoping section is adjusted as described in the manual using the four (originally) supplied mast sections.  The maximum inductance is a bit over 20uH and the DC resistance of the entire coil is about 4 ohms - more on this later.
  • Telescoping section.  This is a stainless steel telescoping rod that is 13-1/8" (33.4cm) long including the threaded stud (12-7/8" or 32.7cm without) when collapsed and 99-11/16" (8' 3-11/16" or 253.2cm) when fully extended - not including the stud.
As with all stainless-steel telescoping whips, you MUST maintain them - keeping them clean and lubricated:  More on this later in this article.
Figure 4:
This is the supplied "radial" kit - a 10-strand chunk of ribbon
cable - the ring to be sandwiched on the bottom of the feed.
Click on the image for a larger version.
  • Counterpoise/Radial cable.  This is in the form of a chunk of 10 conductor ribbon cable terminated with large (0.4", 1cm I.D.) ring lug on one end sized to fit over the M10-1.5 threads.  This cable is about 203" (16' 11" or 516cm) long, including the ring lug that is intended to be sandwiched between the bottom of the coil and the ground stake. As noted later in this article, this radial isn't as useful/convenient/versatile as one might initially think.
  • Padded carrying case.  This zippered case is about 14" x 9" (35.5x23cm) with elastic loops to retain the above antenna components and a zippered "net" pocket to contain the counterpoise/radial cable kit and the instructions.  There is ample room in this case to add additional components such as small-diameter coaxial cable - and enhancements to the antenna, as discussed below. 
  • Instruction manual.  The instructions included with this antenna are marginally better than typical "Chinese English" - apparently produced with the help of an online translator rather than someone with intimate knowledge of the English language.  The result in a combination of head-scratching, laughter and frustration when trying to make sense of them.  Additionally, the instructions that came with my antenna included those for the JPC-7 loaded dipole as well, printed on the obverse side of the manual.

Fully assembled with the originally-supplied components, the length of the antenna is about 13' 5" (411cm) not including the ground spike meaning that it is self resonant - without added inductance - at a bit below the 17 meter band.  This means that at 17 meters and above, the tuning can be done solely with adjustment of the telescoping section and the coil can likely be omitted entirely.  Below 17 meters additional inductance is required which is obtained by moving the slider of the antenna downwards, requiring all but the last 3-4 turns of the coil to obtain resonance on 40 meters.

Comments:

Build quality

I'm quite pleased about the overall build quality:  The design seems to be well thought-out, perhaps inspired by other (similar) products on the market.  The individual mast sections seem to be plenty strong and I've seen no indication of the end sections coming loose.  I have screwed eight of these sections end-to-end and held them horizontal and noticed very little drooping and no "permanent" bends.

The feedpoint - being a combination of aluminum and plastic - seems to be well-built, the bottom section being machined with a flat to accept the SO-239 connector.  The upper section appears to be fiberglass, threaded at the top to accept an aluminum plug into which female threads are tapped to accept threads of the mast sections.

Likewise, the coil itself seems to be well built, the 32 turns of wire set into a spiral groove molded into the body with the coil tap selection having firm, positive action.  As noted previously, the wire comprising the coil is, itself, about 1mm diameter (approximately 18 AWG) and is apparently austenitic (e.g.  non-magnetic) stainless steel.

While this wire is very rugged, the fact that it is stainless means that its resistance is quite high compared to copper - in this case the end-to-end DC resistance is about 4 ohms - but the RF resistance, taking the "skin effect" into account, is likely to be very much higher.

Using Owen Duffy's online skin effect calculator (link) and assuming 1mm diameter, 316 Stainless, the 4 ohms of DC resistance translate as follows to RF resistance including skin effect:

  • 3.5 MHz = 5.2 ohms
  • 7 MHz = 7.2 ohms
  • 14 MHz = 9.6 ohms
  • 28 MHz = 13.6 ohms

While these values would be for the entire coil remember that less than full inductance is typically used  - but the message is clear:  The fewer turns of coil you need to use, the lower the loss!   The total length of 1mm wire is estimated to be about 180 inches (457cm).  By comparison, copper wire of this same diameter and length would have a DC resistance of about 0.1 ohm - or a skin effective resistance of 2 ohms at 28 MHz.  Alternatives will be discussed later.

Using the supplied radials - or not!

Noted in most reviews is the nature of the included radial/counterpoise wire - particularly since there is little or no mention of how it is to be used in the included manual.  Clearly, the single ring lug is intended to be captured between the bottom of the feedpoint section with the SO-239 connector and the ground stake.

For use as a resonant radial, the length of the this cable (203" or 516cm) is approximately correct for 1/4 wavelength at 20 meters, but this is not really suitable for 40 meters.  For best efficacy, the radials should be elevated above the ground by about a foot (25cm) or so so that the 1/4 wave impedance transformation (e.g. the distal end of the radial being open being transformed to a "short" at the antenna end to make it work effectively) but laying it on the ground directly - particularly if it is dry - will usually work quite well.

Being 10 conductor ribbon cable, the opportunity exists to split the wire lengthwise to obtain individual wires to spread radially around the base of the antenna.  This wire - with its PVC insulation and rather small gauge conductor (likely 26 AWG) means that it is difficult for it to lay flat unless it is warmed by the sun on hot ground (or with rocks laid on the wire) - plus a large number of connected-together conductors from a split-apart ribbon cable are the makings of a portable rats-nest of wires that cannot easily wound/unwound later.

Most reviewers/users of this antenna - including myself - don't really like the "ribbon cable radial" system and personally, I have never used it - but I keep it in the kit, just in case.  

Location of the loading coil

While it might be tempting to place the loading coil immediately above the feedpoint, this is not the suggested location, but rather at the top of the four supplied screw-together mast sections immediately below the telescoping section.  This makes sense on several counts:

  • This elevates the coil above the ground, making it easier to adjust as it is at more convenient height (about 4' 3" or 130cm above ground).
  • Because it is the portions of the antenna that conduct the most RF current are those that will radiate the most, those same sections below the coil - and above the connection to the counterpoise - will emit the bulk of RF energy
  • The markings on the coil for 40 and 20 meters assume that you have placed the loading coil in the location described above using the original components in the kit.

From a practical standpoint, placing the loading coil immediately above the feedpoint will also work - albeit with some loss of efficiency - and this may be desirable if the base of the antenna (and radials) itself is elevated - perhaps by being clamping it to a fence post or table.  In this case one might place the coil closer to the feed point to keep it at a reasonable (accessible) height rather than needing to access the coil's tuning slider by standing on a ladder or chair. 

Augmenting/improving the JPC-12 with optional accessories

A bit of perusal among the goods of the various sellers of the JPC-12 (and the related JPC-7 dipole) will reveal that spare parts:  It's a pretty good idea that - if you find that you are using this antenna a lot - to get a few "extra" parts (I strongly suggest an extra telescoping section or two) when things inevitably get worn out or broken.  There are also several "accessories" that may be used with the antenna(s) that might be useful - some of which are discussed below - and other components that you can easily assemble and add to the kit.

Improved ground radial system

For a 1/4 wave vertical - and this antenna is exactly that, albeit electrically lengthened with a coil and tophad on the lower bands - half of the antenna is its mirror reflection from the ground.  As it is unlikely that most people will ever set up their antenna atop a metal surface or in salt water, a set of wires is typically deployed to locally simulate the needed reflective "ground" surface.

The common advice in years past has been to bury many, many ground radials just below the surface of the ground - advice that is practical in terms of avoiding trip-hazards and to provide a degree of lightning protection - equal or better performance may be had by deploying an array of radials that are odd-order quarter-wave multiples (1/4, 3/4, 5/4, etc.) that are elevated slightly above the ground.  Emperical testing (see the linked article below) that as few as three or four elevated, resonant radials can be quite effective - and this number of radials is perfectly manageable in a portable installation.

The accessories described below make it easier to quickly deploy a resonant ground radial system - elevated or not.

The ground radial plate 

Figure 5:
This is the "radial plate" - an add-on accessory.  Spade-lug
terminated radial wires connect easily under the wing nuts.
Click on the image for a larger version.

As shipped, the radial kit (ribbon cable) included with JPC-12 antenna is perfectly usable - but in the opinion of many (including myself) the supplied radials aren't particularly practical or convenient.  From the same seller as the antenna I purchased what is cryptically called a "JPC-12 PAC-12 Network Disk" - seen in Figure 5.

What this really is is an aluminum disk about 4-3/4" (12cm) in diameter with a series of eight wingnuts and screws around the perimeter with a center hole sized appropriate for the M10 stud on the top of the ground rod or one of the antenna elements.  This device makes the connection of individual ground radials equipped with spade lugs much more convenient.

In looking at Figure 5, you may have realized that it's sitting atop its protective pouch to keep the screws from tearing up the inside of the carrying case:  The rear pocket removed from an old pair of blue jeans!

Using individual wires for the radials

Figure 6:
Four radials on kite string winders - each long enough for 60
meters - with markers on the wires for the different bands.
Click on the image for a larger version.
Rather than using the original ribbon cable, I have four lengths of 22 AWG hookup wire on kite string cable winders (a pack of ten cost US$10 from Amazon - including the string!)  These four wires are terminated with spade lugs to slide under the screws on this pate and are each 44' (13.4 meters) long corresponding with the quarter-wavelength at 60 meters.

Marking the radials' lengths

At various points along the length of each of these wires are pieces of marked heat-shrink tubing to indicate the points corresponding to quarter-wavelengths of the various amateur bands from 60 through 10 meters and only as much wire as needed is unspooled from the cable winder to achieve the desired length for the intended band of operation:  These yellow tags can just be seen in Figure 6 among the wire on the winders.

For these marker tags I used heat-shrink tubing cartridges for my Brother label maker - but I could just have easily have written on  light-colored tubing with an indelible marker prior to shrinking them.  To keep these tags from sliding around I put a dab of "Shoe Goo" (rubber repair adhesive) on the wire and slid the tubing over it before applying heat, locking it into place with much greater tenacity than the compression of the tubing shrinkage alone:  Having used these radials in the field a quite a few times, I have yet to have one come loose.

Using elevated radials

From an operational standpoint, just three or four elevated, resonant radials will perform equally to or better to a large number of radials - resonant or not - buried in the ground.  The reason for this - alluded to earlier - is the fact that any open-ended conductor that is an odd multiple of a quarter-wavelength long (e.g. 1/4, 3/4, 5/4) will exhibit a low impedance on the opposite (antenna) end - which is exactly what we want.

Simply laying such a length on the "average" ground will tend to diminish this effect somewhat, but elevating it even a short distance above the ground will preserve it.  For more information and an analysis of vertical antennas with elevated radial systems see the article "A Closer Look at Vertical Antennas with Elevated Ground Systems"  by Rudy, N6LP - LINK.  It's worth noting the admonition of the author of this page to avoid the use of radials that are around 1/2 wavelength long and multiples thereof - likely for the reason that the nature of a free-space half-wavelength conductor is not to provide a low-impedance on their proximal end when the distal end is unterminated!

The obvious hazard of elevated radials is that of tripping - of you, the operator, others in the area, or animals, so it isn't necessarily practical in every situation.  If it is possible to control access to the area with the antenna - or raise the radial above the height of the average person for much of its length - then this is a good choice.

Figure 7:
Fiberglass driveway markers modified to mark/hold radials.
Click on the image for a larger version.

In my operation - typically out in isolated areas - I don't have much worry about tripping anyone other than myself so I obtained some 4' (1.2 meter) long fiberglass driveway marker stakes.  These bright-orange stakes are about 4" long each (122cm) each - much 1--  long to fit in the antenna case, so eight of them were cut to shorter lengths to allow them to fit in the case, yielding two pieces each - the bottom portion with the sharpened point cut to 11-3/4" (30cm) and the top portion cut to 13-3/8" (34cm).  To the bottom portion, I glued (again using "Shoe Goo") a 2" (5cm) long of 8.5mm I.D. stainless steel "Capillary" tubing (found on Amazon) so that the two pieces could be assembled to a single (mostly) non-conductive post about 26" (66cm) long.

Eight of these two-piece posts allow the support of four elevated radials at two points along their length, the radial wire being wrapped once or twice around to form a friction fit to keep them from sliding down.  At the distal end, the remaining lump of wire still on the kite string winder is simply wrapped and hung over the post once a slight amount of tension is pulled on it.

Figure 7 also shows something else:  I made a drawstring bag (again, from an old pair of blue jeans) that keeps all of these post pieces together and it can accommodate some of the extra mast sections, all while fitting in the original padded antenna case.

Comment: 

The reader should be conscious of the fact that for the purposes of this discussion, we are talking about a temporary, portable antenna rather than a permanent installation.  In the case of the latter, a different approach (the deployment of many, many radials, perhaps buried) is reasonable - but for a temporary antenna - where less effort to erect and break down is desirable - the use of four elevated, resonant (e.g. 1/4 wavelength) radials is likely to outperform the same number of radials laid atop the ground.  In either case, however, the antenna will be usable - and that's the entire point!

On-the-ground radials

The use of elevated radials is arguably most important on the lower frequencies of operation of this antenna - namely 40 and 30 meters - where efficiency of this "electrically small" antenna will suffer due to a number of factors, but maximizing the efficiency of the ground plane is one way to mitigate this.  In those cases where it is not practical to elevate the radials, the wires may simply be laid atop the ground.  

As these posts are intended for marking driveways they are bright orange, making them stand out, but near the top they have a piece of white reflective tape so that they will show up at night.  As I had this type of tape on hand I added a piece to the bottom section as well - just below the stainless steel capillary tube - to make them even more visible - particularly if the bottom and top portions are used separately to mark where an on-the-ground radial might be run to warn against a possible trip hazard.

The use of a "Magic Carpet" (e.g. "Faraday Fabric")

There is no reason why one could not use the aforementioned conductive fabric as part of their ground plane - but you would probably have to construct an additional component to connect to the fabric and use it effectively.  For this, a piece of clean aluminum or copper plate laid atop the fabric - possibly weighed down with a rock - should provide a low-impedance connection to it.

While I do own some of this "Faraday Fabric" (obtained from Amazon) I have yet to try it with this antenna - and when I do, I plan to perform an "A/B" comparison.  As of the time of this writing I have yet to see a serious, scientific and well thought-out comparison between a simple radial field and the use of just the fabric:  Most of these comparisons simply demonstrate that it is possible to get a good antenna match while using the fabric - but as we all know, simply getting a match does not mean that the antenna will work:  After all, a dummy load has a great match!

I expect that - at least on the sort of desert ground that I'm likely to encounter - the radials will "win" the contest - although I still plan to do a comparison:  I suspect that using both the fabric and radials will offer decent results - even when tuned to a higher band for which the lengths of the radials are not expected to work (e.g. 20 or 10 meters with 40 meter radials.)

Additional antenna height - both real and "virtual"

Figure 8:
The accessory top had kit consisting of a machined piece that
attaches to the top of the vertical with four telescoping rods.
Click on the image for a larger version.

Any antenna that has to be electrically lengthened with inductance is likely to suffer from efficiency loss as that inductor is unlikely to be comparatively lossy.  As the antenna is mechanically "about" 1/4 wavelength on bands above 20 meters, it make sense, then, that the lower bands that it is intended to cover - particularly 30 and 40 meters - need some additional inductance to bring it to resonance.  It further follows that anything that may be done to make the antenna "taller" will reduce the amount of needed inductance and minimize these losses.

Tophat capacitance

Another accessory available for this antenna is a small tophat attachment for the telescoping vertical section.  Often described as a "PAC-12 Capacity Cap" this consists of what looks like a knurled aluminum knob with five holes drilled around its circumference and yet another hole on the bottom sized to receive the "static ball" (really a short cylinder) atop the telescoping section.

Using a set screw to secure it to the top of the antenna, this kit contains four small telescoping whips (3-1/8" 8 cm long collapsed, 12-1/4" 31c fully extended - not including threads) that screw into the 5/8" (2cm) diameter center disk.  Assembled, the end-to-end length of two of the telescoping elements is 25" (98.4cm) which forms a four-spoke "disk" that adds to the effective height of the main telescoping section of the antenna by increasing the capacitance.  The idea (and hope) is that this allows the reduction of the amount of inductance needed to bring the system to resonance - and it also allows potential coverage of 60 meters as noted later.

The size and weight of this attachment is, in my opinion, about right:  Any larger or heavier, it would likely be too much for the fully-extended main whip to handle and expose it to excessive wind loading.  To be sure, one must always be very careful when handling the whip when fully-extended, anyway and adding the tophat increases the risk of damage.

Figure 9:
The top hat kit assembled - but the rods are not extended.
Click on the image for a larger version.

Testing has shown that the addition of the tophat - when the antenna has previously been tuned for 40 meters - lowers the resonant frequency by approximately 1 MHz indicating an increase of virtual height by about 12 percent at that frequency.  Even with the tophat the antenna falls short of being able to resonate at any 60 meter frequency with the normal complement of parts included with the antenna.

For the higher bands, the top-hat may be enough to eliminate the need for the coil on 20 meters - or at least greatly reduce the amount of coil and thus the potential loss.

Of course, the use of this top hat means that the existing coil marking scheme (e.g. the paint marks that show approximate slider position for the bands) is meaningless as tuning is changed - but if one is already prepared in the field for this (e.g. using an antenna analyzer, added markings to the coil for the new configuration, a paper template marked with pre-determined coil positions) then this is of little consequence.

This tophat kit is constructed fairly well, using a small grub screw with a supplied Allen key to attach it to the top of the telescoping section, but I noted that the key and the screw weren't well matched and couldn't be tightened too much with the key slipping.  Rummaging about in my collection of hardware I found several metric machine screws and a hexagonal brass stand-off with matching threads and I replaced the grub screw with the stand-off, allowing it to be attached firmly to the top of the telescoping section using just my fingers.

Additional mast sections

It should not be surprising to know that you can buy individual mast sections.  These are often described as being "dedicated lengthened vibrator for JPC-7 (PAC-12) multiband portable antenna".  I purchased two more of these sections when I first purchased the antenna, increasing its fully erect height from 13' 5" (411cm) to 15' 7-5/16" (476cm) and coupled with the tophat and the full inductance of the coil allows the antenna itself to resonate at approximately 4.7 MHz, allowing complete coverage of the 60 meter band.

Figure 10:
Four more mast sections to be used in a variety of ways - as
ground supports, or as the "live" mast itself.
Click on the image for a larger version.

At this extended height and with the tophat, this antenna was used in fairly high winds with gusts of 35 MPH (approx 67 kph) with no issues:  Having clamped the ground stake of this antenna to a metal fence post helped keep the antenna vertical and minimize sway certainly helped!

After using the antenna several times, I purchased yet two more mast sections (for a total of eight) - not only to have as spares, but also to elevate the bottom of the antenna still further.  Living in the desert west of the U.S. (Utah) it's often the case that there is only sand into which the ground stake can be pushed and it simply isn't long enough to adequately support the antenna:  Lengthening the ground rod with the addition of another mast section allows the ground stake to be pushed in farther and support the antenna without burying the feedpoint below ground level or stealing one of the mast sections from the antenna and reducing its height.  This is mostly a problem on the lower bands (40 and 30 meters) where one needs as much height as one can get to maximize antenna efficiency.

This extension also facilitates the use of an elevated ground radial system, placing the feedpoint - and the ground radial disk - at a reasonable height.

Maintenance

The telescoping whip(s)

The telescoping whip is certainly the most fragile component included and it - like any other telescoping antenna - is easily broken if one is not careful.  The "safest" way to collapse one of these things is to pull it down - section by section - starting from the bottom:  One should NEVER push it down from the top as that is just asking for problems.

As with any telescoping whips that I own, one of the first things that I do when I get it is to make sure that it is clean of dirt and oxidation (particularly if it has been "pre-owned") as this can cause the metal-on-metal - especially when the two metals are the same - to gall and seize up, making it more difficult to extend or collapse.  If I do find a section that is hard to move, I carefully examine it, often discovering slight scratches, buffing them out with very fine sand paper (1000 grit or finer) and/or steel wool (size 0000 or finer).

The final step - after cleaning with paint thinner or alcohol to remove any dust - particularly if it was just buffed with steel wool or sandpaper - is to put a light coating of oil on all sections when they are fully extended:  I prefer to use a PTFE ("Teflon") based lubricant like "Super Lube" (made by Synco) as it does not dry and become "gummy".  Extending and then retracting the whip a few times does a decent job of spreading out the lubrication - even getting inside the individual sections.

Although much smaller, I did a similar thing to the four telescoping whips that comprise the tophat.

I would consider this "cleaning and lubricating" to be a necessary maintenance item when using this antenna, needing to be done occasionally, with constant vigilance toward possible issues every time it is used.

Inductor slider

The adjustable inductor's components are all stainless steel - including the coil wire itself.  Besides being known for the fact that this material "stains less" than others, it is also known for galling - that is, developing tiny burrs on the surface and jamming up when it is used against the same type of metal:  In the case of stainless screws, nuts and bolts - if these gall, even if you ARE able to remove them without breaking them, they have to be replaced.

While the contact area on the slider is small enough that it is unlikely to gall and get "stuck", I noticed immediately a bit of "roughness" in its movement that indicated excessive metal-on-metal friction:  I could not tell if this was on the contact area of where the slider rubbed across the coil's windings or on the sliding rod itself - but it was probably a combination of both.

This "roughness" in movement was relieved with the application of lubricant - the same "Super Lube" used on the telescoping sections - also making the adjustment easier to do.

Improving the coil

As noted previously, the coil is wound with 18 AWG (1mm dia) stainless steel wire.  It is suspected that one of the main reasons why this type of wire is used despite its terrible losses - as compared with copper - is that this resistive loss increases the feedpoint resistance - but at least in relatively cool temperatures (below 90F or 32C) I wouldn't worry about running key-down for several minutes at 100 watts - or higher power with a low duty-cycle mode like CW or FT-4.

As it happens, one can juggle the proportions of a vertical antenna a bit to vary the feedpoint resistance - but if you consider that these same coils are also used in the JPC-7 dipole, the reasoning behind the use of stainless steel wire becomes more clear.  An electrically-short dipole - such as when the JPC-7 is configured for 40 meters - would ideally have a feedpoint resistance of just a few ohms - but this would not match at all well to a 50 ohm system:  Even a very low-loss antenna tuner would have difficulty coping and placing the tuner away from the antenna through a length of coaxial cable would make the situation even worse!

Having said that, testing was done that revealed that on the JPC-17 - while operating on the lower bands (30, 40 meters) a significant amount of power was being dissipated in the coil - enough to raise its temperature by 135F (75C) at 70-100 watts on 40 meters (lower loss on higher bands) - but rewinding the coil with silver-plated copper wire pretty much eliminated that element of loss.

A future article on this blog will detail the rewinding of this coil along with measurements/comparisons between the original stainless steel and rewound coil for both the JPC-7 dipole and this JPC-12 vertical which will eliminate any nagging worries about power handling capability.

Using the JPC-12 vertical in the field

I have used this vertical in the field a number of times, mostly with the "augmented" kit with the extra mast sections, top hat and ground radial plate and elevated radials - typically on 40 and 60 meters SSB, but also for POTA using CW.  While the signal reports comparing my signal with that of others using full-size antennas unsurprisingly indicates that this doesn't to as well as the others on the lower bands, conditions have generally been good enough that there was little difficulty in copying my signal.

Figure 11:
The JPC-12 vertical out in the wild in a slight breeze.
The tophat is installed as is a section below the radial
plate - along with extra sections to increase height.
Click on the image for a larger version.
 

As the ground here in Utah is usually rather poor making it difficult to simulate the "other half" of a vertical antenna, it is even more important that the radial system be effective.  While I usually configure it to have four radials elevated about 18" (0.5 meters) above the ground, I have also simply laid the radial directly on the sandy soil - or found some convenient sagebrush, scrub oak or some other low plant or small tree to support them off them ground - and have always had pretty good results.

While I like this antenna, I find it to be far less convenient than the JPC-7 loaded dipole in that the vertical takes quite a bit more time to set up, needing a bit of assembly of the various pieces and laying out of the radials.  With resonant radials, changing bands - and trying to maintain optimal performance - also makes it a bit awkward by the fact that the radials need to be shortened/lengthened as appropriate/

Practically speaking, having the radials laid out for 40 meters and running on 60, 30 or 15 meters isn't much of a problem, but picking a band that is an even multiple of the radials' base resonant frequency - being an odd half-wave multiple (e.g. 20 or 10 meters with a 40 meter radial) - will not work well as that is the worst possible radial length (other than zero length) to choose:  The half-wave length will not provide the low impedance at the antenna and it's also likely that the coaxial cable will become most of the radial, possibly causing a "hot rig" in terms of RF and the related ill effects (RF into the audio, computer/radio crashing, extra noise) from doing so.

If, however, I have a bit of extra time and I want a better signal that I would otherwise get from the loaded dipole or a mobile-mounted HF antenna, I would definitely set up the JPC-12.

* * * * *

Comment:  I analyzed the JPC-7 loaded dipole antenna - which is made by the same company and uses many of the same components - and reported on it in previous article, and you may find that discussion HERE

 

 

This page stolen from ka7oei.com

[END]


Observations, analysis and field use of the JPC-7 portable "dipole" antenna

By: KA7OEI
3 November 2023 at 16:47

Figure 1:
The JPC-7 and its original set of components in the case.  On
the left is a zippered section with the balun, strap, feedpoint
and mounting hardware for the elements.  On the right
can be seen the two telescoping sections, the two loading
coils and the four screw-together mast sections.
Click on the image for a larger version.
The JPC-7 (apparently by BD7JPC) is a portable dipole antenna - somewhat similar to the "Buddipole" - in that it is tripod-mounted, with telescoping elements that can be oriented horizontally.  Both use loading coils to increase the electrical length of the antenna, allowing them to operate down to 40 meters in their standard configuration.

I was able to get mine, shipped, via Ali Express for about US$170, but it is also sold domestically (in the U.S.) from a number of vendors - sometimes under the brand name of "Chelegance".

A portable antenna is not the same as a "home" antenna

As you might expect, this antenna is intended for portable use - and easy-to-assemble, quickly-deployable antennas are not likely to offer high performance compared to their "ful-sized, high up in the tree" counterparts that you might have at your home QTH.  Rather, this antenna's height is limited by the tripod on which it is mounted - which, for the lower bands where its height above ground is definitely below 1/4 wavelength - is likely to put it squarely in the "NVIS" (Near Vertical Incident Skywave) category - that is, an antenna with a rather high radiation angle that better-favors nearer stations than being a DX antenna.

Additionally, its total element length as-shipped (with the two screw-in sections and the telescoping whip fully-extended, sans coil on each side) is 125" (3.175 meters) - approximately a quarter-wavelength at 22MHz - near, but above the 15 meter band meaning - that for all HF amateur bands 15 meters and below it requires the addition of the coils' inductance to resonate the two elements.  Being a loaded antenna - and with a small-ish aperture and with coils losses - means that its efficiency IS going to be less than that of its full-sized antenna (e.g. half-wave dipole) counterpart.

Of course, the entire reason for using a "portable" antenna is to enjoy the convenience of an antenna that is quick to deploy and fairly easy to transport - and anyone doing this knows (or should know) that one must often sacrifice performance when doing this!

Having said this, after using the JPC-7 in the field several times I've found that it holds up pretty well against a similar "full size" antenna (e.g. dipole) on the higher bands (20 and up) while on 40 meters, subjective analysis indicates that it's down by "about an S-unit" (e.g. the standard 6 dB IRU S-unit).  For SSB (voice) operation, this is usually tolerable under reasonable conditions and for digital or CW, it may hardly be noticeable.

Figure 2:
The components included with the JPC-7 - except the
strap and the manual.
Click on the image for a larger version.

What is included with the JPC-7:

  • Four aluminum mast sections.  These are hollow tubes with (pressed in?) in screw fittings on the ends - one male and the other female, both with M10-1.5 coarse threads that may be assembled piece-by-piece into a mast/extension.  End-to-end these measure 13-3/16" (33.5cm) each, including the protruding screw - 12-3/4" (32.4cm) from flat to flat.  These are 3/4" (1.9cm) diameter.  There are two of these sections per element to achieve the  125" (3.175 meter) length of each.
  • Telescoping sections.  These are stainless steel telescoping rods that are 13-1/8" (33.4cm) long including the threaded stud (12-7/8" or 32.7cm without) when collapsed and 99-11/16" (8' 3-11/16" or 253.2cm) when fully extended - not including the stud.
As with all stainless-steel telescoping whips, it is strongly recommended that you lubricate the sections as soon as you receive them.  As with about every telescoping whip you will ever see, these sections are "stainless on stainless" and as with many friction surfaces between the same type of metal, they will eventually gall and become increasingly difficult to operate as they scratch each other.  I use PTFE (Teflon) based "Super Lube" for this purpose as it does not dry out and become gummy as normal distillate oils like "3-in-1" or "household" do.  Do not use "lubricants" like "WD-40" as these aren't actually lubricants in the traditional sense in that they tend to evaporate and leave a varnish behind.  If the sections do get stiff over time due to surface abrasion, a buffing with very fine steel wool and/or very fine (1000 or higher) grid sandpaper followed by wiping down and lubricating may help loosen them.
  • Adjustable coils.  These are constructed of what appears to be thermoplastic or possibly nylon with molded grooves for the wire.  This unit is connected to the others via a male threaded stud on the bottom and female threads on the top, both being M10-1.5 like everything else.
The form itself is 4-1/2" (11.4cm) long not including the stud and 1-11/16" (4.3cm) diameter - wound with 34 turns of #18 (1mm) stainless steel wire with an inside diameter of approximately 1.66" (4.21cm) over a length of about 2.725" (6.92cm).  It has a slider with a notched spring that makes contact with the coil and this moves along a stainless steel rod about 0.12" (3mm) diameter that is insulated at the top, meaning that as the slider is moved down, the inductance of the coil is increased.  I suggest that a drop of lubricant (I recommend the PTFE-based "Super Lube" as it doesn't dry and get gummy) be applied to the slider to make it easier to adjust and to minimize the probability of galling.
 
The coils have painted markings indicating "approximate" locations of the tap for both 20 and 40 meters when the telescoping section is adjusted as described in the manual.  These coils are wound with 1mm diameter (approx. 18 AWG) 316 stainless steel wire:  The maximum inductance is a bit over 20uH and the DC resistance of the full coil is about 4 ohms - more on this later.
  • Figure 3:
    A close-up of the feedpoint mount showing the
    brass inserts and index pins.  The holes in the knurled
    knobs are sized to receive the miniature banana plugs
    from the balun.
    Click on the image for a larger version.
    Feedpoint mount.   This is a heavy plastic piece molded about pieces of brass into which the elements/coils are threaded.  There are three 10mm x 1.5mm female threads into the brass inserts plus another female thread of larger size (1/2" NPT) into which the aluminum 5/8" gaffer stud mount is screwed.  On the surfaces with the brass inserts and the 10mm x 1.5mm female threads are a series of index holes into which the element mounts (described below) are seated to allow the elements to be adjusted at various angles.  Electrical connection is made via holes in the brass to receive 2.5mm miniature banana plugs (visible in Figure 3) which contact the adjacent 10mm x 1.5mm female thread bodies.
Element mounts.  These are two heavy-duty nickel-plated brass adapters that are held to the feedpoint mount via 10mm x 1.5mm screws with large handles - both included.  Into the mounting surfaces are holes to receive index pins allow the elements to be rotated to various angles - from a horizontal dipole to a "Vee" configuration - and even to an "L" with one element vertical and the other horizontal.  It can also be configured with just a single element as a plain vertical if one so-chooses - the counterpoise/ground needing to be supplied by the user.  Figure 8, below, offers a better view of how this is used.
  • 5/8" stud (gaffer) mount.  As mentioned earlier, this kit includes a male 5/8" stud mount commonly found on photographic lighting tripods.  The other side of this has 1/2" NPT pipe threads that screw into the feedpoint mount.  This piece is shown in Figure 4.

Figure 4:
5/8 stud mount adapter to be used with
lighting tripods.  The "other" side is a 1/2 inch
NPT pipe thread that screws into the feedpoint mount.
Click on the image for a larger version.

  • 1:1 balun.  This appears to be a "voltage" balun, with DC continuity between the "balanced" and "unbalanced" sections and across the windings themselves.  This is in contrast to a "current" type balun that would typically consist of feedline, twisted pair or two conductors wound as a common-mode choke on a ferrite core. More on this later.
  • Hook-and-loop ("Velcro") strap for the balun.  This is used to attach the balun to the mast to prevent the weight of the coax and balun from pulling on the feedpoint mount.  This strap appears to be generic and doesn't really fit the balun too well unless it is cinched up, so I zip-tied it in place to keep both of them together. 
  • Padded carrying case.  This zippered case is about 14" x 9" (35.5x23cm) with elastic loops to retain the above antenna components and a zippered "net" pocket to contain the components for the antenna mount, balun, and the instructions.  There is ample room in this case to add additional components such as coaxial cable - and enhancements to the antenna, as discussed below.  
  • Instruction manual.  The instructions included with this antenna are only somewhat better than typical "Chinese English" - apparently produced with the help of an online translator rather than someone with intimate knowledge of the English language resulting in a combination of head-scratching, laughter and frustration when trying to make sense of them.  Additionally, the instructions that came with my antenna included those for the JPC-12 vertical as well, printed on the obverse side of the manual.

Construction and build quality

About a year ago I purchased a JPC-12 vertical antenna and it shares many of the same components as this antenna - the only real differences are that this antenna comes with two telescoping whips and loading coils, the center mount for the elements, a 1:1 balun, and the 5/8" stud adapter for the center mount.

Many of these components are the same as supplied with the JPC-12 vertical:  The loading coils, the telescoping whips, and the screw-together antenna sections.  In other words, if you have both antennas, you can mix-match parts to augment the other.  You can, in fact, buy kits of parts for either antenna to supply the missing pieces to convert from one to the other.

Mechanically, this antenna seems to be quite well built:  During use, I have no sense of anything being "about to come apart" or "just barely good enough".  I suspect that the designers of this antenna did so iteratively, and the end product is a result of some refinement over time.  The only really fragile parts are the telescoping whips, but these things are, by definition, fragile - no matter who makes them!

How it is mounted

This antenna does NOT come with any tripod or other support, but it offers three ways of being mounted:

  • 1/2" NPT threads.  The center support, as the primary mounting, has female 1/2" NPT threads.  If you have a piece of pipe with that type of thread on it, you can mount the antenna directly to it.
  • 5/8" male stud mount.  This antenna comes with a machined aluminum mount (seen in Figure 4) that screws into 1/2" NPT threads in the center support that is a 5/8" stud mount - sometimes referred to as a "Gaffer" or "Grip" mount - of the sort found everywhere on tripods used for holding photographic lights.
  • 10mm x 1.5mm thread.  If you want to configure this antenna as a dipole, you also have the option of using a 10mm x 1.5mm thread that is on the side opposite the female threads into which the 5/8" stud mount screws.  While this thread isn't particularly common in the U.S.A., it would seem that this is a common size for portable antennas everywhere else in the world and hardware of this size is available at larger U.S. hardware stores.  As this mounting point may be used as part of the antenna
    Figure 5:
    A homebrew double-female 5/8 stud adapter.  These adapters
    have 3/8" threads and were attached using a thread
    coupler.  This piece was necessary as both the antenna and my
    tripod have male 5/8" stud mounts on them!
    Click on the image for a larger version.
    (when configured in an "L" shape or if configured as a vertical-only)
    so it's the same threads as the screw-in element sections.

For me the 5/8" male stud mount is the most useful as it happens that I have on hand an old gaffer tripod (light stand) of this sort - but there's a catch:  It, too, has a 5/8" male stud mount!  It would seem that these tripods come both ways - with either a male or female 5/8" mount, but for less than US$15 I was able to construct a "double-female" adapter that solved the problem.  From Amazon, I ordered two 5/8 female stud to 3/8"-16 adapters and coupled them together with a 3/8" thread coupler as seen in Figure 5.  The only "trick" with this was that I had to sort through my collection of flat washers to find the combination of thicknesses that resulted in both knobs facing the same direction when the adapters were tightened to the thread coupler.

Element configuration

As with any antenna that you are likely to come across, the only portions of the antenna that actually radiate energy in the far field are those with current flowing through them:  The higher the current, the more energy is radiated.  By extension, the very ends of the wire - or, in this case, the ends of the telescoping section - have essentially zero current and do not radiate.  As the total length of conductors prior to the loading coil (screw-together sections, feedpoint mount, connecting wires) is about 56" (1.42 meters) this represents only about 3.6% of a wavelength at 40 meters.

It is for this reason that the preferred configuration is to have the screw-together sections connected directly to the feedpoint mount, then the loading coil and then the telescoping section, placing the loading coils nearly 30" (75cm) from the feed.  As the total length of the telescoping sections alone put together is about 198" (5 meters) - which is about 12.5% of a wavelength - you might think that they are doing the lions share of radiating - but that's not really the case.

Particularly at lower bands, it is understandable why coil losses are of such importance - and also why even a relatively small amount of lengthening of the antenna can improve performance on the lower frequencies:  Adding two more screw-together sections (one per side) increase the length "before the loading coil" from 56" to 84" (2.13 meters) - or about 5.3% of a wavelength and not only increase the aperture of the antenna, but it will also allow a reduction of the amount of inductance (and coil loss) required to resonate the antenna.

Further improvement can be made by adding a bit of extra length to the telescoping whips by clipping hanging wires to the end of it:  This will further reduce the amount of inductance needed to resonate, but it will also increase the effective portion of the whips that are carrying RF current.  (This is discussed further in the section on 60 meter coverage, below.)

Frequency coverage

This antenna is advertised to cover 40 through 6 meters - and this is certainly true:  When the four supplied mast sections are installed (two per side) the lowest frequency at which it can be resonated with the telescoping rods at full extension and the inductors set at maximum is around 6.7-6.8 MHz - well below the entirety of the 40 meter band.

On 40 meters, the 2:1 VSWR bandwidth was typically around 120 kHz:  A 2:1 VSWR is about the maximum mismatch at which most modern radios will operate at full power before SWR "foldback" occurs, reducing transmit power.  Of course, if your radio has a built-in tuner - even one with a limited range - you will certainly be able to make the radio "happy" across the entire 40 meter band without fussing with the antenna, even if it isn't tuned exactly to your operating frequency.

On the other extreme, with the minimum coil inductance and the two telescoping rods at maximum extension the resonant frequency was about 21.7 MHz:  This means that for all amateur bands 15 meters and lower, you will need the inductors - but for 12 meters and up you can omit them entirely (which is recommended!), bringing the antenna to resonance solely by adjusting the length of the telescoping sections.

Tuning the antenna

This may be where some people have issues.  I am very comfortable using a NanoVNA:  I have several of these as they are both cheap and extremely useful - the only down-side really being that their screens are not easily viewed in direct sunlight - but simply standing with my back to the sun was enough to make it usable as all one is trying to see is the trace on the screen rather than any fine detail.

The biggest advantage of the NanoVNA over a traditional antenna analyzer is that you get the "big picture" of what is going on:  You can instantly see where the antenna is resonant  - and how good the match may be.  More importantly, you can see at a glance if the antenna is tuned high (too little inductance) or too low (too much inductance) and make adjustments accordingly whereas using a conventional antenna analyzer will require you to sweep up and down:  Still do-able, but less convenient.

Tuning is somewhat complicated by two factors:

  • There are two coils to adjust - and they must both be pretty close to each other in terms of adjustment to get the best match.  Simply looking at the coils one can "eyeball" the settings of the slider/contact to get them very close to each other - something that becomes easier with practice.
  • The "resolution" of the inductors' adjustments is limited by the fact that one can make adjustments by one turn at a time with the slider.  At 20 meters and higher, being able to only adjust inductance one turn at a time is likely to result in the best match being just above or below the desired frequency.  At lower frequencies (lots of turns) - say 40 and 30 meters - you can likely get 2:1 or better by adjusting the coil taps alone, but at higher frequencies you will likely need to tune for the best match just below the frequency of interest and then shorten the telescoping rods slightly to bring it right onto frequency.

 Once I'd used the antenna a few times I found that I could change bands in 2-3 minutes as I would:

  • Lower the antenna to shoulder height so that the coils and telescoping rods may be reached.  If you had previously shortened the telescoping elements for fine-tuning a band you should reset them to full length.
  • Set the NanoVNA to cover from the frequency to which it is already tuned and where I want to go:  If I was setting it up for the first time I would set the 'VNA to cover above and below the desired frequency by 5 MHz or so so I could see the resonant point even when it was far off-frequency.  After using it a few times you will remember about where the coil taps need to be set for a particular band.
  • On the NanoVNA I would then set a marker to the desired operating frequency.
  • I would then "walk" both coils up/down to the desired frequency while watching the 'VNA.  As the tuning of the elements interact, you may have to iterate a bit to get the VSWR down.  Again, you may have to tune for best match at a frequency just below the target frequency and then shorten the telescoping sections.
  • I would raise the mast to full height again.  I noticed  a slight increase in resonant frequency (particularly on the lower bands - 40 and 30 meters) by raising the antenna on the order of 50 kHz on 40 meters.  Usually, this doesn't matter, but with a bit of practice/experience you'll be able to compensate for this while tuning.
  • A match of 2:1 or better was easily obtained - but don't expect to get a 1:1 match all of the time as the only adjustments are those of resonating the elements and nothing to take into account the actual feedpoint resistance at resonance.  Practically speaking, there is no performance difference between a 2:1 and 1:1 match unless your radio's power drops back significantly:  An antenna tuner could be used, but this will surely insert more loss than having a modest mismatch!

Figure 6:
As with almost any inductor adjustable using sliders, care
should be taken to assure that only one turn is being touched
by the contact, as shown.
Click on the image for a larger version.
All of that sounds complicated - and it may be, the first time doing it - but I found it to be very quick and easy, particularly after even just a little bit of practice!

Carefully adjusting coil taps

 If you look very carefully at the sliding coil taps you'll notice that if very carefully adjusted that they will contact just one turn of wire - but it is almost easier for the contact spring to bridge two turns of wire, shorting them together.  When this happens the inductance will go down slightly and you may see the resonance go up in frequency unexpectedly.  Additionally, the shorting of two turns can also reduce the "Q" (and efficiency) of the coil slightly.

If you are aware of this situation - which can occur with nearly all tapped inductors adjusted with a slider - you can start to "feel" when the slider bridges two turns of the coil and avoid its happening as you make the adjustments.

* * *

Suggested modifications/additions:

All electrically-short antennas that require series inductance for tuning to resonance - like this one - will lose efficiency due to losses in the coil, but this can be offset - at least somewhat - by increasing the length of the elements themselves.  One of the easiest ways to do this is to purchase a couple of extra screw-on mast sections:  The addition of one on each side will increase the total length of the antenna by about 25" (64cm) and allow a slight decrease in the required inductance - resulting in slightly lower loss and increase the aperture of the antenna slightly.  These additional screw-on sections are typically available from the sellers of the antenna for between US $10 and $15 each but are often called something like "Dedicated lengthened vibrator for JPC-7 (JPC-12)" or similar due to quirks of the translation.

60 meter operation

Figure 7:
The elements may be lengthened by clipping a lead to each
end of the telescoping sections, reducing the amount of
needed inductance - and also allowing resonance on lower
bands - in this case, 60 meters.
Click on the image for a larger version.

While adding two additional sections (on on each side, between the coil and the whip) - and rearranging the antenna with the coils located next to the feedpoint (rather than the usual configuration in which the coils are located away from the feedpoint) - will bring the resonant frequency down to about 5.7 MHz with full inductance and extension of the telescoping sections.  In this configuration, the added length beyond the coil adds significant capacitance, lowering the resonant frequency as compared to the normal coil location

The antenna can be made to cover 60 meters by clipping on short (18" or 46cm) jumper leads to the very end of the antenna elements and let them hang down.  Despite this being a less desirable configuration in terms of RF current distribution, in testing on the air, the signals were about 1 or 2 "S" units below a full-sized dipole, but still quite good for a fairly compact antenna that was  close to the ground in terms of wavelength.

If you wish to use the "stock" antenna on 60 meters rather than buying two extra screw-together sections, you'll need about 48" (1.25 meters)  of wire on each end:  For this I simply used two pair of 24" (approx. 100cm) clip leads connected end-to-end, each pair hanging from the tips of the telescoping section.

Longer is better

Of course these "extension" leads can be used for all bands for which the coils are needed to lower the inductance and reduce losses:  As it will always be the parts of the antenna that carry the most RF current that radiates the vast majority of the signal - and since those portions will always be the sections right near the coils for this type of antenna - adding these dropping wires at the ends won't appreciably affect the antenna pattern or its polarization.

As there is plenty of room to do so in the zipper case, I have since added two extra sections and two sets of "clip leads" permanently into the kit.

Get extra telescoping sections!

Finally, I would order at least two extra telescoping sections as these are the most fragile parts of the antenna kit.  These can also be ordered from the same folks that sell the antennas for US $12-$16 each and are typically referred as something like "304 stainless steel 2.5M whip antenna for PAC-12 JPC7 portable shortwave antenna". 

The reason for ordering two of them is that if the antenna falls over, both whips are likely to be damaged (ask me how I know!):  The cost of getting two extra whips is likely to be less than the cost of fuel for even a modest road trip to wherever you are going, so their price should be kept in perspective.  As the zippered case for the antenna has plenty of extra elastic loops inside, there is ready storage for these two extra whips with no modification.

A word of caution:  However you store them, do not allow the telescoping whips to lay loosely in the case:  If they bash into something else they can be easily dented which may make it impossible for them to be extended/retracted.  For this reason they should be secured in the elastic strap, or individually in a tubes or padded cases.

Note:  There are also available much heavier and longer telescoping whips with the same M10x1.5 thread that would easily allow 60 meter coverage:  I have not tried these to see how well they would work, mechanically, or if it would even be a good idea to do so (e.g. extra stress on the tubes, coils, mounting point - or how stable such a thing might be on a tripod).

Figure 8:
The mounting of the balun, just below the feedpoint mount.
The index holes allow flexibility in the orientation, the
connection being made by 2.5mm banana plugs.
Here, the antenna is shown with the elements configured
one hole higher than "flat", forming a lazy "Vee"
shape as seen in Figures 9 and 10.
Click on the image for a larger version.

Additional comments:

"To vee, or not to vee"

The feedpoint mount has a number of indexed holes that allow the elements to be mounted in a variety of configurations, from flat, in a number of "Vee" configurations, or even an "L" or vertical configuration.  

Personally, I use the flattest "Vee" configuration as seen in Figures 8, 9 and 10.  This configuration keeps the drooping ends of the telescoping whips higher than the feedpoint and helps clear any local obstacles (trees!)  - and just looks cool!

As can be seen in Figure 8, the connection between the balun and the feedpoint is made by plugging 2.5mm miniature banana plugs into the brass receptacles on the feed.  Shown in the photo are connections to the two sides, typically used for a dipole arrangement, but the third, unused connection on the top could be used to hold an element horizontal while one of the side connections hold it vertical - more on the use of this antenna as a vertical in the next section.

It should be no surprise that these 2.5mm miniature banana plugs are quite small and fragile and if one isn't careful - say, by allowing the weight of the balun to be supported by the wires rather than using the hook-and-loop strap - they can be broken.  For this reason I ordered a pack of ten 2.5mm banana plugs from Amazon and made a pair of short (4", 10cm) leads - one end with a small alligator clip and the other with a 2.5mm banana plug - to allow me to make a temporary connection should one get broken off in the field - something that could torpedo an activation if you didn't have spare parts! 

Operating as a vertical antenna

Because of the flexibility of the mounting point, it is possible to use this same kit as a vertical antenna with the second element as a resonant (rod) ground "plane" if - due to space or personal preference - emitting a signal with a vertically-polarized component is desired.  While this will certainly "work", if you do plan to operate with vertical polarization its recommended that you add several (2 or more) wire "radials" or counterpoises.

Because of the included balun (more on this in a moment) the coaxial feedline itself will not act as an effective part of the counterpoise network so rather than connecting additional radials to the shield, the ends of the wire should be clamped under the washer/bolt that holds the horizontally-configured element in place.  Of course, one need not use the balun and connect the coaxial cable directly, but if you choose this option you will be on your own to supply the means to make such a connection.

For best results with the fewest number of radials, choosing lengths that are odd-number quarter wavelengths long (1/4, 3/4, 5/4) and keeping them elevated a foot (25cm) or more off the ground is suggested as this will help minimize "ground" losses.  Having said this, almost no matter what you do, you will probably be able to radiate a useful amount of signal:  Operating CW or digital modes offers an improvement in "talk" capability owing to their efficiency - but if you are planning to operate SSB, it's worth taking a bit of extra time and effort to maximize performance.

Would I operate this antenna in "vertical" mode?  While I don't have plans to do so, I have purchased an extra ground stake of the sort used on the JPC-12 vertical, and the short banana plug/clip lead jumpers that I made could be used to make a temporary connection directly to a coaxial connector.

Nature of the balun

The supplied balun has a 1:1 impedance ratio and has DC connection between the input and output - but since there is a DC connection between all of the conductors, it is more than a simple current balun (e.g. transmission line wound on ferrite).  As the balun seems to work well, I have no reason to break it open to figure out what's inside, but I did a bit of "buzzing" of the connections with a meter to measure inductance and here are the results:

  • Between coax shield and center conductor:  16.9uH
  • Between red and black (on antenna side):   16.9uH
  • Between center coax and black:  38.5uH
  • Between center and red:  3.4uH
  • Between Shield and black:  3.4uH
  • Between Shield and red:  3.4uH
  • The DC resistance between any combination of the leads is well under 1 ohm.

What does this tell us?  The inductance readings of about 16.9uH indicate that this may be a voltage balun providing about 500 ohms of inductive reactance at 5 MHz - more than enough for reasonable efficiency.  The interesting reading is the inductance between the center coaxial connection and the black wire which is only twice the inductance of the input or output windings:  If there was a direct connection between one of the coax and one of the output wires this would imply twice the number of turns and four times the inductance - but since it is only twice, this indicates that the total number of turns in the "center coax to black" route is about sqrt(2) (or 1.414x) as many turns as the primary/secondary - or there is another inductor in there.

Figure 9:
The JPC-7 backgrounded by red rock during a POTA
operating in K-0010.
Click on the image for a larger version.

While I'm sure that the balun is very simple, its exact configuration/wiring escapes me at this time.

Coil losses

As mentioned earlier, the coil is wound with 18 AWG (1mm diameter) type 316 stainless steel wire.  Fortunately, this wire appears is austenitic - which is to say that it is not of the variety that is magnetic and thus has a permeability of unity:  Were it magnetic, this would negatively impact performance significantly.

Knowing the diameter of the coil form and the fact that there are 34 turns, we know that the total length of the wire used is approximately 180 inches (457cm) and measurement shows that the stainless steel wire coil has a total DC resistance of about 4 ohms.  Using Owen Duffy's online skin effect calculator (link) and assuming 1mm diameter, 316 Stainless we can calculate the approximate RF resistance including skin effect - the tendency for RF to flow on the outside skin of a conductor rather than through its cross-section - versus frequency:

  • 3.5 MHz = 5.2 ohms
  • 7 MHz = 7.2 ohms
  • 14 MHz = 9.6 ohms
  • 28 MHz = 13.6 ohms

If I make a very broad assumption that the feedpoint resistance at each coil is about 25 ohms (the two in series being around 50 ohms) we can see that in this hypothetical situation about a third of the total resistance could be due to the coil, and since P = I2R - and if we presume that the current is consistent throughout the coil (it probably is not) we can roughly estimate that the total power loss will be proportional to the resistance implying that about 1/3rd of the total power is lost in the coil.  In practical terms, a 33% power loss is around 4.8dB - still less than one "S" unit, so this loss may go unnoticed under typical conditions.

In operation, we would be unlikely to need all - or even most of the turns of the coil for operating on the higher bands, so the overall coil losses are likely to go down as the need for loading inductance at these frequencies is also significantly reduced:  Since we actually use only about 2/3 of the turns of the coil on 40 meters, the loss is more likely to be something on the order of 5 ohms rather than 7.2, reducing the loss even more.

Note:  K6STI's "coil" program - Link - calculates the loss for this coil as being closer to 8 than 5 ohms - a bit higher than the simple loss calculation of Owen Duffy's wire calculation and likely more representative of in-situ measurements.

When operating on 40 meters with 100 watts of CW or SSB, the coils definitely do get quite warm - but not dangerously so and thus I would presume that the very rough estimates above are likely in the ballpark:  If you operate heavy duty-cycle modes like RTTY or FT-8 and insist on running 100 watts key-down I would occasionally check the coils to be sure that they aren't getting too hot.

By comparison, the calculated DC resistance of  the same length of 18 AWG bare copper wire is under 0.5 ohms, but the RF resistance due to skin effect at 28 MHz is around 2 ohms and about an ohm at 7 MHz - roughly a 7:1 difference meaning that if the above analysis is in any way close to being correct, our losses at 7 MHz when using the full coil (again, we don't!) and presuming that the feedpoint of the individual coil stayed at 25 ohms (it probably won't) our losses would drop from about 30% to less than 5%.

As a consequence, if wound with copper/silver plated I would expect that the not only would the antenna become narrower than the 40 meter 2:1 bandwidth of about 120 kHz - which would make it slightly trickier to tune - I would also expect the feedpoint resistance to drop, possibly increasing the VSWR at the feedpoint.  From a practical standpoint, even a modest antenna tuner capable of handling only 3:1 mismatch should be able to cope with this, but it is likely that some of the gains from using lower-loss wire might be offset by the increase in losses caused by feedline mismatch and the losses within a tuner - both of which could easily exceed 3dB in a portable set-up with moderately-long, small-diameter coax.

Would it be worth rewinding the coil with (readily-available) 18AWG (1mm dia) silver-plated or bare copper wire?  Maybe

Note:  I have since rewound a coil with 18 AWG silver-plated copper jewelry wire and am in the process of doing direct comparisons with it and the original coil wound with stainless-steel wire - expect a blog entry on this in the near-ish future.

Final comments

Figure 10:
Operating 20 meter CW from POTA entity K-6085, with the
Conger mountains and the JPC-7 dipole in the background.
Click on the image for a larger version.

Is this an antenna that is worth getting?  I would have to say "yes".

Remembering that you will also need to supply a suitable tripod mount (e.g. an inexpensive "light stand" ) this antenna is quite portable and, if you have a bit of practice, quick to set up and adjust.  Unlike a vertical antenna, it doesn't need a set of ground radials and it is likely that the antenna itself will be up and above everyone's heads when it is deployed.

Best used on the higher bands (20 and higher) its efficiency will be quite good - certainly equal to or better than a typical mobile antenna.   As this is a large-ish antenna on a tripod, be sure to weigh down the legs and/or attach simple guying to it to prevent it from blowing over in the wind or being knocked over by tripping over the coax:  I can attest personally that the latter can easily happen!

* * *

I also have the JPC-12 vertical (which will be discussed in a future post) and I find this antenna (the JPC-7 loaded dipole, that is) to be far more convenient to use than the vertical (e.g. no radial system), particularly if you plan to change bands several times during the operation - something that is quite likely to happen on the higher bands as propagation varies over the course of a few hours.  For the vertical, best performance requires adjusting the radials as well as the antenna itself, although it would probably work "just fine" if the radials are left at maximum length.  Another advantage of the JPC-7 loaded dipole being a (largely) horizontally-polarized antenna is that in an urban environment it is likely to intercept less noise on receive than a vertical - and it can be inconspicuous in its deployment as compared to a taller vertical.

For the lower bands (40 and 30 meters) the JPC-7 works quite well - particularly if one operates CW or digital modes.  As mentioned, it can also work competently on 60 meters as well with the addition of extra length of the elements by the purchasing of extra rods and/or simply attaching "drooping" wires to the ends of the telescoping rods.

Over the course of several POTA and related activations I have made about 500 contacts with this antenna on the band 60 through 15 meters - on CW and voice:  I'm sure that the antenna works well on 12, 10 and 6 meters as well, but I just haven't tried it on those bands.

Overwhelmingly, the sense has been "If I can hear them, they can hear me." with this antenna as I have worked quite a few QRP and DX stations that I could barely copy above the band's natural QRN level.  Admittedly, some of these times I was on the receiving end of the frenzy - being the activator during POTA operation - but there were many times when I had to stop operating not because I ran out of people to work, but because I ran out of time.

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This page stolen from ka7oei.blogspot.com

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