Some J-Poles That I Have Known 4

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Some J-Poles That I Have Known

Part 4: Some Things We Can and Cannot Do With aJ-Pole

L. B. Cebik, W4RNL

In this final episode of the saga of the J-pole, we shall examine some interesting variations on thebasic J-pole. These ideas will complete my personal investigations into this intriguing antenna--atleast for the moment. However, there are many other sources of information on practical J-polesand techniques for improving them--both in terms of performance and in terms of matching themeasily to 50-Ohm feedlines.

First, we shall look into some suggestions for improving standard J-pole performance by increasingthe length of the radiator. Our goal will be to understand why most of them do not hold promise ofsuccess.

Second, we shall look at a longer version of the J-pole that does work: the collinear J-pole. Alongthe way we shall look at the question of how well it works.

Finally, we shall examine a model of the Jagi, the J-pole-driven Yagi. Why it does work will becomethe final exam to see if we really do understand the J-pole.

Longer is Not Necessarily Better

Over the years, I have heard many suggestions for improving the standard J-pole's performance bysimply making the radiator section longer. Since the basic J-pole radiator is a 1/2 wavelengthwire--end fed, perhaps some of the longer wires with better performance in other contexts will helpthe J-pole to do better than it does--which is pretty good to begin with.


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Fig. 1 illustrates the most common suggestions for increased length that I have heard. The5/8-wavelength radiator idea emerges from ground-plane antenna ideas. A 5/8-wavelength verticalhas theoretically the highest gain of any ground-plane monopole. The 1-wavelength suggestionemerges from the idea that if 1 half-wavelength radiator is good, then 2 must be better. As well,each half-wavelength section ends in a high impedance, which is what the matching section needsto see. The 1.25-wavelength notion stems from the extended double Zepp (EDZ), which isessentially 2 half-wavelength sections at the outer ends with a phasing section in the middle.

Unfortunately, none of these ideas promises much when modeled either in free-space or overground. As I have throughout these notes, I shall place each antenna in this final section 10' or120" above average ground. (Whenever we compare an antenna to a J-pole, the comparator willbe elevated to a height that places its region of highest current at about the same height as theequivalent region of the J-pole. For a standard J-pole at 146 MHz, that region is about 30"-40"above the antenna base.) As well, unless otherwise specified, all J-pole variants in this final set ofnotes will use 0.375" diameter aluminum elements, and the matching section will use a 2" spacing.This construction is both feasible and allows models in NEC-4 that result in average gain test(AGT) values close to ideal (1.00 or 0.0 dB).

To see what happens if we simply extend the length of the J-pole radiator, let's model thesuggested new versions in free space. We shall be especially interested in the elevation patterns,which correspond to the E-plane patterns of vertically polarized antennas like the J-pole.


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Fig. 2 contains a wealth of data, since it contains both the free-space E-plane patterns and thecurrent distribution representations for all three antennas. However, by combining the data, we canbegin to see the way in which end-fed linear elements differ from center-fed elements of the samelength.

The 5/8-wavelength pattern gives us our first warning. We begin to see the emergence of multiplelobes at roughly 45-degree angles to the horizontal and vertical axes of the pattern plot. As weincrease the length of the radiator to a full wavelength, the emergent lobes become fully formed.We are used to seeing such lobe formation in wires without the matching section only when thewire length was about 2 wavelengths.

The corresponding current distribution graphics to the right of Fig. 2 verify the wire length--that is,that I am not presenting models that falsify performance. The 5/8-wavelength graphic shows asingle full half-wavelength rise and fall of current magnitude above the minimum close to thematching section. Of course, the matching section does not start at a current minimum. Therefore,the currents in that section show very significant imbalance--to the point that the section almostfunctions as a simple antenna fold-back rather than as a transmission line.

The full-wavelength current graphic shows 2 full excursions of current above the matching section,


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with a current null about in line with the top of the matching line pair. Since the currents are betterbalanced, the radiator itself largely controls the lobe formation. Nevertheless, with end feed, thepattern shows 4 distinct lobes.

The pattern for the 1.25-wavelength radiator version of the J-pole resembles the pattern we mightexpect from a center-fed 1.5-wavelength wire. The 6 lobes represent in a 1.5-wavelength wire theemergence of the 4 corner lobes of a 2 wavelength wire and the decrease of the horizontal axislobes typical of a wire 1 wavelength or less. The corresponding current distribution graphic seemsto confirm this analysis if we take the lowest current excursion as being completed by theunbalanced match line section.

Those interested in lobe formation for end-fed wires may wish to read the short Appendix to thisepisode to develop the full portrait of current magnitude and phase along a wire longer than 1/2wavelength in order to fully appreciate the lobes in the E-plane patterns for the suggested J-poleimprovements. What the models tell us is that the longer radiators are likely to produce morehigh-angle radiation than low-angle radiation when we place them over a ground.


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Fig. 3 confirms our suspicions. Each J-pole model has its antenna base at 120" above averageground. Each elevation plot lies along the plane of the antenna legs so that a small front-to-backratio is detectable. In each case, the strongest lobes are at much higher angles above the horizonthan we would desire for point-to-point communications on 2 meters. The 5/8-wavelength pattern isusable, but at a lower level than a standard J-pole. The gain at a 6-degree elevation angle is about2.5 dB lower than for a standard J-pole (2.6 dBi vs. 5.1 dBi). The 1.25-wavelength version doesshow a low angle lobe--corresponding to the free-space lobe along the horizontal plot axis.However, this lobe is about 1.5 dB weaker than the main lobe of the standard 1/2-wavelengthJ-pole (3.5 vs. 5.1 dB). The main lobe of the 1.25-wavelength J-pole is indeed quite strong at about6.4 dBi, but the 42-degree elevation angle is hardly ever useful for point-to-point communications.

The lesson that we might take from these models is that the standard-type J-pole's best radiatorlength is in the vicinity of 1/2 wavelength--as adjusted for the match section requirements and theelement diameter. Hence, for a 146-MHz design frequency, the radiator will be somewhat shorterthan the 40.2" true half wavelength. Still, this lesson does not mean that we cannot make longerimproved-performance J-poles. It simply means that we must make them in a more nearly correctmanner.

The Collinear J-Pole

To prevent the formation of lobes the yield high-angle radiation over ground, we must establish thecorrect current phase relationships between radiator sections of long J-poles. One age-oldtechnique is to insert a shorted transmission-line stub between the 1/2-wavelength radiator sectionsthat will effect a 90-degree phase shift between the top end of the lower radiator and the bottomend of the upper radiator. The result is a J-pole version of a rather standard collinear vertical array.

Fig. 4 shows the modeled version of the collinear array. As with many of the models in this series,


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it is a proof-of-principle model, not a construction blue-print. All the wire sections composing themodel are 0.375" diameter, even though one might ordinarily build the 18.5"-long 2"-wide phasingsection of thinner material, such as 0.1" diameter wire. Indeed, the selection of the 2" width resultedfrom modeling needs to keep the wires sufficiently far apart so as not to result in modeling errors.

All dimensions are in inches in the figure. If you compare the model with the corresponding 2"-wide3/8" diameter J-pole in the preceding segment of these notes, you will discover that the short leghas grown from 19.6" to 23.6", with the feed tap moved upward by 4". The half-wavelength radiatorsections are not of equal length: 41" for the upper and 35.4" for the lower. In part, the differentialresults from adjusting the upper section to achieve the desired 50-Ohm feedpoint impedance (inaddition to the matching section adjustments) without harming the overall gain of the system.

Fig. 5 shows the current distribution along the antenna, at least in terms of magnitude. Thephase-line section changes the current phase by 90.5 degrees, and its placement and length arecritical to obtaining full performance from the antenna. Ideally, the current magnitudes at the twojunctions of the phase-line should be equal. However, lengthening the upper radiator results in adetectable variance. The 90-degree phase shift is more significant in this application thanequalization of current magnitudes.

The lower radiator current minimum coincides nicely with the top open end of the matching section.However, since the current magnitudes are not equal between the lines at the top end,considerable imbalance exists along the matching section. The result is a spurious lobe that willbecome evident in elevation patterns for the antenna.


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In Fig. 6, we find the elevation patterns for the 102" long collinear J-pole with the base 10' aboveaverage ground. In the plane of the elements, the antenna shows a maximum gain of about 7.7dBi, with a small (0.4 dB) front-to-back ratio. The average gain of the antenna shows up by lookingat the pattern at 90-degrees to the plane of the elements, as shown in the lower half of the figure.The gain is about 7.4 dBi. This value is about 2.3-2.4 dB higher than the average gain of asingle-radiator J-pole. Indeed, although many folks like to bandy the gain advantage of a collineararrangement as 3 dB greater than a single section, we rarely obtain in real antennas more thanabout a 2.0-2.5 dB increase in gain.

Compared to many vertical antennas, the collinear J-pole shows a remarkable reduction inhigh-angle radiation. For any vertical collinear array, the only place from which to obtain energy forincreased gain at lower elevation angles is from the high-angle energy of a single section. If thesingle section lacks high angle radiation, creating a collinear version of the antenna will rarely yieldimprovements in performance that justify the added structure.

The upper portion of Fig. 6 shows the spurious lobe that results from both the imbalance incurrents in the matching section and from the imbalance of currents in the phasing line. For themodel, the phasing section protrudes in a straight line in the direction of the open end of thematching section. In a physical implementation of the design, the phasing section would likely wraparound the main element axis in a circle.

To evaluate the collinear J-pole--especially in terms of whether the increased height and complexityof construction is warranted--we should compare its performance with some antenna or other.since the J-pole is 102" long, the vertical extended double Zepp, which is about 100" at 146 MHz, isa good comparator.


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The EDZ used in this test is 0.375"-diameter aluminum and 100" long. The length allows the modelto set the base at 120" above ground, since an exact correlation to the collinear J-pole regions ofmaximum radiation is not feasible. In the J-pole, those regions are roughly centered in each of thetwo radiator segments. In the EDZ, the regions of maximum current are located about 1/4wavelength inward from each end--when we feed the antenna at the center. (End-feeding the EDZresults in a somewhat different distribution of current--enough to disrupt the anticipated lobeformation.)

Fig. 7 shows the elevation pattern for the EDZ. Since nothing in the structure disrupts the circularityof the pattern, this single plot suffices for all possible axes along which we might take elevationpatterns. The gain at 5.5 degrees (about the same elevation angle as for the collinear J-pole) is justunder 7.6 dBi, that is, only about 0.2 dB higher than the average gain of the collinear J-pole. Thehigh-angle lobes are reflections of the typical ears that accompany any EDZ pattern. They shrink aswe reduce the length of the antenna--but so to does the overall antenna gain. If we extend thelength much beyond 1.25 wavelength, the ear-lobes will grow to dominate the pattern, resulting in apattern with predominantly high-angle radiation.

For the version shown, the feedpoint impedance is about 120 - j380 Ohms. There are manyschemes for matching an EDZ to a 50-Ohm feedline. One way to do it with lowest loss is to use asection of parallel transmission line and a shorted stub. One might also place a network of fixed orvariable components at the feedpoint. Finally, one can employ transmission line sections for theinner portion of the antenna to effect an impedance transformation within the antenna itself. Thelatter two matching methods tend to reduce overall system gain--that is, to create some loss ofradiated energy--more than the match-line-and-stub system. However, the match-line-and-stubsystem tends to narrow the operating bandwidth of the antenna. (There are notes on feeding EDZsamong the collection at this site.)

I note the matching requirements for the EDZ so that one might make a fair comparison betweenthe EDZ and the collinear J-pole. For roughly equivalent performance, we have roughly equivalentsize and construction complexity--a not too unusual situation for antennas. In which direction onegoes may ultimately rest upon which antenna most closely coincides with one's favorite shoptechniques.


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The collinear J-pole does offer one advantage over many other types with which it might compete:a wide operating bandwidth. Fig. 8 shows the 50-Ohm SWR curve for the modeled collinear array.The band-edge SWR values are 1.41:1 at 144 MHz and 1.35:1 at 148 MHz. I suspect most userswould find these values tolerable.

The Directional J-Pole

The current distribution along the radiator section of a J-pole is perfectly normal, with a maximumlevel at the center and diminishing levels toward the ends. The only variation from what we mightexpect of a center-fed 1/2 wavelength wire is that at the lower end of the radiator, the current doesnot go to zero. In fact, the current may be as high as 20% of maximum value at the radiator center.

Since the current distribution is normal, we might wish to use the J-pole as the driven element in avertically polarized parasitic array. In The ARRL Antenna Compendium, Vol. 5, Michael Hood,KD8JB, presented a 3 element Jagi (J-pole driven Yagi) (pp. 62-65), using his plumbing-pipe J-pole(from Vol. 4 of the Antenna Compendium) as the driven element. Rather than try to model thecomplex arrangement of various pipe sizes that he used, I took a standard J-pole model that used0.375" diameter aluminum with a 2" match-leg spacing as the driven element for a model of a3-element Jagi.


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Fig. 9 shows the dimensions of the final model. I aligned the elements of the driven element, sincethe degree of misalignment of element centers was not severe. Each parasitic element also uses0.375" diameter aluminum. The final dimensions resulted from juggling element spacing andlengths along with the J-pole feed to obtain the best performance and a 50-Ohm feedpointimpedance.

The dimensions for the elements emerged initially from a 3-elements Yagi of standard design, butusing 0.5" diameter elements. Therefore, in checking the performance of the Jagi, I used thisstandard Yagi for comparison, placing the center line at about 140" above ground. The Jagi base is120" above ground, so the center lines are in crude alignment.

Fig. 10 shows the comparative elevation patterns of the two antennas. Over ground, they bothexhibit a maximum forward gain of about 10.3 dBi. As the traces show, the standard Yagi has aslightly smaller set of rearward lobes.


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As shown in Fig. 11, at an elevation angle of 6.2 degrees, both antennas share the same forwardgain and beamwidth (about 110 degrees), typical of Yagis turned for vertically polarized use. Thefront-to-back ratios of the two antennas differ by only about 3 dB (17.4 vs. 20.3 dB), with thestandard Yagi having the advantage. Considering the liberties I took in modeling the Jagi, thedifference is neither unexpected nor operationally significant.

The standard Yagi had a feedpoint impedance in the neighborhood of 40 Ohms at 146 MHz,suitable for direct feed, but likely not for maximum bandwidth without some form of matching. Incontrast, the Jagi had a design frequency impedance of almost exactly 50 Ohms. The band-edge50-Ohm SWR values were 1.74:1 at 144 MHz and 1.83:1 at 148 MHz. The addition of the parasiticelements does affect the operating bandwidth of a J-pole used as its driver, but not sufficiently toprevent full band coverage on 2 meters. Fig. 12 shows the full 50-Ohm SWR curve.

Yes, the Jagi is not only feasible, but is--as well--an interesting variation on the Yagi that solves thefeedline dress question for many vertically polarized applications.

Conclusion--Yes, THE Conclusion


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One could go on almost indefinitely evaluating and analyzing J-pole designs and variations. Thenumber of ways in which individuals have successfully constructed J-poles over the years probablyexceeds the number of variations in almost any other antenna type. As well, numerous folks havedeveloped variations on the feeding scheme for either standard or non-standard J-pole types toeliminate the need for pruning or adjusting the long and short legs and moving the standard J-polefeedpoint tap.

As well, the collinear and parasitic J-pole applications that we examined only scratch the surface ofwhat has been done and what might be done with the J-pole as the starting point. However, myinterest in the J-pole was not to form a catalog of antennas to build. Instead, the goal has been tounderstand a bit better than I did before what is going on in the operation of a J-pole. These notessimply formalize a bit what I learned along the way.

This conclusion does not mean that I shall never add to this series of notes. It simply means that forthe moment, other antennas are exerting a stronger call.

However, I know of no other antenna that has its own limerick:

I know a wonderful aerial: the J-pole. You can build one without stealing a payroll. When you tune it to peak, You'll hear signals so weak, That from work you'll likely go AWOL.

Appendix 1: Linear-Element Equivalents to Long-Radiator Standard J-Poles

To verify the effects of elongating the standard J-pole radiator in terms of the modeled patterns, Iexamined a series of linear vertical elements. The closest equivalent linear element to a givenJ-pole antenna design would yield a free-space pattern very similar to the ones shown in Fig. 2,allowing for the non-symmetry of the J-pole patterns. I fed each linear equivalent element near thebottom, creating an off-center feed system as close to equaling the J-pole feed as possible. Theexact position does not correspond to the length of the open-end match-section leg. Instead, itroughly equates with the effective length of the matching section legs as radiators, given theimbalance of current (considering both magnitude and phase angles) on those legs. Fig. 13 showsthe general scheme of the equivalency test.


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The results of the test were interesting. The J-pole with a 5/8-wavelength radiator has a free spaceelevation (E-plane) pattern very similar to a linear element 3/4-wavelength long and fed about5-10% up from the bottom, as shown in the top pattern of Fig. 14. The J-Pole with a 1-wavelengthradiator shows a free-space elevation pattern very similar to that of a 1.25-wavelength linearelement fed about 15-20% upward from the bottom. The middle pattern of Fig. 14 shows the result.Finally, the J-pole with a 1.25-wavelength radiator has a free-space elevation pattern very close tothat of a 1.75-wavelength linear element fed 10-15% up from the bottom, as shown in the bottomplot.

Compare the plots in Fig. 14 to those in Fig. 2. As well, compare the current distribution graphics inboth figures. In all cases, the elements show zero current at the top end, with typical1/2-wavelength current curves proceeding downward from the top. The variation in the normalcurve occurs at or near the bottom end. In the linear elements, the current below the feedpointdescribes a sharply tapering curve toward zero. The curves in this region and just above thefeedpoint represent the equivalent linear element behavior of the corresponding J-pole within thematching-section region, given the specific current imbalance for each of the elongated models.

The lessons from this exercise are two. First, the imbalance of currents in the J-pole matchingsection make this section part of the total radiating system. Only in the case of the 1/2-wavelength


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radiator are the currents within the matching section sufficiently balanced to yield elevation patternsthat are close enough to those of a center-fed linear element the same length as the radiator toallow us to generally ignore the matching section. As we saw in Fig. 2 of Part 3, if the wires are not very closely spaced--as with a twinlead J-pole--the resulting free-space pattern is offset from thehorizontal plotting axis to be useless in determining antenna behavior. Elements as close togetheras 1" at 146 MHz are far enough apart to require that we perform all analyses above a ground.Hence, in the end, we cannot ignore the radiation from the matching section even for the classicJ-pole with a 1/2-wavelength radiator.

Second, we cannot expect J-poles to perform like rough analogs of their radiator sections alone.The version with a 5/8-wavelength radiator does not perform like a 5/8-wavelength monopole with aground plane system. The 1-wavelength and 1.25-wavelength radiator versions of the J-pole do notperform like elements of similar length in free-space when fed at their centers. The only correctequivalents of J-poles are ones that take into account the radiation from the matching section of theantenna.

Appendix 2: Non-Standard Long-Radiator J-Poles

All of the test models of long-radiator J-poles used standard J-pole configurations in the notes thusfar. It is possible to develop a non-standard J-pole--that is, a J-pole with no shorting strap for thefeed point, but instead a single feed point at the base strap--using longer than a 1/2 wavelengthradiator. Consider the following published design for a 5/8-wavelength J-pole: The elements are3/8" tube or rod, with the long radiator about 59.5" long and the short rod about 14.25" long. Therod spacing is about 6.375". As with all of our J-pole models, we shall place them about awavelength above real ground for deriving patterns.

The resulting antenna will show a 50-Ohm SWR well under 2:1 across all of 2 meters and theadjacent CAP frequencies as well. However, as we saw in the last episode, very wide spacingtends to yield significant pattern distortion relative to the ideal of a circular azimuth pattern. SeeFig. 15.


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The pattern distortion ends up producing a pattern with a significant departure from an azimuth circle, and the higher angle of much of the radiation gives no more gain at the lowest lobe than wemight obtain from a shorter non-standard J-pole. The gain at a 3.1-degree angle averages about5.1 dBi, with peaks that are 70 degrees off a line made by the long and short radiator rods. Thepeak gain is 5.8 dBi. The gain in the direction of the short rod is 5.4 dBi, with a gain of only 3.7 dBiin the opposite direction.

The upshot is that the possibility of making a longer J-pole in non-standard form does not yield thebenefits of lengthening a vertical monopole over a buried ground plane. The J-pole configurationtends to increase high angle radiation so as to negate the value of the added radiator length. Thevery wide spacing may give us some ease of construction, but it contributes as well to patterndistortion. A closer spaced standard or non-standard J-pole with a 1/2-wavelength radiator willperform as well with respect to low-angle gain and better with respect to pattern circularity.

Updated 1-8-2002; 2-4-2002. © L. B. Cebik, W4RNL. Data may be used for personal purposes, butmay not be reproduced for publication in print or any other medium without permission of theauthor.

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