Force 12 Tuning SE Yagis-Elev Radials-1.2

From: Subject: Force 12 Tuning SE Yagis-Elev Radials-1.2 Date: Mon, 3 Dec 2007 18:11:51 -0000 MIME-Version: 1.0 Content-Type: multipart/related; type="text/html"; boundary="----=_NextPart_000_0000_01C835D7.FA44E900" X-MimeOLE: Produced By Microsoft MimeOLE V6.00.2900.3198 This is a multi-part message in MIME format. ------=_NextPart_000_0000_01C835D7.FA44E900 Content-Type: text/html; charset="iso-8859-1" Content-Transfer-Encoding: quoted-printable Content-Location: http://force12inc.com/F12-SE-Yagi-tuning-Elev-Radials-1-2.htm Force 12 Tuning SE Yagis-Elev Radials-1.2

Tuning Shortened-element = Yagis

(which can be applied to verticals = and other=20 antennas, as well)

and

Tuning Elevated = Radials follows=20 the Yagi discussion

Shortened-element Yagis ("SE Yagis") have been in service for = decades. Their=20 performance has advocates who rave about them and adversaries who argue = against=20 them. The usual measuring yardstick is the front-to-back ("F/B") ratio. = This has=20 been the determining factor as to whether or not the SE Yagi is = "working";=20 however, this is an inaccurate assumption. Just because an antenna has a = well-defined pattern does not mean it has any gain.

A basic understanding of antennas shows that pattern is not = necessarily a=20 useful indication of gain. It is commonly thought that if an antenna has = a=20 nicely defined pattern, it must have gain; however, the popular Beverage = receiving antenna has a fine pattern, but it has no gain at all. The = Beverage is=20 a very lossy antenna with a minus gain figure, which is why it "works" = as it=20 does. The key to an antenna having gain is mainly in the design and=20 construction. The most obvious source of losses is in trapped Yagis, = where the=20 elements are not only in less-than-optimum locations, but also the traps = that=20 have loss and do not necessarily place the element on the proper = frequency. Over=20 time, what gain might be there when the trapped antenna is new can drift = out of=20 band, or the elements can drift in opposite directions. Some people have = reported traps on the same element tuned to different frequencies, which = certainly will not help the antenna performance. For this discussion, we = will=20 only address monoband SE Yagis.

SE Yagis have three advantages to full size:

1). They are physically smaller, so the tower and rotator do not have = to be=20 as large and powerful as with full size elements;

2). The shorter elements do not interact as much with other antennas. = A=20 full-size 40 meter Yagi will destructively interact with just about = everything=20 on the same mast.;

3) A 2 element SE Yagi can achieve a higher F/B ratio than using full = size=20 elements. This is a unique circumstance that is shown in real-time = performance=20 and also using a computer model by L.B. Cebik, W4RNL.

There are three (s) electrical consderations for Yagi antennas: gain, = pattern=20 (F/B or front to rear) and operating bandwidth (VSWR bandwidth). In = Yagis with a=20 minimal number of elements, all three cannot be achieved. Designs with=20 additional elements (such as the direct feed 50 ohm designs developed by = myself=20 back in the early 1990's and first produced commercially as the Force 12 = Magnum=20 620 in 1993) can provide all three optimized conditions. This 20 mtr = Yagi has 6=20 elements on a 44' boom. The same peak gain can be achieved with 4 = elements, but=20 over 13.950-14.400 MHz, the 6 element design maintains forward gain = within about=20 0.1dB from the peak, F/B +/- 2dB and the VSWR is less than 1.3:1. For = low band=20 antennas, mechanical considerations begin to be more important and = decisions=20 need be made to prioritize the characteristics, because the number of = elements=20 is usually minimal. In these cases, the F/B and gain curves can go in = opposite=20 directions, so it is important to understand the trade-offs = available.

The operating bandwidth is usually the 2:1 VSWR bandwidth. For some=20 amplifiers (i.e. auto-tune Alpha 87A) this is too wide and the 1.5:1 = VSWR=20 bandwidth is the design goal. As the parasitic reflector element is = coupled=20 tighter (closer in frequency) to the driver frequency (working towards = maximum=20 F/B), the feedpoint impedance goes down, which increases the current in = the=20 elements and might lower the efficiency because of more loss in the = components=20 (cannot handle the increased current efficiently). The VSWR bandwidth = also=20 becomes narrower. This means the pattern might be wonderful, but the = operating=20 bandwidth will be unacceptable and the efficiency less than desired = (forward=20 gain will be less). An operating factor enters in, too, as when the = reflector is=20 tuned very close to the driver frequency, it becomes a director when the = frequency of operation drops below the reflector's frequency, thereby = reversing=20 the direction of the Yagi. In this case, the operating frequency range = must be=20 selected beforehand so that the antenna will not reverse direction in = the=20 desired range. Devices are available to allow frequency agility of the = Yagi for=20 extended operating ranges, such as the relay boxes in service for many = years by=20 Force 12.

Setting an SE Yagi for best F/B generally ensures the forward gain is = within=20 about 85-90% of the maximum, as the pattern indicates the elements are = coupling=20 to each other. This maximum gain is the maximum for THIS design only = with=20 whatever loading system is employed, not 85-90% of what might be = theoretically=20 possible. A general rule is that if there is no discernable F/B (zero), = the=20 parasitic element is improperly tuned. The F/B and forward gain curves = for 2=20 element Yagis do not overlay, meaning the best F/B and highest gain do = not occur=20 on the smae frequency. Oftentimes, the best gain is achieved above the = frequency=20 of best F/B ratio; therefore, it is quite possible to have good gain and = not=20 have the best F/B, provided the Yagi is efficient in its basic design. = On the=20 low bands, the most common focus is in pattern, as it creates the best=20 conditions to hear the DX stations. In this case, gain takes secondary=20 importance (especially if there is no power limit and the lack of gain = can be=20 compensated for by increasing the transmit power!). Besides proper = tuning, the=20 most important factors in maintaining antenna gain are the conductor = size, the=20 quality (efficiency) of the loading system and doing the best to have = the=20 element length as physically long as possible.

Two types of loading are most common: linear loading and coil = loading.=20 Various theories are around as to the effectiveness of each. Whichever = technique=20 is used, or even a combination of both, the element tuning is much more = critical=20 than when using full size elements for best F/B ratio.

Linear loading usually has variables in assembly, where the desired, = exact=20 frequency of the parasitic element(s) is not necessarily "plug and = play." The=20 result is the expected F/B ratio is not always achieved where desired. = The basic=20 linear loading technique is essentially a shorted transmission line stub = and the=20 Q is very high. The loading has classically been placed parallel to the = element=20 and then going towards the center of the element. In these linear = loading=20 structures, the frequency is set by adjusting the tuning jumpers across = the=20 linear loading, which changes the amount of loading. Recent developments = by=20 Force 12 on the "N" series of 40 meter elements uses a much different = design,=20 wherein the loading is pre-set and goes out towards the element tip. = These "N"=20 elements are also longer than typical, being 80-85% of full size and = modeling on=20 NEC showing they are within 0.1dB of full size, while having impressive=20 mechanical and electrical advantages over full size. The frequency = setting on=20 these elements is excellent and predictable. The "N" series elements = have a=20 fixed linear loading structure and the tuning is accomplished by = adjusting the=20 tip length.

Coil loading has been popular, as it is easier to assemble and erect. = If the=20 coils are made with reasonable accuracy on 40 meter SE Yagis, the F/B=20 performance will be good and the antenna will be deemed to be "working." = It will=20 have a pattern, but the gain is determined by the efficiency of the = antenna. The=20 small coils on the popular 40 meter SE Yagis are not in the "high Q" = category,=20 but if the coil loaded Yagi has any amount of gain, it will appear to be = a=20 tremendous antenna. We need to remember that a horizontal, rotatable = dipole is a=20 fine antenna, so anything that has even 2dB over a dipole (2dBd) will be = perceived as very effective and will "work" well in the pile-ups.

Short elements that are efficient will have a narrow operating = bandwidth.=20 This is the bandwidth of acceptable VSWR, which is usually accepted as = being=20 where the VSWR reaches 2:1. (For reference, the 3dB points is where the = VSWR=20 reaches 2.7:1.) Within the 2:1 VSWR bandwidth, the performance of the = shortened=20 element is fairly constant, but does drop off at the edges of the = bandwidth=20 curve. SE Yagis for 80/75 meters is where the tuning is most critical,, = because=20 the operational bandwidth of the individual elements is quite narrow, on = the=20 order of 45-70 kHz. Fortunately, the operating window on 75 meters is = also quite=20 narrow. In the USA, it is usually centered on 3.790-3.800 MHz and an = operational=20 bandwidth of 25-30 kHz is probably sufficient. Shortened elements also = require=20 tighter coupling, which means the reflector element must be tuned much = closer to=20 the driver than in a full size Yagi. Accuracy when using fixed inductors = (coils)=20 is most important and a simple example that anyone can model is to use = coils in=20 a 68' element. With mid-point loading, it will require about 27uH in = each coil.=20 How accurate can you make a coil? If the coil is off by 1% (0.2uH), the=20 frequency of the reflector element (and the F/B) will shift at least 10 = kHz.=20 When trying to optimize in the DX portion of the band at 3.790, 10 khz = is a lot.=20 The same accuracy holds for linear loading structures. A real time = technique is=20 necessary for optimum F/B on SE Yagis. Whether or not the antenna has = gain is=20 left to some other test!

The above example referenced the frequency of the reflector element = and not=20 that of the driver. This is because the F/B ratio is determined by the = frequency=20 of operation of the Yagi, not the frequency to which the driver element = is=20 tuned, or even matched. It is surely useful to have the driver near to = the final=20 frequency, but the reflector setting is the key. The reflector will also = pull=20 the driver frequency down in frequency, closer to the refelctor = frequency. If=20 one experiments a little, in a well-tuned linear loaded SE Yagi, the = reflector=20 will be set to about 3.777 MHz for a desired (matched) driver frequency = of 3.790=20 MHz. In this case, the driver will be pulled about 12 kHz lower in = frequency=20 than when the reflector is not in the circuit (i.e. center of the = reflector=20 element is open). This tuning will produce a F/B ratio in excess of 20dB = at the=20 driver frequency and be >15dB over a range of about 20 kHz, possibly = more,=20 depending on element length, boom length and the loading system.

The first step in tuning an SE Yagi is to have the parasitic element = (i.e.=20 reflector) at approximately the proper frequency. This can be done by = feeding it=20 by itself as a dipole through a 1:1 balun and elevating it as high as = possible.=20 In many cases, 20-25' will be sufficient for this step. If an antenna = analyzer=20 is used (recommended), the point of the lowest VSWR dip on the VSWR = meter is the=20 frequency of the element. If using an MFJ meter with the right-hand = meter=20 reading in ohms, do not use it for any indication at all - only use the = VSWR=20 meter. The "ohms" value makes no difference. It is the frequency = of=20 lowest VSWR that is important. What frequency should be used?

The computer model can aid in this regard for coil loaded elements. = In the=20 finished model, remove the driver and use the reflector as a dipole. = Adjust the=20 frequency in the model until there is zero (0) reactance and this will = give you=20 the frequency of the modeled reflector. In typical 75 mtr SE Yagis using = coils,=20 this will be in the range of 3.780-3.785 MHz for operation in the DX = window=20 3.790-3.800 MHz. If the actual antenna is a linear loaded design (such = as the=20 Force 12 EF-280B), the reflector target will be slightly lower, such as=20 3.775-3.777 MHz. After performing this initial reflector tuning, remove = the=20 balun and short across the reflector center to make it a continuous = element - a=20 functional reflector element. Set the driver for its initial setting at = 3.795=20 MHz and match it to an acceptable level (1:1 is not necessary now).

Initial suggested frequencies for reflector elements are as = follows:

VERY IMPORTANT - When the frequency of operation moves = lower than=20 the reflector frequency, the Yagi will REVERSE direction. When setting = up a 40=20 mtr Yagi for best F/B high in the band (i.e. USA SSB portion at = 7.150-7.300MHz),=20 it will reverse direction in the CW portion (low end) of the band. If = both parts=20 of the band are needed, the Yagi should be set for CW and operated up in = the=20 phone part of the band with less F/B, but still with forward gain. A = relay box=20 (such as available from Force 12, Inc.) can be used to maintain optimum=20 operation in both portions of the band.

Please refer to the drawing for the technique of tuning an SE Yagi in = real-time. The basic principle is this:

A) The actual frequency of best F/B is found by measurement;

B) the reflector frequency is adjusted to move the best F/B into the = desired=20 operating range;

C) the driver is set on frequency and matched.

D) the antenna can be rotated around to the front to measure the F/B = in dB on=20 the receiver's S-mtr. The actual F/B in operation will not necessarily = follow=20 this measurement, as incoming signals will arrive at different = angles.

*Operating = Frequency*	*Reflector = Frequency*	*Operating = Frequency*	*Reflector Frequency 37'=20 el*	*Reflector Frequency 45'=20 el*
*3.500-3.510MHz*	*3.488-3.492MHz*	*7.000-7.060*	*6.960-6.980*	*6.930-6.950*
*3.750-3.755*	*3.737-3.742*	*7.150-7.250*	*7.110-7.130*	*7.080-7.100*
*3.790-3.800*	*3.777-3.780*	*7.200-7.300*	*7.160-7.180*	*7.130-7.150*

	*Drawings and Work Sheets to Print and = Use*
	Main Drawing
	General Work Sheet
	40 Mtr Work Sheet

This is a simple procedure and will give excellent results. Go slowly = and be=20 accurate in the measurements and adjustments. The procedure has been = used on 2=20 element 75/80 mtr Yagis, 75 mtr 2 element vertical, 40 mtr Yagis and 30 = mtr=20 Yagis. The average time for each antenna was less than two hours.

Please let us know of your questions and results. The purpose is to = give the=20 best performance and most enjoyment using these shortened antennas.

Tuning Elevated Radials for 1/4 Wavelength=20 Verticals

Verticals for the low bands have classically been an electrical 1/4=20 wavelength long (tall) and require a radial system for the current = return. The=20 exception is the vertical dipole, which is now more commonplace since = the=20 development of the SVDA antenna system (see the write-up on K5K) and the = new=20 SIGMA series vertical dipoles from Force 12, = Inc. When=20 using a 1/4 wave vertical, laying 120 buried radials (as indicated in = texts for=20 decades) is rarely practical for most of us; therefore, a different, but = efficient approach is needed. The original concept was discovered in an = I.E.E.E.=20 article some years ago where the buried radial systems on commercial AM=20 broadcast antennas were disintegrating over time. Adding elevated = radials was=20 shown to be extremely efficient and a practical solution for the current = return.=20 The concept was put into practice on our first trip to Jamaica for the = A.R.R.L.=20 competition as 6Y4A. It has been used on every installation since that = time and=20 on many other installations world-wide.

We had carefully selected the 6Y4A operating site, which was right on = the=20 ocean with several hundred feet of beach available for vertical = antennas. One of=20 the first antennas we installed was the 160 mtr vertical, followed by = the 80 mtr=20 verticals. Since we were on the ocean, we laid the radials on the = "ground." This=20 consisted of a combination of rock, salt water and grass, all right = adjacent to=20 the ocean. Conventional "wisdom" would say we had done a wonderful job - = hardly.=20 We were unable to have anything close to a 1:1 VSWR, nothing less than = 2:1 at=20 best. The team looked to me for an overnight solution (didn't get much = sleep)=20 and my memory was working well enough to recall the I.E.E.E. article. = After not=20 much sleep, we got up early and did an important test: when we added the = hairpin=20 match to increase the feedpoint up to 50 ohms, the VSWR got worse. The = feedpoint=20 for a full size 1/4 wavelength vertical should be in the low 30 ohm = range.=20 Shortened verticals are lower, often in the 12-20 ohm range. We were = using=20 physically short verticals with efficient linear loading to load them to = an=20 electrical 1/4 wavelength, with an expected feedpoint of less than 20 = ohms. When=20 we added the hairpin to transform the feedpoint impedance higher towards = 50 ohms=20 for an acceptable match, the VSWR got worse. This meant the feedpoint = was=20 already above 50 ohms, which was caused by the added loss (resistance) = of the=20 ground. We now knew the problem and we quickly worked out the "gull = wing"=20 elevation technique for lifting the radials above ground. As soon as the = radials=20 were in the air, the feedpoint impedances became acceptable. It should = be noted=20 that even with the poor match (and high losses) we did use the verticals = that=20 night, with excellent performance, due to the proximity of salt water. = After=20 reducing the losses by elevating the radials, they were even better.

A procedure was developed over the next year to elevate and tune = radials. The=20 drawing below shows both the basic technique for elevating radials, as = well as=20 the height above ground for effectively de-coupling the radials from the = ground.

Any questions or comments, please zip off an e-mail to us at force12info@fix.net.

73, Tom, N6BT

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