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A typical gain pattern for a quarter wave ground plane antenna is:

enter image description here

Image from a similar question and see watermark.

For a situation where the signals of interest are below the antenna in elevation (e.g. antenna on a hill/mountain), would mounting the antenna upside down make any difference?

A naive response would be that the antenna's pattern would be unaffected except to be rotated 180 degrees, i.e.:

enter image description here

An answer to a similar question seems to imply that the radials on a ground plane antenna don't have as much to do with the pattern as the actual earth. My trials at modeling this with EZNEC resulted in no change based on the antenna's orientation, but I don't trust myself.

Also, looking at just the plots would lead you to believe that there is zero chance of receiving a signal from below the antenna's elevations. Which also is hard to believe.

Searching the internet resulted in many variations of "Try it." or "It worked for me back in ...". I'm looking for more specific reasoning.

And in case it matters much for this answer, I am mainly considering the 2m range of frequencies. Also for consideration, height above ground can be assumed to be in the 5 meter range.

Simplified configuration for clarity:

enter image description here

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    $\begingroup$ well, how "high" would you "hang" your antenna? if you just mirror your pattern, you'll notice that everything would be reflected/swallowed by the ground, as it geometrically is directed "downwards"... I'm not quite sure I correctly understand your question. Could you make a short drawing of what you have in mind? $\endgroup$ Commented Jun 20, 2016 at 10:22
  • $\begingroup$ @MarcusMüller I added a height to the question (5m), but that is kind of the point. Does the diagram flip so that everything is upside down? The only thing that changes about the antenna is that the radials are on the top and the vertical is on the bottom. The whole antenna is rotated to point down. $\endgroup$
    – hazzey
    Commented Jun 20, 2016 at 13:25
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    $\begingroup$ I asked for a drawing for a reason :) Now, the diagram cannot flip, because then the main lobes would point down, but there's mother earth in the way. If you make a drawing, you'll notice that problem. $\endgroup$ Commented Jun 20, 2016 at 14:23
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    $\begingroup$ Something to ponder: commercial AM broadcast stations are located on mountains when they are available, and their towers aren't mounted upside-down even though the intended receivers are below the antenna. $\endgroup$ Commented Jun 20, 2016 at 17:33
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    $\begingroup$ Just a point of information... my polar plots you reference are modeling ground mounted antennas, not antennas in freespace or above ground. $\endgroup$
    – JSH
    Commented Jun 21, 2016 at 20:48

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An elevated "ground-plane" antenna with tuned radials has, by itself, a pattern much like a dipole doughnut shape (freespace is what I'm talking about at the moment). Unfortunately we must mount the antenna and feed it with a feedline. This introduces one or more additional conductors below the radials that demonstrably (via simulation and measurement) draw/induce some power from the radials and flow energy below the antenna. See figure 5 of this article. This seems to cause the slight uptilt you most often see in ground-plane antenna documentation. The 3 dB beamwidth in the vertical E-plane is still quite enormous with energy both above and below the level of the antenna.

Some purists do mount these things upside down on a tower side bracket when the antenna site is much much higher than the surrounding users of the radio system. Indeed "beam downtilt" in collinear phased array systems is a serious attribute to study for some radio system circumstances... especially for the shorter wavelengths. Trigonometry helps answer when to consider this approach as I cover here.

That said, the vertical beamwidth of the typical quarter-wave monopole antenna is so big, mounting it upside down is probably not going to make any difference for most circumstances.

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If you were to flip the antenna upside-down, ideally with no part of the antenna touching the ground, then your antenna radiation pattern wouldn't change all that much, as you've discovered on EZNEC. Two things have changed compared to a 'normal' ground-mounted vertical: you've elevated the radials, and you've flipped the antenna.

(The following explanation may displease physicists as being overly simplified, but I think it's useful for the average ham. This is ham.stackexchange.com, not physics.stackexchange.com.)

By elevating the radials you've changed the way that the antenna works. Instead of a 1/4 λ monopole mirrored by the ground that you've made highly conductive with your radials, you now have a dipole. Half of your dipole is the vertical conductor, which creates vertically-polarized radiation. The elevated radials, which should be tuned to be 1/4 λ long, work to counter-balance the vertical part of the antenna. (Some people use the word 'counterpoise' for elevated verticals, but that word has been overly used and abused so much that the late L.B. Cebik, W4RNL, argued that the word should be retired.) Verticals with elevated radials work very well, but because the verticals must be tuned, they are essentially single-band antennas (plus odd harmonics).

So you've flipped the antenna. The pattern of the signal is very similar to a 'normal' ground-mounted vertical because the pattern is the result of a vertically-polarized signal radiated close to the earth and not in free space. Flipping the antenna but not flipping the earth just doesn't do much to change the pattern.

There is no particular reason to flip the antenna just because the antenna is on a mountaintop. Vertically-polarized antennas on mountaintops are common but I've yet to see a flipped one, ha ha. Antenna modeling is almost always done over an idealized flat earth, but experience shows that the signal from a mountaintop antenna makes it down into the valley. There is a program called HFTA or HF Terrain Analysis by Dean Straw N6BV, which comes with the ARRL Antenna Book, that can be used to model propagation over actual terrain that isn't perfectly flat, but the software only works with horizontally-polarized antennas.

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To answer this very graphically:

Flipping the diagram geometrically can't work:

Diagrams

What you've actually build is kind of a waveguide, consisting of two grounded planes below (earth) and above (virtual earth spanned by radials) your antenna; in this rotation-symmetrical setup, the H-field only exists in horizontal direction, and the E-field between the two planes will only exist vertically.

In other words: if we assume the virtual ground plane to be a perfect circle, then this looks like a lot of dipoles standing tightly next to each other between that plane's edge and the ground, being fed with exactly the same signal. Since this, for symmetry reasons, won't have any horizontal gain, the only gain we can have is vertical; but there's no vertical group factor in a group of horizontally shifted dipoles, so this will really just have the radiation pattern of a half-length dipole.

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  • $\begingroup$ Leave it to you, @Marcus, to come up with this one. You crack me up. The two grounds would be loosely coupled, of course, but still. $\endgroup$
    – SDsolar
    Commented May 12, 2017 at 23:56
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    $\begingroup$ @SDsolar yeah, and, admittedly, the "very large hovering ground plane" would be something strictly out of a scify book, but still :) $\endgroup$ Commented May 13, 2017 at 8:14
  • $\begingroup$ Of course, if Earth were surrounded by at atmospheric layer that contained mobile ions, the situation in the final illustration may not be so completely unrealistic. We might even hypothesize the feasibility of global communication under the right conditions... $\endgroup$ Commented Feb 24, 2019 at 14:33
  • $\begingroup$ @PhilFrost-W8II woah! How sci-fi would that be?! :D $\endgroup$ Commented Feb 24, 2019 at 14:56
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Please see my graphic below.

A λ/2, center-fed dipole has about 0.7 dB more gain than a λ/4 ground plane, but otherwise their v-pol, free-space radiation patterns are very similar.

Whether the vertical conductor of a λ/4 ground plane is pointing to the zenith or the nadir, its radiation toward the earth would produce nearly the same reflections from the earth (other things equal).

So its net, far-field radiation patterns would be very similar for both installation configurations.

enter image description here

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UHF inverted ground plane antennas on balloons and other aircraft are used for this very reason. The radiation pattern gives the most gain at low radiation angles (which are at greatest distance to ground), less vertically down (closest) and theoretically none above. I'd be interested in the calculated radiation pattern of a ground plane with sloping radials (e.g. ground plane sloping radials ) which I expect is somewhere between a dipole and ground plane.

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  • $\begingroup$ RE: The radiation pattern gives the most gain at low radiation angles (which are at greatest distance to ground), less vertically down (closest) and theoretically none above. >>> That is a popular belief, Steve, but you might want to review the information in my Answer here. $\endgroup$ Commented Feb 19, 2020 at 13:24
  • $\begingroup$ Welcome to ham.stackexchange.com, Steve! $\endgroup$
    – rclocher3
    Commented Feb 19, 2020 at 23:04

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