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Re: Topband: Monopole Elev Pattern w.r.t. Earth Conductivity

To: <topband@contesting.com>
Subject: Re: Topband: Monopole Elev Pattern w.r.t. Earth Conductivity
From: "Richard Fry" <rfry@adams.net>
Reply-to: Richard Fry <rfry@adams.net>
Date: Sat, 27 Oct 2012 08:02:08 -0500
List-post: <topband@contesting.com">mailto:topband@contesting.com>
Guy Olinger wrote:
So far NEC4 has predicted any real measurements, regardless
of operator skill.

Presumably the above text was meant to read "So far NEC4 has _NOT_ predicted any real measurements, regardless of operator skill."

Some may not recall the comparison of groundwave fields calculated by NEC to those measured with an accurate, calibrated field intensity meter by a broadcast consulting engineer, posted here some months ago (link below). Best-fit earth conductivity for the measured path was about 6 mS/m.

The fields calculated by NEC are shown on the top half of the page. Note the close agreement between the data shown by the blue line there, and the solid line below the inverse distance field in the consultant's data plotted at the bottom of that page. This is at at least one case where NEC and real-world data agree.

Another important observation to be made from that NEC data is that space-wave radiation from elevation angles below ~2 degrees equals the radiation in the groundwave at 1,300 meters downrange. For further distances downrange the space wave exceeds the groundwave, as the space wave is decaying at a 1/r rate, and the groundwave decays at greater than 1/r, due to earth losses and eventually, earth curvature. This is shown by the green line on the NEC chart starting to exceed the blue line at an h-distance of 8,000 meters.

For long enough point-point paths along the surface the earth, the groundwave essentially is zero, and the much greater space wave radiation from such low elevation angles can produce nighttime skywave coverage over the longest, single hop paths.

This type of performance also applies to the monopoles of 5/8WL and less used by ham operators on Topband and the HF bands (regardless of earth conductivity at/near the monopole site).

The first thing would be to prove that NEC4's null at 50 km is a fantasy.

The fields in the groundwave itself do not provide coverage by ionospheric skip, and there is little point in examining the groundwave 50 km downrange (or anywhere else) to prove or disprove this.

NEC properly calculates zero field for its far-field plot of the elevation pattern of a monopole over a non-perfect ground plane, and not much more at vertical angles below 5 degrees or so. And a NEC near-field plot properly does _not_ show this "notch" for distances sufficiently close to the radiator. These calculations are not in conflict when properly understood.

The fields providing the greatest single-hop skip range are produced by the elevation plane fields within a few wavelengths of the radiator that are directed toward the lowest elevation angles. Those space-wave fields are much greater than the groundwave for sufficiently long paths along the surface of the earth. And those fields exist at much lower elevation angles than shown by a NEC far-field plot, alone.

NEC calculates all of these fields accurately. It is only their (mis)understanding and incomplete use that leads to the concept of "takeoff angle" for the elevation patterns of monopoles over a non-perfect ground plane.

http://i62.photobucket.com/albums/h85/rfry-100/Measured_vs_NEC2D_Fields2.jpg

R. Fry
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Topband reflector - topband@contesting.com

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