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Buried ground radial analysis software Version 2
Choosing Length & Number of Shallow-Buried Radials, Version 2Author: R.J.Edwards G4FGQ © 5th August 2004A buried radial is a lossy single-wire transmission line. It has four primary parameters, R,L,C & G. It has secondary parameters: Alpha the attenuation constant and Beta the phase constant closely related to the velocity factor. The characteristic impedance is complex with components Ro and Xo. All these parameters can be estimated from line dimensions of length, wire diameter and burial depth in conjunction with soil resistivity and permittivity. The most important 'measurements' are the input impedance of all the radials in parallel at the system's focal point, and antenna input impedance. The final figure of interest is antenna radiating efficiency given by Rr/(Rr+Rs), where Rr is antenna radiation resistance and Rs is the radial system's input resistance. Loss along a radial wire is proportional to length. As length increases input impedance converges towards its characteristic impedance Zo. At roughly 14 dB convergence is practically complete, input impedance ceases to change and radiating efficiency reaches a maximum. At that distance from the input end little current flows in a radial. There is nothing to be gained in efficiency by extending it any further. To lengthen a radial beyond the point when Zin = Zo serves no practical purpose insofar as transmitter performance is concerned. The Number of Radials Accuracy of Estimation Behaviour of a System of N Radials Attenuation per 1/4 wavelength of line decreases at the higher frequencies. Consequentially, at 30 MHz attenuation is small enough to see peaks and troughs in input impedance as length is increased up to 3/4-wavelengths and beyond. At 2 MHz and lower, line attenuation per 1/4-wave is high enough to damp down peaks and troughs in input impedance. The first peak at 1/4-wave is almost nonexistent. The best way to see these two effects is to vary length while observing the small maximum in efficiency at approximately 1/4-wavelength of line where the line's input resistance versus line length passes through a minimum. Except at VLF, Zo of a radial wire has a positive angle. This is due to normal wire inductance in conjunction with the large shunt conductance of the soil. Zo increases with frequency which is not good for efficiency. This is due to skin effect in the wire and the increase in wire resistance versus frequency. The program includes a simplified model of a vertical or an inverted-L antenna of the same length. This helps to show how a radial system affects radiating efficiencies of antennas of different lengths. The antenna base-loading coil or capacitor is a reminder that ground reactance is tuned-out by a tuner simultaneously with the antenna input reactance. The program user must judge the number of decibels attenuation at which the line's input impedance can be assumed to have converged on Zo. The behaviour of the antenna efficiency calculation will be taken into account. The user may have reason to bias his judgment above or below a typical value of 14 dB. If a user has confidence in the accuracy of his knowledge about ground resistivity he may decide to shorten radials to 1/4-wavelength at a particular frequency to take advantage of the small improvement in efficiency which occurs at that length and frequency even though the Zin = Zo limit may not be met. At very high ground resistivities the loss in the ground is small, large standing waves occur on the radials and they behave similar to elevated radials. It becomes necessary to cut them to be 1/4-wave resonant. Or change antenna type. Remember that a 1/4-wavelength along a buried radial is determined by its own propagation velocity. This depends on soil properties including permittivity. The free-space velocity value must be disregarded. Frequency may be varied between 1 KHz and 30 MHz. Zo and VF are small at VLF. Attenuation per 1/4-wavelength is large. The latter determines whether peaks and troughs will occur in the input-impedance versus frequency curve. None occur at LF and VLF. Zin smoothly converges onto Zo. Table of Ground Characteristics
Ground Characteristics
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it from Your Computer Also see Version 3 of this program. This page was last modified: Tue, 31 Aug 2010 02:59:44 GMT
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