An Optimal Electric Dipole Antenna Model and Its Field Propagation
An optimal electric dipole antennas model is presented and analyzed, based on the hemispherical grounding equivalent model and the superposition principle. The paper also presents a full-wave electromagnetic simulation for the electromagnetic field propagation in layered conducting medium, which is...
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2016-01-01
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Series: | International Journal of Antennas and Propagation |
Online Access: | http://dx.doi.org/10.1155/2016/8601497 |
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doaj-9ac5191b13c84d7bb074c8aec0faebfc2020-11-24T22:51:20ZengHindawi LimitedInternational Journal of Antennas and Propagation1687-58691687-58772016-01-01201610.1155/2016/86014978601497An Optimal Electric Dipole Antenna Model and Its Field PropagationYidong Xu0Lili Guo1Wei Xue2Korochentsev Vladimir3Junwei Qi4College of Information and Communication Engineering, Harbin Engineering University, Harbin 150001, ChinaCollege of Information and Communication Engineering, Harbin Engineering University, Harbin 150001, ChinaCollege of Information and Communication Engineering, Harbin Engineering University, Harbin 150001, ChinaSchool of Engineering, Far Eastern Federal University, Vladivostok 690950, RussiaCollege of Information and Communication Engineering, Harbin Engineering University, Harbin 150001, ChinaAn optimal electric dipole antennas model is presented and analyzed, based on the hemispherical grounding equivalent model and the superposition principle. The paper also presents a full-wave electromagnetic simulation for the electromagnetic field propagation in layered conducting medium, which is excited by the horizontal electric dipole antennas. Optimum frequency for field transmission in different depth is carried out and verified by the experimental results in comparison with previously reported simulation over a digital wireless Through-The-Earth communication system. The experimental results demonstrate that the dipole antenna grounding impedance and the output power can be efficiently reduced by using the optimal electric dipole antenna model and operating at the optimum frequency in a vertical transmission depth up to 300 m beneath the surface of the earth.http://dx.doi.org/10.1155/2016/8601497 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Yidong Xu Lili Guo Wei Xue Korochentsev Vladimir Junwei Qi |
spellingShingle |
Yidong Xu Lili Guo Wei Xue Korochentsev Vladimir Junwei Qi An Optimal Electric Dipole Antenna Model and Its Field Propagation International Journal of Antennas and Propagation |
author_facet |
Yidong Xu Lili Guo Wei Xue Korochentsev Vladimir Junwei Qi |
author_sort |
Yidong Xu |
title |
An Optimal Electric Dipole Antenna Model and Its Field Propagation |
title_short |
An Optimal Electric Dipole Antenna Model and Its Field Propagation |
title_full |
An Optimal Electric Dipole Antenna Model and Its Field Propagation |
title_fullStr |
An Optimal Electric Dipole Antenna Model and Its Field Propagation |
title_full_unstemmed |
An Optimal Electric Dipole Antenna Model and Its Field Propagation |
title_sort |
optimal electric dipole antenna model and its field propagation |
publisher |
Hindawi Limited |
series |
International Journal of Antennas and Propagation |
issn |
1687-5869 1687-5877 |
publishDate |
2016-01-01 |
description |
An optimal electric dipole antennas model is presented and analyzed, based on the hemispherical grounding equivalent model and the superposition principle. The paper also presents a full-wave electromagnetic simulation for the electromagnetic field propagation in layered conducting medium, which is excited by the horizontal electric dipole antennas. Optimum frequency for field transmission in different depth is carried out and verified by the experimental results in comparison with previously reported simulation over a digital wireless Through-The-Earth communication system. The experimental results demonstrate that the dipole antenna grounding impedance and the output power can be efficiently reduced by using the optimal electric dipole antenna model and operating at the optimum frequency in a vertical transmission depth up to 300 m beneath the surface of the earth. |
url |
http://dx.doi.org/10.1155/2016/8601497 |
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