基于电磁理论和实测数据的近距离和极低天线高度的传播模型

N. DeMinco, P. McKenna, R. Johnk
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引用次数: 0

摘要

只提供摘要形式。该摘要描述了电信科学研究所(ITS)开发的无线电波传播模型,该模型是创建短距离移动到移动传播模型的调查结果。ITS审查和评估了目前可用的无线电波传播模型,得出的结论是,这些模型都不适合满足超短距离(2米至2公里)和极低天线高度(1至3米)的要求。该模型适用于150 ~ 6000 MHz的频率范围。已经开发的组合模型是基于电磁场物理理论的分析计算和在三种截然不同的环境中进行的实际测量:农村,城市低层/郊区和密集的城市高层。分析工作的结果可在ITS报告中找到解析法包括计算未扰动电场和根据电场振幅作为距离、频率和地面常数的函数计算损耗。无干扰场是指发射天线在离地面不同距离和高度上产生的电场,在接收天线位置附近不存在任何场干扰因素。ITS报告通过大量实例表明,在大多数情况下,用无扰动电场法计算的传播损耗与更精确的理论方法之间的差异很小无扰动电场法包括近场效应、复合双射线模型、天线高度、地面常数、天线近场和远场响应以及表面波。无扰动场模型可用于2公里以内的距离。它特别适用于小于30米的近距离。该组合模型在2公里范围内有效。测量是伪移动的,因为发射器的位置是固定的,接收器按照预定的驱动模式在环境中移动。真实环境中的环境杂波会导致非视距条件,其中散射和衍射占主导地位,即使是非常短的路径差异。环境杂波有两个方面会导致无线电波传播问题。首先是静态背景的特征,如建筑物、栅栏、树木等植被、电线杆和电线、标牌等。其次是动态背景特征,如车辆和行人交通。本报告将介绍分析模型和如何使用测量数据来创建组合模型,以表示真实的无线电波传播环境。本文还将给出三种不同环境下的一些传播预测结果。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
A propagation model for close-in distances and very low antenna heights based on both electromagnetic theory and measured data
Summary form only given. This abstract describes a radio-wave propagation model that was developed at the Institute for Telecommunication Sciences (ITS) as the result of an investigation to create a short-range mobile-to-mobile propagation model. ITS reviewed and evaluated currently available radio-wave propagation models and came to the conclusion that none of these models were suitable for addressing the requirements of ultra-short distances (2 meters to 2 km) and very low antenna heights (1 to 3 meters). The model is valid for frequencies from 150 to 6000 MHz. The combined model that has been developed is based on both analytical calculations from the physics of electromagnetic field theory and actual measurements performed in three vastly different environments: rural, urban low-rise/suburban and dense urban high-rise. The results of the analytical work are available in an ITS report.1 The analytical method involves the calculation of the undisturbed electric field and calculation of the loss based on the amplitude of the electric field as a function of distance, frequency, and the ground constants. The undisturbed field is that electric field produced by a transmitter antenna at different distances and heights above ground without any field-disturbing factors in the proximity of the receiver antenna location. The ITS report shows via numerous examples that for most scenarios the difference between the propagation loss computed by undisturbed electric field method and a more exact theoretical methods is minimal.1 The undisturbed electric field method includes near-field effects, the complex two-ray model, antenna heights, ground constants, antenna near-field and far-field response and the surface wave. The Undisturbed-Field Model can be used for distances out to 2 km. It is particularly applicable for close-in distances less than 30 meters. The combined model is valid out to distances of 2 km. The measurements are pseudo-mobile, since the transmitter location is fixed and the receiver is moved through the environment following a predetermined driving pattern. Environmental clutter in the real environment can give rise to non-line-of-sight conditions in which scattering and diffraction dominate, even for very short path differences. There are two facets of the environmental clutter that contribute to the radio-wave propagation problem. First are the features of the static background, such as buildings, fences, trees and other vegetation, utility poles and wires, signage, etc. Second are the dynamic background features, such as vehicular and pedestrian traffic. This presentation will describe both the analytical model and how the measured data were used to create the combined model to represent a real radio-wave propagation environment. Some of the propagation prediction results for the three different environments will also be presented.
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