高精度露天场地衰减计算的新校正因子(4)

A. Maeda, S. Takeya, Y. Kami
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Introduction A report has previously been made on the precise measure­ ments of site attenuation of horizontally polarized waves and on the theoretical analysis of the results. This time, analysis was made on the site attenuation of vertically polarized waves using the same analysis method. Good agreement was obtained between the calculated and actually measured values. Especially the height pattern of the attenuation value at the receiving point, on which we have concentrated for some time, showed good agreement between the calculated and measured values in the same manner as for the horizontally polarized waves. Our previous report took the frequency at which the retlection coefficient (T) of the antenna measured from the cable end becomes minimum as the resonant frequency of the tuned dipole antenna. However measurements of the site attenua­ tion at this freqiency showed us that this frequency is not appropriate for use as the tuned frequency. * I At present the resonant frequency of the antenna is found by a cut and try method. These measurements were conduct­ ed provisionally with a half wavelength dipole antenna, so there was no need to measure the resonant frequency. 1. Calculation Procedure Calculation was made on using terms for all e ffects between the transmitting and receiving antennas, as shown in Fig. 1. As shown in the Appendix, the current distribution of tuned dipole antenna was assumed to be a sinusoidal distribution.*2 1.1 Site attenuation of horizontally polarized waves The interrelations of antennas was considered as shown in Fig. 2. *1 : We had assumed that this method was not truly appro­ priate from the results of our calculations on antennas, but we dared to try to determine antenna resonance frequency using this method of measurement because no other appropriate method was found. We realized that this frequency is inappropriate, though, because of inconsistency between the measured and calculated values of height pattern. Our analysis of the tuned dipole antenna will be reported at another opportunity. CH2294-7/86/000-0354 $01 .0 0 (6 )l 986 IEEE 354 *2 : Further detailed analysis on antenna current distri­ bution. Mr. T. Kawana et al. reported 2) an analysis using the moment method. 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引用次数: 0

摘要

迄今为止,我们所发表的关于开放场地场地衰减的精确测量和理论分析值的论文都是针对水平极化的。在实际测量值和计算值之间得到了约1db的良好一致性。影响衰减的个别项被累加到公式中,以考虑所涉及的所有因素,我们认为我们已经达到了实际目的的足够精度。这一次,我们扩展了计算,使其适用于垂直极化。采用与水平极化相同的方法,对接收点衰减值的测量高度图与计算高度图的一致性进行了研究,得到了很好的一致性。以前曾报道过水平极化波现场衰减的精确测量和结果的理论分析。这次采用相同的分析方法对垂直极化波的场地衰减进行了分析。计算值与实测值吻合较好。特别是我们研究了一段时间的接收点衰减值的高度分布,计算值与实测值的吻合程度与水平极化波的吻合程度相当。我们之前的报道将从电缆端测得的天线反射系数(T)最小的频率作为调谐偶极子天线的谐振频率。然而,对该频率的现场衰减测量表明,该频率不适合用作调谐频率。目前天线的谐振频率是通过试切法确定的。这些测量是临时用半波长偶极子天线进行的,因此不需要测量谐振频率。1. 对发射天线和接收天线之间的所有效应用项进行计算,如图1所示。如附录所示,假设调谐偶极子天线的电流分布为正弦分布。*2 1.1水平极化波的站点衰减考虑天线的相互关系如图2所示。*1:从我们对天线的计算结果来看,我们已经假设这种方法并不真正合适,但由于没有找到其他合适的方法,我们敢于尝试使用这种测量方法来确定天线谐振频率。然而,我们意识到这个频率是不合适的,因为高度模式的测量值和计算值之间不一致。我们对调谐偶极子天线的分析将在另一个机会报告。CH2294-7/86/000-0354 $01 .0 0 (6)l 986 IEEE 354 *2:天线电流分布的进一步详细分析。T. Kawana等人报告了一项使用矩量法的分析。结果表明,如果假设天线上的电流分布为正弦分布,则最大振幅差仅为20%左右,而在整个天线长度(相当于天线的有效长度)上积分的电流差小于5%。这5%的差异在我们场地衰减测量的不确定度范围内。图1计算中包含的辐射波和再辐射波简图。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
New Correction Factor for High-precision Open-site Attenuation Calculation (4)
The papers that we have given so far for precise measure­ ments and theoretical analysis values of site attenuation for open sites have all been for horizontal polarization. Good agreement within about 1 dB has been obtained between actual measurements and calculated values. The individual terms influencing the attenuation were cumulatively added to the formula to account for all factors involved, and we think that we have achieved sufficient accuracy for practical purposes. This time we have extended the calculation to make it suitable for vertical polarization. The agreement of the measured and calculated height pattern of the attenuation value at the receiving point was studied in the same manner as for horizontal polarization and excellent agreement was obtained. Introduction A report has previously been made on the precise measure­ ments of site attenuation of horizontally polarized waves and on the theoretical analysis of the results. This time, analysis was made on the site attenuation of vertically polarized waves using the same analysis method. Good agreement was obtained between the calculated and actually measured values. Especially the height pattern of the attenuation value at the receiving point, on which we have concentrated for some time, showed good agreement between the calculated and measured values in the same manner as for the horizontally polarized waves. Our previous report took the frequency at which the retlection coefficient (T) of the antenna measured from the cable end becomes minimum as the resonant frequency of the tuned dipole antenna. However measurements of the site attenua­ tion at this freqiency showed us that this frequency is not appropriate for use as the tuned frequency. * I At present the resonant frequency of the antenna is found by a cut and try method. These measurements were conduct­ ed provisionally with a half wavelength dipole antenna, so there was no need to measure the resonant frequency. 1. Calculation Procedure Calculation was made on using terms for all e ffects between the transmitting and receiving antennas, as shown in Fig. 1. As shown in the Appendix, the current distribution of tuned dipole antenna was assumed to be a sinusoidal distribution.*2 1.1 Site attenuation of horizontally polarized waves The interrelations of antennas was considered as shown in Fig. 2. *1 : We had assumed that this method was not truly appro­ priate from the results of our calculations on antennas, but we dared to try to determine antenna resonance frequency using this method of measurement because no other appropriate method was found. We realized that this frequency is inappropriate, though, because of inconsistency between the measured and calculated values of height pattern. Our analysis of the tuned dipole antenna will be reported at another opportunity. CH2294-7/86/000-0354 $01 .0 0 (6 )l 986 IEEE 354 *2 : Further detailed analysis on antenna current distri­ bution. Mr. T. Kawana et al. reported 2) an analysis using the moment method. It shows that if the current distribution on the antenna is saaumed to have sinusoidal distribution the maximum amplitude difference is only about 20%, and that the difference was less than 5% for the current integrated over the entire antenna length (equivalent to antenna's effective length). This 5% difference falls within the range of uncertainty in our site attenuation measurement. 3)S IT E R T T E N U R T IO N C d B 3 SESSION 5A Fig. 1 Scematic diagram of radiated and re-radiated waves included in our calculations.
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