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2( d1 + d2 ) v=h d1 d2 Notice that v will be positive for obstructed paths and negative for clear LOS paths After finding v, based on the theory of the diffraction of electric fields over a knife edge, the loss may be approximated by: when 08 v 0 602 + 9v + 165v2 A(v) 602 + 911v 127v2 when 0< v 24 when v > 24 12953 + 20 log v

(37)

Relative to isotropic antenna with linear polarization Relative to dipole antenna with linear polarization

Example:



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Let s assume a single tree on an 18-GHz, 5-mi-long path The distance of the tree to the rst site is 1 mi The obstacle height is 30 ft above center of the Fresnel s zone and k=4/3 Calculate attenuation due to the diffraction Note: Keep in mind the consistency of the units for obstacle height, wavelength, and the distance We will use feet for this example

dBic Relative to isotropic antenna with circular polarization dBdc Relative to dipole antenna with circular polarization

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h = 30 ft k=4/3

First we calculate parameter v: 2 26400 28 0055 5280 21120

Remember that antennas with different polarization do not communicate and also do not interfere with each other





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A(v) 12953 + 20 log 28 219 dB This is a theoretical analysis of a completely blocked path, something we should never use in real-life microwave path design For cases where h = 0 (grazing) we have v = 0, and from the formula, we can see that attenuation will be very close to 6 dB Although sufficient for a quick analysis, an ideal knife-edge rarely occurs in practice, so there is another, modified and more realistic set of formulas that take into consideration the finite radius of the obstacle If a knife-edge approximation is considered, the values given in Figure 34 are reasonable approximations Having an obstacle-free 60 percent of first Fresnel zone gives 0 dB obstruction loss In case of more than one obstacle, the well-known approach by Bullington assumes that all the obstacles can be replaced with one equivalent knife-edge obstacle The Epstain-Peterson method sums all the individual, single-knife obstacle losses The Deygout method determines the largest obstacle and focuses on the calculations related to it The Deygout method tends to overestimate the true path losses when there are a large number of obstacles (edges) or when they are very close together (Causebrook offered corrections for those cases) The Giovanelli method is a result of another development of the Deygout method

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The recommended models for diffraction loss are given by the ITU-R Recommendation P526 The latest version of this document should be used as it is regularly updated and improved

Antenna efficiency is the ratio of power actually radiated from the antenna to the power provided to the antenna terminals Radiation in an antenna is caused by radiation resistance, which can be measured only as a part of the total resistance, including the loss resistance The loss resistance usually results in heat generation rather than radiation, and therefore reduces efficiency Impedance of an antenna can be easily measured with specialized equipment Measuring the radiation pattern requires a sophisticated setup, including an anechoic chamber (to exclude radiation noise) designed for antenna measurements, precise placement of measuring equipment, and specialized equipment that rotates the antenna during the measurements All of the antenna parameters are expressed in terms of a transmission antenna but are identically applicable to a receiving antenna due to reciprocity The measurement of impedance at the load, where the power is consumed, is most critical For a transmitting antenna, the load is the antenna itself, while for a receiving antenna, the load is the receiver rather than the antenna The reading range of an RFID antenna depends on many variables: the antenna size, the tag size, the tag s orientation with respect to the transmitting antenna, the antenna location with respect to other materials, and the ambient electrical and magnetic noise within the band of interest The impedance of an antenna should match that of its connecting transmission line The polarization of an antenna should match with the tag orientation Antennas used for transmission have a maximum specified power rating, beyond which heating, arcing, or sparking may occur in the components, which

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