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Reflection on the Earth s surface may give rise to multipath propagation Depending on the path geometry, the direct ray at the receiver may be interfered with by the ground-reflected ray, and the reflection loss can be significant Since the refraction properties of the atmosphere are constantly changing (k-value changes), the reflection loss varies (fades) The loss due to reflection on the ground is dependent on the total reflection coefficient of the ground and the phase shift Figure 35 illustrates the signal strength as a function of the total reflection coefficient The highest value (AMax) of signal strength is obtained for a phase angle of 0 , and the lowest value (AMin) is for a phase angle of 180 The reflection coefficient is dependent on the frequency, grazing angle (angle between the ray beam and the horizontal plane), polarization, and other ground properties The grazing angle of radio-relay paths is very small usually less than 1 It is strongly recommended to avoid ground reflection, which can be achieved by shielding the path against the indirect ray For large grazing angles, the difference between vertical and horizontal polarization is substantial Changing the antenna heights can move the location of the reflection point This approach, usually known as the hi-lo technique, forces the reflection point to move closer to the lowest antenna by affecting the height of the higher antenna The grazing angle increases, and the path becomes less sensitive to k-value variations



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Signal strength [dB]

may cause them to be damaged or destroyed This, of course, is a concern only for transmitting antennas; the power received by an antenna rarely exceeds the microwatt range

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Space diversity also provides good protection against reflection, and it is usually applied for paths over open water surfaces Obviously, on many paths, particularly at higher frequencies, it is difficult to obtain an accurate estimate of the effective surface reflection coefficient because of various uncertainties such as the surface conductivity, surface roughness, and so on, and the degree of subjectivity currently needed to obtain a calculation The calculation procedure may only be a rough guide in such situations to help identify problem paths or to help choose one path from another, even if this possibility exists in the first place The contribution resulting from reflection loss is not automatically included in the link budget However, when reflection cannot be avoided, the fade margin may be adjusted by including this contribution as additional loss in the link budget 33 Fading and Fade Margins

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The isotropic radiator is a purely theoretical antenna that radiates equally in all directions It is considered to be a point in space with no dimensions and no mass This antenna cannot physically exist, but is useful as a theoretical model for comparison with all other antennas Most antennas gains are measured with reference to an isotropic radiator and are rated in dBi (decibels with respect to an isotropic radiator) An isotropic antenna s radiation pattern is spherical

Fading is defined as the variation of the strength of a received radio carrier signal due to atmospheric changes and/or ground and water reflections in the propagation path Fading types normally considered when planning microwave point-to-point paths are as follows:

Rain fading Refraction-diffraction fading (k-type fading)

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