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Radwin 2000+ SERIES - About the Fresnel Zone; Figure 19-1 Fresnel Zone

Radwin 2000+ SERIES
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RADWIN2000+SeriesUserManual Release4.2.40 194
AbouttheFresnelZone
19.4AbouttheFresnelZone
TheFresnelzoneisanellipticallyshapedconicalzoneofelectromagneticenergythat
propagatesfromthetransmittingantennatothereceivingantenna.Itisalwayswidestinthe
middleofthe pathbetweenthetwoantennas.
Figure191:Fresnelzone
Fresnellossisthepathlossoccurringfrommultipathreflectionsfromreflectivesurfaces
suchaswater,andinterveningobstaclessuchasbuildingsormountainpeakswithinthe
Fresnelzone.
Radiolinksshouldbedesignedtoaccommodateobstructionsandatmosphericconditions,
weatherconditions,largebodiesofwater,andotherre
flectorsandabsorbersof
electromagneticenergy.
TheFresnelzoneprovidesuswithawa ytocalculatetheamountofclearancethatawireless
waveneedsfromanobstacletoensurethattheobstacledoesnotattenuatethesignal.
ThereareinfinitelymanyFresnelzoneslocatedcoaxiallyaroundthecenterofthedir
ect
wave.TheouterboundaryofthefirstFresnelzoneisdefinedasthecombinedpathlengthof
allpaths,whicharehalfwa velength(1/2)ofthefrequencytransmittedlongerthanthe
directpath.Ifthetotalpathdistanceisonewavelength(1)longerthanthedirectpath,then
theouterboundaryissaidtobetwoFresnelzones.OddnumberFresnelzonesreinforcethe
directwavepathsignal;evennumberFresnelzonescancelthedirectwavepathsignal.
TheamountoftheFresnelzoneclearanceisdeterminedbythewavelengthofthesignal,the
pathlength,andthedistancetotheobstacle.Forreliability,pointtopointlinksar edesigned
tohaveatleast60%ofthefirstFresnelzonecleartoavoidsignificantattenuation.

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