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The ns Manual (formerly ns Notes and Documentation)1 - NM Lab at ...

The ns Manual (formerly ns Notes and Documentation)1 - NM Lab at ...

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EnvironmentβOutdoor Free space 2Shadowed urban area 2.7 to 5In building Line-of-sight 1.6 to 1.8Obstructed 4 to 6Table 18.1: Some typical values of p<strong>at</strong>h loss exponent βEnvironment σ dB (dB)Outdoor 4 to 12Office, hard partition 7Office, soft partition 9.6Factory, line-of-sight 3 to 6Factory, obstructed 6.8Table 18.2: Some typical values of shadowing devi<strong>at</strong>ion σ dB<strong>The</strong> shadowing model co<strong>ns</strong>ists of two parts. <strong>The</strong> first one is known as p<strong>at</strong>h loss model, which also predicts the mean receivedpower <strong>at</strong> distance d, denoted by P r (d). It uses a close-in distance d 0 as a reference. P r (d) is computed rel<strong>at</strong>ive to P r (d 0 ) asfollows.P r (d 0 )P r (d) = ( dd 0) β(18.4)β is called the p<strong>at</strong>h loss exponent, <strong>and</strong> is usually empirically determined by field measurement. From Eqn. (18.1) we know th<strong>at</strong>β = 2 for free space propag<strong>at</strong>ion. Table 18.1 gives some typical values of β. Larger values correspond to more obstructio<strong>ns</strong><strong>and</strong> hence faster decrease in average received power as distance becomes larger. P r (d 0 ) can be computed from Eqn. (18.1).<strong>The</strong> p<strong>at</strong>h loss is usually measured in dB. So from Eqn. (18.4) we have[ ]P r (d)P r (d 0 )dB( ) d= −10β logd 0(18.5)<strong>The</strong> second part of the shadowing model reflects the vari<strong>at</strong>ion of the received power <strong>at</strong> certain distance. It is a log-normalr<strong>and</strong>om variable, th<strong>at</strong> is, it is of Gaussian distribution if measured in dB. <strong>The</strong> overall shadowing model is represented by[ ] ( )Pr (d)d= −10β log + X dB (18.6)P r (d 0 )dBd 0where X dB is a Gaussian r<strong>and</strong>om variable with zero mean <strong>and</strong> st<strong>and</strong>ard devi<strong>at</strong>ion σ dB . σ dB is called the shadowing devi<strong>at</strong>ion,<strong>and</strong> is also obtained by measurement. Table 18.2 shows some typical values of σ dB . Eqn. (18.6) is also known as a log-normalshadowing model.<strong>The</strong> shadowing model extends the ideal circle model to a richer st<strong>at</strong>istic model: nodes can only probabilistically communic<strong>at</strong>ewhen near the edge of the communic<strong>at</strong>ion range.189

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