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Handbook of Propagation Effects for Vehicular and ... - Courses

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Theoretical Modeling Considerations 11-19<br />

scattered multipath echoes. The resulting signal amplitude has a Ricean probability<br />

density characterized by a constant ratio <strong>of</strong> direct to scattered power. In the shadowed<br />

state, the amplitude <strong>of</strong> the line-<strong>of</strong>-sight signal is assumed to have lognormal statistics.<br />

When combined with constant level diffuse multipath, the probability density (11-40)<br />

derived by Loo applies.<br />

The overall probability density <strong>of</strong> the received voltage is developed analogously to the<br />

derivation <strong>of</strong> (11-57) as<br />

f v<br />

2<br />

( v)<br />

= ( 1 − S)<br />

2Kv<br />

exp[<br />

− K(<br />

v + 1)<br />

) ] I ( 2Kv)<br />

×<br />

∞<br />

∫<br />

0<br />

1 ⎡<br />

exp⎢−<br />

z ⎣<br />

2<br />

( 20log(<br />

z)<br />

− m)<br />

2 2 ⎤<br />

K ( v z ) I ( Kv<br />

z)<br />

dz<br />

2s<br />

2<br />

0<br />

−<br />

8.<br />

686<br />

+ S<br />

s<br />

+<br />

⎥<br />

⎦<br />

0<br />

2<br />

2Kv<br />

π<br />

(11-58)<br />

where S, K, K , m, <strong>and</strong> s are the five model parameters already described in the previous<br />

section.<br />

Table 11-5: Parameter Values <strong>for</strong> the Lognormal Shadowing Model<br />

Parameter Range <strong>of</strong> Values Remarks<br />

K 22 to 13 dB Low to high multipath, unshadowed<br />

K 21 to 18 dB Low to high multipath, shadowed<br />

m -1 to -10 dB Light to heavy shadowing<br />

s 0.5 to 3.5 dB Light to heavy shadowing<br />

S 0.0 to 1.0 No shadowing to frequent shadowing<br />

The parameters given in Table 11-5 were determined by a least square error fit <strong>of</strong> the<br />

statistical model to propagation data collected using a helicopter as the source plat<strong>for</strong>m.<br />

11.4.4.1 Discussion<br />

As was the case <strong>for</strong> the other statistical models, the lognormal shadowing model has been<br />

fit to measured cumulative fade distributions quite well. One would expect an increased<br />

multipath power level to go h<strong>and</strong>-in-h<strong>and</strong> with shadowing conditions. The small range<br />

<strong>and</strong> low level found <strong>for</strong> K seem to indicate that the model does not adequately uncouple<br />

shadowing <strong>and</strong> scattering. The range <strong>of</strong> applicability <strong>of</strong> the model vis-à-vis elevation<br />

angle has also not been specified.<br />

Because <strong>of</strong> the complexities in evaluating (11-58), a much simpler empirical model (in<br />

the next section) was derived from the statistical results by curve fitting procedures.<br />

11.4.5 Simplified Lognormal Shadowing Model<br />

This model [Barts <strong>and</strong> Stutzman, 1991; Barts et al., 1987] has the inputs S, K, K , m, <strong>and</strong><br />

s, which have been defined in the previous two sections <strong>and</strong> assume the values

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