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

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10-8<br />

10.5 Urban Three-State Fade Model (UTSFM)<br />

<strong>Propagation</strong> <strong>Effects</strong> <strong>for</strong> <strong>Vehicular</strong> <strong>and</strong> Personal Mobile Satellite Systems<br />

Employing concepts described in Section 10.4, an Urban Three-State Fade Model was<br />

developed by Akturan <strong>and</strong> Vogel [1997]. This model, hereafter referred to by the<br />

acronym UTSFM, has the <strong>for</strong>m<br />

fν ( ν, α ) = C( α ) f Rice( ν) + S( α ) f Loo( ν) + B( α) fLoo(<br />

ν)<br />

, (10-8)<br />

where in (10-8) is the elevation angle. Using photogrammetric measurements in urban<br />

Japan, hence<strong>for</strong>th generically referred to as “Tokyo” although other Japanese cities were<br />

also involved, Akturan <strong>and</strong> Vogel [1997] have characterized C, S, B as a function <strong>of</strong> α .<br />

These values, which have been averaged over the 360° azimuth, are tabulated in Table<br />

10-4. In Figure 10-5 are plotted a family <strong>of</strong> CDF’s employing (10-8), the values in Table<br />

10-4 at the mid-range <strong>of</strong> the angular intervals, <strong>and</strong> the parameters in the right-h<strong>and</strong><br />

column <strong>of</strong> Table 10-3. We note the dramatic effect elevation angle has on fade at any<br />

given fixed exceedance probability level. For example, at the 10% level, the fades range<br />

between approximately 6 dB at 82° <strong>and</strong> 28 dB at 7°. Between 12° <strong>and</strong> 67° at the 10%<br />

level, the fade increases at a rate <strong>of</strong> approximately 0.2 dB per degree (e.g., from 15 dB to<br />

25.5 dB). All the curves in Figure 10-5 contain a terraced shape region between<br />

approximately 5 to 13 dB where a relatively small percentage change takes place. Such a<br />

result indicates that increasing the fade margin beyond approximately 5 dB may not “pay<br />

<strong>of</strong>f” until 13 dB is exceeded. The curves in Figure 10-5 may be employed at any urban<br />

location (<strong>for</strong> L-B<strong>and</strong>) under the assumption that the path-state mixture vector is given by<br />

(10-7), implying the urban environment <strong>of</strong> Tokyo is similar to the urban location being<br />

modeled.<br />

Table 10-4: Tabulation <strong>of</strong> azimuth averaged values <strong>of</strong> C, S <strong>and</strong> B in (10-8) <strong>for</strong> different<br />

elevation angle intervals <strong>for</strong> Tokyo, Japan.<br />

Elevation Angle<br />

Interval (°)<br />

C S B<br />

Elevation Angle<br />

Interval (°)<br />

C S B<br />

0-4 0.02 0.03 0.95 45-49 0.67 0.05 0.27<br />

5-9 0.07 0.06 0.86 50-54 0.72 0.05 0.23<br />

10-14 0.17 0.08 0.75 55-59 0.76 0.04 0.20<br />

15-19 0.28 0.08 0.64 60-64 0.80 0.03 0.17<br />

20-24 0.37 0.08 0.56 65-69 0.83 0.03 0.14<br />

25-29 0.44 0.07 0.48 70-74 0.86 0.03 0.11<br />

30-34 0.51 0.07 0.42 75-79 0.89 0.02 0.09<br />

35-39 0.58 0.06 0.36 80-84 0.92 0.02 0.06<br />

40-44 0.63 0.06 0.31 85-89 0.93 0.02 0.06

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