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

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8-30<br />

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

(Duluth, MN), 42.3° (Boulder, CO), 44.7° (Kansas City, MO), 49.6° (Little Rock, AK),<br />

<strong>and</strong> 55.4° (Houston, TX). A series <strong>of</strong> measurements were made at different locations<br />

within each house (e.g., 16) <strong>and</strong> related to measurements made outside the house to<br />

obtain the relative attenuation. The average attenuation <strong>and</strong> st<strong>and</strong>ard deviation <strong>for</strong> each<br />

house were subsequently determined.<br />

8.5.1 Experimental Results<br />

Wells emphasizes in his results: (1) two building types; wood siding <strong>and</strong> brick veneer,<br />

(2) two insulation types; ceiling, <strong>and</strong> ceiling <strong>and</strong> walls, <strong>and</strong> (3) two room exposure types;<br />

one or more exposed walls <strong>and</strong> no exposed walls. An exposed wall implied that the line<strong>of</strong>-sight<br />

path passed through a single wall, whereas an unexposed wall scenario implied<br />

that another room or another wall sheltered the wall. A four factor model including<br />

frequency (4 levels), construction type (2 levels), insulation type (2 levels), <strong>and</strong> room<br />

position (2 levels) was developed <strong>and</strong> summarized by the listing in Table 8-17.<br />

To obtain the overall attenuation <strong>for</strong> a particular structure from Table 8-17, we<br />

execute the following example steps: (1) The “Average Value” <strong>of</strong> 6.3 dB is added to<br />

values described in subsequent steps. (2) For a frequency <strong>of</strong> 2.569 GHz, we add +1.16 dB<br />

to the average value. (3) For a brick veneer construction, we add +0.58 dB. (4) For a<br />

structure with insulation in both ceiling <strong>and</strong> walls, add +0.8 dB. (5) For a room with<br />

unexposed walls, add +0.30 dB. The overall attenuation is 9.14 dB <strong>for</strong> the above<br />

combination <strong>of</strong> effects. Wells culls out several “high attenuation” structures. These are<br />

two mobile homes (average attenuation <strong>of</strong> 23.6 dB) <strong>and</strong> two wood frame houses with<br />

interior walls <strong>and</strong> ceiling comprised <strong>of</strong> plasterboard backed with aluminum foil (average<br />

attenuation <strong>of</strong> 17.1 dB). Wells also shows that no significant attenuation occurs as a<br />

function <strong>of</strong> elevation angle.<br />

Wells summarized the above results as follows: (1) On average, the signal level<br />

varied by 0.6 dB as a function <strong>of</strong> position <strong>of</strong> a room within each house. (2) Houses<br />

having brick veneer gave rise to a 1.2 dB higher attenuation than houses with wood<br />

siding. (3) Insulation in ceiling <strong>and</strong> walls caused about 1.6 dB higher attenuation than<br />

insulation in ceiling only. (4) Insulation <strong>and</strong> plasterboard with aluminum backing caused<br />

attenuations between 14.6 to 22 dB. (5) The attenuation at 2.569 GHz was approximately<br />

2.9 dB larger than at 860 MHz. (6) Horizontal polarization at 860 MHz gave<br />

approximately 1.8 dB higher attenuation than vertical polarization.

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