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

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8-12<br />

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

Table 8-6: Parameter values <strong>for</strong> st<strong>and</strong>ard deviation versus b<strong>and</strong>width as given by (8-4)<br />

<strong>and</strong> (8-5).<br />

Site<br />

1 1.6 0.12 0.61<br />

2 1.6 0.03 0.56<br />

3 2.6 2.82 -0.31<br />

4 1.7 0.42 0.42<br />

5 1.4 -0.02 0.55<br />

6 2.4 1.9 0.31<br />

8.3 Slant-Path Building Penetration Measurements at L- <strong>and</strong> S-B<strong>and</strong><br />

In this section, we describe the results <strong>of</strong> another campaign <strong>of</strong> Vogel et al. [1995a, 1995b]<br />

who executed L- <strong>and</strong> S-B<strong>and</strong> slant path fade measurements in six different buildings<br />

employing a tower-mounted transmitter <strong>and</strong> a dual frequency receiver system. Separate<br />

circularly polarized antennas were used at the receiving end <strong>of</strong> the link. The objective <strong>of</strong><br />

this set <strong>of</strong> measurements was to provide inside building signal loss in<strong>for</strong>mation associated<br />

with personal communications satellite design. In particular, the correlation <strong>of</strong> fading<br />

inside buildings between frequencies near 1620 MHz <strong>and</strong> 2500 MHz was examined. The<br />

measurements described in the previous section [Vogel <strong>and</strong> Torrence, 1993] were<br />

targeted towards the application <strong>of</strong> broadcasting from geostationary satellites as they used<br />

a relatively directive receiving antenna in their measurements. In the ef<strong>for</strong>t described<br />

here, azimuthally omni-directional antennas were employed which interact to a greater<br />

degree with the multipath environment.<br />

8.3.1 Experimental Description<br />

The measurement system is comprised <strong>of</strong> a single transmitting antenna located<br />

approximately 20 m from the ground atop a tower mounted on a van. Transmissions<br />

were executed in one <strong>of</strong> two modes. Mode 1 corresponded to the case in which<br />

transmission occurred at simultaneous fixed frequencies <strong>of</strong> 1618 <strong>and</strong> 2492 MHz. Mode 2<br />

corresponded to the case in which simultaneous radiation occurred at two swept<br />

frequency ranges, namely, 1580-1780 MHz <strong>and</strong> 2330-2530 MHz. The L- <strong>and</strong> S-B<strong>and</strong><br />

receiving antennas were spaced 5 cm apart <strong>and</strong> both were mounted on a positioner<br />

(described in the previous section) capable <strong>of</strong> automatically scanning either in the vertical<br />

or horizontal at 5 cm increments over a range <strong>of</strong> 80 cm (16 positions). As mentioned, the<br />

receiving antennas had patterns that were azimuthally omni-directional with a peak gain<br />

at about 30° in elevation. When Mode 1 was selected, the processed outputs were<br />

relative power level versus time <strong>for</strong> L- <strong>and</strong> S-B<strong>and</strong> with a time sampling rate <strong>of</strong> 100 Hz.<br />

When Mode 2 was selected, processing resulted in frequency spectra over ±80 MHz<br />

relative to the center frequencies <strong>of</strong> 1680 <strong>and</strong> 2430 MHz with about 1 MHz resolution<br />

<strong>and</strong> obtained over a 0.1 s sweep duration. In this mode, 160 sample pairs <strong>for</strong> L- <strong>and</strong><br />

S-B<strong>and</strong> were saved to a computer file <strong>for</strong> every sweep lasting 0.1 s. Subsequent to the

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