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Final report on link level and system level channel models - Winner

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WINNER D5.4 v. 1.4<br />

5.6 Interpretati<strong>on</strong> of results<br />

5.6.1 Path-loss<br />

5.6.1.1 Scenario A1<br />

5.6.1.1.1 Proposed path-loss model<br />

The results for path loss <strong>and</strong> shadowing have been summarized in Table 5.45.<br />

Table 5.45: Path-loss <strong>and</strong> shadowing characteristics in the indoor envir<strong>on</strong>ment.<br />

Indoor LOS (c-c) NLOS (r–c)<br />

PL at 5.25 GHz<br />

SF st<strong>and</strong>ard deviati<strong>on</strong> at<br />

5.25 GHz<br />

46.8 +18.7 log10(d),<br />

d >1m<br />

s = 3.1 dB<br />

PL (d)= 38.8+36.8 log10(d)<br />

d >5m<br />

s = 3.5 dB<br />

5.6.1.1.2 Probability of LOS<br />

The probability of line-of-sight (LOS) propagati<strong>on</strong> vs. distance is a functi<strong>on</strong> we denote the pLOS<br />

functi<strong>on</strong>. For scenario A1, this characteristic can be derived analytically because the geometry of the<br />

scenario is known exactly.<br />

A simple ad-hoc fit of the derived pLOS functi<strong>on</strong> is given as:<br />

p LOS (d) = 1 – (1 – x 3 ) 1/3 * (1 – 5 / 50), (5.55)<br />

where x = 1 - log 10 (d / 2.5) / log 10 (100 / 2.5).<br />

5.6.1.2 Scenario B5a<br />

We use the path-loss model of [PT00] as given below. We assume that it is applicable from 30 meters to<br />

2km distance with a correcti<strong>on</strong> term for frequency, i.e.<br />

( fc<br />

/ 2.5GHz) + 23.5log10( d + δ<br />

slow<br />

Loss = 36 .5 + 20log10<br />

) , 300 m < d < 8 km (5.56)<br />

We note that for the 30m to 300m range (for which [PT00] presents no measurements), the path-loss<br />

model almost coincides with cases in [Dug99] with the smallest path-loss. These cases are probably the<br />

<strong>on</strong>es with the least obstructed LOS. The model of [PT00] is for 2.5GHz. For other centre-frequencies, fc,<br />

it seems reas<strong>on</strong>able to translate by using the free-space frequency dependence as the propagati<strong>on</strong> scenario<br />

(e.g. path-loss exp<strong>on</strong>ent) is close to free-space propagati<strong>on</strong>.<br />

The shadow fading is Gaussian with mean zero <strong>and</strong> st<strong>and</strong>ard deviati<strong>on</strong> σ SF = 3.4 dB based <strong>on</strong> [PT00].<br />

5.6.1.3 Scenario B5b<br />

Based <strong>on</strong> the observati<strong>on</strong> of numerous papers that the path loss follows approximately a free-space law<br />

before the breakpoint distance we will assume that loss is given by<br />

Loss<br />

( r) = −20log( /( 4πr)<br />

) + σ free + δ free,<br />

r ≤ rb<br />

λ , d < 1 km (5.57)<br />

where the first part is recognized as the free-space path-loss, d free is a Gaussian distributed r<strong>and</strong>om<br />

variable (shadow fading), with st<strong>and</strong>ard deviati<strong>on</strong> s free = 3 dB. This path-loss model (i.e., (4.10)) can be<br />

used for a maximum distance of 1 km. Many measurements seem to show path loss lower than the freespace<br />

before the breakpoint <strong>and</strong> indeed it can happen due to c<strong>on</strong>structive multi-path. However, to avoid<br />

producing overly optimistic results the extra loss s free has been introduced such that the probability of a<br />

lower than free-space loss is <strong>on</strong>ly some 14%. The breakpoint distance is calculated as<br />

( h − h )( h − h )<br />

b 0 b 0<br />

rb = 4<br />

(5.58)<br />

λ<br />

where we, somewhat pessimistically, set the effective ground <strong>level</strong> h0<br />

to 1.6 meter. For distances larger<br />

than r b we set the path loss to<br />

Loss<br />

( r) = free − 20log10( λ /( 4πrb<br />

)) + 40log( r / rb ) + δ bey<strong>on</strong>d,<br />

r > rb<br />

σ , (5.59)<br />

where the first two teRMS corresp<strong>on</strong>d to the (mean) path-loss at b<br />

r <strong>and</strong> d bey<strong>on</strong>d is a Gaussian shadowfading<br />

term with mean zero <strong>and</strong> st<strong>and</strong>ard deviati<strong>on</strong> 7 dB.<br />

Page 127 (167)

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