Final report on link level and system level channel models - Winner
Final report on link level and system level channel models - Winner
Final report on link level and system level channel models - Winner
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WINNER D5.4 v. 1.4<br />
transmitter locati<strong>on</strong>s. The mean of the difference in <strong>on</strong>e locati<strong>on</strong> was 12 dB <strong>and</strong> for the other 7 dB. In the<br />
paper the path-loss model of [SMI+00] is found to fit the 1.9 GHz measurements <strong>on</strong> LOS streets. This<br />
model is given by<br />
PL<br />
LOS<br />
= e<br />
−sr<br />
λ<br />
π<br />
⎛<br />
⎜<br />
⎝ 4<br />
2<br />
⎞<br />
⎟<br />
⎠<br />
1<br />
e<br />
r<br />
t<br />
1<br />
+ R e<br />
r<br />
− jkrt − jkr n<br />
m<br />
2<br />
(5.36)<br />
where rt<br />
is the line-of-sight path-length, R is the reflecti<strong>on</strong> coefficient of the road surface, <strong>and</strong> s is the<br />
visibility factor. The variable r rm is the distance via reflecti<strong>on</strong> which is described as<br />
r<br />
(( h − h ) + ( h − h )) 2<br />
2<br />
rm = r +<br />
(5.37)<br />
b 0 m 0<br />
where hb<br />
<strong>and</strong> hm<br />
are the base- <strong>and</strong> mobile-stati<strong>on</strong> heights <strong>and</strong> h0<br />
is an effective surface height which is<br />
different from zero due to reflecti<strong>on</strong>s from cars <strong>and</strong> other obstacles. A best fit to the eighteen LOS streets<br />
was found to be h<br />
0 = 1.2m <strong>and</strong> s = 0.001. The RMS-error from this model in the eighteen LOS streets is<br />
listed in a table. We notice that the breakpoint distance which is based <strong>on</strong> the clearance of the first Fresnel<br />
z<strong>on</strong>e with the parameters of the paper appears at such a short distance as 60 meters. The path-loss curve is<br />
similar to a fourth-order slope bey<strong>on</strong>d the breakpoint. We calculate an average the RMS error to be 7.1<br />
dB from this data. The RMS-delay spread is <str<strong>on</strong>g>report</str<strong>on</strong>g>ed to be 15-20% lower at 5.9 GHz than at 1.9 GHz.<br />
From inspecti<strong>on</strong> of the plots in the paper it appears that for LOS cases the delay-spread is 100-150 ns<br />
quite independently of the frequency.<br />
The paper [SMI+00] presents measurements with the transmitter at a height of 4 meters <strong>and</strong> the receiver<br />
at 2.7 meters in a Japanese residential area at 3.5 GHz. The height of the buildings is <strong>on</strong> average eight<br />
meters <strong>and</strong> is therefore higher than the antennas. If the ground <strong>level</strong>, h<br />
0 , is set to zero then breakpoint<br />
distance appears at 678 meters. The measurements up to 460 meters c<strong>on</strong>firmed that free-space<br />
propagati<strong>on</strong> c<strong>on</strong>diti<strong>on</strong>s existed. Delay-spreads never exceeded 200 ns for the LOS measurements. The<br />
plotted power-delay profiles for LOS case seemed to show approximately the form of an exp<strong>on</strong>ential<br />
decay plus a direct path.<br />
The paper [MKA02] studies the impact of the traffic intensity in an urban area <strong>on</strong> the effective ground<br />
<strong>level</strong>. In the paper the base-stati<strong>on</strong> height is 4meters <strong>and</strong> the mobile-stati<strong>on</strong> height 1.6 meter or 2.7 meter.<br />
Measurements are d<strong>on</strong>e at 3.35, 8.45 <strong>and</strong> 15.75 GHz. The effective ground <strong>level</strong> is estimated to about 0.5<br />
meter during night-time <strong>and</strong> 1.4meter during daytime. The paper also presents RMS-delay-spread values<br />
versus path loss during night-time. From these figures we deduce that it is less than 200 ns at midnight<br />
before the breakpoint distance. Bey<strong>on</strong>d the breakpoint a 3.6 to 4.6 path-loss slope is observed. The<br />
st<strong>and</strong>ard deviati<strong>on</strong> around the mean value seems to be about ±5 dB before the breakpoint <strong>and</strong> ±10 dB<br />
after the breakpoint. A formula for the delay-spread is fitted to the data as<br />
s<br />
[ ns] exp( β )<br />
= , (5.38)<br />
where β is 0.050 during day-time <strong>and</strong> 0.049 during night time. The sample-points used for the fitting of<br />
this formula c<strong>on</strong>tain measurements at 3.35, 8.45 <strong>and</strong> 15.75 GHz. The paper does not state any variati<strong>on</strong><br />
with frequency.<br />
In [FBR+94] micro-cell measurements at 1900 MHz are analyzed for path loss <strong>and</strong> delay-spread with an<br />
MS height of 1.7meter <strong>and</strong> base-stati<strong>on</strong> heights of 3.7, 8.5, <strong>and</strong> 13.3. A path-loss model is fitted where a<br />
free-space propagati<strong>on</strong> law is used up to the breakpoint <strong>and</strong> a 3rd or 4th order law is recommended<br />
bey<strong>on</strong>d that point, shadow fading estimates are in the range 7-8 dB. No effective street-<strong>level</strong> modelling is<br />
used – maybe measurements were d<strong>on</strong>e when there was no traffic? An exp<strong>on</strong>ential dependence between<br />
the path loss <strong>and</strong> delay-spread as in previous reference is also found – however this time the model<br />
c<strong>on</strong>siders the maximum delay-spread. A visual inspecti<strong>on</strong> of the viewgraph of the paper seems to c<strong>on</strong>firm<br />
that typical delay-spreads obey the formula of [MKA02] given above.<br />
In [FDS+94] measurements were d<strong>on</strong>e with the transmitter at 4meter height <strong>and</strong> the receiver <strong>on</strong> the top of<br />
a Van at 2.5 meters. The measurements were d<strong>on</strong>e <strong>on</strong> Southampt<strong>on</strong> University Campus at 1.8 GHz. The<br />
results for LOS show a K-factor between 1 <strong>and</strong> 30 at range of up to the breakpoint. In c<strong>on</strong>trast for the<br />
NLOS measurements the K-factor is between 0 <strong>and</strong> 2.<br />
In [KVV05] polarizati<strong>on</strong> is analyzed in various urban scenarios. The <strong>on</strong>e, most similar to what is<br />
c<strong>on</strong>sidered here, is the urban micro-cell LOS case although the base-stati<strong>on</strong> is c<strong>on</strong>siderably more elevated<br />
than what we are c<strong>on</strong>sidering here <strong>and</strong> the mobile-stati<strong>on</strong> is less (BS height 10 meters, MS height 1.6<br />
meter in the measurements). For this scenario an XPR of around 9 dB is obtained.<br />
In [MIS01] directi<strong>on</strong>al measurements in an urban area with rotating antennas at 8.45 GHz are presented.<br />
The base-stati<strong>on</strong> height is four or eight meters while the mobile-stati<strong>on</strong> height is 3.0 meters. The angle-<br />
PL dB<br />
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