According to ITU-R Rec. P.526-2, the diffraction loss L
p (d) can be derived by the received field strength E referred to the free space E
0 :
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body | $-{{L}_{d}}(p)=20\log \frac{E}{{{E}_{0}}}=F(X)+G({{Y}_{1}})+G({{Y}_{2}})$ |
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(Eq. 220)
with:
X
is the normalized radio path between transmitter and receiver
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body | $X=2.2\beta \ {{f}^{\frac{\ 1}{3}}}\ a_{e}^{\frac{-2}{3}}\ d$ |
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is the normalized antenna height of the
transmitter
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body | $Y=9.6\ \cdot {{10}^{-3}}\beta \ {{f}^{\frac{2}{3}}}\ a_{e}^{\frac{-1}{3}}\ h{}_{i}$ |
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is the normalized antenna height of the receiver
where:
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is a parameter derived from the earth admittance factor K
:
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f is
is the frequency in MHz
e is is the equivalent earth radius in km (definition see below)
d is is the distance in km
i is is the antenna height above ground in m with =1 or 2 for the transmitter or receiver, respectively
The distance-dependent term F
is is given by the semi-empirical formula:
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body | $F(X)=11+10\log (X)-17.6X$ |
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(Eq. 221)
The antenna height gain G
is is given by the formula set:
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body | $G(Y)=17.6{{(Y-1.1)}^{\frac{1}{2}}}-5\log (Y-1.1)-8$ |
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body | $G(Y)=20\log (Y+0.1{{Y}^{3}})$ |
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for
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body | $G(Y)=2+20\log K+9\log (Y/K)\left[ \log (Y/K)+1 \right]$ |
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for
for
where
is the normalized earth surface admittance factor (see ITU-R Rec. P.526), default value 10e-5:
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