DTU Satellite Systems and Design Course CubeSat Communication
DTU Satellite Systems and Design Course CubeSat Communication
DTU Satellite Systems and Design Course CubeSat Communication
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Danish Space Research Institute<br />
Danish Small <strong>Satellite</strong> Programme<br />
Digital <strong>Communication</strong> - 4<br />
To proceed, we rewrite the “Ebno” equation in the dB-domain:<br />
or<br />
10⋅log(E b /N 0 ) = 10⋅log(P r ) - 10⋅log(B/1 Hz) - 10⋅log(k/1 J/K) - 10⋅log(T/1 K) [dB]<br />
E b /N 0 = P r - 10⋅log(B/1 Hz) - 10⋅log(k/1 J/K) - 10⋅log(T/1 K) [dB]<br />
where E b /N 0 is now expressed in dB <strong>and</strong> P r in dBW or dBm. As usual proper reference<br />
values must be used to make the arguments to the logs dimensionless.<br />
We complete ignore the inconsistency of writing E b /N 0 in the dB expression. E b /N 0 is<br />
now a symbol, not a calculation.<br />
Combining this with the link budget equation P r = P t + G t + G r -L p [dB], we get:<br />
E b /N 0 = (P t + G t ) + G r - L p - 10⋅log(B/1 Hz) - 10⋅log(k/1 J/K) - 10⋅log(T/1 K) [dB]<br />
The quantity P t + G t is denoted EIRP (Equivalent Isotropically Radiated Power):<br />
E b /N 0 = EIRP + G r - L p - 10⋅log(B/1 Hz) - 10⋅log(k/1 J/K) - 10⋅log(T/1 K) [dB]<br />
FH 2001-08-27 Cubesat_<strong>Communication</strong>.ppt<br />
Slide # 20