Propagation Slide Show; 25

Application of this model:

Joint interference signal, due to addition of M Rayleigh interferers
N.B. The sum of m Rayleigh phasors is again a Rayleigh phasor, but with different temporal behaviour
Fading after maximum ratio diversity combining
Self interference in dispersive channel
Mathematical approximation for Rician fading

Mathematical model of Nakagami fading

The sum of m exponentially distributed powers is Gamma distributed.

where

G(m) is the gamma function; G(m+1) = m!

m is the 'shape' factor

The local-mean power E [p_t ] = m.

The amplitude is Nakagami m-distributed