In this mode, the ILT is randomly placed in a circular area, the simulation radius is automatically derived from the density and activity of transmitters. The influence of the closest interferer can be estimated by having a
distance d
ILT->VLR following a Rayleigh distribution
as defined in ANNEX 10: and where the parameter
is related to the density of transmitters
Image Removed
| Mathinline |
|---|
| body | $\sigma =\frac{1}{\sqrt{2\pi \ dens_{ILT}^{active}}}$ |
|---|
|
(Eq.
173182)
wherehere:
Image Removed (Eq. 174)
...
| Mathinline |
|---|
| body | $den{{s}_{ILT}}^{active}=den{{s}_{ILT}}.{{p}_{ILT}}.activit{{y}_{ILT}}(time)$ |
|---|
|
(Eq. 183)
For this mode, the path distance factor is fixed to a Rayleigh distribution and is not editable.