4.1. Radio Continuum to Far Infrared Ratio
The radio continuum emission at 5 GHz has been
computed from the calculations of stellar Lyman
continuum photons through the gas and the dust and
integrating the emission (without any assumption about the
optical depth). The flux density at 60 µm is taken as a
representative of far-IR emission. The ratio of radio
continuum emission at 5 GHz and flux density at 60 µm
(F5GHz / Fµm) are presented in
Figure 5.
This ratio is extremely sensitive to the density distribution as
shown in Figure 7. Whereas for the O4 case, the ratio is very sensitive
to 100 for both the
types of density distributions,
for the other two cases (O7 and B0.5), only the r-1
density distribution is very sensitive to
100 (above 0.01).