A new, empirical model for NO densities is developed, to include physi
cally reasonable variations with local time, season, latitude and sola
r cycle. Model calculations making full allowance for secondary produc
tion, and ionising radiations at wavelengths down to 25 Angstrom, then
give values for the peak density N(m)E that are only 6% below the emp
irical IRI values for summer conditions at solar minimum. At solar max
imum the difference increases to 16%. Solar-cycle changes in the EUVAC
radiation model seem insufficient to explain the observed changes in
N(m)E, with any reasonable modifications to current atmospheric consta
nts. Hinteregger radiations give the correct change, with results that
are just 2% below the IRI values throughout the solar cycle, but give
too little ionisation in the E-F valley region. To match the observed
solar increase in N(m)E, the high-flux reference spectrum in the EUVA
C model needs an overall increase of about 20% (or 33% if the change i
s confined to the less well defined radiations at lambda, < 150 Angstr
om). Observed values of NmE show a seasonal anomaly, at mid-latitudes,
with densities about 10% higher in winter than in summer (for a const
ant solar zenith angle). Composition changes in the MSIS86 atmospheric
model produce a summer-to-winter change in N(m)E of about -2% in the
northern hemisphere, and +3% in the southern hemisphere. Seasonal chan
ges in NO produce an additional increase of about 5% in winter, near s
olar minimum, to give an overall seasonal anomaly of 8% in the souther
n hemisphere. Near solar maximum, reported NO densities suggest a much
smaller seasonal change that is insufficient to produce any winter in
crease in N(m)E. Other mechanisms, such as the effects of winds or ele
ctric fields, seem inadequate to explain the observed change in N(m)E.
It therefore seems possible that current satellite data may underesti
mate the mean seasonal variation in NO near solar maximum. A not unrea
sonable change in the data, to give the same 2:1 variation as at solar
minimum, can produce a seasonal anomaly in N(m)E that accounts for 35
-70% of the observed effect at all times.