Ionosphere is the charged
or the ionized region of the atmosphere above about 60 Km. This region
is
divided into different layers or regions; D, E, F1 and F2. These
regions
correspond to different altitude and electron density levels. The
ionosphere
structure is variable with day and night, seasons and different
latitudes. In
the night region, the D and F1 layers disappear. The density profiles
of day
and night time of midlatitude region is shown in figure1.

The F2 layer
does not
disappear at sunset, instead its density slowly decreases throughout
the night.
Occasionally the nighttime F2 region becomes unstable at midlatitudes.
At these
times the density of the plasma is not smoothly varying with height;
instead it
contains sharp gradients and density structures.
Ionospheric Irregularities
The ionospheric irregularities mentioned above are temporal and spatial variations of the electron density lasting from a couple minutes to a few hours. In the lower latitudes of the F region of the ionosphere, these irregularities are called Equatorial Spread F. Occurrence of similar irregularities in the midlatitude F region is also called spread F, but at the midlatitudes the mechanism of formation of spread F is not understood. Density perturbations form the basis of spread F. Gravity waves are also widely recognized as a major cause for these density perturbations.The following
figure shows
an ionogram for a normal event.
FIGURE 2
(Midlatitude
Non-Spread F event for a
15 minute sweep on November 20, 2004 at 1 UT)
FIGURE 3
(Midlatitude Spread F event for a 15
minute sweep on November 21, 2004 at 1 UT)
Ionograms
obtained for
spread F show thickness or spread in the F region which is more than
that
obtained for a normal ionosphere (figure 3). Instead of a relatively
thin band
of reflections, the ionograms made during a spread F event seem to show
multiple echoes at different heights for the same frequency. This is
called
range spreading. It is also possible for the ionograms to show bands of
echoes
from the same height for multiple frequencies. This is called frequency
spreading.
Figures 2 and 3
also show a
second hop or echo in the ionogram. This is due to the double
reflection of the
pulse from the ionosphere to ground to ionosphere and back at the
receiver.
Thus the wave is reflected twice before being received and hence it is
almost
twice the height of the first echo.
Ionospheric
sounding is one
of the oldest and most accurate ways to study the ionosphere.
Ionosondes are
used to send signals in the ionosphere. These signals when reflected
back
indicate presence of ionization. The frequency at which the reflection
occurs
is related to the plasma density at the altitude from which the echo
occurs.