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DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

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ionosonde<br />

Each sporadic E layer can be described by three<br />

parameters: hEs, foEs, <strong>and</strong> fbEs. Finally, two<br />

further important parameters are fmin, the minimum<br />

frequency returned from the ionosphere<br />

<strong>and</strong> recorded on the ionogram <strong>and</strong> M(3000)F2.<br />

These parameters are tabulated hourly, together<br />

with other information, <strong>and</strong> exchanged between<br />

World Data Centers. There is now a serious<br />

attempt to collect these data in real time <strong>and</strong><br />

construct global maps of the ionosphere. To obtain<br />

the electron density profile in real height<br />

units, sometimes called true height, it is necessary<br />

to invert the ionogram, <strong>and</strong> correct for the<br />

time delay caused by the ionosphere. See criticalfrequency,<br />

ionosonde, ionosphericsounding,<br />

plasma frequency.<br />

ionosonde A swept frequency pulsed radio<br />

transmitter on the ground cosited with a receiver<br />

forming a vertically directed radar system.<br />

A single frequency pulse is transmitted upwards<br />

<strong>and</strong> may be reflected from the ionosphere,<br />

the reflected signal being observed with the receiver.<br />

This process is repeated at a sequence<br />

of frequencies usually starting at a frequency of<br />

1.0 MHz <strong>and</strong> finishing at around 20 MHz. A picture<br />

of the ionization above the ionosonde is then<br />

built up into an ionogram. This is constructed<br />

by displaying the returned signal as a function<br />

of frequency (on the horizontal axis) <strong>and</strong> time<br />

delay (on the vertical axis). See ionogram.<br />

ionosphere The layer of the Earth’s atmosphere<br />

extending from the top of the mesosphere<br />

(typically 80 to 90 km above the surface)<br />

to about 500 km. The thermosphere, or<br />

ionosphere, is the uppermost layer of a planetary<br />

atmosphere. It is also often called the<br />

upper atmosphere. It is characterized by low<br />

density ( 3 × 10 −9 gm/cm 3 ; number density<br />

7 × 10 −11 /cm 3 ) <strong>and</strong> pressure ( 0.1 Pa),<br />

<strong>and</strong> substantial ionization of the atoms, resulting<br />

in significant free electron density, which<br />

is a function of solar activity. The temperature<br />

increases rapidly with increasing altitude up to<br />

about 200 km, followed by a leveling off in the<br />

300 to 500 km region. This heating is the result<br />

of photoionization <strong>and</strong> photodissociation of<br />

molecules into atoms <strong>and</strong> ions by direct absorption<br />

of solar photons.<br />

© 2001 by CRC Press LLC<br />

252<br />

ionospheric absorption Radio waves passing<br />

through the ionosphere experience interactions<br />

with the free electrons <strong>and</strong> may lose energy<br />

by these interactions if the electrons experience<br />

collisions with the neutral atmosphere.<br />

This process is called absorption, or sometimes<br />

non-deviative absorption, because the radiowave<br />

path through the absorbing region is not<br />

affected by the absorption. Collisions between<br />

electrons <strong>and</strong> the neutral atmosphere increase<br />

with decreasing altitude, so the D region is<br />

particularly important for absorption processes.<br />

Absorption varies as the inverse square of the<br />

frequency, so the losses are larger at low HF<br />

frequencies. In normal circumstances, during<br />

the daytime, ionospheric absorption prevents<br />

radio frequencies greater than about 2 or 3 MHz<br />

propagating via the ionosphere unless very large<br />

powers are transmitted. During nighttime, when<br />

the D-region ionization drops to very low levels,<br />

these same transmissions can propagate by the<br />

ionosphere to large distances. During a solar<br />

flare, X-ray radiation from the sun can increase<br />

significantly, resulting in greater ionization of<br />

the D region <strong>and</strong> subsequently larger absorption<br />

of radio waves. These increases may be sufficiently<br />

large to prevent all HF signals propagating<br />

by the ionosphere. See D region, short wave<br />

fadeout, solar flare.<br />

ionosphericindex Anindexusuallybasedon<br />

observations of the F region critical frequency<br />

(foF2), which gives a measure of the solar cycle<br />

effects on the ionosphere. There are a variety<br />

of ionospheric indices of which the best known<br />

are IF2 <strong>and</strong> T. Both these indices are calculated<br />

in similar ways. First, past data are used to estimate<br />

calibration curves then, using current data<br />

with the calibration curves, an index is calculated<br />

that best represents the solar cycle effects<br />

for this epoch. Ionospheric indices are effective<br />

because the F region is strongly dependent on<br />

changes in solar activity. The correlation between<br />

the monthly median hourly foF2 <strong>and</strong> the<br />

smoothed sunspot number, for a location, can be<br />

higher than 0.95. Ionospheric indices are often<br />

used with HF propagation models for predicting<br />

propagation conditions. See ionospheric radio<br />

propagation path.

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