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DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

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aurora australis<br />

Earth’s magnetic field. They enter the Earth’s<br />

upper atmosphere where the field lines intersect<br />

the atmosphere, i.e., in the polar regions. There<br />

they excite atoms in the high thin atmosphere at<br />

altitudes of 95 to 300 km. The red <strong>and</strong> green<br />

colors are predominantly produced by excitations<br />

of oxygen <strong>and</strong> nitrogen. The polar lights<br />

are typically seen within 5000 km of the poles,<br />

but during times of intense solar activity (which<br />

increases the electron population), they can become<br />

visible at midlatitudes as well. Any body<br />

thatpossessesbothamagneticfield<strong>and</strong>anatmosphere<br />

can produce aurorae. Aurorae are commonly<br />

seen not only on Earth but also the Jovian<br />

planets of Jupiter <strong>and</strong> Saturn.<br />

aurora australis Southern light, aurora in<br />

the southern hemisphere. See aurora.<br />

aurora borealis Northern light, aurora in the<br />

northern hemisphere. See aurora.<br />

auroral cavity A region on magnetic field<br />

lines which guides the aurora, typically within<br />

10,000 km or so of Earth, where abnormally low<br />

ion densities are observed at times of strong aurora,<br />

presumably caused by it.<br />

auroral electrojet A powerful electric current,<br />

flowing in the auroral oval in the ionospheric<br />

E-layer, along two branches that meet<br />

near midnight. The branches are known as the<br />

eastward <strong>and</strong> westward auroral electrojets, respectively,<br />

<strong>and</strong> the region in which they meet,<br />

around 2200 magnetic local time, is the Harang<br />

discontinuity.<br />

The electrojets are believed to be Hall currents<br />

in the ionospheric E-layer <strong>and</strong> to be a<br />

secondary effect of the currents linking Birkel<strong>and</strong><br />

currents of region 1 with those of region 2.<br />

Because of Fukushima’s theorem, the magnetic<br />

disturbance due to the Birkel<strong>and</strong> current sheets<br />

on the ground is very weak, <strong>and</strong> the main signature<br />

of their circuit — which can be quite strong<br />

— comes from the electrojets. The usual way<br />

of estimating the current flowing in that circuit<br />

— which is a major signature of substorms —<br />

is therefore by means of the AE, AL, <strong>and</strong> AU<br />

indices which gauge the strength of the electrojets.<br />

© 2001 by CRC Press LLC<br />

auroral oval Circular region several degrees<br />

wide around the geomagnetic pole at a geomagnetic<br />

latitude of about ±70 ◦ , its center shifted by<br />

about 200 km towards the nightside; the region<br />

in which aurora is observed at any instant, covering<br />

the region of the diffuse aurora, which is also<br />

where the discrete aurora can be seen. The auroral<br />

oval can be seen in satellite images in UV<br />

as a closed circle. From Earth, in visible light,<br />

in the auroral oval aurora can be seen nearly<br />

each night, during polar night for a full 24 hours.<br />

Shapes <strong>and</strong> structure of the aurora vary with local<br />

time: with a rather diffuse auroral brightening<br />

between local noon <strong>and</strong> midnight, quiet arcs<br />

during the evening hours up to around 21 local<br />

time, followed by homogeneous or rayed<br />

b<strong>and</strong>s or draperies, which after about 3 local<br />

time, are complemented by patches at the southern<br />

rim of the auroral oval. These patches, together<br />

with short arcs, dominate the appearance<br />

of the aurora during the morning hours. The<br />

size of the auroral oval varies greatly; it grows<br />

during magnetic storms <strong>and</strong> may sometimes extend<br />

well beyond the region where aurora is ordinarily<br />

seen (auroral zone). At magnetically<br />

quiet times the oval shrinks <strong>and</strong> may assume a<br />

non-circular “horsecollar” shape, narrower near<br />

noon. Physically, the auroral oval is related to<br />

upward flowing Birkel<strong>and</strong> currents coupling the<br />

ionosphere <strong>and</strong> magnetosphere. See Birkel<strong>and</strong><br />

current.<br />

auroral zone The region where auroras are<br />

ordinarily seen, centered at the magnetic pole<br />

<strong>and</strong> extending between magnetic latitudes 66 ◦<br />

<strong>and</strong> 71 ◦ . The auroral zone is generally derived<br />

from ground observations of discrete aurora, but<br />

it also approximates the statistical average of the<br />

auroral oval, averaged over many nights.<br />

autumnal equinox The epoch at the end of<br />

Northern hemisphere summer on which the sun<br />

islocatedattheintersectionofthecelestialequator<br />

<strong>and</strong> the ecliptic; on this day, about September<br />

21, the night <strong>and</strong> day are of equal length<br />

throughout the Earth. The date of autumnal<br />

equinox is the beginning of the Southern hemispherespring.<br />

Autumnalequinoxalsoreferstoa<br />

direction of the celestial sphere: 12 h RA, 0 ◦ declination,<br />

antipodal to the direction of the vernal<br />

equinox. See vernal equinox. After autumnal

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