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DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

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magnetopause<br />

forealkalivaporinstrumentsareoftenused, generally<br />

in conjunction with fluxgates. These are<br />

absolute instruments, observing the intensity of<br />

the magnetic field by the frequency at which a<br />

swept-frequency radio signal causes enhanced<br />

absorption of a light beam in a glass cell filled<br />

with alkali vapor. Rubidium or strontium vapor<br />

is generally used, <strong>and</strong> the beam is emitted from<br />

the same element, in a narrow frequency range.<br />

The mechanism is based on optical pumping of<br />

energy sub-states of these atoms.<br />

Other instruments (used mainly on the<br />

ground) include the proton precession magnetometer,<br />

on which the widespread technique<br />

of nuclear magnetic resonance in medicine is<br />

based. The Overhauser effect magnetometer is<br />

related to this but it is more precise, <strong>and</strong> it can<br />

be used as an alternative to the alkali vapor instrument<br />

in geomagnetic survey satellites.<br />

magnetopause The boundary of the magnetosphere,<br />

separating plasma attached to the<br />

Earth from that flowing with the solar wind.<br />

The magnetopause is defined by the surface on<br />

which the pressure of the solar wind is balanced<br />

by that of the Earth’s magnetic field. The “nose”<br />

of the magnetopause, on the sunward side of<br />

the Earth is ∼ 15 Earth radii away, on average.<br />

As the pressure of the solar wind changes, the<br />

magnetopause shrinks or exp<strong>and</strong>s accordingly.<br />

The idea of a magnetopause has been around<br />

since about 1930 when Chapman <strong>and</strong> Ferraro<br />

proposed a theory that explained geomagnetic<br />

storms as interactions of the Earth’s magnetosphere<br />

with plasma clouds ejected from the sun.<br />

The magnetopause was first discovered in 1961<br />

by NASA’s Explorer 12 spacecraft.<br />

magnetosonic wave See magnetoacoustic<br />

wave.<br />

magnetosphere The planetary region of<br />

space where a body’s magnetic field can be detected.<br />

As the solar wind plasma embedded<br />

with interplanetary magnetic field (IMF) flows<br />

around the planet, it interacts with the Earth’s<br />

magnetic field <strong>and</strong> confines it to a cavity called<br />

the magnetosphere. Since the solar wind is supersonic,<br />

a shock known as Bow shock is formed<br />

on the sunward side of the magnetosphere. The<br />

solar wind then flows across the bow shock <strong>and</strong><br />

© 2001 by CRC Press LLC<br />

300<br />

its speed is reduced from supersonic to subsonic.<br />

The solar wind ahead is deflected at a boundary<br />

between the magnetosphere <strong>and</strong> the solar wind<br />

known as the magnetopause. The subsolar point<br />

on the magnetopause is about 10 Earth radii from<br />

the center of the Earth. The bow shock is about<br />

3 Earth radii from the sunward side of the magnetopause<br />

at the subsolar point. The region between<br />

the bow shock <strong>and</strong> the magnetopause is<br />

called the magnetosheath.<br />

At the magnetopause, the solar wind pressure<br />

outside is balanced by the magnetic field<br />

pressure inside the magnetosphere. As the solar<br />

wind sweeps past the Earth, the magnetic field<br />

lines from the polar cap are pulled toward the<br />

nightside to form a geomagnetic tail. This tail<br />

can be observed as far as 1000 Earth radii, as<br />

the combined pressure of the field <strong>and</strong> plasma<br />

prevent its closing on the night side. Moreover,<br />

the polar cap magnetic field lines do not<br />

close resulting in a thin sheet in the equatorial<br />

plane known as the neutral sheet across which an<br />

abrupt field reversal occurs. The region where<br />

magnetic field lines from sub-auroral latitudes<br />

tend to close is known as plasma sheet of thickness<br />

about 1 Earth radii. The plasma sheet consists<br />

of energetic particles in the energy range of<br />

about 1 to 10 kev <strong>and</strong> is the source of radiation<br />

belt particles.<br />

magnetospheric substorms Apart from<br />

quiet variations in the Earth’s magnetic field like<br />

solar quiet (S q) <strong>and</strong> lunar variations resulting<br />

from the generation of ionospheric currents by<br />

solar <strong>and</strong> lunar tides, other observed variations<br />

are far from constant <strong>and</strong> without any periodicity.<br />

Such variations result from the interaction<br />

of solar wind with the geomagnetic field<br />

of the Earth <strong>and</strong> are denoted by D. These are<br />

called magnetospheric storms <strong>and</strong> have characteristic<br />

times of minutes to days. The magnetospheric<br />

storm consists of frequently occurring<br />

small storms called magnetospheric substorms.<br />

The intensity of the storm is given in terms of<br />

the AE (auroral electrojet) index <strong>and</strong> of the substorm<br />

by the Dst index. Each substorm is associated<br />

with injection of energetic protons of<br />

few tens of kev in the Van Allen belts. When<br />

frequent injection occurs, a proton belt known<br />

as ring current is formed whose strength is given<br />

in terms of Dst. At first there is a sudden com-

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