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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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ning signal was heard as a sharp, short duration<br />

crackle on a radio receiver. This bursty crackle<br />

of interference was called an atmospheric, to<br />

distinguish it from the internal <strong>and</strong> local site interference.<br />

The sum of many atmospherics from<br />

remote lightning strokes all over the world produces<br />

a steady background noise limit at these<br />

radio frequencies called atmospheric noise. Atmospherics<br />

were observed at lower frequencies<br />

<strong>and</strong> used as a measure of thunderstorm activity.<br />

Early receivers for this application were sometimes<br />

caller spheric receivers.<br />

atmospheric tide Oscillations in any atmospheric<br />

field with periods that are simple integer<br />

fractions of either a lunar or a solar day. In<br />

addition to being somewhat excited by the gravitational<br />

potential of the sun <strong>and</strong> moon, atmospheric<br />

tides are strongly forced by daily variations<br />

in solar heating. The response of these<br />

forcings is by internal gravity waves. Unlike<br />

ocean tides, atmospheric tides are not bound<br />

by coastlines but are oscillations of a spherical<br />

shell.<br />

atomic mass The mass of an isotope of an<br />

element measured in atomic mass units. The<br />

atomic mass unit was defined in 1961, by the<br />

International Union of Pure <strong>and</strong> Applied Physics<br />

<strong>and</strong> the International Union of Pure <strong>and</strong> Applied<br />

Chemistry, as 1/12 of the mass of the carbon<br />

isotope counting 6 neutrons (<strong>and</strong> 6 protons) in<br />

its nucleus.<br />

atomic number The number of protons in<br />

the nucleus of a given element.<br />

atomic structure calculations — one-electron<br />

models The calculation of possible states of<br />

an electron in the presence of an atomic nucleus.<br />

The calculations consist in obtaining the electron<br />

distribution or wave function about the nucleus<br />

for each state. This is achieved by solving<br />

the Schrödinger equation for the electron<br />

wave function in a fixed Coulomb potential generated<br />

by the nucleus of the atom. The quantified<br />

nature of the possible solutions or states<br />

appear naturally when the conditions of continuity<br />

<strong>and</strong> integrability are applied to the wave<br />

functions. An important characteristic of the<br />

one-electron models is that they can be solved<br />

© 2001 by CRC Press LLC<br />

aurora<br />

exactly; the wave functions may be expressed<br />

in terms of spherical harmonics <strong>and</strong> associated<br />

Laguerre polynomials. Relativistic treatment is<br />

done through Dirac’s equation. Dirac’s equation<br />

leads to the fine structure as a relativistic correction<br />

to Schrödinger’s solution. Another important<br />

result of Dirac’s equations is that even for<br />

non-relativistic cases one finds that the electron<br />

has two possible states, generally interpreted as<br />

two possible states of intrinsic angular momentum<br />

or spin.<br />

atomic time Time as measured by one or<br />

more atomic clocks, usually a cesium-beam<br />

atomic clock or a hydrogen maser. Measured<br />

since January 1, 1958, it is the most uniform<br />

measure of time available <strong>and</strong> has, therefore, replaced<br />

Universal Time as the st<strong>and</strong>ard.<br />

attenuation coefficient In propogation of a<br />

signal, beam, or wave through a medium, with<br />

absorption of energy <strong>and</strong> scattering out of the<br />

path to the detector, the attenuation coefficient<br />

α is<br />

α = d −1 ln (S/S0) ,<br />

where this is the natural logarithm, <strong>and</strong> S <strong>and</strong> S0<br />

are the current intensity <strong>and</strong> the initial intensity.<br />

Since α is an inverse length, it is often expressed<br />

in terms of decibel per meter, or per kilometer.<br />

See beam attenuation coefficient, diffuse attenuation<br />

coefficient.<br />

attenuation efficiency factor The sum of the<br />

absorption plus scattering efficiency factors.<br />

aulacogen Mantle plumes create regions of<br />

elevated topography which typically have three<br />

rift valleys at about 120 ◦ apart; these are aulacogen.<br />

These are also known as triple junctions,<br />

<strong>and</strong> they participate in the formation of new<br />

ocean basins. An example is the southern end of<br />

the Red Sea. Typically two arms participate in<br />

the opening of an ocean, <strong>and</strong> the third is known<br />

as a failed arm. The St. Lawrence river valley is<br />

a failed arm associated with the opening of the<br />

Atlantic Ocean.<br />

aurora Polar lights. The aurora borealis<br />

(northern lights) <strong>and</strong> aurora australis (southern<br />

lights). Energetic electrons are trapped from the<br />

solar wind <strong>and</strong> spiral around the field lines of the

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