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DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

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which are successively poorer in volatile content.<br />

C1 chondrites do not contain chondrules<br />

but are chemically very similar to other chondrites.<br />

chondrite, ordinary The most common<br />

form of meteorite. Composed mostly of olivine<br />

with significant amounts of other metallic silicates.<br />

Ordinary chondrites are further classified<br />

according to their iron content into H (high iron),<br />

L (low iron), <strong>and</strong> LL (very low iron) chondrites.<br />

An additional subdivision, E (enstatite), is characterized<br />

by lower Mg/Si ratios, which give rise<br />

to a composition richer in enstatite <strong>and</strong> containing<br />

little olivine.<br />

chondrule Small spheroidal (∼ 1 mm)<br />

glassy bead of silicates (olivine or enstatite)<br />

found within stony meteorites, called chondrites.<br />

Chondrules generally have a composition<br />

very similar to the matrix material of the<br />

chondrite in which they are embedded, but this<br />

material has undergone an episode of melting<br />

<strong>and</strong> rapid quenching early in the history of solar<br />

system formation. The actual process causing<br />

the melting is poorly understood.<br />

Christoffel symbol See affine connection,<br />

metricity of covariant derivative.<br />

chromatic aberration A situation arising in<br />

lens-based (refracting) optical instruments, in<br />

which light of different colors cannot be brought<br />

into focus at the same point, arising because<br />

glass or other lens material is dispersive <strong>and</strong> so<br />

produces different deviation of the path of light<br />

of different colors.<br />

chromosphere The layer in the sun or a cool<br />

star between the photosphere <strong>and</strong> corona. The<br />

layer is relatively thin <strong>and</strong> at a temperature of<br />

about 10,000 K in the sun. During a total solar<br />

eclipse, it is seen as a red ring (hence the name)<br />

around the moon’s shadow. Outside eclipse, it<br />

contributes emission lines to the spectrum of the<br />

sun (or star). The intensity of the chromosphere<br />

varies through the solar cycle.<br />

chromospheric evaporation The upward<br />

flow of hot plasma in a solar flare resulting<br />

from the fast deposition of energy in the chro-<br />

© 2001 by CRC Press LLC<br />

cigar distribution<br />

mosphere. In the chromospheric evaporation<br />

process, the energy released during a solar flare<br />

rapidly dissipates in the chromosphere (typically<br />

assumed to involve non-thermal electron<br />

beams or a thermal conduction front). The chromosphere<br />

is suddenly heated to coronal temperatures<br />

<strong>and</strong> subsequently exp<strong>and</strong>s upward. Evidence<br />

for these flows generally comes from<br />

blueshifts measured in spectral lines, such as<br />

those observed by a Bragg Crystal Spectrometer.<br />

chromospheric heating The process behind<br />

the enhanced temperature of the sun’s chromosphere<br />

above that of the sun’s surface (photosphere).<br />

Radiation is the bulk energy loss mechanism<br />

in the chromosphere, conductive losses<br />

being negligible, <strong>and</strong> both the photosphere <strong>and</strong><br />

corona contribute to its heating. The amount of<br />

heating required to balance radiative losses in<br />

the chromosphere is about 4 × 10 3 Wm −2 for<br />

quiet sun <strong>and</strong> coronal hole regions. This rises<br />

to ∼ 2 × 10 4 Wm −2 for the chromosphere in<br />

active regions. The exact nature of the heating<br />

mechanism is uncertain.<br />

chronological future/past The chronological<br />

future/past I ± (S) of a set S is defined as<br />

the union of all points that can be reached from<br />

S by a future/past-directed time-like curve. (A<br />

time-like curve must be of non-zero extent, thus<br />

isolated points are excluded.)<br />

CHUMP (Charged Hypothetical Ultra<br />

Massive Particle) In the framework of gr<strong>and</strong><br />

unification models, hypothetical CHUMPs are<br />

among the c<strong>and</strong>idates to explain the missing<br />

mass problem in the universe (the fact that the<br />

observed luminous matter cannot account for the<br />

dynamical properties observed on large scales).<br />

As they carry an electric charge, they need to<br />

be very massive, otherwise they would already<br />

have been detected. An example of such a particle<br />

is the vorton, which would appear in theories<br />

having current-carrying cosmic strings. See<br />

dark matter, vorton.<br />

cigar distribution In plasma physics, a pitch<br />

angle distribution in which the highest intensities<br />

are field aligned, so that a contour of the flux

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