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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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comet, artificial<br />

in 2003, rendezvous with Comet Wirtanen in<br />

2112-13, <strong>and</strong> RoL<strong>and</strong> (the l<strong>and</strong>er) will make further<br />

measurements on the surface of the comet.<br />

comet, artificial See barium release.<br />

comminution The breaking up <strong>and</strong> fragmentation<br />

of a rock or other solid. The Earth’s crust<br />

is comminuted on a wide range of scales by tectonic<br />

process. In California the crust has been<br />

fragmented into blocks on scales of microns to<br />

tens or hundreds of kilometers. Fault gouge is an<br />

example of comminution on the smallest scale.<br />

common envelope A binary star system enters<br />

a common envelope phase when one, or<br />

both, of the stars in the binary overfills its Rochelobe<br />

<strong>and</strong> the cores orbit within one combined<br />

stellar envelope. Common envelope phases occur<br />

in close binaries where the Roche-lobe overflowing<br />

star exp<strong>and</strong>s too rapidly for the accreting<br />

star to incorporate the accreting material.<br />

Most common envelope phases occur when a<br />

star moves off the main sequence <strong>and</strong> exp<strong>and</strong>s<br />

toward its giant phase (either in Case B or Case<br />

C mass transfer phases). The st<strong>and</strong>ard formation<br />

scenarios of many short-period binary systems<br />

(e.g., low-mass X-ray binaries, double neutron<br />

stars) require a common envelope phase<br />

which tightens the orbital separation <strong>and</strong> ejects<br />

the common envelope.<br />

common envelope binary Binary stars that<br />

are so close to one another that both fill their respective<br />

Roche surfaces, resulting in a common<br />

envelope that surrounds both stars.<br />

comoving frame In general relativity coordinates<br />

are just labels for space-time points <strong>and</strong><br />

have no a priori physical meaning. It is, however,<br />

possible to associate those labels to part<br />

of the matter present in the universe, in which<br />

case one has a material realization of a reference<br />

frame. Since such coordinates follow the<br />

matter in its motion, the corresponding frame is<br />

said to be comoving. A fundamental requisite<br />

is that the trajectories of the objects considered<br />

do not cross at any point; otherwise the map<br />

of coordinates would become singular in such<br />

points. A useful, but not necessary, property<br />

is that those objects interact only gravitation-<br />

© 2001 by CRC Press LLC<br />

ally, so as to track geodesics in the background<br />

spacetime.<br />

compact group of galaxies Isolated group<br />

of galaxies for which the separation between the<br />

galaxies is comparable to the size of the galaxies<br />

themselves; groups of galaxies isolated by<br />

Hickson from the Palomar Observatory Sky Survey<br />

according to three criteria: (1) there are at<br />

least four members whose magnitudes differ by<br />

less than three magnitudes from the magnitude<br />

of the brightest member; (2) if RG is the radius<br />

of the circle on the sky containing all group<br />

members, then the distance to the nearest galaxy<br />

outside the group must be larger than 3 RG (in<br />

other words, the group must be reasonably isolated<br />

<strong>and</strong> not an obvious part of a larger structure);<br />

(3) the mean surface brightness within RG<br />

should be brighter than 26 mag per square second<br />

of arc, i.e., the group must not contain vast<br />

empty sky areas <strong>and</strong> hence should be “compact”.<br />

compaction As rocks are buried to a greater<br />

depth in a sedimentary basin, the “lithostatic”<br />

pressure increases. This causes the rock to compact.<br />

The void space, or “porosity” of the rock,<br />

decreases with increasing depth, <strong>and</strong> the density<br />

increases.<br />

compact steep spectrum radio sources<br />

A class of radio sources which includes radio<br />

galaxies <strong>and</strong> quasars unresolved at resolution<br />

≈ 2 arcsecs. They are differentiated from<br />

other core-dominated radio sources by showing<br />

a steep radio spectrum. Observations at higher<br />

resolution show that compact steep spectrum radio<br />

sources are either classical lobe dominated<br />

sources whose lobe size is less than the size of<br />

the galaxy or quasars with a core single-side jet<br />

morphology. In both cases, the radio morphology<br />

appears often to be disrupted <strong>and</strong> irregular.<br />

Compact steep spectrum radio sources are<br />

thought to be young radiogalaxies which are exp<strong>and</strong>ing<br />

or, alternatively, radio sources in which<br />

the expansion of the radio plasma is hampered<br />

by interstellar or intergalactic medium.<br />

compensation In geophysics, the positive<br />

mass of major mountain belts is compensated by<br />

the negative mass of crustal mountain roots. The<br />

crustal rocks are lighter than the mantle rocks be-

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