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DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

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continental plate<br />

types of continental margins, active <strong>and</strong> passive.<br />

An active margin is also a plate boundary, usually<br />

a subduction zone. An example is the west<br />

coast of South America. A passive margin is not<br />

an active plate boundary. An example is the east<br />

coast of the United States.<br />

continental plate In geophysics, the large<br />

pieces of material comprising the outer surface<br />

of the lithosphere. Plates are about 50 km<br />

in thickness <strong>and</strong> support the continents, which<br />

float on the denser viscous-fluid mantle below<br />

them. Current knowledge defines 15 major<br />

plates: Pacific, Philippine, Juan De Fuca, Cocos,<br />

Nazca, Antarctic, Scotia, South American,<br />

North American, Caribbean, Arabian, Indian,<br />

African, Eurasian, <strong>and</strong> Australian.<br />

continental shelf Shallow oceanic margins<br />

underlain by continental crust. The water depth<br />

is usually taken to be less than 1 km.<br />

continental shelf waves The waves that are<br />

generatedbytheslopingcontinentalshelftopography.<br />

In the Northern Hemisphere, the continental<br />

shelf wave propagates along a constant<br />

topography line with the coast on the right.<br />

continuum In mechanics, a description that<br />

ignores the granular or quantum nature of matter.<br />

In spectroscopy, the part of a spectrum without<br />

apparent lines, arising from solid, liquid, or<br />

gaseous sources, in which atomic lifetimes are<br />

too short to produce specific line emission or<br />

absorption.<br />

contravariant vector See vector.<br />

convection Large-scale flow of gases (or<br />

other fluids) in stars (or elsewhere) that carries<br />

heat energy from one place to another. In the<br />

stellar context, hot currents rise, cool ones fall,<br />

<strong>and</strong> the solar granulation is direct evidence for<br />

the occurrence of convection near the surface of<br />

the sun. Convection sets in whenever a stellar<br />

temperature gradient is steeper than the adiabatic<br />

one:<br />

− dT<br />

dr >−<br />

<br />

1 − 1<br />

<br />

T dp<br />

γ p dr<br />

© 2001 by CRC Press LLC<br />

where γ is the ratio of specific heats. This can<br />

happen either when gas is quite opaque to radiation<br />

(as it is near the surfaces of cool stars,<br />

including the sun, where hydrogen is in the process<br />

of being ionized) or when a nuclear reaction<br />

depends on a very high power of temperature, as<br />

does the CNO cycle at the cores of massive stars.<br />

Stars are fully convective during early phases<br />

of their formation (guaranteeing initial chemical<br />

homogeneity) <strong>and</strong> throughout their lives for<br />

stars of less than 0.3 solar masses. Convection<br />

is the primary way that material inside stars is<br />

mixed from one zone to another. In relatively<br />

dense regions of stars, convection will carry all<br />

the available energy, <strong>and</strong> the temperature gradient<br />

will be very nearly adiabatic. At lower densities,<br />

convection becomes inefficient, radiation<br />

carries much of the energy, <strong>and</strong> the temperature<br />

gradient can be much steeper.<br />

In the absence of any adequate theory of convection<br />

(or other turbulent processes in fluids),<br />

convection is often treated in the Mixing Length<br />

Approximation, in which gas is assumed to rise<br />

or fall through a fixed fraction of the pressure<br />

scale height (half is typical) <strong>and</strong> then come into<br />

temperature equilibrium with its surroundings,<br />

depositing its extra heat or soaking up its deficit.<br />

The approximation is more than 50 years old,<br />

<strong>and</strong> modern numerical computations of gas flow<br />

processes are just beginning to replace it in st<strong>and</strong>ard<br />

computations of stellar structure <strong>and</strong> evolution.<br />

The absence of an adequate theory of<br />

convective energy transport is one of the major<br />

remaining uncertainties in our underst<strong>and</strong>ing of<br />

stellar physics. See CNO cycle, solar granulation.<br />

convection zone A layer in a star in which<br />

convection currents provide the main energy<br />

transport mechanism. In the sun, a convection<br />

zone extends from just below the photosphere<br />

down to about 0.7 R⊙.<br />

convective adjustment One way to parameterize<br />

the physical process of convection in climate<br />

modeling. For example, in a simple version,<br />

one first examines the relative humidity<br />

<strong>and</strong> lapse rate in each grid column at the end of<br />

each time step of integration; if the lapse rate<br />

is superadiabatic, the temperature profile is adjusted<br />

to dry static neutrality in a manner that

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