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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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ight point A transient H-alpha brightening<br />

of flare intensity, less than 20 millionths of the<br />

solar hemisphere in area. Such a brightening<br />

when covering a larger area becomes classified<br />

as a solar flare.<br />

brittle behavior (brittle fracture) A phenomenologicaltermdescribingthenatureofmaterial<br />

failure. According to the simplest or “classical”<br />

view, brittle behavior (brittle fracture) of<br />

a solid material is a discrete event in which the<br />

failure of the solid occurs, without significant<br />

prior deformation <strong>and</strong> without warning, at a particular<br />

stress. In general, material is described<br />

as “brittle” when fracture occurs with no preceding<br />

appreciable permanent deformation. Sometimes<br />

brittle behavior refers to failure following<br />

limited amounts of inelastic strain that are small<br />

compared with the elastic strain.<br />

brittle-ductile transition A temperature<br />

range over which the principal failure mechanism<br />

of a rock body (such as the continental<br />

crust) under deviatoric stress changes from brittle<br />

to ductile. Brittle failure takes place at low<br />

temperatures by developing fractures or slipping<br />

along pre-existing fractures. Ductile failure<br />

takes place at higher temperatures <strong>and</strong>, observed<br />

at the macroscopic scale, by continuous<br />

deformation. The transition occurs due to the<br />

activation of diffusion or dislocation creep at elevated<br />

temperatures <strong>and</strong> is affected by the rate of<br />

ductile deformation <strong>and</strong> the pore fluid pressure<br />

in the brittle region. In the Earth’s continental<br />

crust, this transition is marked by the absence<br />

of earthquakes below a certain depth where the<br />

temperature is higher than about 300 to 400 ◦ C.<br />

In the oceanic crust <strong>and</strong> mantle, the transition<br />

occurs at higher temperatures.<br />

brittle-plastic transition See brittle-ductile<br />

transition.<br />

broad line radio galaxies Radio galaxies<br />

showing optical spectra very similar to, <strong>and</strong><br />

in several cases almost indistinguishable from,<br />

those of Seyfert-1 galaxies. Broad line radio<br />

galaxies are type 1, low-luminosity, radio-loud<br />

active galactic nuclei; the radio-loud counterpart<br />

of Seyfert-1 galaxies. Differences between<br />

Seyfert-1 <strong>and</strong> Broad Line Radio galaxies en-<br />

© 2001 by CRC Press LLC<br />

brown dwarf<br />

compass the morphology of the host galaxy<br />

(Seyfert-1 are mostly, albeit not exclusively, spirals,<br />

while broad line radio galaxies are hosted<br />

by ellipticals) <strong>and</strong> some features of the optical<br />

spectrum, like weaker singly ionized iron emission<br />

<strong>and</strong> larger internal absorption due to dust in<br />

broad line radio galaxies. See Seyfert galaxies.<br />

broad line region The region where the<br />

broad lines of active galactic nuclei are produced.<br />

The strongest lines observed in the optical<br />

<strong>and</strong> UV spectrum are the Balmer lines of<br />

hydrogen, the hydrogen Lyman α line, the line<br />

from the three times ionized carbon at 154.9 nm,<br />

<strong>and</strong> some recombination lines from singly ionized<br />

<strong>and</strong> neutral helium. Since no forbidden<br />

lines are observed, the broad line region is most<br />

likely a relatively high density region with particle<br />

density in the range 10 9 to 10 13 ions per cubic<br />

centimeter. The broad line region is believed to<br />

be very close to the central source of radiating<br />

energy of the active galactic nucleus. Observations<br />

of variation of broad line profiles <strong>and</strong> fluxes<br />

suggest that the broad line regions line emitting<br />

gas is confined within 1 pc in Seyfert-1 galaxies.<br />

Models of the broad line regions invoke a large<br />

number of dense emitting clouds, rapidly rotating<br />

around a central illuminating source. Alternatively,<br />

it has been suggested that at least part<br />

of the emission of the broad line regions could<br />

come from the middle <strong>and</strong> outer region of the<br />

accretion disk suspected to be a universal constituent<br />

of the central engine of active galactic<br />

nuclei.<br />

brown dwarf A sphere of gas with the composition<br />

of a star (that is, roughly 3 4 hydrogen,<br />

1<br />

4 helium, <strong>and</strong> at most a few percent of heavier<br />

elements) but with a mass low enough that the<br />

center never, as the object contracts out of interstellar<br />

gas, gets hot enough for hydrogen burning<br />

to balance the energy being lost from the surface<br />

of the sphere. Very young brown dwarfs can be<br />

as bright as low-mass stars (10−4 to 10−5 of the<br />

solar luminosity), but they fade with time until<br />

they are too cool <strong>and</strong> faint to see. The number<br />

of brown dwarfs in our galaxy is not very well<br />

known. They are probably not common enough<br />

(at least in the galactic disk) to contribute much<br />

to the dark matter, but small numbers have been<br />

observed (a) in young clusters of stars, (b) as

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