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DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

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temperature is ∼ 10 K everything except H2,<br />

He, <strong>and</strong> Ne freezes out <strong>and</strong> ice mantles form<br />

on grains. In regions where H < H2 the less<br />

abundant heavier atoms such as O, C, <strong>and</strong> N can<br />

react with one another to form oxidized species<br />

such as CO, CO2, <strong>and</strong> presumably O2 <strong>and</strong> N2.<br />

Where H > H2 the heavy atoms are reduced <strong>and</strong><br />

the ice mantles are dominated by molecules such<br />

as H2O, CH4, <strong>and</strong> NH3. When these ices are exposed<br />

to cosmic rays <strong>and</strong> UV photons, bonds are<br />

broken <strong>and</strong> the resulting unstable species react<br />

to form more complex materials, in some cases<br />

organic molecules of the type seen in meteorites<br />

<strong>and</strong> interplanetary dust particles.<br />

grain chemistry: diffuse interstellar In the<br />

diffuse interstellar medium (i.e., visual extinction<br />

Av ≤ 2 magnitudes, or nH ≤∼ 10 1 cm −3 ),<br />

where ice is not stable, the dust is essentially<br />

bare <strong>and</strong> grain surfaces are available as catalysts<br />

<strong>and</strong> reactants. Since hydrogen is the most abundant<br />

atom, H2 formation from hydrogen atoms<br />

is by far the most common surface reaction.<br />

grains: in other galaxies Extragalactic extinction<br />

curves are comparable to those within<br />

the Milky Way galaxy, consistent with grains in<br />

other galaxies being of similar size <strong>and</strong> composition<br />

to those in our own. Most spiral galaxies<br />

seem to have similar dust-to-gas ratios as in our<br />

own, although there are some exceptions.<br />

grains, interstellar: destruction <strong>and</strong> formation<br />

Grains presumably form in the outflows<br />

from cool evolved (red giant) stars, novae <strong>and</strong><br />

supernovae ejecta <strong>and</strong> grow as they mix with interstellar<br />

molecules, accreting ice mantles <strong>and</strong><br />

sticking to one another. Such interstellar grains<br />

may be fragmented or destroyed by shocks, collisions,<br />

sputtering, or incorporation into forming<br />

stars. A typical grain lifetime is thought to be<br />

approximately 10 8 years.<br />

grains, interstellar: size <strong>and</strong> composition<br />

A wide-spread interstellar grain size is inferred<br />

from optical, IR, <strong>and</strong> UV extinction curves<br />

throughout our galaxy. The grains are usually<br />

deduced to have sizes in the range of 0.01<br />

to 0.2 µm, are probably of irregular (perhaps<br />

fractal) shape, <strong>and</strong> composed of (presumably<br />

amorphous) silicates, carbon, SiC, or metal ox-<br />

© 2001 by CRC Press LLC<br />

gr<strong>and</strong> unification<br />

ides. The position <strong>and</strong> profile of the 2175<br />

Å bump is consistent with some of the carbon<br />

grains being graphitic, or composed from<br />

amorphous or diamond-like carbon containing<br />

graphitic (π-bonded) domains. In the diffuse<br />

instersellar medium where radiation is abundant,<br />

these grains are probably bare, but in dense<br />

molecular clouds, where the radiation is attenuated<br />

<strong>and</strong> the average temperature low, ice mantles<br />

condense on the surfaces of these grains.<br />

grain size A measure of particle size in a<br />

sediment. Often refers to the median grain size<br />

in a sample. Typically determined by sieving.<br />

grain size analysis A process of determining<br />

sediment grain size. Most commonly done<br />

using a stack of sieves of varying size.<br />

gr<strong>and</strong> potential The thermodynamic potential<br />

equal to<br />

= U − TS− µN ,<br />

with U the internal energy, S the entropy, µ the<br />

chemical potential, <strong>and</strong> N the number of particles<br />

in the system.<br />

gr<strong>and</strong> unification Modern particle physics<br />

describes interactions through the exchange of<br />

so-called gauge particles, whose existence is due<br />

to an underlying symmetry. For instance, the<br />

gauge particle we know as the photon exists because<br />

of the invariance of the physics under local<br />

phase variation, which is a U(1) symmetry.<br />

When the universe had a temperature corresponding<br />

to a typical photon energy of roughly<br />

250 GeV, the symmetry of particle physics interactions<br />

is believed to have been that of the group<br />

product SU(3) × SU(2) × U(1) describing the<br />

strong <strong>and</strong> electroweak interactions.<br />

Whenever a symmetry is exact, as is the case<br />

for electromagnetism, the corresponding gauge<br />

particle is massless (as is the photon), while if it<br />

is broken, the gauge particle is massive <strong>and</strong> the<br />

interaction is much weaker (short range). This is<br />

in particular the case for the weak interaction. It<br />

is currently expected that the product symmetry<br />

we have at the electroweak level is just part of<br />

a larger (simple <strong>and</strong> compact) symmetry group<br />

that unifies forces <strong>and</strong> interaction — hence the<br />

name gr<strong>and</strong> unification. This larger group could<br />

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