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DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

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the difference between the number of generators<br />

ofG <strong>and</strong>H, or said otherwise, to the number of<br />

generators of G that are not generators of H.<br />

Actually, the theorem is more general, also applying<br />

in the case the symmetry is broken, but<br />

not spontaneously.<br />

A particularly simple example is the Goldstone<br />

model. There we have a breaking scheme<br />

U(1) →{1} <strong>and</strong> the production of one Goldstone<br />

particle. See Goldstone model, spontaneous<br />

symmetry breaking.<br />

Gondwanal<strong>and</strong> Continent in existence prior<br />

to the opening of the South Atlantic Ocean, consisting<br />

of South America, Africa, <strong>and</strong> Australia.<br />

Goto–Nambu string Structureless vacuum<br />

vortex defects that can be macroscopically described<br />

by a simple cosmic string equation of<br />

state T =U = const., where U is the string<br />

energy per unit length <strong>and</strong> T is its tension.<br />

The motion is derived by finding ξ0 <strong>and</strong> ξ1 that minimize the action:<br />

<br />

√−γd2 S=−U ξ<br />

where, the string being a one-dimensional object,<br />

its history can be represented by a surface in<br />

spacetime x µ (ξ a ) with internal worldsheet coordinates<br />

ξ 0 =t, ξ 1 =ℓ. γ is the determinant<br />

of the induced metric on the two-dimensional<br />

worldsheet of the string evolving in time. The<br />

integr<strong>and</strong> essentially represents the element of<br />

surface area swept out by the string in spacetime.<br />

One can then say that the string evolves<br />

in such a way as to extremize the area of its<br />

spacetime worldsheet. See cosmic string, cusp<br />

(cosmic string), energy per unit length (cosmic<br />

string), fundamental tensors of a worldsheet,<br />

Higgs mechanism.<br />

GPS See global positioning system.<br />

graben Common features on most planetary<br />

surfaces<strong>and</strong>oftensynonymouswiththetermrift<br />

valley. They are long, narrow troughs bounded<br />

by two (sometimes more) parallel normal faults,<br />

giving rise to a downdropped valley surrounded<br />

by high plateaus. Graben are created when two<br />

blocks of rock are pulled apart by tensional tec-<br />

© 2001 by CRC Press LLC<br />

gradual commencement storm<br />

tonic forces. Divergent boundaries are usually<br />

characterized by graben.<br />

GRACE (Gravity Recovery <strong>and</strong> Climate<br />

Experiment) AnapprovedEarthSystemScience<br />

Pathfinder NASA space mission which will<br />

employ a satellite-to-satellite microwave tracking<br />

system between two spacecraft to measure<br />

the Earth’s gravity field <strong>and</strong> its time variability.<br />

The mission is scheduled to be launched in 2001<br />

<strong>and</strong> will operate over five years.<br />

gradient For a scalar function f of coordinates,<br />

the collection of partial derivatives with<br />

respect to the coordinates: {f,i} (the ,i indicating<br />

partial derivative with respect to coordinate<br />

i). Or, more formally, the 1−formconstructed<br />

by<br />

f,idx i .<br />

See 1-form, partial derivative.<br />

gradient drift See drift, gradient.<br />

gradient Richardson number Ri The nondimensional<br />

ratio Ri =N 2 /(∂u/∂z) 2 between<br />

the stabilityN 2 <strong>and</strong> the vertical shear∂u/∂z of a<br />

stably stratified water column, which is subject<br />

to vertical gradients of the horizontal currents<br />

u. A necessary condition for turbulence to occur<br />

(typically Kelvin–Helmholtz instabilities) is<br />

the conditionRi < 0.25. In natural systems (atmosphere,<br />

oceans, lakes, etc.) the experimental<br />

determination of Ri depends on the scale over<br />

whichN 2 <strong>and</strong>(∂u/∂z) are determined. The rate<br />

of mixing, generally increasing asRi decreases,<br />

is not a unique function of Ri.<br />

gradual commencement storm Geomagnetic<br />

storms may commence gradually, the<br />

storm having no well-defined onset time. These<br />

storms may persist for many days, geomagnetic<br />

activity increasing irregularly, sometimes to major<br />

storm levels. Geomagnetic activity associated<br />

with gradual commencement storms may<br />

recur every 27 days, consistent with the solar<br />

rotation. They are thought to be due to highspeed<br />

solar wind streams arising in long-lived<br />

coronal hole regions on the sun. See geomagnetic<br />

storm.<br />

205

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