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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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interconnection field<br />

interconnection field A magnetic field component,<br />

derived from a scalar potential (see harmonic<br />

model), added to an empirical model of<br />

the closed magnetosphere to turn it into a model<br />

of the open magnetosphere. It may be added<br />

either to obtain a better fit to data, or to create<br />

a testbed model of the open magnetosphere for<br />

testing various theoretical notions. Often a constant,<br />

southward-directed field is used to obtain<br />

this effect.<br />

interface-controlledcreep Inrheology, adeformation<br />

mechanism for diffusion creep. In an<br />

interface-controlled creep, macroscopic strain<br />

is caused by diffusion mass transport involving<br />

creation <strong>and</strong>/or deposition of vacancies at grainboundary<br />

<strong>and</strong> their diffusion, through some<br />

rearrangement of atomic structures at grainboundaries.<br />

Interface-controlled creep assumes<br />

that the interface reaction is fast compared to<br />

diffusion, so the overall rate of deformation is<br />

controlled by grain boundary reaction. One example<br />

is the case where the rate of generation or<br />

absorption of vacancies is controlled by the mobility<br />

of grain-boundary dislocations. The constitutive<br />

equation for interface-controlled creep<br />

can be expressed as<br />

ε=C σ2 D<br />

κTµbd<br />

where D is the diffusion coefficient, b the thickness<br />

of grain boundary, σ the differential stress,<br />

d the grain size, the atomic volume, κ Boltzmann’s<br />

constant, C a numerical coefficient depending<br />

on the grain shape <strong>and</strong> the boundary<br />

conditions for σ, T the temperature, µ the shear<br />

modulus, <strong>and</strong> ε the strain.<br />

interference fading Results from interference<br />

between signals arriving at a receiver by<br />

two or more different paths. The multiple paths<br />

may arise from sky wave <strong>and</strong> ground wave paths,<br />

two polarization modes, <strong>and</strong> various combinations<br />

of multi-mode sky-wave paths, scattering<br />

from ionization irregularities or combinations<br />

of any of these options. Interference fading is a<br />

collective term for the observed fading statistics<br />

whereas multipath fading specifically describes<br />

the path structure of the received radio signal.<br />

In a more restricted sense, interference fading<br />

© 2001 by CRC Press LLC<br />

246<br />

(sometimes called diffraction fading) may describe<br />

multiple paths formed within the region<br />

of the ionosphere where the radio wave for a single<br />

mode is reflected <strong>and</strong> the resulting fading is<br />

attributed to local ionization irregularities. Interference<br />

fading occurs with an associated period<br />

of 1 sec or larger. See fading.<br />

interglacial For the last 4 million years covering<br />

the Holocene (recent) <strong>and</strong> the Pleistocene<br />

epochs, the Earth has been primarily in ice ages.<br />

An interglacial is a period of relative warming.<br />

The last interglacial occurred about 120,000<br />

years ago; the current interglacial began about<br />

20,000 years ago. The record indicates that interglacials<br />

have a length of about 20,000 years.<br />

interior Schwarzschild space-time In general<br />

relativity, the spacetime described by the<br />

metric<br />

ds 2 =<br />

⎛ <br />

−⎝3<br />

1 − r2 <br />

1<br />

− 1 −<br />

R2 r2<br />

R2 ⎞2<br />

⎠ dt 2<br />

+ dr2<br />

1 − r2<br />

R2 <br />

2<br />

+ r dθ 2 + sin 2 θdφ 2<br />

describing the gravitational field interior to a<br />

static, incompressibleperfect fluid sphere of ra-<br />

3<br />

dius r1, density µ =<br />

8πR2 <br />

, <strong>and</strong> pressure<br />

<br />

1 −<br />

p = µ<br />

r2<br />

R2 <br />

− 1 − r2 1<br />

R2 <br />

3 1 − r2 1<br />

R2 <br />

− 1 − r2<br />

R2 .<br />

The total mass of the sphere is m = 4π 3 µr3 1 .<br />

The pressure is regular at the center provided<br />

r 2 1 < (8/9)R2 . This condition sets an upper<br />

limit on the mass of the sphere.<br />

intermediate shock Results from the steepening<br />

of an intermediate MHD wave that is a<br />

purely traverse wave with velocity perturbations<br />

perpendicular to both the wave vector ko <strong>and</strong><br />

the average magnetic field Bo. Intermediate<br />

shocks can exist only in anisotropic media. In an<br />

isotropic plasma, such as the solar wind, a steepened<br />

intermediate wave does not form a shock

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