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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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focal mechanisms<br />

rays arriving parallel from infinity appear to diverge<br />

(negative focal length).<br />

focal mechanisms Earthquakes send out<br />

compressional P-waves that are either compressional<br />

or tensional. The azimuthal variation in<br />

the first arrivals defines the focal mechanism.<br />

This variation provides information on whether<br />

the fault displacement was thrust, normal, or<br />

strike-slip <strong>and</strong> information on the orientation of<br />

the fault.<br />

focus In optics, the point where light rays<br />

converge <strong>and</strong>/or from which light rays (appear<br />

to) diverge.<br />

In geometry, in a circle, the center of the circle.<br />

In an ellipse, each of the two points on the<br />

major axis located at aɛ from the center, where<br />

a is the semimajor axis, <strong>and</strong>ɛ is the eccentricity.<br />

In a hyperbola, the point located inside the hyperbola,<br />

on the axis a distance ofa(ɛ− 1) from<br />

the point the orbit crosses the axis, such that the<br />

transverse distance to the orbit at that point is<br />

a(ɛ 2 − 1). Here a is called the semiaxis of the<br />

hyperbola, <strong>and</strong> ɛ is 1/(cosα) with α the slope<br />

of the asymptote to the hyperbola.<br />

In a parabola, the point inside the parabola<br />

on the axis of the parabola a distance p/2 from<br />

the point the orbit crosses the axis, such that the<br />

transverse distance to the orbit at that point is<br />

2p.<br />

In Newtonian physics, gravitational motion<br />

is an orbit that is a conic section (circle, ellipse,<br />

parabola, hyperbola) with the sun at one focus.<br />

focused transport equation Model suggested<br />

by Roelof (1969) to describe the interplanetary<br />

transport of charged energetic particles<br />

in terms of field-parallel propagation, focusing<br />

on the diverging interplanetary magnetic<br />

field, <strong>and</strong> pitch-angle scattering:<br />

∂f<br />

∂t<br />

1 −µ2<br />

+µv v<br />

2ζ<br />

∂f ∂<br />

−<br />

∂µ ∂µ<br />

=Q(so,µ,t).<br />

<br />

κ(µ) ∂f<br />

<br />

∂µ<br />

Here f is the phase space density, v the particle<br />

speed,µ the particle’s pitch-angle,κ(µ) the<br />

pitch-angle diffusion coefficient (see diffusion,<br />

in pitch-angle space, slab model), s the spatial<br />

coordinate along the Archimedian spiral, <strong>and</strong><br />

© 2001 by CRC Press LLC<br />

178<br />

ζ =−B(s)/(∂B/∂s) the focusing length (see<br />

focusing). The term Q on the right-h<strong>and</strong> side<br />

describes a particle source.<br />

focusing In plasma physics, reduction of a<br />

particle’s pitch angle as it propagates outward<br />

in a slowly diverging magnetic field such as the<br />

interplanetary magnetic field. Focusing can be<br />

characterized by a focusing length ζ<br />

ζ=− B(s)<br />

∂B/∂s<br />

withs being the spatial scale along the magnetic<br />

field B. In interplanetary space, the divergence<br />

of the magnetic field would reduce a particle’s<br />

pitch-angle from nearly 90 ◦ on the sun to about<br />

0.7 ◦ at the orbit of Earth.<br />

Focusing is a direct consequence of the constancy<br />

of the magnetic moment (first adiabatic<br />

invariant). Its reverse effect is the increase of<br />

the particle’s pitch angle in a convergent magnetic<br />

field, eventually leading to mirroring. See<br />

adiabatic invariant, interplanetary propagation,<br />

magnetic mirror.<br />

foehn Hot winds on the down-slope side of a<br />

mountain on which background winds impinge.<br />

There are two basic types of foehns of thermodynamic<br />

<strong>and</strong> dynamic causes, respectively.<br />

Thermodynamic foehns occur when the lower<br />

atmosphere is humid <strong>and</strong> the uplift by the mountain<br />

forces water vapor to condense on the upstream<br />

side, causing temperature increases on<br />

the down-slope side. Dynamic foehns occur<br />

when the atmosphere is strongly stratified on the<br />

up-slope side <strong>and</strong> the air near the surface cannot<br />

flow over the mountain <strong>and</strong> is blocked. As the<br />

upper air is forced to descend downslope, adiabatic<br />

compression raises its temperature. The<br />

second-type of foehn occurs when the Froude<br />

number U/Nh is below a certain critical value,<br />

where U is the background wind speed, N the<br />

Brunt–Väisälä frequency, <strong>and</strong> h the height of the<br />

mountain.<br />

fog A situation in which clouds form at<br />

ground level which reduces visibility below<br />

1 km; consisting of water droplets too small to<br />

fall out of suspension.

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