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DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

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creases to roughly 2 × 10 6 e/cm 3 during maximum<br />

sunspot activity. The density falls off to<br />

below 10 4 e/cm 3 at night. The F1 layer merges<br />

into the F2 layer at night. The F2 layer exists<br />

from about 250 to 400 km above the surface of<br />

the Earth. The F2 layer is the principal reflecting<br />

layer for HF communications during both<br />

day <strong>and</strong> night. The longest distance for one-hop<br />

F2 propagation is usually around 4000 km. The<br />

F2 layer has about 10 6 e/cm 3 <strong>and</strong> is thus usually<br />

the most densely ionized ionospheric layer.<br />

However, variations are usually large, irregular,<br />

<strong>and</strong> particularly pronounced during ionospheric<br />

storms. During some ionospheric storms, the<br />

F region ionization can reduce sufficiently so<br />

that the F2 region peak electron density is less<br />

than the F1 region peak density. See ionosphere,<br />

ionogram, ionosphericstorm, spreadF,traveling<br />

ionospheric disturbance, winter anomaly.<br />

frequency of optimum traffic (FOT) See<br />

Optimum Working Frequency (OWF).<br />

Fresnel reflectance The fraction of radiant<br />

energy in a narrow beam that is reflected from a<br />

surface at which there is an index of refraction<br />

mismatch.<br />

Fresnel zone Any one of the array of concentric<br />

surfaces in space between transmitter<br />

<strong>and</strong> receiver over which the increase in distance<br />

over the straight line path is equal to some integer<br />

multiple of one-half wavelength. A simplification<br />

allowing approximate calculation of<br />

diffraction.<br />

fretted channels One channel type considered<br />

to indicate fluvial activity on Mars. Fretted<br />

channels are a channel type affecting much of<br />

the fretted terrain, thus straddling the highl<strong>and</strong>–<br />

lowl<strong>and</strong> boundary of Mars. Their formation<br />

is restricted to two latitude belts centered on<br />

40 ◦ N <strong>and</strong> 45 ◦ S <strong>and</strong> spanning ≈ 25 ◦ wide. They<br />

are most extensive between longitude 280 ◦ W<br />

to 350 ◦ W. They extend from far in the upl<strong>and</strong>s<br />

down to the lowl<strong>and</strong> plains <strong>and</strong> represent broad,<br />

flat-floored channels, in which flow lines are a<br />

common feature. See fretted terrain.<br />

fretted terrain Part of the highl<strong>and</strong>–lowl<strong>and</strong><br />

boundary region of Mars, lying along a great<br />

© 2001 by CRC Press LLC<br />

friction slope<br />

circle having a pole at ≈ 145 ◦ W <strong>and</strong> 55 ◦ N. The<br />

terrain also exists around the high-st<strong>and</strong>ing terrain<br />

retained in the northern lowl<strong>and</strong> plains. It is<br />

characterized by flat-topped outliers of cratered<br />

upl<strong>and</strong>s, termed plateaux, mesas, buttes, <strong>and</strong><br />

knobs depending on their size. The differences<br />

in size are thought to reflect different<br />

extents of fracturing <strong>and</strong> subsequent modification,<br />

whereby greater fracturing <strong>and</strong> modification<br />

created the smaller l<strong>and</strong>forms.<br />

Plateaux, mesas, <strong>and</strong> buttes are generally<br />

considered to have formed during creation of<br />

the relief difference. Alternatively, it has been<br />

proposed that they represent flat-topped table<br />

mountains that formed due to the interaction<br />

of basaltic lava <strong>and</strong> ground water at low eruption<br />

rates. The final form of the fretted terrain<br />

has also been accounted for as representing the<br />

shorelines of a sea <strong>and</strong> by scarp retreat owing<br />

to mass wasting <strong>and</strong> sublimation of volatiles, or<br />

ground-water sapping.<br />

friction The process whereby motion of one<br />

object past another is impeded, or the force producing<br />

this impediment. Friction is caused by<br />

microscopic interference between moving surfaces,<br />

<strong>and</strong>/or by microscopic fusion between the<br />

surfaces, which must be broken to continue motion.<br />

Friction is dissipative, producing heat from<br />

ordered kinetic energy. The frictional shear<br />

stress on a surface S ′ f is a fraction of the normal<br />

stress on the surface Sn so that<br />

S ′ f<br />

= fSn<br />

where f is the coefficient of friction. This is<br />

known as Amontons’s law <strong>and</strong> f has a typical<br />

value of 0.6 for common surfaces in contact, <strong>and</strong><br />

in geophysical processes. Friction controls the<br />

behavior of geophysical faults.<br />

friction factor A coefficient that indicates<br />

the resistance to a flow or movement. Generally<br />

empirical <strong>and</strong> dimensionless (e.g., Darcy–<br />

Weisbach friction factor).<br />

friction slope Energy loss, expressed as head<br />

(energy loss per unit weight of fluid) per unit<br />

length of flow. Appears in the Manning Equation.<br />

183

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