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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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adiation cooling<br />

planets (Jupiter, Saturn, Uranus, <strong>and</strong> Neptune)<br />

also carry such radiation belts, as does Mercury,<br />

but Venus <strong>and</strong> Mars have very weak magnetic<br />

fields <strong>and</strong> do not.<br />

radiation cooling The transfer of heat energy<br />

away from an object by the net outward transport<br />

of radiation. In geophysics, at night, there<br />

is no incoming solar radiation, <strong>and</strong> the outgoing<br />

radiation from the Earth’s surface exceeds<br />

the incoming radiation. The loss of radiant energy<br />

lowers the temperature of the surface, <strong>and</strong><br />

the radiational cooling in surface layers of the<br />

atmosphere often causes a strong inversion of<br />

lapse rate. In atmosphere radiational processes,<br />

the vertical variations are much larger than their<br />

horizontal variations. Thus, the radiation cooling<br />

rate CR can be expressed approximately by<br />

its vertical component. That is<br />

CR = 1 ∂FN<br />

ρCp ∂h<br />

where ρ is air density, Cp is specific heat at<br />

constant pressure, FN is vertical component of<br />

net radiation flux, <strong>and</strong> h is height.<br />

radiation gauge In linearized (weak field)<br />

descriptions of gravity, one may use the restricted<br />

coordinate transformations to achieve<br />

h α α = 0, h0µ = 0, <strong>and</strong> h αµ ,µ = 0 (where<br />

µ = 0, 1, 2 or 3) for the linearized gravitational<br />

potentialhab in a source-free region. (The<br />

comma denotes partial derivative.) Gravitational<br />

potentials meeting these requirements are<br />

said to be in the radiation gauge. See linearized<br />

gravitation, summation convention.<br />

radiation pressure The transfer of momentum<br />

to an object by radiation through the scattering,<br />

absorption, <strong>and</strong> emission of the radiation.<br />

The momentum transported by a single photon<br />

is given by p=hν/c where h is Planck’s constant,<br />

ν is the frequency of the photon, <strong>and</strong> c<br />

is the speed of light. The change in the momentum<br />

of a flux of photons as it is reflected<br />

(or absorbed) results in a net pressure being applied<br />

to the object. If the radiation is reflected,<br />

then the momentum transferred by the photon is<br />

twice the normal incident momentum.<br />

© 2001 by CRC Press LLC<br />

386<br />

radiation tide Periodic variations in sea level<br />

primarily related to meteorological changes,<br />

such as the twice daily cycle in barometric pressure,<br />

daily l<strong>and</strong> <strong>and</strong> sea breezes, <strong>and</strong> seasonal<br />

changes in temperature. Other changes in sea<br />

level due to meteorological changes that are r<strong>and</strong>om<br />

in phase are not considered to be part of the<br />

radiation tides.<br />

radiation zone An interior layer of the sun,<br />

lying between the core <strong>and</strong> the convection zone,<br />

where energy transport is governed by radiation.<br />

In the radiation zone of the sun, the temperature<br />

is a little cooler than the core, <strong>and</strong> as a result<br />

some atoms are able to remain intact. Their<br />

opacity influences the flow of radiation through<br />

this zone.<br />

radiative-convective equilibrium An equilibriumstatewheretheoutgoingradiationwould<br />

be equal to the absorbed radiation at all latitudes.<br />

radiative transfer equation The linear integrodifferential<br />

equation that describes the rate<br />

of change with distance of the radiance in a collimated<br />

beam at a specified location, direction,<br />

<strong>and</strong> wavelength; the equation accounts for all<br />

losses (e.g., due to absorption <strong>and</strong> scattering out<br />

of the beam) <strong>and</strong> gains (e.g., by emission or scattering<br />

into the beam).<br />

radio absorption Absorption occurring to<br />

radio waves as a result of interaction between<br />

an electromagnetic wave <strong>and</strong> free electrons in<br />

the ionosphere. See ionospheric absorption.<br />

radioactive Containing isotopes that undergo<br />

radioactive decay to another isotope, or<br />

another element, by emitting a subatomic particle:<br />

typically electron (beta particle) or helium<br />

nucleus (alpha particle). In some cases, the<br />

radioactive nucleus undergoes an internal rearrangement<br />

<strong>and</strong> emits an energetic gamma ray (a<br />

photon), without changing its atomic number or<br />

atomic weight.<br />

radioactive decay The process by which<br />

unstable atomic nuclei (radioisotopes) spontaneously<br />

break down into one or more nuclei of<br />

other elements. During this process, energy <strong>and</strong><br />

subatomic particles are released. The radioac-

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