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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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adioisotopes<br />

Radio Frequency B<strong>and</strong>s<br />

Designation B<strong>and</strong> Frequency Wavelength<br />

Extremely Low Frequency ELF 0.003 – 3 kHz 100,000 – 100 km<br />

Very Low Frequency VLF 3 – 30 kHz 100 – 10 km<br />

Low Frequency LF 30 – 300 kHz 10 –1km<br />

Medium Frequency MF 300 kHz –3MHz 1km –100 m<br />

High Frequency HF 3 – 30 MHz 100 – 10 m<br />

Very High Frequency VHF 30 – 300 MHz 10 –1m<br />

Ultra High Frequency UHF 300 MHz – 3GHz 1m–10 cm<br />

Super High Frequency SHF 3 – 30 GHz 10 –1cm<br />

Extra High Frequency EHF 30 – 300 GHz 1 cm –1mm<br />

radioisotopes The isotopes of elements<br />

which are unstable <strong>and</strong> change into other elements<br />

via radioactive decay.<br />

radio lobe Extended, often irregular <strong>and</strong> filamentary<br />

region of radio emission observed at<br />

the end of radio jets on opposite sides of the nucleus,<br />

in powerful radio galaxies <strong>and</strong> quasars.<br />

Radio lobes often extend beyond the optical image<br />

of a galaxy <strong>and</strong> typically reach end-to-end<br />

sizes of 50 kpc to 1 Mpc (the largest radio lobes<br />

known span 9 Mpc). The radio spectral energy<br />

distribution of lobes decreases sharply with increasing<br />

frequency; lobes are said to be steep<br />

spectrum sources in opposition to radio cores<br />

which show a flat spectral specific flux distribution.<br />

Emission is due to synchrotron processes,<br />

as in radio cores, but produced by electrons with<br />

lower energy. A prototypical lobe-dominated<br />

radio source is the elliptical galaxy Centaurus A<br />

(the brightest radio source in the Centaurus constellation),<br />

with two lobes extending far beyond<br />

the optical image of the galaxy, each ∼ 300 kpc<br />

in projected linear size.<br />

radiometer An instrument used to measure<br />

radiant energy, as opposed to the number of photons.<br />

radiometric dating A method of obtaining<br />

absolute ages of geological specimens by comparing<br />

relative concentrations of parents <strong>and</strong><br />

daughter elements for a particular radioactive<br />

decay.<br />

radiometry The science of the measurement<br />

of radiant energy.<br />

© 2001 by CRC Press LLC<br />

388<br />

radio stars Stars whose radio emission is<br />

strong enough to be detected from Earth. This<br />

is rather rare <strong>and</strong> generally associated with extreme<br />

youth (see stellar activity) or presence of a<br />

companion (see RS Canum Venaticorum stars).<br />

Radio stars are particularly important because<br />

they permit coordinate systems on the sky determined<br />

separately from radio <strong>and</strong> optical data<br />

to be combined.<br />

radius of deformation A horizontal length<br />

scale defined as r = c/f, where c is the phase<br />

speed of long gravity waves in the ocean or atmosphere,<br />

<strong>and</strong> f = 2 sin θ is the Coriolis parameter<br />

with being the angular velocity of<br />

Earth’s rotation <strong>and</strong> θ latitude. For motion of<br />

horizontal scales larger than the deformation radius,<br />

rotation effects are dominant, whereas for<br />

motion of smaller horizontal scales, rotation effects<br />

are less important. On the equator, f vanishes<br />

<strong>and</strong> the equatorial radius of deformation is<br />

defined as rE = √ c/β where β = 2 cos θ is<br />

the meridional gradient of the Coriolis parameter.<br />

radon A radioactive colorless noble gas, Rn.<br />

Atomic number 86, natural atomic number 222.<br />

Melting temperature 202 K; boiling temperature<br />

211.3K.Radon exhibits an orange to yellow fluorescense<br />

in the solid state. Radon is produced<br />

as a daughter element in α− decay of radium.<br />

The longest-lived isotope is 222 Rn which has a<br />

half-life of 3.825 days, much longer than that of<br />

the other known isotopes ( 210 Rn to 221 Rn). All<br />

isotopes decay by α emission; 210 Rn <strong>and</strong> 211 Rn<br />

also have an electron capture branch, <strong>and</strong> 221 Rn<br />

also has a β− decay branch.

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