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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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state of saturation, i.e., the ratio of the actual vapor<br />

pressure (e) to the saturation vapor pressure<br />

(E). The relative humidityf is (as a percentage)<br />

f= e<br />

× 100% .<br />

E<br />

Relative humidity expresses the saturation status<br />

of air. Generally the relative humidity decreases<br />

duringthedaytimeastemperatureincreases, <strong>and</strong><br />

increases at night as the temperature falls.<br />

relativistic jets Collimated ejection of matter<br />

at a velocity close to the speed of light, giving<br />

rise to highly elongated, often knotted structures<br />

in radio-loud active galactic nuclei, for example,<br />

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

Radio jets usually originate from an unresolved<br />

core <strong>and</strong> physically connect, or point, to extended<br />

lobes. Linear sizes of jets mapped at radio<br />

frequencies in external galaxies range from<br />

several kpc or tens of kpc, down to the minimum<br />

size resolvable with very long baseline<br />

interferometers (∼ 1 parsec). Parsec-size jets<br />

show several indications of relativistic motion,<br />

including apparent superluminal motion, <strong>and</strong> jet<br />

one-sidednessascribedtorelativisticbeamingof<br />

radiation. It is less clear whether jets observed at<br />

scales of several kiloparsecs are still relativistic.<br />

It is thought that only the most powerful radio<br />

galaxies, class II according to Fanaroff <strong>and</strong> Riley,<br />

<strong>and</strong> quasars may sustain a relativistic flow<br />

along kiloparsec-sized jets. Jets emit radiation<br />

over a wide range of frequencies. This suggests<br />

that the radio emission is electron synchrotron<br />

radiation. Galactic objects, like the evolved binary<br />

system SS 433, <strong>and</strong> galactic superluminal<br />

sources are also believed to harbor relativistic<br />

jets. See superluminal source.<br />

relativistic time delay The elongation of the<br />

travel-time of an electromagnetic signal, caused<br />

by the signal’s passing through a gravitational<br />

field. This typically occurs when a radar signal<br />

is sent from the Earth, reflected back from another<br />

planet to be received at the Earth, perhaps<br />

passing near the sun on the way. When the path<br />

of the signal does not come near the sun, the<br />

time-lapse between the emission of the signal<br />

<strong>and</strong> its reception on the Earth is almost the same<br />

as calculated from Newton’s theory. However, if<br />

the signal passes near the sun, the distance cov-<br />

© 2001 by CRC Press LLC<br />

residence time (replacement time or average transit time) (TR)<br />

ered by the signal becomes longer because the<br />

sun curves the spacetime in its neighborhood.<br />

When the planet <strong>and</strong> the Earth are on opposite<br />

sides of the sun, <strong>and</strong> the path of the signal just<br />

grazes the sun’s surface, one finds for the relativistic<br />

time delay t:<br />

t = GM<br />

c 3<br />

<br />

ln 4RERp/d 2<br />

,<br />

where M is the mass of the sun, RE is the distance<br />

from the sun to the Earth, Rp is the distance<br />

from the sun to the planet, <strong>and</strong> d is the<br />

radius of the sun. Here G is Newton’s gravitational<br />

constant, <strong>and</strong> c is the speed of light. The<br />

planets used in the measurement are Mercury,<br />

Venus, the artificial satellites Mariner 6 <strong>and</strong><br />

7, <strong>and</strong> Mars (where artificial satellites orbiting<br />

Mars or l<strong>and</strong>ed on Mars were used as reflectors).<br />

The value oft predicted by Einstein’s relativity<br />

theory for the situation described above is<br />

240 ms (Shapiro, 1964). This is now one of the<br />

st<strong>and</strong>ard experimental tests of the relativity theory<br />

(along with perihelion shift, light deflection,<br />

<strong>and</strong> the gravitational redshift).<br />

relativity See general relativity, special relativity.<br />

relaxation time Characteristic time to represent<br />

rate of relaxation phenomena. For instance,<br />

for a viscoelastic body which is characterized<br />

by Maxwell model, stress decreases exponentially<br />

with time when a deformation is applied<br />

at a time <strong>and</strong> is subsequently kept constant. The<br />

time that stress becomes 1/e (e is base of natural<br />

logarithms) of the initial value is called relaxation<br />

time. Each material has its own relaxation<br />

time.<br />

rem An obsolete unit of radiation dose equivalent,<br />

equal to 100 ergs per gram.<br />

remote sensing reflectance In oceanography,<br />

the ratio of the “water-leaving” radiance in<br />

air to the downward plane irradiance incident<br />

onto the sea surface [sr −1 ].<br />

residence time (replacement time or average<br />

transit time) (TR) The average length of time<br />

that a parcel of water spends in a hydrologic<br />

reservoir; the minimum period required for all<br />

395

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