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DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

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epoch An arbitrary fixed instant of time used<br />

as a chronological reference for calendars, celestial<br />

reference systems, star catalogs, or orbital<br />

motions. Prior to 1984, star catalog coordinates<br />

were commonly referred to the mean<br />

equator <strong>and</strong> equinox of the beginning of the<br />

Besselian year (see year). Thereafter, the Julian<br />

year (365.25 days) has been used.<br />

equant A point in the Ptolemaic description<br />

of orbits about which the center of the epicycle<br />

moved at constant angular velocity as it moved<br />

along the deferent. The equant was equidistant<br />

on the opposite side of the center of deferent<br />

from the Earth. See deferent, epicycle.<br />

equation of continuity Any of a class of<br />

equationsthatexpressthefactthatsomequantity<br />

(mass, charge, energy, etc.) cannot be created or<br />

destroyed. Such equations typically specify that<br />

the rate of increase of the quantity in a given region<br />

of space equals the net current of the quantity<br />

flowing into the region. Thus, the change<br />

of a property ɛ (e.g., mass) inside a volume element<br />

results from the convergence of a flux<br />

C(ɛ) across the boundaries of the volume <strong>and</strong><br />

from sources <strong>and</strong> sinks S(ɛ) inside the volume:<br />

∂ɛ<br />

∂t +∇·C(ɛ)=S(ɛ).<br />

The most common application is the conservation<br />

of mass<br />

∂ρ<br />

∂t<br />

=−∇ ·(ρu) =−∇ ·j<br />

with ρ being the density <strong>and</strong> j=ρu the mass<br />

current. Using the total derivative instead of the<br />

partial one, this can be written as<br />

dρ<br />

dt<br />

∂ρ<br />

= s+u·∇ρ=−ρ ·∇u.<br />

∂t<br />

equation of state An equation relating the<br />

pressure, volume, <strong>and</strong> temperature (or some<br />

othersetofthermodynamicalvariables)ofasubstance<br />

or system.<br />

equation of state (cosmic string) Foranaccurate<br />

macroscopic description of a vacuum vortex<br />

defect as a cosmic string, one needs the string<br />

© 2001 by CRC Press LLC<br />

equatorial anomaly<br />

equations of state, which give both the string<br />

energy per unit length U <strong>and</strong> its tension T (in<br />

general both are variable), <strong>and</strong> also the relation<br />

between them. The simplest example of equation<br />

of state is T =U= const, corresponding<br />

to the Goto–Nambu string.<br />

Also conducting cosmic strings can be described<br />

by fitting analytical expressions to the<br />

numerical solutions of the classical equations<br />

of motion for the microscopic fields. The best<br />

analytical expression available for the Witten<br />

model is known as the Carter–Peter equation<br />

of state. See Carter–Peter model, conducting<br />

string, energy per unit length (cosmic string),<br />

Goto–Nambu string, tension (cosmic string),<br />

wiggle (cosmic string).<br />

equation of state of pure water Potential<br />

densityofpurewaterisafunctionoftemperature<br />

only. For actual values see Chen <strong>and</strong> Millero<br />

(1986).<br />

equation of time The hour angle of the true<br />

(observed) sun minus the hour angle of the (fictitious)<br />

mean sun of mean solar time.<br />

equator The locus of a point traveling around<br />

the globe that is equidistant from the north <strong>and</strong><br />

south poles forms the equator.<br />

equator, geomagnetic (1.) The line around<br />

the Earth, along which the vertical component<br />

of the magnetic field is zero. Approximately<br />

equidistant from both magnetic poles, but distorted<br />

from that shape by non-dipole harmonics<br />

of the Earth’s magnetic field.<br />

(2.) A term sometimes applied to the equatorial<br />

surface of the magnetosphere.<br />

equatorial anomaly Although processes in<br />

the ionospheric F region are complex, it is still<br />

reasonable to expect the maximum daytime ionization<br />

to fall roughly near to the location of<br />

the overhead sun. However, in the equatorial<br />

region, <strong>and</strong> most noticeable near equinox,<br />

the daytime maximum in ionization splits forming<br />

crests 20 ◦ to 30 ◦ to the north <strong>and</strong> south of<br />

the dip equator, leaving an ionization trough<br />

at the dip equator. This is called the equatorial<br />

anomaly. It is formed by a process analogous<br />

to a fountain, ionization near the dip equa-<br />

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