29.03.2013 Views

DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

Electra<br />

Electra Magnitude 3.8 type B5 star at RA<br />

03 h 44 m , dec +24.06’; one of the “seven sisters”<br />

of the Pleiades.<br />

electric drift See drift, electric.<br />

electric field, parallel See parallel electric<br />

field.<br />

electric regime (cosmic string) It has been<br />

known since the seminal work of E. Witten in<br />

1985 that a current can build up in a cosmic<br />

string. As current generation proceeds via r<strong>and</strong>om<br />

choices of the phase of the current carrier,<br />

the resulting current can be of two distinct kinds,<br />

timelike or spacelike, depending on whether its<br />

time component is greater or smaller than its<br />

space component (there is also the possibility<br />

that they are equal, leading to a so-called lightlike<br />

current, but this is very rare at the time of<br />

current formation <strong>and</strong> would only occur through<br />

string intercommutation). Explicitly, setting the<br />

phase of the current carrier as a function of the<br />

time t <strong>and</strong> the string coordinate z in the form<br />

ϕ=ωt −kz ,<br />

withω <strong>and</strong>k arbitraryparameters, onec<strong>and</strong>efine<br />

a state parameter through<br />

w=k 2 −ω 2 ,<br />

the case w 0) corresponding<br />

to a timelike (respectively, spacelike)<br />

current.<br />

In the timelike case, the configuration is said<br />

to be in the electric regime, whereas for spacelike<br />

currents it is in the magnetic regime. The<br />

reason for these particular names stems from the<br />

possibility that the current is electromagnetic in<br />

nature, which means coupled with electric <strong>and</strong><br />

magnetic fields. Then, for the electric regime,<br />

one can always find a way to locally remove the<br />

magnetic field <strong>and</strong> thus one is led to describe<br />

solely an electric field surrounding a cosmic<br />

string. The same is true in the magnetic regime,<br />

where this time it is the electric field that can be<br />

removed <strong>and</strong> only a magnetic field remains. See<br />

current carrier (cosmic string), current generation<br />

(cosmic string), intercommutation (cosmic<br />

string).<br />

© 2001 by CRC Press LLC<br />

148<br />

electroglow A light emitting process in the<br />

upper atmospheres of Jupiter, Saturn, Uranus,<br />

<strong>and</strong> Saturn’s satellite Titan. Sunlight dissociates<br />

some H2 <strong>and</strong> ionizes the hydrogen; the electrons<br />

are accelerated <strong>and</strong> interact with H2, producing<br />

the glow.<br />

electromagnetic current meter A device<br />

that uses Faraday’s Law of magnetic induction<br />

to measure flow velocities. The current meter<br />

head establishes a magnetic field. A moving<br />

conductor (water) creates an electrical potential<br />

that is measured by the instrument. The electrical<br />

potential is proportional to the speed of the<br />

current. Often used for one- or two-dimensional<br />

velocity measurements.<br />

electromagnetic induction This is the generation<br />

of currents in a conductor by a change in<br />

magnetic flux linkage, which produces a magnetic<br />

field that opposes the change in the inducing<br />

magnetic field, as described by Faraday’s<br />

laws <strong>and</strong> Lenz’s law. In geophysics, this can<br />

be used to study the conductivity of the mantle<br />

through measurement of its response to magnetic<br />

fluctuations originating in the ionosphere<br />

<strong>and</strong>/or magnetosphere. Maxwell’s equations<br />

can be used to show that in the appropriate limit,<br />

a magnetic field obeys a diffusion equation:<br />

∂B<br />

∂t =−∇×<br />

<br />

1<br />

µ0σ ∇×B<br />

<br />

where σ is the local conductivity. Fluctuating<br />

external fields of frequency ω diffuse into<br />

a layer at the top of the mantle with a skin depth<br />

√ 2/µ0σω. The induced field is then essentially<br />

a reflection of this external field from the skindepth<br />

layer, <strong>and</strong> it has a phase relative to the external<br />

field that relates the conductivity structure<br />

of the layer to the frequency of the signal (essentially,<br />

long period signals penetrate deeper <strong>and</strong><br />

therefore depend more on deeper conductivity<br />

than do short period signals).<br />

electromagnetic radiation Radiation arising<br />

from the motion of electric charges, consisting<br />

of variations in the electric <strong>and</strong> magnetic<br />

fields, <strong>and</strong> propagating at the speed of light. Depending<br />

on the wavelength, observable as radio,<br />

infrared, visible light, ultraviolet, X-rays,<br />

or gamma rays.

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!