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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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twistor<br />

object that is carried away at speed v (from an<br />

identical object that remains at rest) to a different<br />

location <strong>and</strong> is returned to its original location<br />

accumulates less total time interval than does its<br />

nonmoving “twin”. In principle, if the motions<br />

are at a substantial fraction of the speed of light<br />

<strong>and</strong> the distances are substantial (light years),<br />

one could demonstrate this effect with human<br />

twins. For instance, if one newborn twin travels<br />

5 light years at a speed of 0.99c(c = speed of<br />

light) <strong>and</strong> then returns at the same speed, the<br />

stay-at-home twin would see the return at age<br />

10, while the elapsed time for (the age of) the<br />

traveling twin would be<br />

<br />

Age = t<br />

1 − v2<br />

c 2<br />

= 10 yr. × 0.14<br />

= 1.4 yr .<br />

The paradox is with everyday experience, where<br />

these effects are so small as to be unnoticeable.<br />

The effect has been verified in atomic<br />

clocks flown around the Earth, in the operation<br />

of atomic accelerators, <strong>and</strong> in the correct operation<br />

of the global positioning satellite system.<br />

See Lorentz transformation, special relativity.<br />

twistor An element of the four-dimensional<br />

spinor representation space of the group<br />

SU(2,2). Following work in 1962–1963 with<br />

R.P. Kerr, the notion of a twistor was put forward<br />

by R. Penrose as a possible mathematical<br />

tool for formulating the quantum theory of<br />

gravitation. In the theory of relativity, a twistor<br />

represents the state of a massless particle.<br />

two-flow equations The two coupled differential<br />

equations for irradiances obtained by<br />

integrating the radiative transfer equation over<br />

the hemispheres of downward <strong>and</strong> upward directions.<br />

2-form A rank-2 antisymmetric covariant<br />

tensor. A basis for 2-forms is the antisymmetric<br />

tensor product of pairs of 1-form basis forms.<br />

For instance, if {dxβ } is a basis for 1-forms, then<br />

{dxβ ∧ dxα } is a basis for 2-forms. Here ∧ is<br />

the antisymmetric tensor product, i.e.,<br />

dx β ∧ dx γ = 1 β γ γ β<br />

dx ⊗ dx − dx ⊗ dx<br />

2<br />

<br />

© 2001 by CRC Press LLC<br />

490<br />

with ⊗ the tensor product. See tensor.<br />

two-ribbon flare A large flare that has developed<br />

as a pair of bright str<strong>and</strong>s (ribbons) on<br />

both sides of the main inversion (“neutral”) line<br />

of the magnetic field of the active region, usually<br />

most prominent in Hα. Two-ribbon flares result<br />

in a substantial reconfiguration of the coronal<br />

magnetic field.<br />

two-stream approximation The two-flow<br />

approximation. See two-flow equations.<br />

two-stream instability A broad term referring<br />

to any of a number of resonant <strong>and</strong> nonresonant<br />

instabilities driven by the streaming of<br />

charged particles relative to the main body of a<br />

collisionless plasma.<br />

type I radio burst The metric type I burst<br />

is continuous radio emission from the sun, basically<br />

the normal solar radio noise. It can be<br />

enhanced during the late phase of a flare. The<br />

radio noise is unstructured, no frequency drift<br />

can be identified.<br />

type II radio burst In the metric type II<br />

burst, a relatively slow frequency drift can be observed,<br />

indicating a propagation of the electron<br />

source at a speed of about 1000 km/s. It is interpreted<br />

as evidence for a shock wave propagating<br />

through the solar corona, but it should be noted<br />

that the shock itself is not generating the radio<br />

emission but rather the electrons accelerated at<br />

the shock. As these electrons stream away from<br />

the shock, they generate small type III like structures,<br />

giving the burst the appearance of a herringbone<br />

in the frequency time diagram with the<br />

type II burst as the backbone <strong>and</strong> the type III<br />

structures as fish-bones. The type II burst is<br />

often split into two parallel frequency b<strong>and</strong>s, interpreted<br />

as forward <strong>and</strong> reverse shocks.<br />

Type II radio bursts can also be observed with<br />

frequencies in the kilometer range (kilometric<br />

type II radio burst). The drift characteristic is<br />

similar to that of the metric counterpart, the frequency<br />

indicates that these bursts are excited in<br />

interplanetary space. Consequently, the kilometric<br />

type II burst is interpreted as the signature<br />

of a shock propagating through interplanetary<br />

space. It should be noted, however, that

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