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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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tidal period The time between two points of<br />

equal phase in a tidal curve. Commonly measured<br />

between two high or two low tides.<br />

tidal prism The volume of water that is exchanged<br />

between a tidal estuary <strong>and</strong> the sea in<br />

one tidal period. Equivalent to the average tide<br />

range within the estuary times the area of the<br />

estuary. Since the range will vary in space <strong>and</strong><br />

time, the volume is not simply a horizontal slice,<br />

but a complicated function.<br />

tidal radius The radius within which all the<br />

luminous matter of a cluster or a galaxy is contained.<br />

The tidal radius can be measured for<br />

globular clusters <strong>and</strong> for galaxies belonging to<br />

clusters, which are found to have well-definite<br />

outer limits (in contrast with brightness profiles<br />

of isolated elliptical galaxies, described by de<br />

Vaucouleurs or Hubble’s–Reynolds law). The<br />

name arises from the underst<strong>and</strong>ing that in the<br />

case of a cluster galaxy, repeated encounters<br />

with nearby galaxies can lead to tidal stripping<br />

of the outer stars, which are loosely gravitationally<br />

bound, <strong>and</strong> to the evaporation of the outer<br />

envelope, leaving only stars which are inside the<br />

tidal radius.<br />

tidal stripping The escape of gas <strong>and</strong> stars<br />

gravitationally bound to a system, such as a<br />

galaxy or a globular cluster, due to tidal forces<br />

exerted by an object external to the system. For<br />

example, in a cluster of galaxies, tidal stripping<br />

may remove loosely bound stars from the galaxy<br />

outer envelope; in a close encounter between<br />

galaxies, stars <strong>and</strong> gas can be transferred from<br />

one galaxy to the other.<br />

tidal tail A highly elongated feature produced<br />

by tidal forces exerted on a spiral galaxy<br />

by a companion galaxy. A most notable example<br />

of tidal tails is observed in the “Antennae”<br />

pair of galaxies (NGC 4038 <strong>and</strong> NGC 4039),<br />

where the tidal tail extends for a projected linear<br />

size of ≈100 kpc, much larger than the size of<br />

the galaxies themselves. Computational models<br />

show that very extended tails, like the ones<br />

in the Antennae, are produced by a prograde encounter<br />

between galaxies, i.e., an encounter between<br />

a spiral galaxy <strong>and</strong> an approaching com-<br />

© 2001 by CRC Press LLC<br />

time dilatation<br />

panion galaxy which moves in the same sense<br />

of the spiral rotation.<br />

tide The response of the solid or fluid components<br />

of a planet or other astronomical body,<br />

under the influence of tidal forces.<br />

tide range The vertical distance between<br />

high tide <strong>and</strong> low tide at a point. Will vary in<br />

time because of temporal variation in the tide<br />

signal.<br />

tilt angle In solar magnetohydrodynamics,<br />

on the source surface, a neutral line separates<br />

the two hemispheres of the sun with opposing<br />

magnetic polarity. The maximum excursion of<br />

this neutral line with respect to the heliographic<br />

equator is called tilt angle. Since this neutral<br />

line is carried outwards as the heliospheric current<br />

sheet, the tilt angle also defines the waviness<br />

of the current sheet <strong>and</strong>, therefore, is an important<br />

parameter in the modulation of the galactic<br />

cosmic radiation.<br />

In terrestrial magnetospheric research, it is<br />

the angle between the z-axis in GSM coordinates<br />

<strong>and</strong> the dipole axis of the Earth. The GSM<br />

x-y plane can be viewed as providing an approximate<br />

north–south symmetry plane of the magnetosphere<br />

(see equatorial surface). A tilt angle<br />

ψ = 0 0 , therefore, signifies a magnetosphere<br />

with the dipole axis perpendicular to the equator,<br />

<strong>and</strong> the larger ψ, the more the axis departs<br />

from the perpendicular. Sunward inclination of<br />

the dipole gives ψ > 0, tailward inclinations<br />

ψ

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