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DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

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P<strong>and</strong>ora<br />

domes. Most occur in the lowl<strong>and</strong> plains far<br />

from the largest shields, <strong>and</strong> often near the lowl<strong>and</strong><br />

coronas. “Tick-like” features also show<br />

a pattern similar to the pancake domes, both in<br />

their spatial distribution <strong>and</strong> morphological similarities.<br />

Thus, it is thought that many ticks are<br />

modified dome features.<br />

P<strong>and</strong>ora Moon of Saturn, also designated<br />

SXVII. It was discovered on Voyager photos in<br />

1980. Its orbit has an eccentricity of 0.004, an<br />

inclination of essentially 0, <strong>and</strong> a semimajor axis<br />

of 1.42 × 10 5 km. Its size is 57 × 42 × 31<br />

km, its mass is 2.2 × 10 17 kg, <strong>and</strong> its density<br />

0.71 g cm −3 . It has a geometric albedo of 0.9,<br />

<strong>and</strong> orbits Saturn once every 0.629 Earth days.<br />

P<strong>and</strong>ora is the outer shepherd of Saturn’s F ring.<br />

Pangaea In geophysics, the single supercontinent<br />

in which all the continental areas were<br />

connected, <strong>and</strong> which broke up under continental<br />

drift about 180 million years ago.<br />

Papapetrou spacetimes (1953) Stationary<br />

empty space-times for which the norm <strong>and</strong> curl<br />

scalars of the Killing vector are in a functional<br />

relationship. Their asymptotic expansion lacks<br />

the mass monopole term, so they are in a sense<br />

zero-mass gravitational fields.<br />

PAR See photosynthetically available radiation.<br />

paraboloid A figure of revolution based on<br />

a parabola. The preferred shape for reflecting<br />

telescope primaries because it brings all rays<br />

parallel to the axis to a focus at the same unique<br />

point.<br />

parallax Motion of nearby stars against the<br />

more distant background stars, as a result of the<br />

different vantage points from the Earth’s orbit at<br />

different times of the year. Essentially a baseline<br />

of 2 AU (astronomical units) is used to give<br />

a perspective on the distance to the star. See<br />

astronomical unit, parsec.<br />

parallel electric field The component E|| of<br />

the electric field in a plasma parallel to the magnetic<br />

field vector. Because charges can easily<br />

flow along magnetic field lines, in many plasma<br />

© 2001 by CRC Press LLC<br />

352<br />

configurations E|| is expected to be virtually<br />

zero. However, observations on auroral field<br />

lines (e.g., that of beams of ions) suggest that a<br />

non-zero E|| may exist there, balanced either by<br />

the mirror force (see quasi neutral equilibrium)<br />

or by turbulent plasma processes. The ambipolar<br />

electric field, in which a relatively small E||<br />

is balanced by gravity, is another example.<br />

Parker limit A limit on the cosmological<br />

flux of magnetic monopoles:<br />

FM ≤ 10 −15 cm −2 · sec −1 .<br />

Acceleration of magnetic monopoles in the presence<br />

of a magnetic fieldB (like that of a galaxy,<br />

for instance), makes the magnetic field energy<br />

density decrease with time. The characteristic<br />

decay time is<br />

eB<br />

τd = ,<br />

4πnM vM<br />

where e is the electric charge, nM the magnetic<br />

monopole number density, <strong>and</strong> 〈vM 〉 their averagevelocity.<br />

Asthetimenecessarytoregenerate<br />

the magnetic field in a galaxy is comparable to<br />

the galactic rotation period τr ∼ 108 years, the<br />

limit results from the requirement that the decay<br />

time τd be larger than τr (so that magnetic<br />

monopoles do not affect galactic physics noticeably).<br />

The maximum allowed flux is much less<br />

than what is expected for monopoles formed at<br />

the gr<strong>and</strong> unified energy scale. See monopole,<br />

monopole excess problem.<br />

parsec The distance corresponding to a<br />

parallax of one second of arc. A unit of distance<br />

defined as the distance at which 1 astronomical<br />

unit (AU) subtends an angle of 1 sec of arc. It is<br />

equal to 206264.806 AU = 3.08568×10 16 m =<br />

3.26166 light years.<br />

partial derivative For a function f of multiple<br />

independent variables xa , the derivative<br />

with respect to one variable, say xi , computed<br />

by treating the other independent variables xa ,<br />

a = i constant. Notation:<br />

∂f<br />

∂xi partial pressure In any mixture of gases, of<br />

each component gas, the pressure that the gas

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