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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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period The amount of time for some motion<br />

to return to its original state <strong>and</strong> to repeat its<br />

motion.<br />

period-luminosity relation The relation between<br />

the luminosity of Cepheid variable stars<br />

<strong>and</strong> the variability period of these stars. The<br />

basic trend is that those stars with longer periods<br />

are brighter. By measuring the period of<br />

Cepheid variables, astronomers can use this relationship<br />

to deduce the intrinsic luminosity of<br />

these stars. Combined with a measurement of<br />

the apparent luminosity, the distance of Cepheid<br />

variables can be estimated. The Hubble Space<br />

Telescope has been used to detect Cepheid variables<br />

out to the Virgo cluster, measuring the distance<br />

of the Virgo cluster to roughly a 10% accuracy.<br />

See Cepheid variable.<br />

permafrost Soil or subsoil that is permanently<br />

frozen for two or more years, typical of<br />

arctic regions, or in other arctic climates (such<br />

as high altitude) where the temperature remains<br />

below 0 ◦ C for two or more years.<br />

permeability In electromagnetism, the relation<br />

between the microscopic magnetic field B<br />

<strong>and</strong> the macroscopic field (counting material polarizability)<br />

H. In fluid flow, permeability, also<br />

called the intrinsic permeability, characterizes<br />

the ease with which fluids flow through a porous<br />

medium. Theoretically, permeability is the intrinsic<br />

property of a porous medium, independent<br />

of the fluids involved. In reality, the permeabilitiesofsomerocksorsoilsareaffectedbythe<br />

fluid. Permeability in fluid flow has the dimension<br />

of area. For an anisotropic porous medium,<br />

the permeability is a tensor. See Darcy’s law.<br />

permeability coefficient In electromagnetism,<br />

the coefficientµ in the relation B =µH<br />

between the microscopic magnetic field B <strong>and</strong><br />

the macroscopic field H. In general, µ may be<br />

a3× 3 linear function of position, with time<br />

hysteresis, though it is often taken to be a scalar<br />

constant. In fluid flow, the coefficient measuring<br />

how easily water molecules can cross the surface<br />

film. For clear water (Davies <strong>and</strong> Rideal, 1963),<br />

it is equal to 5 ms −1 .<br />

© 2001 by CRC Press LLC<br />

perturbative solution<br />

persistent current See current generation<br />

(cosmic string).<br />

perturbation theory A tool that can be applied<br />

to questions ranging from classical mechanics<br />

to quantum theory. Independent of the<br />

actual question, the basic idea is to find an approximate<br />

solution of the equations for a complex<br />

system by first solving the equations of<br />

a physically similar system chosen so that its<br />

solution is relatively easy. Then the effects of<br />

small changes or perturbations on this solution<br />

are studied. In classical mechanics, for instance,<br />

the motion of a planet around the sun is studied<br />

first <strong>and</strong> the influences of the other planets are<br />

added later.<br />

Formally, a complex system is described by<br />

a set of coupled non-linear partial differential<br />

equations. If only small-amplitude disturbances<br />

are considered, such a system can be simplified<br />

by linearization of the equations: whenever two<br />

oscillating quantities are multiplied, since both<br />

are small, their product is a higher order term<br />

<strong>and</strong> can be ignored. If these results are to be<br />

applied to a real situation, however, one always<br />

has to take one step back <strong>and</strong> justify whether<br />

the amplitudes calculated in the real situation<br />

are small enough so that the non-linear terms<br />

actually are negligible compared with the linear<br />

ones.<br />

perturbative solution An approximate solution,<br />

usually found to a problem that is too<br />

difficult to be solved by an exact calculation. In<br />

a perturbative solution there exists at least one<br />

small dimensionless parameter (ε) that must be<br />

distinctly smaller than 1. Then, ε 2 ≪ ε. The<br />

equations to be solved are exp<strong>and</strong>ed in power<br />

series with respect to ε <strong>and</strong> in the first step all<br />

terms proportional to ε n where n>1 are assumed<br />

to be equal to zero. In the next step, the<br />

already found first approximation is substituted<br />

for the terms proportional to ε, the terms proportional<br />

to ε n where n>2 are assumed equal to<br />

zero both in the equation <strong>and</strong> in the solution,<br />

<strong>and</strong> the coefficient of ε 2 is determined. The<br />

procedure can, in principle, go to an arbitrarily<br />

high degree of approximation, but in practice<br />

the calculations often become prohibitively<br />

complicated in the second step (this happens,<br />

e.g., with Einstein’s equations in almost every<br />

357

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