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DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

DICTIONARY OF GEOPHYSICS, ASTROPHYSICS, and ASTRONOMY

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potential<br />

Potassium-argon ages are reliable to hundreds<br />

of millions of years.<br />

potential In nonrelativistic conservative mechanical<br />

systems, a scalar function φ from which<br />

the mechanical forces are obtained as proportional<br />

to ∇φ. Examples are the electric potential<br />

<strong>and</strong> the gravitational potential.<br />

In fluid mechanics, in situations where the<br />

fluid velocity vector v is irrotational, v may be<br />

obtained as the gradient of a velocity potential.<br />

potential density The density that a parcel<br />

of fixed composition would acquire if moved<br />

adiabatically to a given pressure level (called<br />

reference pressure).<br />

potential energy The ability to do a specific<br />

amount of work. In conservative mechanical<br />

systems, work (energy) can be done on the<br />

system <strong>and</strong> stored there. This stored work is<br />

called potential energy (units of Joules or ergs<br />

in metric systems). A prototypical example is<br />

a system consisting of a stone moved to the top<br />

of a mountain. Work is required to move it to<br />

the top; once there, the system contains potential<br />

energy, which can be recovered (as heat or<br />

as thermal energy) by allowing the stone to roll<br />

down the mountain. A related gravitational example<br />

is in the storage of water behind a dam;<br />

potential energy is converted to work by allowing<br />

the water to flow through a turbine. Electrostatics<br />

provides another example, in which work<br />

must be done to bring a positive charge from infinity<br />

to add to a collection of positive charge.<br />

Such a collection has potential energy which can<br />

be recovered by allowing the charges to freely<br />

accelerate away from one another; the energy<br />

can then be collected as kinetic energy, as the<br />

charges move off to infinity.<br />

Potential energy may also be mechanical (a<br />

compressed spring) or chemical, such as the energy<br />

stored in unstable compounds (e.g., nitroglycerine)<br />

or in flammable substances (e.g., H2<br />

<strong>and</strong> O2 gases mixed). It also exists in extractable<br />

form in the nuclei of heavy atoms (e.g., U235 ),<br />

which release it as kinetic energy when undergoing<br />

fission; <strong>and</strong> in a system of neutrons <strong>and</strong><br />

protons, which will, at appropriate densities <strong>and</strong><br />

pressures, release some potential energy as ki-<br />

© 2001 by CRC Press LLC<br />

374<br />

netic, in fusion to form helium <strong>and</strong> heavier nuclei.<br />

potential height Dynamic height.<br />

potential instability Also called “convective<br />

instability”. Stratification instability caused<br />

by convective activities, i.e., the lower layer<br />

has higher moisture <strong>and</strong> becomes saturated first<br />

when being lifted, <strong>and</strong> hence cools thereafter<br />

at a slower rate than does the upper, drier portion,<br />

until the lapse rate of the whole layer<br />

becomes equal to the saturation adiabatic <strong>and</strong><br />

any further lifting results in instability. In<br />

general, use ∂θsw<br />

∂θse<br />

< 0or < 0 as the<br />

∂Z ∂Z<br />

criterion of convective instability. (θsw <strong>and</strong><br />

θse are pseudo-wet-bulb potential temperature<br />

<strong>and</strong> pseudo-equivalent potential temperature,<br />

respectively.)<br />

potential temperature The temperature <br />

that a parcel of fixed composition would acquire<br />

if moved adiabatically to a given pressure<br />

level (called reference pressure). For instance<br />

in saltwater, is the temperature that<br />

would be measured after a water parcel, which<br />

shows the measured in situ temperature T, has<br />

been moved isentropically (without exchanging<br />

heat or salt) through the ambient water masses<br />

to a reference depth, usually taken at the surface:<br />

dθ<br />

dz = dT<br />

dz −<br />

<br />

dT<br />

dz . The difference between <br />

ad<br />

<strong>and</strong> T is given by θ(z) = T(z)− <br />

z0 dT<br />

z dz<br />

ad dz′ .<br />

potential theory In geophysics, the area<br />

that utilizes gravitational potentials to determine<br />

the interior structure of a body. Study of a<br />

body’s gravitational potential (obtained by perturbations<br />

on an orbiting body) provides information<br />

about the distribution of interior mass,<br />

how much the primary body varies from hydrostatic<br />

equilibrium, the response of a body to tidal<br />

forces, <strong>and</strong> how much isostatic equilibrium surface<br />

features have undergone.<br />

potential vorticity (Rossby, 1940) In a shallow<br />

homogeneous layer, the potential vorticity<br />

is a conserved dynamic quantity Q as the ratio<br />

between the absolute vorticity <strong>and</strong> the thickness<br />

of the layer, defined by Q = (f + ζ)/H, where<br />

f is the planetary vorticity (i.e., Coriolis param-

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