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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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Nasmyth spectrum F(k/k η)<br />

10 6<br />

10 4<br />

10 2<br />

10 0<br />

10 2<br />

10 4<br />

10 4<br />

10 3<br />

10 2<br />

10 1<br />

normalized wavenumber k/k<br />

η<br />

Universal spectrum of oceanic turbulence according<br />

to Nasmyth. The circles are the measured points <strong>and</strong><br />

they are plotted against the cyclic wavenumber nor-<br />

malized by the Kolmogorov wavenumberkη.<br />

<strong>and</strong> has a Lorentzian shape given by:<br />

φ(ν)=<br />

γ/4π 2<br />

γ/4π 2 +(ν) 2<br />

whereγ is the radiation damping constant. In a<br />

description in terms of classical radiation theory,<br />

γ= 8π2e2 ,<br />

3mecλ2 where e <strong>and</strong> me are the charge <strong>and</strong> mass of the<br />

electron, <strong>and</strong> c is the speed of light.<br />

natural remanent magnetism Many volcanic<br />

rocks contain magnetic minerals. When<br />

these rocks cool from the molten state, they are<br />

permanently magnetized by the Earth’s magnetic<br />

field at that time. This natural remanent<br />

magnetism provides information on the time<br />

evolution of the Earth’s magnetic field <strong>and</strong> continental<br />

drift.<br />

nautical mile A unit of length equal to exactly<br />

1852 m.<br />

nautical twilight See twilight.<br />

Navier–Stokes equations The complicated<br />

set of partial differential equations for the motion<br />

of a viscous fluid subject to external forces.<br />

neap tide The tide produced when the gravitational<br />

pull of the sun is in quadrature, i.e., at<br />

© 2001 by CRC Press LLC<br />

10 0<br />

nearly diurnal free wobble<br />

right angles, to that of the moon. They occur<br />

twice a month at about the times of the lunar<br />

first <strong>and</strong> last quarters. In these situations the<br />

difference between high <strong>and</strong> low tides is unusually<br />

small, with both the high tide lower <strong>and</strong> the<br />

low tide higher than usual.<br />

NEAR A Near Earth Asteroid Rendezvous<br />

(NEAR) spacecraft that was the first Discovery<br />

mission launched on February 17, 1996. NEAR<br />

took photographs of Comet Hyakutake in March<br />

1996, flew by C-asteroid 253 Mathilde on June<br />

27, 1997, <strong>and</strong> S-asteroid 433 Eros on December<br />

23, 1998, <strong>and</strong> also past the Main Belt asteroid<br />

Illya. It began orbiting S-asteroid 433 Eros in<br />

February 2000.<br />

Its primary mission was to explore 433 Eros<br />

in detail for approximately 1 year. The mission<br />

will help answer basic questions about the nature<br />

<strong>and</strong> origin of near-Earth objects, as well as provide<br />

clues about how the Earth itself was formed.<br />

Studies were made of the asteroid’s size, shape,<br />

mass, magnetic field, composition, <strong>and</strong> surface<br />

<strong>and</strong> internal structure. It achieved this using<br />

the spacecraft’s X-ray/gamma ray spectrometer,<br />

near infrared imaging spectrograph, multispectral<br />

camera fitted with a CCD imaging detector,<br />

laser altimeter, <strong>and</strong> magnetometer. A radio<br />

science experiment was performed using the<br />

NEAR tracking system to estimate the gravity<br />

field of the asteroid. Periapsis of the orbit was as<br />

low as 24 km above the surface of the asteroid.<br />

Although NEAR has no l<strong>and</strong>ing legs, on February<br />

12, 2001 it was l<strong>and</strong>ed on the surface of Eros<br />

at a speed of about 1.9 m/s. It photographed on<br />

the way down, the last image from 120 m altitude.<br />

Remarkably it continued to function, after<br />

impact sending back γ -ray data.<br />

nearly diurnal free wobble The retrograde<br />

motion of the Free Core Nutation (FCN) as<br />

viewed from points fixed on the Earth. The wobble<br />

appears from the Earth to have frequencies<br />

of ωwobble = ωnutation − , where is the frequency<br />

of the Earth’s rotation. Very long baseline<br />

interferometry observations, which measure<br />

the nutation in space relative to fixed stars,<br />

place the FCN frequency ωnutation ≈ 433.2 cycles/sidereal<br />

day.<br />

329

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