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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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spring<br />

tion <strong>and</strong> produces fluctuations in signals coming<br />

from the outer ionosphere known as Scintillations.<br />

Spread F tend to occur in the night. See<br />

F region, ionosphere.<br />

spring Season of the year in the northern<br />

hemisphere between the vernal equinox, about<br />

March 21 <strong>and</strong> the summer solstice, about June<br />

21; in the southern hemisphere between the autumnal<br />

solstice, about September 21, <strong>and</strong> the<br />

winter solstice, about December 21. See also<br />

cosmic spring.<br />

spring tide Tide which occurs when the<br />

Earth, sun, <strong>and</strong> moon are nearly co-linear. Under<br />

these conditions the gravitational field gradients<br />

of the sun <strong>and</strong> moon reinforce each other.<br />

The high tide is higher <strong>and</strong> low tide is lower than<br />

the average. Spring tides occur twice a month<br />

near the times of both new moon <strong>and</strong> full moon.<br />

sprites Short-lived luminosities observed<br />

at high altitudes above thunderstorms, apparently<br />

associated with upward discharges of thunderstorm<br />

electricity. They appear as columnar<br />

diffuse reddish glows between 30 km <strong>and</strong><br />

80 km above ground, branching into the upper<br />

atmosphere lasting tens of milliseconds, following<br />

large positive cloud-to-ground lightning<br />

strokes. It is currently believed that such lightning<br />

strokes leave in the cloud a residual charge<br />

of 200 Coulombs or more, creating a significant<br />

voltage difference between the cloud top <strong>and</strong><br />

the ionosphere. This induces a heating of the<br />

middle atmosphere, which produces the sprites<br />

when electrons collisionally excite atmospheric<br />

nitrogen, that emits red light in flashes with several<br />

milliseconds duration.<br />

Studied from the ground, aircraft <strong>and</strong> from<br />

the space shuttle, sprites appear to be most common<br />

above large mesoscale convection features,<br />

such as the storm systems of the American Midwest.<br />

Ground observations indicate that an active<br />

system can generate as many as 100 sprites<br />

in the course of several hours. Discovered in<br />

1990. See elves, blue jet.<br />

squall A sudden strong wind or brief storm<br />

that persists for only a few minutes, often associated<br />

with thunderstorm activity <strong>and</strong> sometimes<br />

accompanied by rain or snow.<br />

© 2001 by CRC Press LLC<br />

442<br />

s (slow) process The capture of free neutrons<br />

by nuclei of iron <strong>and</strong> heavier elements on a time<br />

scale slower than the average for beta-decays of<br />

unstable nuclei (cf. r process). The s process is<br />

the primary source of those isotopes of elements<br />

from Z = 30 to 82 with the largest binding energies<br />

(the “valley of beta stability”). It occurs<br />

in asymptotic giant branch stars <strong>and</strong> in the corresponding<br />

evolutionary stage of more massive<br />

stars. The main sources of free neutrons (which<br />

require some mixing between zones dominated<br />

by different nuclear reactions) are<br />

13 C(α, n) 16 O <strong>and</strong><br />

14 N(α, γ ) 18 O(α, γ ) 22 Ne(α, n) 25 Mg<br />

(the latter being more important in massive<br />

stars). Among the important products of the s<br />

process are barium (because it is dominated by<br />

s process nuclides <strong>and</strong> can be seen in the atmospheres<br />

of cool, evolved stars) <strong>and</strong> technitium<br />

(because of its short half life). s-process production<br />

of elements does not reach beyond lead<br />

<strong>and</strong> bismuth because of the set of unstable elements<br />

before reaching uranium <strong>and</strong> thorium. A<br />

typical s-process chain is<br />

174<br />

Y b(n, γ )<br />

175<br />

Yb(e<br />

−<br />

¯νe) 175 Lu(n, γ ) 176 Lu(n, γ )<br />

177<br />

Lu(e<br />

−<br />

¯ν)<br />

177<br />

Hf (n, γ )<br />

178<br />

Hf (n, γ )<br />

179<br />

Hf<br />

179<br />

Hf (n, γ )<br />

180<br />

Hf (n, γ )<br />

181<br />

Hf (e<br />

−<br />

¯νe)<br />

181<br />

T a(n, γ )<br />

182 <br />

Ta e<br />

− <br />

¯νe<br />

182 W(n, γ ) 184 W(n, γ )<br />

<strong>and</strong> so forth, onward to Re,Os, etc. The time<br />

scales of the beta decays range from minutes to<br />

months.<br />

The cross-section to capture the next neutron<br />

is smallest for nuclides with filled shells,<br />

so that products of the s process with N =<br />

26, 50, 82, <strong>and</strong> 126 are particularly abundant.<br />

See asymptotic giant branch star, beta decay, r<br />

process.<br />

S stars Cool (3000 to 3600 K) giant stars<br />

which have greatly enhanced s-process elements<br />

(such as zirconium, barium, yttrium, <strong>and</strong> technetium)<br />

<strong>and</strong> have an atmospheric C/O number<br />

ratio very close to unity. Their optical spectra<br />

are characterized by strong absorption b<strong>and</strong>s of<br />

ZrO, as well as TiO, <strong>and</strong> carbon-rich compounds<br />

such as CN <strong>and</strong> C2. Most are believed to be on<br />

the asymptotic giant branch (AGB) of the H-R

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