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Passage to a Ringed World - NASA's History Office

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72 PASSAGE TO A RINGED WORLD<br />

polar configuration, particularly in the<br />

outer magne<strong>to</strong>sphere where it stretches<br />

the magnetic field lines in the equa<strong>to</strong>rial<br />

plane. This ring current, caused<br />

by electrons and ions drifting around<br />

the planet in opposite directions, is<br />

probably primarily due <strong>to</strong> the energetic<br />

particles discussed later in this<br />

chapter. The effect of this ring current<br />

is moderate when compared with Jupiter,<br />

however. Another major contribution<br />

<strong>to</strong> Saturn’s <strong>to</strong>tal magnetic field<br />

comes from currents flowing in the<br />

magne<strong>to</strong>pause, which result from interaction<br />

with the solar wind.<br />

Cassini’s Dual Technique Magne<strong>to</strong>meter,<br />

measuring the magnetic field,<br />

and the Cassini Plasma Spectrometer,<br />

measuring the currents, will help map<br />

the current systems. These measurements,<br />

<strong>to</strong>gether with those taken by<br />

the other Cassini plasma instruments,<br />

will allow scientists <strong>to</strong> make a global<br />

model of Saturn’s magnetic field<br />

throughout the magne<strong>to</strong>sphere.<br />

Major Magne<strong>to</strong>spheric Flows<br />

There are two primary sources of energy<br />

driving magne<strong>to</strong>spheric processes:<br />

the planet’s rotation and the solar<br />

wind. Correspondingly, there are two<br />

types of large-scale plasma flow within<br />

the magne<strong>to</strong>sphere — corotation<br />

and convection. The nature of the<br />

large-scale circulation of particles in<br />

the magne<strong>to</strong>sphere depends on which<br />

source is dominant. At Earth, the energy<br />

is derived primarily from the solar<br />

wind; at Jupiter it is derived from the<br />

planet’s rapid rotation rate. Saturn’s<br />

magne<strong>to</strong>sphere is especially interesting<br />

because it is somewhere in be-<br />

tween: both energy sources should<br />

play an important role.<br />

Saturn’s ionosphere is a thin layer of<br />

partially ionized gas at the <strong>to</strong>p of the<br />

sunlit atmosphere. Collisions between<br />

particles in the atmosphere and the<br />

ionosphere create a frictional drag<br />

that causes the ionosphere <strong>to</strong> rotate<br />

<strong>to</strong>gether with Saturn and its atmosphere.<br />

The ionosphere, which extends<br />

from 1500 kilometers above<br />

the surface (defined as the visible<br />

cloud layer) <strong>to</strong> about 5000 kilometers,<br />

has a maximum density of about<br />

10,000 electrons per cubic centimeter<br />

at about 2000–3000 kilometers.<br />

The rotation of Saturn’s magnetic<br />

field with the planet creates a large<br />

electric field that extends in<strong>to</strong> the<br />

magne<strong>to</strong>sphere. The electromagnetic<br />

forces due <strong>to</strong> the combination of this<br />

electric field and Saturn’s magnetic<br />

field cause the charged magne<strong>to</strong>spheric<br />

plasma particles <strong>to</strong> “corotate”<br />

(rotate <strong>to</strong>gether with Saturn and its<br />

internal magnetic field) as far out as<br />

Rhea’s orbit (about nine R ). S<br />

Convection, the other large-scale<br />

flow, is caused by solar wind pulling<br />

the magnetic field lines <strong>to</strong>ward the<br />

tail. This leads <strong>to</strong> a plasma flow<br />

from day side <strong>to</strong> night side on open<br />

field lines and <strong>to</strong> a return flow from<br />

night side <strong>to</strong> day side on closed field<br />

lines (particularly near the equa<strong>to</strong>rial<br />

plane).<br />

On the dawn side, the corotation<br />

and convective flows will be in the<br />

same direction, but on the dusk side,<br />

they are opposing flows. The interaction<br />

of these flows may be responsible<br />

for some of the large variability<br />

observed in the outer magne<strong>to</strong>sphere.<br />

While at present we can only speculate<br />

about the consequences of these<br />

plasma flow patterns, we may expect<br />

some answers from investigations by<br />

Cassini’s plasma instruments (especially<br />

the Cassini Plasma Spectrometer<br />

and the Magne<strong>to</strong>spheric Imaging<br />

Instrument).<br />

Magne<strong>to</strong>spheric Plasma Regions<br />

Saturn’s magne<strong>to</strong>sphere can be<br />

broadly divided in two parts: a fairly<br />

quiet inner magne<strong>to</strong>sphere extending<br />

<strong>to</strong> about 12 R (beyond all moons<br />

S<br />

except Titan), and an extremely variable<br />

hot outer magne<strong>to</strong>sphere. In<br />

both regions, the plasma particles<br />

are concentrated in a disk near the<br />

equa<strong>to</strong>rial plane, where most plasma<br />

particle sources are located.<br />

In their brief passages through<br />

Saturn’s inner and outer magne<strong>to</strong>spheres,<br />

Pioneer and both Voyagers<br />

passed through several different<br />

plasma regions. The spacecraft observed<br />

a systematic increase in electron<br />

temperature with distance from<br />

Saturn, ranging from one electron<br />

volt (equivalent <strong>to</strong> a temperature of<br />

11,600 kelvins) at four R in the in-<br />

S<br />

ner magne<strong>to</strong>sphere and increasing<br />

<strong>to</strong> over 500 electron volts in the outer<br />

magne<strong>to</strong>sphere.<br />

The thickness of the plasma disk increases<br />

with distance from Saturn.<br />

Inside about four R a dense (about<br />

S<br />

100 per cubic centimeter) popula-

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