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Passage to a Ringed World - NASA's History Office

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altitudes down <strong>to</strong> 40 kilometers<br />

above the surface, will be obtained<br />

primarily by direct impact of the atmosphere<br />

on a cold filter target. The<br />

second sample will be obtained at<br />

about 20 kilometers by pumping the<br />

atmosphere through the filter.<br />

After each collection, the filter will be<br />

transferred <strong>to</strong> an oven and heated <strong>to</strong><br />

three successively higher temperatures,<br />

up <strong>to</strong> about 650 degrees Celsius,<br />

<strong>to</strong> vaporize and pyrolyze the<br />

collected material. The product at<br />

each temperature will be swept up by<br />

nitrogen carrier gas and transferred<br />

<strong>to</strong> the GCMS for analysis.<br />

Gas Chroma<strong>to</strong>graph and Mass Spectrometer.<br />

The Gas Chroma<strong>to</strong>graph<br />

and Mass Spectrometer (GCMS) provides<br />

a quantitative analysis of the<br />

composition of Titan’s atmosphere.<br />

Atmospheric samples are transferred<br />

in<strong>to</strong> the instrument by dynamic pressure<br />

as the Probe descends through<br />

the atmosphere. The Mass Spectrometer<br />

constructs a spectrum of the molecular<br />

masses of the gas driven in<strong>to</strong> the<br />

instrument. Just prior <strong>to</strong> landing, the<br />

inlet port of the GCMS is heated <strong>to</strong><br />

vaporize material on contact with<br />

the surface. Following a safe landing,<br />

the GCMS can determine Titan’s surface<br />

composition.<br />

The GCMS uses an inlet port <strong>to</strong> collect<br />

samples of the atmosphere and<br />

has an outlet port at a low pressure<br />

point. The instrument contains three<br />

chroma<strong>to</strong>graphic columns. One<br />

column has an absorber chosen<br />

<strong>to</strong> separate carbon monoxide, nitrogen<br />

and other gases. Another column<br />

has an absorber that will separate<br />

nitriles and other highly polar compounds.<br />

The third is <strong>to</strong> separate hydrocarbons<br />

up <strong>to</strong> C . The mass range<br />

8<br />

is 2–146 amu.<br />

The Mass Spectrometer serves as the<br />

detec<strong>to</strong>r for the Gas Chroma<strong>to</strong>graph,<br />

for unseparated atmospheric samples<br />

and for samples provided by the<br />

ACP. Portions of the GCMS are identical<br />

in design <strong>to</strong> the Orbiter’s INMS.<br />

Descent Imager and Spectral Radiometer.<br />

The Descent Imager and Spectral<br />

Radiometer (DISR) uses several instrument<br />

fields of view and 13 sensors,<br />

operating at wavelengths of 350–<br />

1700 nanometers, <strong>to</strong> obtain a variety<br />

of imaging and spectral observations.<br />

The thermal balance of the atmosphere<br />

and surface can inferred by<br />

measuring the upward and downward<br />

flux of radiation.<br />

Solar aureole sensors will measure<br />

the light intensity around the Sun resulting<br />

from scattering by aerosols,<br />

permitting calculations of the size and<br />

number density of suspended particles.<br />

Infrared and visible imagers will<br />

observe the surface during the latter<br />

stages of the descent. Using the<br />

Probe’s rotation, the imagers will<br />

build a mosaic of pictures of the Titan<br />

landscape. A side-looking visible imager<br />

will view the horizon and take<br />

pictures of the clouds, if any exist. For<br />

spectral measurements of the surface,<br />

a lamp will be turned on shortly before<br />

landing <strong>to</strong> provide enough light<br />

for measuring surface composition.<br />

The DISR will obtain data <strong>to</strong> help determine<br />

the concentrations of atmospheric<br />

gases such as methane and<br />

argon. DISR images will also determine<br />

if the local surface is solid or liquid.<br />

If the surface is solid, DISR will<br />

reveal <strong>to</strong>pographic details. If the surface<br />

is liquid, and waves exist, DISR<br />

will pho<strong>to</strong>graph them.<br />

DISR sensors include three framing<br />

imagers, looking downward and horizontally;<br />

a spectrometer dispersing<br />

light from two sets of optics looking<br />

downward and upward; and four<br />

solar aureole radiometers. The spectral<br />

range of the imagers is 660–<br />

1000 nanometers; the spectrometer’s<br />

range is 480–960 nanometers; the<br />

aureole radiometers operate at 475–<br />

525 and 910–960 nanometers, with<br />

two different polarizations.<br />

Separate downward- and upwardlooking<br />

optics are linked by fiberoptic<br />

bundles <strong>to</strong> an infrared grating spectrometer.<br />

The infrared detec<strong>to</strong>rs have<br />

a spectral range of 870–1700 nanometers.<br />

There are also two violet<br />

pho<strong>to</strong>meters, looking downward<br />

and upward with a bandwidth of<br />

350–470 micrometers.<br />

To provide reference and timing for<br />

the other measurements, the DISR<br />

uses a Sun sensor <strong>to</strong> measure the solar<br />

azimuth and zenith angle relative<br />

<strong>to</strong> the rotating Probe.<br />

The interior of the<br />

Huygens Probe,<br />

showing its science<br />

instruments.<br />

TOOLS OF DISCOVERY 117

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