The determination of the composition of materials that make up comets
is essential in trying to understand the origin of these primitive obj
ects. The ices especially could be made in several different astrophys
ical settings including the solar nebula, protosatellite nebulae of th
e giant planets, and giant molecular clouds that predate the formation
of the solar system. Each of these environments makes different ices
with different composition. In order to-understand the origin of comet
s, one needs to determine the composition of each of the ice phases. F
or example, it is of interest to know that comets contain carbon monox
ide, CO, but it is much more important to know how much of it is a pur
e solid phase, is trapped in clathrate hydrates, or is adsorbed on amo
rphous water ice. In addition, knowledge of the isotopic composition o
f the constituents will help determine the process that formed the com
pounds. Finally, it is important to understand the bulk elemental comp
osition of the nucleus. When these data are compared with solar abunda
nces, they put strong constraints on the macro-scale processes that fo
rmed the comet. A differential scanning calorimeter (DSC) and an evolv
ed-gas analyzer (EGA) will make the necessary association between mole
cular constituents and their host phases. This combination of instrume
nts takes a small (tens of mg) sample of the comet and slowly heats it
in a sealed oven. As the temperature is raised, the DSC precisely mea
sures the heat required, and delivers the gases to the EGA. Changes in
the heat required to raise the temperature at a controlled rate are u
sed to identify phase transitions, e.g., crystallization of amorphous
ice or melting of hexagonal ice, and the EGA correlates the gases rele
ased with the phase transition. The EGA consists of two mass spectrome
ters run in tandem. The first mass spectrometer is a magnetic-sector i
on-momentum analyzer (MAG), and the second is an electrostatic time-of
-flight analyzer (TOF). The TOF acts as a detector for the MAG and ser
ves to resolve ambiguities between fragments of similar mass such as C
O and N-2. Because most of the compounds of interest for the volatile
ices are simple, a gas chromatograph is not needed and thus more integ
ration time is available to determine isotopic ratios. A gamma-ray spe
ctrometer (GRS) will determine the elemental abundances of the bulk co
metary material by determining the flux of gamma rays produced from th
e interaction of the cometary material with cosmic-ray produced neutro
ns. Because the gamma rays can penetrate a distance of several tens of
centimeters, a large volume of material is analyzed. The measured com
position is, therefore, much more likely to be representative of the b
ulk comet than a very small sample that might have lost some of its vo
latiles. Making these measurements on a lander offers substantial adva
ntages over trying to address similar objectives from an orbiter. For
example, an orbiter instrument can determine the presence and isotopic
composition of CO in the cometary coma, but only a lander can determi
ne the phase(s) in which the CO is located and separately determine th
e isotopic composition of each reservoir of CO. The bulk composition o
f the nucleus might be constrained from separate orbiter analyses of d
ust and gas in the coma, but the result will be very model dependent,
as the ratio of gas to dust in the comet will vary and will not necess
arily be equal to the bulk value. (C) 1997 Published by Elsevier Scien
ce Ltd.