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cosmochemistry
cosmochemistry Cosmochemistry is concerned with experimental, observational, and theoretical studies of the chemical, isotopic, and mineralogical composition of extraterrestrial materials such as cometary dust particles (e.g., the Giotto mission to comet P/Halley), interplanetary dust particles (known as IDPs) collected using high-flying aircraft), lunar samples, and meteorites. The seminal work by Harold Urey, Hans Suess, and Harrison Brown on the chemical processes involved in the origin and evolution of the Solar System and the abundances of the elements led to the emergence of cosmochemistry as a separate sub-discipline in the late 1940s.
Historically, two major areas in cosmochemistry research have been: (1) the determination of the solar-system abundances of the elements, and (2) the chemical behaviour of the elements in a solar composition (i.e. hydrogen-rich) environment. These two topics are interwoven because the observed elemental abundances in primitive meteorites (chondrites) are generally correlated with the volatility of the elements, or their compounds, in material of solar composition. Before proceeding some commonly used terms need to be defined. Chondrites are stony meteorites that contain small, melted beads known as chondrules and finer-grained material known as matrix. Some chondrites also contain calcium, aluminium-rich inclusions (CAIs), which are dominated by calcium, aluminium, and titanium-bearing refractory oxides and silicates. Observational studies indicate that the chondrules, mineral fragments, inclusions, and matrix in chondrites formed in the solar nebula and have been little altered since that time by planetary processes (e.g., aqueous alteration, igneous differentiation). The chondrites are divided into three groups; carbonaceous, ordinary, and enstatite chondrites, on the basis of their major element composition and mineralogy. These three major classes are further subdivided into different petrographic types. The most primitive chondrites, in the sense of most closely reproducing the elemental abundances in the photosphere of the Sun, are the CI (or Cl) carbonaceous chondrites. Solar abundances of the elementsTo a very good approximation, the abundances of most elements in the CI carbonaceous chondrites and in the Sun are identical. The few exceptions to this generalization are: light elements such as lithium, which are destroyed by thermonuclear reactions in the Sun; atmophile elements such as hydrogen, oxygen, carbon, nitrogen, and the noble gases, which are incompletely condensed in meteorites; and some rare elements such as mercury, germanium, lead, and tungsten, which are difficult to analyse in the Sun or in meteorites. To a lesser extent there is also a good correspondence between elemental abundances in the Sun and in all chondrites. This close relationship has led cosmochemists to believe that chondrites are relatively unaltered samples of material that condensed in the solar nebula. Over 30 years of meteorite studies and chemical equilibrium modelling of nebular chemistry demonstrate that evidence of nebular chemical reactions is preserved, with varying degrees of alteration by subsequent processes such as thermal metamorphism and aqueous alteration, in chondritic meteorites.Cosmochemical behaviour of the elementsChemical analyses of chondrites and interplanetary dust particles, and thermochemical equilibrium calculations of chemistry in hydrogen-rich solar material, show that the elemental fractionations in chondrites and IDPs are primarily the result of volatility controlled processes such as gas Æ solid condensation and solid Æ gas evaporation in the solar nebula. The occurrence of some characteristic mineral morphologies, such as enstatite (MgSiO3) whiskers with screw dislocations, in some IDPs shows that gas Æ solid condensation was directly responsible for growing some minerals.Cosmochemists therefore classify the elements according to their chemical behaviour in hydrogen-rich solar material. Refractory elements are the first elements to condense from solar composition gas. Both lithophiles (preferentially found in oxides or silicates, or both) and siderophiles (preferentially found in metals) with low vapour pressures, or that form compounds with low vapour pressures, fall into this category. The condensation of iron metal alloy and magnesian silicates (MgSiO3, enstatite, and Mg2SiO4, forsterite) divides the refractory elements from the moderately volatile elements. In turn, troilite (FeS) condensation divides the moderately and highly volatile elements. Finally, water-ice condensation separates the highly volatile elements (e.g., lead, indium, bismuth, and thallium) from the atmophile elements (hydrogen, carbon, nitrogen, and the noble gases). Table 1 summarizes the major condensation reactions in solar composition material. Refractory lithophiles include the alkaline earths (e.g. calcium and magnesium) the lanthanides (rare earth elements, or REE), the actinides, aluminium, and elements in groups 3b (scandium, yttrium), 4b (titanium, zirconium, and hafnium), and 5b (vanadium, niobium, and tantalum) of the periodic table. The refractory siderophiles are the platinum-group metals (except palladium), molybdenum, tungsten, and rhenium. As shown in Table 1, the refractory lithophiles and siderophiles constitute about 1 per cent by mass of the total condensable material (rock + ices) in the solar nebula. Extensive studies of the chemical composition of stony meteorites show that these refractory elements behave as a group in most meteorites: that is, their abundances in different types of meteorites are either enriched or depleted by about the same factor. Large enrichments, which are 20 times solar elemental abundances on average, of the refractory lithophile and siderophile elements are found in CAIs in the Allende meteorite and other carbonaceous chondrites. The CAIs have a mineralogy dominated by minerals rich in calcium, aluminium, and titanium such as hibonite, CaAl12O19, melilite, a solid-solution of gehlenite, Ca2Al2SiO7, and åkermanite, Ca2MgSi2O7, spinel, MgAl2O4, and perovskite, CaTiO3.
Table 1 gives the 50 per cent condensation temperatures for metallic iron alloy and forsterite (Mg2SiO4). Metallic iron and magnesian silicates account for most of the rocky material in solar composition matter. The large excess of molecular hydrogen (H2) in solar gas leads to extremely low oxygen fugacities and the FeO content of the magnesian silicates is insignificant until low temperatures of about 400–600 K. At these temperatures olivine and pyroxene solid solutions containing ∼20 mole per cent of fayalite (Fe2SiO4) and ferrosilite (FeSiO3) are predicted to form and any remaining iron metal is predicted to form magnetite at a pressure-independent temperature of about 400 K. However, slow solid-state diffusion at 400–600 K may inhibit solid-solid reactions such as the formation of FeO-rich silicates over the estimated 105-107 year lifetime of the solar nebula. The moderately volatile elements have condensation temperatures intermediate between those of the major elements iron, magnesium, and silicon and troilite, FeS. The elements in this group are geochemically diverse and include sodium, potassium, rubidium, chromium, manganese, copper, silver, gold, zinc, boron, gallium, phosphorus, arsenic, antimony, sulphur, selenium, tellurium, fluorine, and chlorine. The highly volatile elements condense at temperatures below 719 K, where troilite forms. These elements include mercury, bromine, cadmium, indium, thallium, lead, and bismuth. The condensation chemistry of many of the moderately and highly volatile elements is not well known because of uncertainties in the relevant thermodynamic data. As Fig. 1 shows, hydrogen is the most abundant element and H2 is therefore the most abundant gas in material of solar composition. At sufficiently high temperatures, dissociation to atomic H occurs. However, the phase boundary where abundances of H2 and H are equal is at lower pressures and higher temperatures than those expected in the solar nebula. H2 remains in the gas until temperatures of about 5 K, where it will condense out as solid hydrogen. It is unlikely that temperatures as low as this were ever reached in the solar nebula. About 0.1 per cent of all hydrogen condenses out as water-ice at temperatures of 150–250 K, depending on the total pressure. Hydrated silicates such as serpentine and talc are also predicted to form by reactions between anhydrous silicate grains and water vapour in the nebular gas at temperatures below 300 K at 10−4 bar. However, although they are thermodynamically favourable, these reactions probably did not occur in the solar nebula because the vapour phase hydration of rock in a near-vacuum is a very slow process. Theoretical studies of hydration kinetics in the solar nebula and petrographic studies of water-bearing chondrites both suggest that the production of hydrated minerals occurred on the meteorite parent bodies. It is thus very likely that water-ice is the first H-bearing condensate to form. Carbon chemistry is significantly more complex. To a good first approximation, carbon monoxide (CO) is the dominant carbon gas at high temperatures and low pressures and methane (CH4) is the dominant carbon gas at low temperatures and high pressures in solar composition material. The two gases are converted by the net thermochemical reaction: CO(g) + 3H2(g) = CH4(g) + H2O(g). (The symbol g denotes the gaseous state). Increasing the H2 pressure (essentially the total pressure in solar material) or decreasing the temperature drives this reaction to the right and yields more CH4. The CO-CH4 boundary is in the region of 600 K at 10−4 bar total pressure. CO is more abundant at higher temperatures, and CH4 is more abundant at lower temperatures. As first noted by Urey and later quantified by Lewis and Prinn, the kinetics of the COÆCH4 conversion may be so slow under the pressure and temperate conditions expected in the solar nebula that CO cannot be converted to CH4 within the lifetime of the nebula. An exception to this occurs in the giant protoplanetary subnebulae, which are higher-density environments that are predicted to exist around Jupiter and the other gas giant planets during their formation. The COÆCH4 conversion is predicted to take place in these environments. At low temperatures in the outer solar nebula and the giant protoplanetary subnebulae, CO and CH4 may react with water-ice to form the clathrate hydrates CO·6H2O(s) and CH4·6H2O(s) (The symbol s denotes the solid state.) (Clathrates are solids in which one chemical component is enclosed in the structure of another, as if in a cage.) The formation of these clathrate hydrates requires sufficiently rapid diffusion of CO or CH4 through the water-ice crystal lattice. Theoretical models, which use experimentally determined activation energies for clathrate formation, predict that CH4 clathrate hydrate can form in the giant protoplanetary subnebulae but that CO clathrate hydrate cannot form in the lower-density environment of the outer solar nebula. The most important features of nitrogen chemistry are that N2 is the major nitrogen gas at high temperatures and low pressures while NH3 is the major nitrogen gas at low temperatures and high pressures. The two species are converted by the reaction N2 + 3H2 = 2NH3, which is analogous to the reaction which converts CO and CH4. Reduction of N2 to NH3 is also predicted to be kinetically inhibited in the solar nebula and to be both thermodynamically favoured and kinetically facile in the giant protoplanetary subnebulae. This is true even when the possible catalytic effects of grains of metallic iron are taken into account. Thus, N2 is predicted to be the dominant nitrogen gas throughout the solar nebula, and NH3 is predicted to be the dominant nitrogen gas throughout the giant protoplanetary subnebulae. At low temperatures in the outer solar nebula, N2·6H2O(s) becomes thermodynamically stable, but its formation is probably inhibited by two factors. One is the limited availability of water-ice, which may already be totally consumed by reactions to form other hydrates and clathrates. The other is the expected kinetic inhibition of clathrate hydrate formation in the outer solar nebula. In this case, N2, like CO, will not condense until temperatures of about 20 K (at 10−4 bar pressure) are reached, where the solid ices form. On the other hand, NH3·H2O formation is predicted in the giant protoplanetary subnebulae, because it is both thermodynamically favoured and kinetically facile. The noble gases helium, neon, argon, krypton, and xenon display fairly simple chemistry in material of solar composition. All are present in the gas as the monatomic elements and argon, krypton, and xenon undergo condensation to either ices or clathrate hydrates at sufficiently low temperatures. Condensation of the pure ices will occur at slightly lower temperatures than condensation of the clathrate hydrates. The formation of these species, like the clathrates of CO and N2, may, however, be kinetically inhibited. Temperatures of about 20 K (at 10−4 bar pressure) are required for the quantitative condensation of argon, krypton, and xenon as pure ices. Neither helium nor neon will condense out of the gas because temperatures of 5 k or below are required for this to happen. Bruce Fegley Bibliography Kerridge, J. F. and Matthews, M. S. (eds) (1988) Meteorites and the early Solar System. University of Arizona Press, Tucson. |
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Cite this article
PAUL HANCOCK and BRIAN J. SKINNER. "cosmochemistry." The Oxford Companion to the Earth. 2000. Encyclopedia.com. 30 May. 2012 <http://www.encyclopedia.com>. PAUL HANCOCK and BRIAN J. SKINNER. "cosmochemistry." The Oxford Companion to the Earth. 2000. Encyclopedia.com. (May 30, 2012). http://www.encyclopedia.com/doc/1O112-cosmochemistry.html PAUL HANCOCK and BRIAN J. SKINNER. "cosmochemistry." The Oxford Companion to the Earth. 2000. Retrieved May 30, 2012 from Encyclopedia.com: http://www.encyclopedia.com/doc/1O112-cosmochemistry.html |
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Astrochemistry
AstrochemistryIn the night sky, the expanses of space between the stars of the Milky Way appear to be empty. In fact this space is occupied by a very thin gas that is mostly hydrogen and that has mere traces (less than 0.1% by number of atoms) of other elements such as oxygen, carbon, and nitrogen. The gas is also dusty; it contains grains of dust (particulate matter) that, like an interstellar fog, impede one's view of the stars. This gas is not evenly spread in space, but is clumpy. Although on average there is approximately one hydrogen atom for every cubic centimeter of interstellar space, a clump may be one thousand or more times as dense as a comparable volume of average density. Since about 1970 astronomers have been finding that these denser regions contain a great variety of molecules; about 120 different molecular species have been identified in the interstellar medium. A few of them are listed in the accompanying table. The study of these molecules in the Milky Way and in other galaxies is called astrochemistry. How Do Astronomers Detect These Molecules?Astronomers identify interstellar atoms and molecules via spectroscopy . For example, interstellar sodium atoms that happen to be in a line of sight going from a point on Earth's surface toward a bright star absorb light emitted by that star at a wavelength that is characteristic of sodium atoms (about 589 nanometers; 2.3 × 10−5 inches). Most interstellar molecules are detected by spectroscopic analysis that measures absorption or emission at radio wavelengths rather than those corresponding to visual light. Astronomers use large radio telescopes to detect radiation emitted by interstellar molecules. These emissions arise because the molecules are set to rotating when they collide with each other. The molecules lose energy and slow down in their rotations by emitting radiation at wavelengths that are specific for them, such that each emission is a "signature" of one type of molecule. For example, the molecule carbon monoxide, CO, may emit at various radio wavelengths, including 2.6 millimeters (0.1 inches), 1.3 millimeters (0.05 inches),0.65 millimeters (0.03 inches), and 0.32 millimeters (0.01 inches). Interstellar gas is usually very cold (around 10 degrees above absolute zero), but even under these conditions the molecular collisions are energetic enough to keep the molecules rotating and, therefore, emitting radiation. Sometimes these interstellar molecules may be located in warmer regions. If the gas of which they are a part is close to a star, or becomes heated
because one clump collides with another, the temperature of the molecules may rise considerably, perhaps to several thousand degrees above absolute zero. In these cases, the collisions between gas molecules are correspondingly more energetic, and molecules may be set to vibrating as well as rotating. For example, a carbon monoxide molecule, CO, vibrates to-and-fro as if the two atoms are connected by a coiled spring. A vibrating molecule also eventually slows down and loses energy (unless it is involved in further collisions) by emitting radiation that is again specific to that particular molecule. In the example of CO, that radiation has a wavelength of about 4.7 micrometers (18.5 × 10−5 inches), the detection of which necessitates the use of large telescopes that are sensitive to infrared radiation. How Are Interstellar Molecules Formed?The Milky Way, like all other galaxies, was formed from intergalactic gas that was essentially atomic. So where do the molecules come from? One can deduce that they are not left over from the processes that formed the Milky Way because scientists can detect molecules in regions in which they are (currently) being rapidly destroyed; therefore there must be a formation process in operation now. For example, the hydroxyl molecule, OH, can be observed in rather low density interstellar gas regions (containing about 100 H atoms per cubic centimeter) in which it is being destroyed by stellar radiation in a time frame, typically, of ten thousand years. This seems a long time but because the Galaxy has been in existence for a much longer time (about 15 billion years), the OH radicals (and many other species) must have been formed relatively recently in the Galaxy's history. Simple collisions between O and H atoms do not lead to the formation of OH molecules, because the atoms bounce apart before they are able to form a chemical bond. Similarly, low temperature collisions between O atoms and H2 molecules are also unreactive. Astronomers have now determined that much of the chemistry of interstellar space occurs via ion-molecule reactions. Cosmic rays (fast-moving protons and electrons pervading all of interstellar space) ionize molecular hydrogen (H2) and the resulting ions (H2+) react quickly with more H2 to form other ions (H3+). The H3+ ions drive a chemistry that consists of simple two-body reactions. The extra proton in H3+ is quite weakly bound (relative to the bonding of one proton to another in H2); in a collision an H3+ molecule easily donates its proton to some other species, creating a new molecule. For example, an H3+ ion reacts with an O atom to give OH+, a new species: O + H3+ → OH+ + H and the OH+ then reacts with H2 molecules to make, successively, H2O+ and H3O+ ions OH+ → H2O+ → H3O+ This process of H abstraction finishes here, because the O+ ion in H3O+ has saturated all its valencies with respect to H atoms. However, the H3O+ ion has a strong attraction for electrons because of its positive charge, and the ion-electron recombination leads to dissociation of the ion-electron complex into a variety of products, including OH (hydroxyl) and H2O (water). Other exchange reactions occur; for example, CO may be formed through the neutral exchange C + OH → CO + H Similar ion-molecule reactions drive the chemistries of other atoms, such as C and N, to yield ions such as CH3+ and NH3+. These ions can then react with other species to form larger and more complex molecules. For example, methanol (CH3OH) may be formed by the reaction of CH3+ ions with H2O molecules, followed by recombination of the product of that reaction with electrons CH3+ + H2O → CH3OH2+ CH3OH2+ + e− → CH3OH + H Ion-molecule reactions, followed by ion-electron recombinations and supplemented by neutral exchanges, are capable of forming the majority of the observed interstellar molecular species. Very large gas-phase reaction networks, involving some hundreds of species interacting in some thousands of chemical reactions, are routinely used to describe the formation of the observed interstellar molecules in different locations in models of interstellar chemistry. Does the Dust Play a Role in Astrochemistry?The dust has several important chemical roles. Obviously, it may shield molecules from the destructive effects of stellar radiation. It also has more active roles. We have seen that free atoms in collision may simply bounce apart before they can form a chemical bond. By contrast, atoms adsorbed on the surface of a dust grain may be held together until reaction occurs. It is believed that molecular hydrogen is formed in this way (i.e., through heterogeneous catalysis ) and is ejected from dust grain surfaces into the gas volume with high speed and in high states of vibration and rotation. Other simple molecules, such as H2O, CH4, and NH3, are also likely to form in this way. In the denser clumps where the gas is very cold, the dust grains are also at a very low temperature (around 10 degrees above absolute zero). Gasphase molecules colliding with such grains tend to stick to their surfaces, and over a period of time the grains in these regions accumulate mantles of ice: mostly H2O ice, but also ices containing other molecules such as CO, CO2, and CH3OH. Astronomers can detect these ices with spectroscopy. For example, water ice molecules absorb radiation at a wavelength about 3.0 micrometers (11.8 × 10−5 inches), having to do with the O–H vibration in H2O molecules; the molecules do not rotate because they are locked into the ice. In instances in which such ice-coated dust grains lie along a line of sight toward a star that shines in the infrared, this 3.0 micrometer (11.8 × 10−5 inch) absorption is very commonly seen. Interstellar solid-state chemistry can occur within these ices. Laboratory experiments have shown that ices of simple species such as H2O, CO, or NH3 can be stimulated by ultraviolet radiation or fast particles (protons, electrons) to form complex molecules, including polycyclic aromatic hydrocarbons (PAHs) containing several benzene-type rings. The detection by astronomers of free interstellar benzene (C6H6) in at least one interstellar region suggests that this solid-state chemistry may be the route by which these molecules are made. What Role Do Molecules Play in Astronomy?The primary role that interstellar molecules play is a passive one: Their presence in regions so obscured by dust that we cannot see into them using optical telescopes is used to probe these regions. The most dramatic example of this is the discovery of the so-called giant molecular clouds in the Milky Way and other galaxies via the detection of the emission of 2.6 micrometers (10.2 × 10−5 inches) wavelength radiation by CO molecules present in these clouds. The existence of these huge gas clouds, containing up to a million times the mass of the Sun, was not suspected from optical observations because these clouds are completely shrouded in dust. However, radio astronomy has shown that these clouds are the largest nonstellar structures in the Galaxy, and that they will provide the raw material for the formation of millions of new stars in future billions of years of the Galaxy's evolution. The radiation from molecules that we detect can represent a significant loss of energy from an interstellar cloud. Some molecules are very effective coolants of interstellar gases and help to maintain the temperatures of these gases at very low values. This cooling property is very important in clumps of gas that are collapsing inward under their own weight. If such a collapse can continue over vast stretches of time, then ultimately a star will form. In the early stages, it is important that the clumps remain cool, otherwise the gas pressure might halt the collapse. In these stages, therefore, the cooling effect of the molecules' emission of radiation is crucial. The formation of stars like the Sun is possible because of the cooling effect of molecules. Interstellar chemistry is therefore one factor determining the rate of star formation in the Galaxy. Astrochemists have shown that it takes about one million years for the molecules of a collapsing cloud to be formed; this is about the same amount of time as that required for the collapse itself to become established. The accompanying image illustrates a region of star formation in the Galaxy. Astrochemistry also has a role that is particularly significant to the human species here on planet Earth. The planet was formed as a byproduct of the formation of the star that is the Sun, and is in effect the accumulation of dust grains that were the debris of large chunks of matter that subsequently impacted and stuck together. Earth is still subject to the occasional impacts of debris left over from the formation of the solar system. These impacts, now seen as a source of potential danger, in fact once brought prebiotic material to Earth. The oceans arose from the arrival of icy comets, and carbon, nitrogen, and elemental metals were brought by asteroid impacts. These elements and others are necessary for life on Earth, and a new discipline, astrobiology, is coming into being: Its aim is to study the transport of prebiological material in the Galaxy and the development of life within suitable environments in the universe. ConclusionAstrochemistry extends chemistry into regimes of exceptionally low density and temperature; it involves gas-phase, surface, and solid-state processes. Its products, the molecules, have opened up a new approach to astronomy. see also Spectroscopy. David A. Williams BibliographyBernstein, Max P.; Sandford, Scott A.; and Allamandola, Louis J. (1999). "Life's Far Flung Raw Materials." Scientific American 281(1):42–49. Dyson, John E., and Williams, David A. (1997). The Physics of the Interstellar Medium. Philadelphia: Institute of Physics Publishing. Greenberg, J. Mayo (2000). "The Secrets of Stardust." Scientific American 283(6):70–75. Hartquist, Thomas W., and Williams, David A. (1995). The Chemically Controlled Cosmos: Astronomical Molecules from the Big Bang to Exploding Stars. New York: Cambridge University Press. Internet ResourcesAstrobiology. New Scientist. Available from <http://www.newscientist.com/hottopics/astrobiology>. The Star Formation Newsletter. Science Magazine. Available from <http://www.eso.org/gen-fac/pubs/starform/star-form-list.html>. |
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Cite this article
Williams, David A.. "Astrochemistry." Chemistry: Foundations and Applications. 2004. Encyclopedia.com. 30 May. 2012 <http://www.encyclopedia.com>. Williams, David A.. "Astrochemistry." Chemistry: Foundations and Applications. 2004. Encyclopedia.com. (May 30, 2012). http://www.encyclopedia.com/doc/1G2-3400900043.html Williams, David A.. "Astrochemistry." Chemistry: Foundations and Applications. 2004. Retrieved May 30, 2012 from Encyclopedia.com: http://www.encyclopedia.com/doc/1G2-3400900043.html |
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astrochemistry
astrochemistry The study of chemical reactions that occur naturally in space. Molecules are able to form in space at very low temperatures (e.g. 20 K) and at pressures far lower than are achievable in a laboratory on Earth. Many chemical species that are unstable on Earth exist in space, and are detectable by their spectral lines at radio, infrared, optical, and ultraviolet wavelengths. There are two broad types of formation process: chemistry in gas clouds (including photodissociation) and chemistry on the surfaces of dust grains. Many astrochemical reactions involve only gases. In some cases atoms or molecules in the gas may become ionized by the passage of cosmic rays, and the subsequent reactions between ions and molecules are more rapid as a result. In the other main process, dust particles act as catalysts, providing a surface on which atoms, ions, and molecules can stick and then react. The dust also acts as a shield and prevents starlight from breaking up the molecules again. Heating of the dust by newly formed stars may release complex molecules from the grains back into the gas cloud and drive a new series of chemical reactions. See also Interstellar Molecule.
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Cite this article
"astrochemistry." A Dictionary of Astronomy. 1997. Encyclopedia.com. 30 May. 2012 <http://www.encyclopedia.com>. "astrochemistry." A Dictionary of Astronomy. 1997. Encyclopedia.com. (May 30, 2012). http://www.encyclopedia.com/doc/1O80-astrochemistry.html "astrochemistry." A Dictionary of Astronomy. 1997. Retrieved May 30, 2012 from Encyclopedia.com: http://www.encyclopedia.com/doc/1O80-astrochemistry.html |
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cosmochemistry
cosmochemistry See astrochemistry.
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Cite this article
"cosmochemistry." A Dictionary of Astronomy. 1997. Encyclopedia.com. 30 May. 2012 <http://www.encyclopedia.com>. "cosmochemistry." A Dictionary of Astronomy. 1997. Encyclopedia.com. (May 30, 2012). http://www.encyclopedia.com/doc/1O80-cosmochemistry.html "cosmochemistry." A Dictionary of Astronomy. 1997. Retrieved May 30, 2012 from Encyclopedia.com: http://www.encyclopedia.com/doc/1O80-cosmochemistry.html |
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