Comets are among the oldest and most primitive objects in the Solar System. Originating from the Oort Cloud or the Kuiper Belt, they follow highly eccentric orbits that sometimes bring them to cross Earth's orbit. As they approach the Sun, their icy nucleus sublimates, forming a coma and a spectacular tail pushed by the solar wind. This phenomenon makes comets valuable indicators of large-scale gravitational dynamics and chemical witnesses of the original solar nebula.
Comets formed about 4.6 billion years ago, during the early moments of the protoplanetary disk surrounding the young Sun, well before the final formation of Earth. Their origin lies in the coalescence of dust grains and volatile ices in the cold, outer regions of the Solar System, primarily in the Kuiper Belt (for short-period comets) and the Oort Cloud (for long-period comets).
The physical processes governing their formation include accretion through low-velocity collisions of micrometric particles, condensation of water, CO, CO2, and other volatile compounds, as well as the preservation of complex organic molecules synthesized in the solar nebula or inherited from the interstellar medium. These icy bodies have undergone virtually no significant thermal transformation or internal differentiation, giving them an almost primordial state.
Earth, on the other hand, formed a little later through the accretion of rocky planetesimals in the hotter region of the inner solar disk, about 4.54 billion years ago. Thus, comets represent time capsules of the early Solar System, preserving within them chemical elements and prebiotic molecules that predate the appearance of Earth. Their study allows us to trace the physicochemical conditions prevailing during the genesis of the planetary system, long before the emergence of terrestrial life.
Unlike planets, whose orbits are almost circular, comets have very elongated trajectories. Their eccentricity \(e\) can approach 1, with orbits ranging from highly elliptical (periodic comets like Halley, \(e \approx 0.97\)) to parabolic or hyperbolic (non-periodic comets like C/2012 S1 ISON). Their periods can vary from a few years to several million years. Their orbit is mainly influenced by gravitational interactions with the giant planets and the passage of nearby stars that disturb the Oort Cloud.
Comet Name | Eccentricity \(e\) | Period (years) | Probable Origin | Appearance Date |
---|---|---|---|---|
1P/Halley | 0.967 | 75.3 | Kuiper Belt | 1986 |
C/1995 O1 (Hale-Bopp) | 0.9951 | ~2,533 | Oort Cloud | 1997 |
2P/Encke | 0.850 | 3.3 | Kuiper Belt | 2023 |
C/2020 F3 (NEOWISE) | 0.9992 | 6,800 | Oort Cloud | 2020 |
C/2012 S1 (ISON) | 1.0000 | Non-periodic | Oort Cloud | 2013 |
109P/Swift-Tuttle | 0.963 | 133 | Oort Cloud | 1992 |
153P/Ikeya–Zhang | 0.990 | 366 | Oort Cloud | 2002 |
73P/Schwassmann–Wachmann | 0.693 | 5.4 | Kuiper Belt | 2022 |
45P/Honda–Mrkos–Pajdušáková | 0.824 | 5.25 | Kuiper Belt | 2017 |
C/2011 L4 (PANSTARRS) | 1.0000 | Non-periodic | Oort Cloud | 2013 |
C/2006 P1 (McNaught) | 1.0000 | Non-periodic | Oort Cloud | 2007 |
21P/Giacobini-Zinner | 0.705 | 6.6 | Kuiper Belt | 2018 |
C/2013 A1 (Siding Spring) | 1.0006 | Non-periodic | Oort Cloud | 2014 |
7P/Pons–Winnecke | 0.633 | 6.4 | Kuiper Belt | 2015 |
C/2021 A1 (Leonard) | 1.0001 | Non-periodic | Oort Cloud | 2021 |
67P/Churyumov–Gerasimenko | 0.641 | 6.45 | Kuiper Belt | 2021 |
122P/de Vico | 0.962 | 74.4 | Oort Cloud | 1995 |
C/2014 Q2 (Lovejoy) | 0.9980 | ~11,500 | Oort Cloud | 2015 |
144P/Kushida | 0.087 | 7.6 | Kuiper Belt | 2010 |
141P/Machholz | 0.755 | 5.2 | Kuiper Belt | 2010 |
C/2001 Q4 (NEAT) | 0.9991 | ~37,000 | Oort Cloud | 2004 |
255P/Levy | 0.493 | 5.3 | Kuiper Belt | 2020 |
C/2017 T2 (PANSTARRS) | 0.9992 | Non-periodic | Oort Cloud | 2020 |
96P/Machholz | 0.959 | 5.2 | Kuiper Belt | 2023 |
C/2023 A3 (Tsuchinshan-ATLAS) | 1.0008 | Non-periodic | Oort Cloud | 2024 (expected) |
Source: NASA JPL Small-Body Database | NASA ADS - Astrophysics Data System
Comets are celestial bodies composed of a heterogeneous mixture of volatile ices (H2O, CO, CO2, CH3OH…), mineral dust (amorphous or crystalline silicates), complex organic compounds, and metallic grains. Their internal structure is likened to that of a porous aggregate, described as a "cosmic sandcastle."
The Rosetta mission revealed that the nucleus of comet 67P/Churyumov–Gerasimenko is not monolithic but consists of two distinct lobes, likely resulting from the low-velocity accretion of two objects. Analysis of the geological layers on the surface suggests stratification in shells or filaments, indicative of a primitive accumulation process in the protoplanetary disk.
The average density measured by Rosetta for 67P is about 0.53 g/cm³, just half that of compact water ice, indicating an internal porosity greater than 70%. This low density is strong evidence of the loosely compacted nature of the nucleus, inconsistent with significant thermal fusion or annealing.
Gravimetric observations and radar imagery from the probe have revealed local variations in density, likely correlated with the distribution of volatile materials or internal fracturing. No large cavities were detected, confirming the hypothesis of microscopic rather than macroscopic porosity.
The behavior of a comet is strongly governed by its orbital eccentricity and its distance from the Sun. As it approaches perihelion, the rapid increase in temperature induces the sublimation of surface ices, generating internal pressure that can cause gas jets, collapses, or fractures.
The Deep Impact and Rosetta missions have highlighted asymmetric activity between the sunlit hemisphere and the hemisphere plunged into cometary night. These thermal effects are amplified by the low thermal inertia of the cometary regolith. The rotation of the nucleus, sometimes chaotic, can generate cycles of mechanical stress that promote fragmentation.
Recent physical models attempt to link topography, orbital evolution, and long-term outgassing to a dynamic of progressive erosion, which leads comets to lose their activity and become inert objects (extinct asteroids or dormant comets).
The close passage of a comet is a spectacular but potentially dangerous event. Although comet impacts are rare compared to asteroid impacts, their very high relative velocity (up to 70 km/s) gives them destructive kinetic energy. The hypothetical impact of cometary fragments is considered in some extinction scenarios.
Comets, formed in the cold regions of the outer Solar System, contain ices, silicates, and a rich organic chemistry. These small bodies have preserved intact prebiotic molecules dating back to the protosolar nebula, making them valuable witnesses to the early stages of cosmic chemistry.
Analysis of the dust collected by the Stardust mission on comet 81P/Wild 2 revealed the presence of many organic compounds, including methanol (CH3OH), formaldehyde (H2CO), formic acid (HCOOH), and polycyclic aromatic hydrocarbons (PAHs). These molecules are possible precursors to simple amino acids.
Spectrometric analyses of carbonaceous meteorites (such as Murchison) have detected amino acids (glycine, alanine, isovaline...), which has strengthened the hypothesis that these molecules can be of cometary or asteroidal origin. In 2009, NASA confirmed the presence of glycine in Stardust particles, after purification and exclusion of any terrestrial contamination.
The Rosetta mission, using the COSAC spectrometer on board the Philae lander, identified several organic compounds on comet 67P/Churyumov–Gerasimenko. Among them: glycine (NH2CH2COOH), phosphorus (a key element of DNA), as well as multiple amines and nitriles, suggesting complex organic chemistry already in place in the early days of the Solar System.
These discoveries strengthen the hypothesis of chemical panspermia, according to which elementary building blocks of life (but not life itself) could have been brought to Earth by comets during the late heavy bombardment (around 3.8 billion years ago). Comets would thus have played a role in enriching the terrestrial prebiotic environment with organic compounds.
However, the temperature and pressure conditions during a cometary impact still raise the question of the stability of these molecules upon atmospheric entry. Laboratory experiments (e.g., the STONE or ESA COMET project) tend to show that some amino acids can survive these extreme conditions, provided they are buried in a protective mineral matrix.
Molecule | Chemical Formula | Detection Location | Identification Method |
---|---|---|---|
Glycine | NH2CH2COOH | Comet 81P/Wild 2 (Stardust) | GC-MS after hydrolysis and purification |
Formic Acid | HCOOH | Comet Hale-Bopp | IRAM Radio Spectroscopy |
Formaldehyde | H2CO | Comet 67P (Rosetta/ROSINA) | Mass Spectrometry (ROSINA-DFMS) |
Hydrogen Cyanide (HCN) | HCN | Comet Halley (Giotto) | UV and Radio Spectroscopy |
Polycyclic Aromatic Hydrocarbons (PAHs) | CnHm (variable) | Comet 81P/Wild 2 (Stardust) | UV Fluorescence, Chromatography |
Methanol | CH3OH | Comet 67P (ROSINA) | Mass Spectrometry |
Urea | CH4N2O | Comet 67P (Philae-COSAC) | In situ Analysis by Chromatography |
Ethanol | C2H5OH | Comet 67P (ROSINA) | Mass Spectrometry |
Acetone | CH3COCH3 | Comet 67P (ROSINA) | Mass Spectrometry |
Phosphorus | P | Comet 67P (ROSINA) | High-Resolution Mass Spectrometry |
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