Unlike ʻOumuamua, which had an
asteroidal appearance, 2I/Borisov's nucleus was surrounded by a
coma, a cloud of dust and gas.) in November 2019
Size and shape Early estimates of nucleus 2I/Borisov diameter have ranged from . 2I/Borisov has, unlike Solar System comets, noticeably shrunk during Solar System flyby, losing at least 0.4% of its mass before
perihelion. Also, the amplitude of non-gravitational acceleration places an upper limit of 0.4 km on nucleus size, consistent with a previous
Hubble Space Telescope upper limit of 0.5 km. A study with
CSA's
NEOSSat found a period of 13.2 ± 0.2 days, which is unlikely to be the nuclear spin.
Monte Carlo simulations based on the available orbit determinations suggest that the equatorial obliquity of 2I/Borisov could be about 59 degrees or 90 degrees; the latter is favored for the latest orbit determination.
Chemical makeup and nucleus structure David Jewitt and
Jane Luu estimate from the size of its coma the comet is producing 2 kg/s of dust and is losing 60 kg/s of water. They extrapolate that it became active in June 2019 when it was between 4 and 5 AU from the Sun. 2I/Borisov's composition appears uncommon yet not unseen in Solar System comets, being relatively depleted in water and
diatomic carbon (C2), but enriched in
carbon monoxide and
amines (R-NH2). The molar ratio of carbon monoxide to water in 2I/Borisov tail is 35–105%, resembling the unusual blue-tailed comet
C/2016 R2 (PanSTARRS) in contrast to the average ratio of 4% for Solar System comets. 2I/Borisov has also produced a minor amount of neutral nickel emission attributed to an unknown volatile compound of nickel. The nickel to iron abundance ratio is similar to Solar System comets.
Trajectory As seen from Earth, the comet was in the northern sky from September until mid-November. It crossed the ecliptic plane on 26 October near the star
Regulus, and the
celestial equator on 13 November 2019, entering the southern sky. On 8 December 2019, the comet reached
perihelion (closest approach to the Sun) and was near the inner edge of the asteroid belt. In late December, it made its closest approach to Earth, 1.9 AU, and had a solar elongation of about 80°. Due to its 44°
orbital inclination, 2I/Borisov did not make any notable close approaches to the planets. 2I/Borisov entered the Solar System from the direction of
Cassiopeia near the border with
Perseus. This direction indicates that it originates from the
galactic plane, rather than from the
galactic halo. It will leave the Solar System in the direction of
Telescopium. In interstellar space, 2I/Borisov takes roughly years to travel a
light-year relative to the Sun. 2I/Borisov's trajectory is extremely
hyperbolic, having an
orbital eccentricity of 3.36. This is much higher than the 300-plus known weakly
hyperbolic comets, with heliocentric eccentricities just over 1, and even ʻOumuamua with an eccentricity of 1.2. 2I/Borisov also has a
hyperbolic excess velocity (v_\infty) of , much higher than what could be explained by perturbations, which could produce velocities when approaching an infinite distance from the Sun of less than a few km/s. These two parameters are important indicators of 2I/Borisov's interstellar origin. For comparison, the
Voyager 1 spacecraft, which is leaving the Solar System, is traveling at . 2I/Borisov has a much larger eccentricity than ʻOumuamua due to its higher excess velocity and its significantly higher perihelion distance. At this larger distance, the Sun's gravity is less able to alter its path as it passes through the Solar System. == Observation ==