Where is it now
- Distance from Sun
- 24.195 AU
- True anomaly
- 187.14°
- Distance from Earth
- 25.163 AU
- As of
- 11 October 2026
Two-body Kepler propagation — accurate to ~0.1% for major planets over decades, less so for highly-perturbed bodies. Use JPL Horizons for high precision.
In the sky
- Right ascension
- 12h 38m 48s
- Declination
- -19° 07′ 04″
- Constellation
- Corvus
- Distance from Earth
- 25.16 AU
- Elongation from the Sun
- 13.94° — too close to the Sun to observe
Favours the southern hemisphere; low or below the horizon from far north.
From your location
See how high it is right now, whether it is up after civil twilight, and when it rises and sets where you are.
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Two-body approximation, good to about a degree for the planets — enough to find the constellation and know whether it is up.
Orbital elements
- Semi-major axis
- 13.813 AU
- Eccentricity
- 0.9289
- Inclination
- 19.19°
- Orbital period
- 51.34 years
- Perihelion
- 0.983 AU
- Aphelion
- 26.643 AU
- Longitude of ascending node
- 329.43°
- Argument of periapsis
- 41.48°
- Epoch · J2000
- 2448619.5
- Orbit class · HTC
- Halley-type comet
- Earth MOID · 29.3 LD
- 0.0753 AU
- Tisserand (Jupiter)
- 1.517
Orbit quality
Orbit reasonably well determined (uncertainty code 3).
- Observations used
- 136
- Data arc
- 587 days
- First observed
- 14 June 1991
- Last observed
- 21 January 1993
- Residual RMS
- 0.74 ″
- Solution · Otto Matic
- 15 April 2021
Physical properties
- Mean radius
- 5.80 km
Visual & observation
- Absolute magnitude (H)
- 8.9
- Total magnitude M₁ · K₁ 14.5
- 8.9
Discovery & classification
Also known as 1991 L3 · C/1991 L3 · 1991 XI · 1991q
Close approaches 3 on record
Top-down view of the ecliptic, Earth at the centre, for the 2042-11-21 11:56 UTC close approach of Levy. Catalogue miss distance 182.8 LD · 7.03 × 10⁷ km. The curve is the geocentric path from 2042-11-18 to 2042-11-24, with a mark at UTC midnights and an arrow for the direction of motion. The circle is the Moon’s mean orbit; the Moon is plotted at closest approach. A ray shows the Sun’s direction. The labelled distance is the full separation. The drawn radius is the part that lies in the ecliptic plane. At closest approach the object is north of the ecliptic. The path is approximate: a two-body Kepler propagation of the catalogue orbital elements, not a numerical integration. The Moon’s position is approximate. The inset is a heliocentric view and is approximate.
| When (UTC) | Body | Distance | Lunar distances | Relative speed |
|---|---|---|---|---|
| 2042-11-21 11:56:00 | Earth | 0.4697 AU | 182.8 LD | 22.5 km/s |
| 2094-08-03 00:02:00 | Earth | 0.4441 AU | 172.8 LD | 28.2 km/s |
| 2097-03-04 18:51:00 | Satrn | 1.4197 AU | 552.5 LD | 12.8 km/s |
Next ten from today. 1 lunar distance = 384,400 km. Source: JPL close-approach data.
Sources
- visual properties: JPL SBDB (lookup)
- visual properties: JPL SBDB (lookup)
- visual properties: JPL SBDB (lookup)
- visual properties: JPL SBDB (lookup)
- physical properties: JPL SBDB (lookup)
- orbital elements: JPL SBDB