Where is it now
- Distance from Sun
- 3.885 AU
- True anomaly
- 192.94°
- Distance from Earth
- 3.381 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
- 05h 39m 18s
- Declination
- +16° 02′ 24″
- Constellation
- Taurus
- Distance from Earth
- 3.37 AU
- Elongation from the Sun
- 113.85° — well clear of the Sun
Favours the northern hemisphere; low or below the horizon from far south.
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
- 2.436 AU
- Eccentricity
- 0.6808
- Inclination
- 8.74°
- Orbital period
- 3.8 years
- Perihelion
- 0.778 AU
- Aphelion
- 4.095 AU
- Longitude of ascending node
- 205.01°
- Argument of periapsis
- 33.67°
- Epoch · J2000
- 2461200.5
- Orbit class · APO
- Apollo
- Earth MOID · 27.0 LD
- 0.0695 AU
- Tisserand (Jupiter)
- 3.126
Orbit quality
Orbit very well determined (uncertainty code 0).
- Observations used
- 3,476
- Data arc
- 35.32 years
- First observed
- 16 September 1990
- Last observed
- 9 January 2026
- Residual RMS
- 0.37 ″
- Solution · Otto Matic
- 10 January 2026
Physical properties
- Rotation period
- 2.62 hours
Visual & observation
- Absolute magnitude (H)
- 14.73
Discovery & classification
- Discovered by
- Spacewatch
- Discovery date
- 14 October 1990
- Discovery site
- Kitt Peak
Also known as 1990 TG1 · 2000 YP29
Close approaches 19 on record
Top-down view of the ecliptic, Earth at the centre, for the 2066-07-02 09:50 UTC close approach of 30825. Catalogue miss distance 72.4 LD · 2.78 × 10⁷ km. The curve is the geocentric path from 2066-06-29 to 2066-07-05, 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 a geocentric ecliptic ephemeris from JPL Horizons. The inset is a heliocentric view and is approximate.
| When (UTC) | Body | Distance | Lunar distances | Relative speed |
|---|---|---|---|---|
| 2035-10-08 14:14:00 | Venus | 0.0697 AU | 27.1 LD | 11.4 km/s |
| 2060-02-14 04:25:00 | Juptr | 1.7356 AU | 675.5 LD | 8.7 km/s |
| 2066-07-02 09:50:00 | Earth | 0.1859 AU | 72.4 LD | 13.2 km/s |
| 2071-11-09 04:10:00 | Juptr | 1.2494 AU | 486.2 LD | 6.7 km/s |
| 2083-09-06 06:41:00 | Juptr | 1.0489 AU | 408.2 LD | 5.8 km/s |
| 2095-07-22 08:28:00 | Juptr | 1.0154 AU | 395.2 LD | 5.6 km/s |
| 2107-06-19 05:39:00 | Juptr | 1.0976 AU | 427.2 LD | 5.9 km/s |
| 2119-06-04 05:49:00 | Juptr | 1.4364 AU | 559.0 LD | 7.2 km/s |
| 2146-05-29 15:34:00 | Earth | 0.1133 AU | 44.1 LD | 9.9 km/s |
| 2183-04-09 13:12:00 | Earth | 0.1021 AU | 39.7 LD | 14.5 km/s |
Next ten from today. 1 lunar distance = 384,400 km. Source: JPL close-approach data.
Sources
- visual properties: JPL SBDB (lookup)
- physical properties: JPL SBDB (lookup)
- orbital elements: JPL SBDB