Where is it now
- Distance from Sun
- 0.988 AU
- True anomaly
- 109.41°
- Distance from Earth
- 1.194 AU
- As of
- 22 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
- 11h 26m 32s
- Declination
- +27° 44′ 21″
- Constellation
- Leo
- Distance from Earth
- 1.2 AU
- Elongation from the Sun
- 52.76° — near the Sun — look low at dusk or dawn
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
- 0.961 AU
- Eccentricity
- 0.1374
- Inclination
- 30.02°
- Orbital period
- 344.1 days
- Perihelion
- 0.829 AU
- Aphelion
- 1.093 AU
- Longitude of ascending node
- 344.05°
- Argument of periapsis
- 4.68°
- Epoch · J2000
- 2461200.5
- Orbit class · ATE
- Aten
- Earth MOID · 39.3 LD
- 0.1009 AU
- Tisserand (Jupiter)
- 6.152
Orbit quality
Orbit very well determined (uncertainty code 0).
- Observations used
- 772
- Data arc
- 17.88 years
- First observed
- 2 February 2008
- Last observed
- 19 December 2025
- Residual RMS
- 0.35 ″
- Solution · Otto Matic
- 3 September 2026
Physical properties
- Rotation period
- 2.62 hours
Visual & observation
- Absolute magnitude (H)
- 19.45
Discovery & classification
- Discovered by
- LINEAR
- Discovery date
- 2 February 2008
- Discovery site
- Socorro
Also known as 2008 CL1
Close approaches 46 on record
Top-down view of the ecliptic, Earth at the centre, for the 2040-03-01 19:58 UTC close approach of 776617. Catalogue miss distance 73.7 LD · 2.83 × 10⁷ km. The curve is the geocentric path from 2040-02-27 to 2040-03-04, 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 |
|---|---|---|---|---|
| 2035-12-14 11:59:00 | Venus | 0.1204 AU | 46.9 LD | 18.3 km/s |
| 2040-03-01 19:58:00 | Earth | 0.1893 AU | 73.7 LD | 15.7 km/s |
| 2040-09-06 11:59:00 | Earth | 0.1784 AU | 69.4 LD | 17.5 km/s |
| 2041-03-07 08:46:00 | Earth | 0.1726 AU | 67.2 LD | 15.5 km/s |
| 2050-02-06 00:46:00 | Venus | 0.1171 AU | 45.6 LD | 18.4 km/s |
| 2056-09-15 04:46:00 | Earth | 0.1962 AU | 76.4 LD | 17.6 km/s |
| 2057-03-05 22:06:00 | Earth | 0.1156 AU | 45.0 LD | 15.1 km/s |
| 2066-02-04 20:51:00 | Venus | 0.1326 AU | 51.6 LD | 18.4 km/s |
| 2073-03-04 13:53:00 | Earth | 0.1031 AU | 40.1 LD | 15.1 km/s |
| 2080-03-30 09:05:00 | Venus | 0.1112 AU | 43.3 LD | 18.4 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