614134
Add to an observing list or journal →614134 (2008 TC4)
Where is it now
- Distance from Sun
- 0.908 AU
- True anomaly
- 223.1°
- Distance from Earth
- 0.288 AU
- As of
- 16 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
- 09h 25m 49s
- Declination
- +10° 21′ 58″
- Constellation
- Leo
- Distance from Earth
- 0.29 AU
- Elongation from the Sun
- 63.33° — well clear of the Sun
Visible from both hemispheres.
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
- 0.78 AU
- Eccentricity
- 0.5544
- Inclination
- 10.65°
- Orbital period
- 251.8 days
- Perihelion
- 0.348 AU
- Aphelion
- 1.213 AU
- Longitude of ascending node
- 212.53°
- Argument of periapsis
- 324.36°
- Epoch · J2000
- 2461200.5
- Orbit class · ATE
- Aten
- Earth MOID · 1.4 LD
- 0.0035 AU
- Tisserand (Jupiter)
- 7.301
Orbit quality
Orbit very well determined (uncertainty code 0).
- Observations used
- 180
- Data arc
- 12.94 years
- First observed
- 6 October 2008
- Last observed
- 14 September 2021
- Residual RMS
- 0.49 ″
- Solution · Otto Matic
- 20 December 2022
Visual & observation
- Absolute magnitude (H)
- 21.65
Discovery & classification
- Discovered by
- LINEAR
- Discovery date
- 7 October 2008
- Discovery site
- Socorro
Also known as 2008 TC4
Close approaches 299 on record
Top-down view of the ecliptic, Earth at the centre, for the 2026-10-17 04:02 UTC close approach of 614134. Catalogue miss distance 118.5 LD · 4.56 × 10⁷ km. The curve is the geocentric path from 2026-10-14 to 2026-10-20, 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. 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 |
|---|---|---|---|---|
| 2026-10-17 04:02:00 | Earth | 0.3045 AU | 118.5 LD | 25 km/s |
| 2026-12-22 09:23:00 | Merc | 0.0909 AU | 35.4 LD | 29.6 km/s |
| 2026-12-22 09:23:00 | Mercury | 0.0909 AU | 35.4 LD | 29.6 km/s |
| 2027-08-15 23:38:00 | Merc | 0.099 AU | 38.5 LD | 25.6 km/s |
| 2027-08-15 23:38:00 | Mercury | 0.099 AU | 38.5 LD | 25.6 km/s |
| 2028-10-23 12:37:00 | Earth | 0.0701 AU | 27.3 LD | 13.6 km/s |
| 2030-09-17 11:53:00 | Earth | 0.2421 AU | 94.2 LD | 12.1 km/s |
| 2032-06-17 21:00:00 | Merc | 0.0722 AU | 28.1 LD | 22.6 km/s |
| 2032-06-17 21:00:00 | Mercury | 0.0722 AU | 28.1 LD | 22.6 km/s |
| 2032-08-17 19:32:00 | Earth | 0.1799 AU | 70.0 LD | 16.1 km/s |
Next ten from today. 1 lunar distance = 384,400 km. Source: JPL close-approach data.
Sources
- visual properties: JPL SBDB (lookup)
- orbital elements: JPL SBDB