2014 WT202
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Where is it now
- Distance from Sun
- 0.909 AU
- True anomaly
- 21.75°
- Distance from Earth
- 1.691 AU
- As of
- 23 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
- 15h 31m 49s
- Declination
- -25° 07′ 43″
- Constellation
- Libra
- Distance from Earth
- 1.69 AU
- Elongation from the Sun
- 26.08° — near the Sun — look low at dusk or dawn
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
- 0.966 AU
- Eccentricity
- 0.0631
- Inclination
- 23.39°
- Orbital period
- 346.6 days
- Perihelion
- 0.905 AU
- Aphelion
- 1.027 AU
- Longitude of ascending node
- 58.8°
- Argument of periapsis
- 185.72°
- Epoch · J2000
- 2461200.5
- Orbit class · ATE
- Aten
- Earth MOID · 14.7 LD
- 0.0378 AU
- Tisserand (Jupiter)
- 6.178
Orbit quality
Orbit very well determined (uncertainty code 2).
- Observations used
- 91
- Data arc
- 360 days
- First observed
- 23 November 2014
- Last observed
- 18 November 2015
- Residual RMS
- 0.46 ″
- Solution · Otto Matic
- 15 April 2021
Visual & observation
- Absolute magnitude (H)
- 21.1
Discovery & classification
Close approaches 113 on record
Top-down view of the ecliptic, Earth at the centre, for the 2031-11-21 16:28 UTC close approach of 2014 WT202. Catalogue miss distance 159.9 LD · 6.15 × 10⁷ km. The curve is the geocentric path from 2031-11-18 to 2031-11-24, 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 south 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 |
|---|---|---|---|---|
| 2031-11-21 16:28:00 | Earth | 0.4109 AU | 159.9 LD | 17.5 km/s |
| 2032-06-21 01:54:00 | Earth | 0.3313 AU | 128.9 LD | 14.9 km/s |
| 2032-11-20 10:20:00 | Earth | 0.1168 AU | 45.5 LD | 12.6 km/s |
| 2033-05-22 00:27:00 | Earth | 0.1102 AU | 42.9 LD | 12.8 km/s |
| 2033-11-21 22:06:00 | Earth | 0.1904 AU | 74.1 LD | 13 km/s |
| 2034-04-24 11:32:00 | Earth | 0.2798 AU | 108.9 LD | 14.9 km/s |
| 2034-11-23 06:37:00 | Earth | 0.4826 AU | 187.8 LD | 18.2 km/s |
| 2050-07-16 13:31:00 | Earth | 0.4966 AU | 193.3 LD | 16.9 km/s |
| 2050-11-20 23:27:00 | Earth | 0.3014 AU | 117.3 LD | 15.3 km/s |
| 2051-06-09 23:57:00 | Earth | 0.2352 AU | 91.5 LD | 13.8 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