Where is it now
- Distance from Sun
- 0.911 AU
- True anomaly
- 265.21°
- Distance from Earth
- 1.532 AU
- As of
- 21 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
- 16h 03m 10s
- Declination
- -24° 06′ 38″
- Constellation
- Scorpius
- Distance from Earth
- 1.53 AU
- Elongation from the Sun
- 34.68° — 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
- 0.923 AU
- Eccentricity
- 0.1643
- Inclination
- 8.11°
- Orbital period
- 323.9 days
- Perihelion
- 0.771 AU
- Aphelion
- 1.075 AU
- Longitude of ascending node
- 58.74°
- Argument of periapsis
- 317.73°
- Epoch · J2000
- 2461200.5
- Orbit class · ATE
- Aten
- Earth MOID · 3.0 LD
- 0.0077 AU
- Tisserand (Jupiter)
- 6.46
Orbit quality
Orbit reasonably well determined (uncertainty code 5).
- Observations used
- 111
- Data arc
- 2 days
- First observed
- 18 May 2013
- Last observed
- 20 May 2013
- Residual RMS
- 0.26 ″
- Solution · Otto Matic
- 20 August 2026
Visual & observation
- Absolute magnitude (H)
- 26.6
Discovery & classification
Close approaches 39 on record
Top-down view of the ecliptic, Earth at the centre, for the 2036-01-28 16:14 UTC close approach of 2013 KT1. Catalogue miss distance 58.4 LD · 2.25 × 10⁷ km. The curve is the geocentric path from 2036-01-25 to 2036-01-31, 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 |
|---|---|---|---|---|
| 2032-05-14 02:31:00 | Venus | 0.108 AU | 42.0 LD | 3.4 km/s |
| 2036-01-28 16:14:00 | Earth | 0.1502 AU | 58.4 LD | 7.2 km/s |
| 2044-01-06 01:50:00 | Earth | 0.1328 AU | 51.7 LD | 5.4 km/s |
| 2051-12-10 08:54:00 | Earth | 0.1632 AU | 63.5 LD | 6.2 km/s |
| 2052-04-28 17:09:00 | Earth | 0.1059 AU | 41.2 LD | 4.8 km/s |
| 2054-06-27 11:51:00 | Venus | 0.0944 AU | 36.8 LD | 5.3 km/s |
| 2059-11-25 20:51:00 | Earth | 0.1845 AU | 71.8 LD | 6.8 km/s |
| 2060-05-15 02:06:00 | Earth | 0.0586 AU | 22.8 LD | 5 km/s |
| 2062-06-26 17:28:00 | Venus | 0.0692 AU | 26.9 LD | 4.3 km/s |
| 2067-11-27 18:23:00 | Earth | 0.1805 AU | 70.2 LD | 6.7 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