Where is it now
- Distance from Sun
- 0.761 AU
- True anomaly
- 123.43°
- Distance from Earth
- 1.039 AU
- As of
- 15 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 25m 10s
- Declination
- -18° 03′ 12″
- Constellation
- Ophiuchus
- Distance from Earth
- 1.04 AU
- Elongation from the Sun
- 44.3° — 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
- 0.713 AU
- Eccentricity
- 0.4335
- Inclination
- 6.88°
- Orbital period
- 220 days
- Perihelion
- 0.404 AU
- Aphelion
- 1.022 AU
- Longitude of ascending node
- 176.81°
- Argument of periapsis
- 11.02°
- Epoch · J2000
- 2461200.5
- Orbit class · ATE
- Aten
- Earth MOID · 0.7 LD
- 0.0018 AU
- Tisserand (Jupiter)
- 7.959
Orbit quality
Orbit poorly determined (uncertainty code 6).
- Observations used
- 22
- Data arc
- 27 days
- First observed
- 20 September 2025
- Last observed
- 17 October 2025
- Residual RMS
- 0.43 ″
- Solution · Otto Matic
- 5 November 2025
Visual & observation
- Absolute magnitude (H)
- 26.35
Discovery & classification
Listed by JPL impact monitoring; see the Sentry table for current probabilities.
Close approaches 96 on record
Top-down view of the ecliptic, Earth at the centre, for the 2028-09-14 01:51 UTC close approach of 2025 SQ4. Catalogue miss distance 13.5 LD · 5.17 × 10⁶ km. The curve is the geocentric path from 2028-09-11 to 2028-09-17, 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 |
|---|---|---|---|---|
| 2028-09-14 01:51:00 | Earth | 0.0346 AU | 13.5 LD | 9.7 km/s |
| 2031-08-05 09:03:00 | Venus | 0.1181 AU | 46.0 LD | 18.4 km/s |
| 2031-09-12 04:40:00 | Earth | 0.0992 AU | 38.6 LD | 11.9 km/s |
| 2032-03-14 20:37:00 | Venus | 0.1033 AU | 40.2 LD | 14.2 km/s |
| 2032-09-08 17:35:00 | Merc | 0.0932 AU | 36.3 LD | 25.1 km/s |
| 2032-09-08 17:35:00 | Mercury | 0.0932 AU | 36.3 LD | 25.1 km/s |
| 2032-10-27 01:18:00 | Venus | 0.1479 AU | 57.6 LD | 10.8 km/s |
| 2033-11-23 05:28:00 | Merc | 0.0764 AU | 29.7 LD | 23.3 km/s |
| 2033-11-23 05:28:00 | Mercury | 0.0764 AU | 29.7 LD | 23.3 km/s |
| 2034-09-12 07:56:00 | Earth | 0.1772 AU | 68.9 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)
- orbital elements: JPL SBDB