2023 JL1 is an asteroid in the Apollo orbit class. Its orbit takes it from 0.84 AU to 1.19 AU from the Sun; one orbit takes 373.7 days. Orbit from the JPL solution of 13 May 2023.
Where is it now
- Distance from Sun
- 0.953 AU
- True anomaly
- 78.69°
- Distance from Earth
- 0.202 AU
- As of
- 3 November 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
- 10h 04m 41s
- Declination
- +14° 26′ 51″
- Constellation
- Leo
- Distance from Earth
- 0.2 AU
- Elongation from the Sun
- 73.64° — 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
- 1.015 AU
- Eccentricity
- 0.1714
- Inclination
- 10.18°
- Orbital period
- 373.7 days
- Perihelion
- 0.841 AU
- Aphelion
- 1.189 AU
- Longitude of ascending node
- 50.55°
- Argument of periapsis
- 283.83°
- Epoch · J2000
- 2461200.5
- Orbit class · APO
- Apollo
- Earth MOID · 4.8 LD
- 0.0122 AU
- Tisserand (Jupiter)
- 5.981
Orbit quality
Orbit poorly determined (uncertainty code 6).
- Observations used
- 31
- Data arc
- 2 days
- First observed
- 11 May 2023
- Last observed
- 13 May 2023
- Residual RMS
- 0.27 ″
- Solution · Otto Matic
- 13 May 2023
Visual & observation
- Absolute magnitude (H)
- 27.29
Discovery & classification
Close approaches 39 on record
Top-down view of the ecliptic, Earth at the centre, for the 2027-11-12 15:56 UTC close approach of 2023 JL1. Catalogue miss distance 32.7 LD · 1.26 × 10⁷ km. The curve is the geocentric path from 2027-11-09 to 2027-11-15, 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 |
|---|---|---|---|---|
| 2027-11-12 15:56:00 | Earth | 0.0839 AU | 32.7 LD | 6.3 km/s |
| 2028-11-23 20:47:00 | Earth | 0.0687 AU | 26.7 LD | 9.1 km/s |
| 2029-12-01 22:09:00 | Earth | 0.2106 AU | 81.9 LD | 12.9 km/s |
| 2030-12-09 04:54:00 | Earth | 0.3565 AU | 138.7 LD | 17.1 km/s |
| 2064-04-29 13:58:00 | Earth | 0.4004 AU | 155.8 LD | 18.1 km/s |
| 2065-05-05 14:46:00 | Earth | 0.2588 AU | 100.7 LD | 14.1 km/s |
| 2066-05-11 03:00:00 | Earth | 0.1168 AU | 45.4 LD | 10.3 km/s |
| 2067-05-15 04:31:00 | Earth | 0.0265 AU | 10.3 LD | 7 km/s |
| 2068-04-30 09:03:00 | Earth | 0.171 AU | 66.5 LD | 5.4 km/s |
| 2069-03-16 09:15:00 | Earth | 0.2598 AU | 101.1 LD | 5.5 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