| Epoch (TDB) | 2025-11-21 (JD 2461000.5) |
|---|---|
| Eccentricity (e) | 0.6415543673 ± 9.37e-04 |
| Semi-major axis (a) | 2.1629683747 AU ± 5.02e-03 |
| Inclination (i) | 6.36935519° ± 7.20e-03 |
| Long. of Asc. Node (Ω) | 196.94571726° ± 1.26e-03 |
| Arg. of Perihelion (ω) | 115.06628504° ± 4.63e-03 |
| Mean Anomaly (M) | 25.92915328° ± 9.64e-02 |
| Mean Motion (n) | 0.3098396703°/day ± 1.08e-03 |
| Perihelion dist (q) | 0.77530657 AU ± 2.71e-03 |
| Aphelion dist (Q) | 3.55063018 AU ± 8.48e-03 |
| Orbital Period | 3.18108486 yr ± 1.11e-02 |
| H (abs. magnitude) | 27.89 |
|---|---|
| G (slope) | 0.15 |
| Source | IAA |
|---|---|
| Solution Date | 2026-06-03 |
| RMS Residual | 0.270″ |
| Uncertainty | 2 |
| Orbit Type | Apollo |
| MOID | 0.000118 AU |
| Observations Used | 15 |
| Oppositions | 1 |
| Arc Total | 2025-2025 |
| First Observation Used | 2025-10-12 |
| Last Observation Used | 2025-10-14 |
| Date | Type | RA | Dec | Mag | Band | Observatory |
|---|---|---|---|---|---|---|
| 2025-10-12 11:00:35 | C | 01 58 40.580 | -00 22 00.41 | – | X | F51 |
| 2025-10-12 11:16:42 | C | 01 58 41.565 | -00 22 07.60 | – | X | F51 |
| 2025-10-12 11:32:49 | C | 01 58 42.549 | -00 22 14.61 | – | X | F51 |
| 2025-10-12 11:48:52 | C | 01 58 43.534 | -00 22 21.60 | – | X | F51 |
| 2025-10-12 20:29:14 | B | 02 00 17.871 | -00 21 20.54 | – | W | M21 |
| 2025-10-12 20:32:58 | C | 02 00 15.26 | -00 27 36.3 | – | V | L01 |
| 2025-10-12 20:38:27 | C | 02 00 15.65 | -00 27 38.3 | – | V | L01 |
| 2025-10-12 20:43:56 | C | 02 00 16.01 | -00 27 40.3 | – | V | L01 |
| 2025-10-12 21:00:36 | B | 02 00 19.486 | -00 21 32.50 | – | W | M21 |
| 2025-10-12 21:41:09 | B | 02 00 22.82 | -00 27 53.1 | – | V | I93 |
| 2025-10-12 21:50:33 | B | 02 00 23.46 | -00 27 55.5 | – | V | I93 |
| 2025-10-12 21:59:28 | B | 02 00 24.03 | -00 27 58.6 | – | V | I93 |
| 2025-10-14 04:12:46 | C | 02 02 41.640 | -00 28 55.80 | – | V | 807 |
| 2025-10-14 04:28:40 | C | 02 02 41.590 | -00 28 57.70 | – | V | 807 |
| 2025-10-14 04:44:35 | C | 02 02 41.520 | -00 28 59.90 | – | V | 807 |