| Epoch (TDB) | 2025-11-21 (JD 2461000.5) |
|---|---|
| Eccentricity (e) | 0.2904428000 |
| Semi-major axis (a) | 1.4011476000 AU |
| Inclination (i) | 12.43835000° |
| Long. of Asc. Node (Ω) | 2.08209000° |
| Arg. of Perihelion (ω) | 149.83103000° |
| Mean Anomaly (M) | 240.05142000° |
| Mean Motion (n) | 0.5942624000°/day |
| Perihelion dist (q) | 0.99419440 AU |
| Aphelion dist (Q) | 1.80810080 AU |
| Orbital Period | 1.65853950 yr |
| H (abs. magnitude) | 26.20 |
|---|---|
| G (slope) | 0.15 |
| Source | MPC |
|---|---|
| Solution Date | — |
| RMS Residual | 0.420″ |
| Uncertainty | 7 |
| Orbit Type | Apollo |
| MOID | 0.026229 AU |
| Observations Used | 16 |
| Oppositions | 1 |
| Arc Total | — |
| First Observation Used | — |
| Last Observation Used | 2018-03-22 |
| Date | Type | RA | Dec | Mag | Band | Observatory |
|---|---|---|---|---|---|---|
| 2018-03-20 10:57:52 | C | 14 32 27.43 | -04 45 59.9 | – | U | G96 |
| 2018-03-20 11:08:47 | C | 14 32 22.87 | -04 49 14.8 | – | U | G96 |
| 2018-03-20 11:23:31 | C | 14 32 16.92 | -04 53 33.3 | – | U | G96 |
| 2018-03-20 12:10:02 | C | 14 31 58.20 | -05 07 09.2 | – | U | I52 |
| 2018-03-20 12:10:50 | C | 14 31 57.85 | -05 07 25.5 | – | U | I52 |
| 2018-03-20 12:12:25 | C | 14 31 57.16 | -05 07 52.2 | – | U | I52 |
| 2018-03-21 11:47:11 | C | 14 24 00.99 | -11 44 24.8 | – | U | G96 |
| 2018-03-21 11:47:45 | C | 14 24 00.75 | -11 44 35.1 | – | U | G96 |
| 2018-03-21 11:48:21 | C | 14 24 00.49 | -11 44 43.8 | – | U | G96 |
| 2018-03-21 11:48:55 | C | 14 24 00.31 | -11 44 52.5 | – | U | G96 |
| 2018-03-22 07:23:08 | C | 14 17 46.03 | -16 40 29.6 | – | U | 807 |
| 2018-03-22 07:30:44 | C | 14 17 43.18 | -16 42 20.0 | – | U | 807 |
| 2018-03-22 07:38:06 | C | 14 17 40.40 | -16 44 07.0 | – | U | 807 |
| 2018-03-22 10:13:42 | C | 14 16 50.58 | -17 25 29.5 | – | U | H01 |
| 2018-03-22 10:25:54 | C | 14 16 46.02 | -17 28 23.9 | – | U | H01 |
| 2018-03-22 10:33:36 | C | 14 16 43.17 | -17 30 13.6 | – | U | H01 |
| 2018-03-22 10:43:33 | C | 14 16 39.45 | -17 32 35.1 | – | U | H01 |