2025-09-17 / UCAC4 350-130209 / (2184) Fujian
| # | OBS | Observer | Occ | Meth. | Instr. | CC |
TSRC | UT1 | UT2 | UT3 | UT4 | UT2E | UT3E | Dur. | Chrd |
| 1 |
show |
Tomas Janik |
O+ |
CCD |
T600 |
CZ |
GPS |
19:44:56 |
19:45:18.0 |
19:45:20.4 |
19:45:58 |
0.300 |
0.300 |
2.40 |
27.1 |
UT1/UT4: Begin/End of observation | UT2/UT3: Begin/End of occultation | Dur: Reported duration in seconds | Chrd: Corresponding chord length in km |
More
1 observation found in db: sodis
Available (probably) matching predictions (click on the link to switch):
Sky projection (artificial light) for occ. time: 2025-09-17, 19:45 UT (JD = 2460936.323)
| DAMIT | Q | P (h) | λ, β | JD0 | JD-JD0 | φ0 | Version | Modified | Vol-equiv D | Cmnt |
| # 4835 | 1.0 | 7.458 |
244°, 45° |
2.457319e6 | 3617.3 | 0.0° |
None | 2020-10-05 |
not scaled |
2019-10-23 |
| # 4836 | 1.0 | 7.458 |
77°, 48° |
2.457319e6 | 3617.3 | 0.0° |
None | 2020-10-05 |
not scaled |
2019-10-23 |
Q: model quality flag (0-5, 5=highest) | P: rotation period | λ,β: ecl. lon. and lat. of spin axis (J2000) | JD: initial time (epoch) | φ0: initial rotation angle for JD0
Image size: 300px. Transparent image background for copy & paste
| Map with groundtrack and observer stations |
| Event Details |
|
Occultation UUID [and DB] : 7b70a960-ddb7-11f0-547e-9858dc4dabb7 [observed]
Occultation Date + Time : 2025-09-17 at 19:41:56 UT +/- 0.0 min [1]
Object Designation : (2184) Fujian
Orbit Class : MBA
Star Designation : GDR3 4094434242160614144
Star Coordinates (ICRF) : RA = 18 15 43.8130, DE = -20 00 18.066 [2]
Star Magnitudes : G = 14.87 mag, RP = 14.03 mag, BP = 15.57 mag
Object Magnitude : V = 17.34 mag
Estimated Magnitude Drop : 2.6 mag
Estimated Max. Duration : 2.3 sec
Object Mean Diameter : 26.3 km (src: astorb)
Speed of the shadow : 11.3 km/s
Elongation to Moon & Sun : 145° (sunlit = 16%), Sun = 99°
Cross-track uncertainty : 0.4 mas = 0 km = 0.03 path-width (1-sig)
RUWE and duplicate source : 1.02 mas, dup.src = 0 (0:false, 1:true)
Ephemeris Reference : JPL#87
Note : FP:true
[1] time t0 of closest geocentric approach c/a, [2] including proper motion until t0
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