| Parameter |
Value |
| Designation |
C/2022 U1 (Leonard) |
| Type |
C |
| Perihelion (tp_cal, UTC) |
2024-03-25T21:34:52.720320Z |
| Orbit solution date (soln_date, UTC) |
2025-10-28T16:12:34Z |
| Obs used |
1325 |
| NEO |
- |
| M1 |
10.200 |
| K1 |
7.000 |
| PC |
0.030 |
| Discovery observation (MPC, UTC) |
2022-10-20T08:05:31.920000Z |
| Discovery magnitude (MPC) |
19.84 G |
| Discovery observatory (MPC) |
G96 · Mt. Lemmon Survey |
Osculating Elements
| Parameter |
Value |
| Epoch (epoch_cal, TDB) |
2024-05-01.0000000 |
| e |
0.99936570 |
| q (au) |
4.202017 |
| a (au) |
6624.693105 |
| i (deg) |
128.149455 |
| Ω (om, deg) |
72.526035 |
| ω (w, deg) |
78.588952 |
| M (ma, deg) |
0.000066 |
Magnitude
Scatter + Global Linear
$$
M_a = (9.049 + 2.890\cdot 2.5\log_{10} r) + \epsilon - 2.5\log_{10}\Phi(\theta) + 5\log_{10}\Delta
$$
$$
\theta = 180^\circ - \alpha
$$
$$
\Phi(\theta) = \frac{\delta_{90} D(\theta) + 1}{\delta_{90} + 1},\quad D(\theta) = k\cdot \Phi_{HG}(\theta; g_f) + (1-k)\cdot \Phi_{HG}(\theta; g_b)
$$
$$
\Phi_{HG}(\theta; g) = \left(\frac{1+g^2}{1+g^2-2g\cos\theta}\right)^{3/2},\quad \Phi_{HG}(90^\circ)=1
$$
Model Parameters
| Parameter |
Value |
| H0 |
9.049 |
| n |
2.890 |
| gf |
0.998 |
| gb |
-0.501 |
| k |
1.000 |
| δ90 |
10.000 |
| Parameter |
Symbol |
Range |
Description |
| Absolute magnitude at 1 AU from Sun and Earth |
H0 |
-5 to 20 |
Intrinsic brightness of the comet |
| Photometric slope parameter |
n |
2 to 6 |
Rate of brightness change with heliocentric distance |
| Forward scattering asymmetry factor |
gf |
0.8 to 1 |
Degree of forward scattering |
| Backward scattering asymmetry factor |
gb |
-1 to -0.5 |
Degree of backward scattering |
| Partitioning coefficient |
k |
0.8 to 1 |
Ratio between forward/backward scattering contributions |
| Dust-to-gas brightness ratio |
δ90 |
1 to 10 |
Relative contribution of dust scattering to gas emission |
Reference: EPSC-DPS2025-160
Residuals (Piecewise)
$$\epsilon = a \log_{10} r_{\mathrm{au}} + b$$
| Start (UTC) |
End (UTC) |
a |
b |
| 2022-09-23 |
2024-02-17 |
+0.7895 |
-0.107 |
| 2024-04-10 |
2025-08-18 |
-1.8554 |
+0.902 |
log10 r = log10(heliocentric distance / AU), Δ = geocentric distance (AU)
Finding Chart
Ephemeris
| Date/Time (UTC) |
RA (J2000) |
Dec (J2000) |
Nearest HIP |
Dist from HIP (arcmin) |
| 2026-03-26 00:00 |
18:17:57.20 |
-06:21:10.3 |
HIP 89712 |
17.18 |
| 2026-03-26 12:00 |
18:17:51.92 |
-06:21:14.3 |
HIP 89712 |
17.95 |
| 2026-03-27 00:00 |
18:17:46.49 |
-06:21:18.3 |
HIP 89712 |
18.80 |
| 2026-03-27 12:00 |
18:17:40.90 |
-06:21:22.5 |
HIP 89712 |
19.74 |
| 2026-03-28 00:00 |
18:17:35.16 |
-06:21:26.8 |
HIP 89712 |
20.76 |
| 2026-03-28 12:00 |
18:17:29.26 |
-06:21:31.1 |
HIP 89712 |
21.85 |
| 2026-03-29 00:00 |
18:17:23.21 |
-06:21:35.6 |
HIP 89712 |
23.01 |
| 2026-03-29 12:00 |
18:17:17.00 |
-06:21:40.2 |
HIP 89712 |
24.24 |
| 2026-03-30 00:00 |
18:17:10.64 |
-06:21:44.8 |
HIP 89712 |
25.54 |
| 2026-03-30 12:00 |
18:17:04.13 |
-06:21:49.7 |
HIP 89712 |
26.90 |
| 2026-03-31 00:00 |
18:16:57.46 |
-06:21:54.6 |
HIP 89712 |
28.32 |
| 2026-03-31 12:00 |
18:16:50.63 |
-06:21:59.7 |
HIP 89712 |
29.80 |
| 2026-04-01 00:00 |
18:16:43.65 |
-06:22:04.9 |
HIP 89712 |
31.34 |
| 2026-04-01 12:00 |
18:16:36.51 |
-06:22:10.2 |
HIP 89712 |
32.93 |
| 2026-04-02 00:00 |
18:16:29.22 |
-06:22:15.7 |
HIP 89427 |
32.41 |
| 2026-04-02 12:00 |
18:16:21.77 |
-06:22:21.4 |
HIP 89427 |
31.16 |
| 2026-04-03 00:00 |
18:16:14.17 |
-06:22:27.2 |
HIP 89427 |
29.95 |
| 2026-04-03 12:00 |
18:16:06.41 |
-06:22:33.1 |
HIP 89427 |
28.79 |
| 2026-04-04 00:00 |
18:15:58.49 |
-06:22:39.3 |
HIP 89427 |
27.70 |
| 2026-04-04 12:00 |
18:15:50.42 |
-06:22:45.6 |
HIP 89427 |
26.69 |
| 2026-04-05 00:00 |
18:15:42.19 |
-06:22:52.0 |
HIP 89427 |
25.77 |
| 2026-04-05 12:00 |
18:15:33.80 |
-06:22:58.7 |
HIP 89427 |
24.98 |
| 2026-04-06 00:00 |
18:15:25.26 |
-06:23:05.5 |
HIP 89427 |
24.33 |
| 2026-04-06 12:00 |
18:15:16.56 |
-06:23:12.5 |
HIP 89427 |
23.85 |
| 2026-04-07 00:00 |
18:15:07.70 |
-06:23:19.8 |
HIP 89427 |
23.55 |
| 2026-04-07 12:00 |
18:14:58.68 |
-06:23:27.2 |
HIP 89427 |
23.45 |
| 2026-04-08 00:00 |
18:14:49.51 |
-06:23:34.8 |
HIP 89427 |
23.57 |
| 2026-04-08 12:00 |
18:14:40.18 |
-06:23:42.6 |
HIP 89427 |
23.91 |
| 2026-04-09 00:00 |
18:14:30.70 |
-06:23:50.7 |
HIP 89427 |
24.48 |
| 2026-04-09 12:00 |
18:14:21.06 |
-06:23:58.9 |
HIP 89427 |
25.27 |
| 2026-04-10 00:00 |
18:14:11.26 |
-06:24:07.4 |
HIP 89427 |
26.27 |
| 2026-04-10 12:00 |
18:14:01.30 |
-06:24:16.2 |
HIP 89427 |
27.48 |
| 2026-04-11 00:00 |
18:13:51.18 |
-06:24:25.1 |
HIP 89427 |
28.86 |
| 2026-04-11 12:00 |
18:13:40.91 |
-06:24:34.3 |
HIP 89226 |
27.60 |
| 2026-04-12 00:00 |
18:13:30.49 |
-06:24:43.7 |
HIP 89226 |
26.15 |
| 2026-04-12 12:00 |
18:13:19.90 |
-06:24:53.4 |
HIP 89226 |
24.88 |
| 2026-04-13 00:00 |
18:13:09.16 |
-06:25:03.4 |
HIP 89226 |
23.82 |
| 2026-04-13 12:00 |
18:12:58.26 |
-06:25:13.6 |
HIP 89226 |
23.01 |
| 2026-04-14 00:00 |
18:12:47.21 |
-06:25:24.1 |
HIP 89226 |
22.50 |
| 2026-04-14 12:00 |
18:12:36.00 |
-06:25:34.8 |
HIP 89226 |
22.32 |
| 2026-04-15 00:00 |
18:12:24.63 |
-06:25:45.9 |
HIP 89226 |
22.50 |
| 2026-04-15 12:00 |
18:12:13.11 |
-06:25:57.2 |
HIP 89226 |
23.04 |
| 2026-04-16 00:00 |
18:12:01.44 |
-06:26:08.8 |
HIP 89226 |
23.93 |