| Parameter |
Value |
| Designation |
C/2014 E2 (Jacques) |
| Type |
C |
| Perihelion (tp_cal, UTC) |
2014-07-02T12:20:22.404480Z |
| Orbit solution date (soln_date, UTC) |
2021-04-15T23:32:50Z |
| Obs used |
4812 |
| NEO |
- |
| M1 |
12.000 |
| K1 |
6.500 |
| PC |
- |
Osculating Elements
| Parameter |
Value |
| Epoch (epoch_cal, TDB) |
2014-08-02.0000000 |
| e |
0.99903625 |
| q (au) |
0.663916 |
| a (au) |
688.887878 |
| i (deg) |
156.392754 |
| Ω (om, deg) |
56.391597 |
| ω (w, deg) |
344.037051 |
| M (ma, deg) |
0.001662 |
Magnitude
Scatter + Global Linear
$$
M_a = (11.111 + 3.563\cdot 2.5\log_{10} r) + \epsilon - 2.5\log_{10}\Phi(\theta) + 5\log_{10}\Delta
$$
$$
\theta = 180^\circ - \alpha
$$
$$
\Phi(\theta) = \frac{\delta_{90} D(\theta) + 1}{\delta_{90} + 1},\quad D(\theta) = k\cdot \Phi_{HG}(\theta; g_f) + (1-k)\cdot \Phi_{HG}(\theta; g_b)
$$
$$
\Phi_{HG}(\theta; g) = \left(\frac{1+g^2}{1+g^2-2g\cos\theta}\right)^{3/2},\quad \Phi_{HG}(90^\circ)=1
$$
Model Parameters
| Parameter |
Value |
| H0 |
11.111 |
| n |
3.563 |
| gf |
1.000 |
| gb |
-0.909 |
| k |
0.991 |
| δ90 |
9.677 |
| 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 |
| 2014-02-23 |
2014-04-03 |
+6.1865 |
-2.097 |
| 2014-04-03 |
2014-06-29 |
+14.8621 |
-3.609 |
| 2014-07-08 |
2014-08-30 |
+9.4649 |
-1.555 |
| 2014-08-30 |
2015-06-08 |
-2.1676 |
-0.724 |
log10 r = log10(heliocentric distance / AU), Δ = geocentric distance (AU)
Ephemeris
| Date/Time (UTC) |
RA (J2000) |
Dec (J2000) |
Nearest HIP |
Dist from HIP (arcmin) |
| 2026-09-20 00:00 |
17:41:17.43 |
-10:43:04.8 |
HIP 86702 |
24.37 |
| 2026-09-20 12:00 |
17:41:17.47 |
-10:43:19.0 |
HIP 86702 |
24.32 |
| 2026-09-21 00:00 |
17:41:17.54 |
-10:43:33.2 |
HIP 86702 |
24.26 |
| 2026-09-21 12:00 |
17:41:17.65 |
-10:43:47.3 |
HIP 86702 |
24.20 |
| 2026-09-22 00:00 |
17:41:17.79 |
-10:44:01.5 |
HIP 86702 |
24.12 |
| 2026-09-22 12:00 |
17:41:17.96 |
-10:44:15.7 |
HIP 86702 |
24.05 |
| 2026-09-23 00:00 |
17:41:18.17 |
-10:44:29.9 |
HIP 86702 |
23.96 |
| 2026-09-23 12:00 |
17:41:18.42 |
-10:44:44.1 |
HIP 86702 |
23.87 |
| 2026-09-24 00:00 |
17:41:18.70 |
-10:44:58.3 |
HIP 86702 |
23.78 |
| 2026-09-24 12:00 |
17:41:19.02 |
-10:45:12.5 |
HIP 86702 |
23.67 |
| 2026-09-25 00:00 |
17:41:19.37 |
-10:45:26.6 |
HIP 86702 |
23.56 |
| 2026-09-25 12:00 |
17:41:19.75 |
-10:45:40.8 |
HIP 86702 |
23.45 |
| 2026-09-26 00:00 |
17:41:20.17 |
-10:45:55.0 |
HIP 86702 |
23.33 |
| 2026-09-26 12:00 |
17:41:20.63 |
-10:46:09.1 |
HIP 86702 |
23.20 |
| 2026-09-27 00:00 |
17:41:21.12 |
-10:46:23.3 |
HIP 86702 |
23.06 |
| 2026-09-27 12:00 |
17:41:21.64 |
-10:46:37.4 |
HIP 86702 |
22.92 |
| 2026-09-28 00:00 |
17:41:22.20 |
-10:46:51.5 |
HIP 86702 |
22.78 |
| 2026-09-28 12:00 |
17:41:22.79 |
-10:47:05.6 |
HIP 86702 |
22.62 |
| 2026-09-29 00:00 |
17:41:23.42 |
-10:47:19.7 |
HIP 86702 |
22.46 |
| 2026-09-29 12:00 |
17:41:24.08 |
-10:47:33.8 |
HIP 86702 |
22.30 |
| 2026-09-30 00:00 |
17:41:24.77 |
-10:47:47.9 |
HIP 86702 |
22.13 |
| 2026-09-30 12:00 |
17:41:25.50 |
-10:48:02.0 |
HIP 86702 |
21.95 |
| 2026-10-01 00:00 |
17:41:26.26 |
-10:48:16.0 |
HIP 86702 |
21.77 |
| 2026-10-01 12:00 |
17:41:27.06 |
-10:48:30.1 |
HIP 86702 |
21.58 |
| 2026-10-02 00:00 |
17:41:27.89 |
-10:48:44.1 |
HIP 86702 |
21.39 |
| 2026-10-02 12:00 |
17:41:28.76 |
-10:48:58.1 |
HIP 86702 |
21.19 |
| 2026-10-03 00:00 |
17:41:29.65 |
-10:49:12.0 |
HIP 86702 |
20.98 |
| 2026-10-03 12:00 |
17:41:30.59 |
-10:49:26.0 |
HIP 86702 |
20.77 |
| 2026-10-04 00:00 |
17:41:31.55 |
-10:49:39.9 |
HIP 86702 |
20.56 |
| 2026-10-04 12:00 |
17:41:32.55 |
-10:49:53.8 |
HIP 86702 |
20.34 |
| 2026-10-05 00:00 |
17:41:33.58 |
-10:50:07.7 |
HIP 86702 |
20.11 |
| 2026-10-05 12:00 |
17:41:34.65 |
-10:50:21.6 |
HIP 86702 |
19.88 |
| 2026-10-06 00:00 |
17:41:35.75 |
-10:50:35.5 |
HIP 86702 |
19.65 |
| 2026-10-06 12:00 |
17:41:36.88 |
-10:50:49.3 |
HIP 86702 |
19.41 |
| 2026-10-07 00:00 |
17:41:38.05 |
-10:51:03.1 |
HIP 86702 |
19.16 |
| 2026-10-07 12:00 |
17:41:39.25 |
-10:51:16.8 |
HIP 86702 |
18.92 |
| 2026-10-08 00:00 |
17:41:40.48 |
-10:51:30.6 |
HIP 86702 |
18.66 |
| 2026-10-08 12:00 |
17:41:41.74 |
-10:51:44.3 |
HIP 86702 |
18.41 |
| 2026-10-09 00:00 |
17:41:43.04 |
-10:51:57.9 |
HIP 86702 |
18.15 |
| 2026-10-09 12:00 |
17:41:44.37 |
-10:52:11.6 |
HIP 86702 |
17.89 |
| 2026-10-10 00:00 |
17:41:45.73 |
-10:52:25.2 |
HIP 86702 |
17.63 |
| 2026-10-10 12:00 |
17:41:47.13 |
-10:52:38.7 |
HIP 86702 |
17.36 |
| 2026-10-11 00:00 |
17:41:48.55 |
-10:52:52.3 |
HIP 86702 |
17.09 |