41P/Tuttle–Giacobini–Kresák

41P/Tuttle–Giacobini–Kresák
Comet Tuttle–Giacobini–Kresák on March 3, 2017 near Messier 108 and the Owl Nebula.
Discovery
Discovered byHorace Parnell Tuttle
Michel Giacobini
Ľubor Kresák
Discovery dateMay 3, 1858
Designations
  • P/1858 J1, P/1907 O1
  • P/1951 H1
  • 1858 III, 1907 III, 1951 IV
  • 1962 V, 1973 VI
  • 1978 XXV, 1990 II
Orbital characteristics[2][3]
EpochSeptember 13, 2023 (JD 2460200.5)
Observation arc72.38 years
Earliest precovery dateApril 26, 1951
Number of
observations
5,250
Aphelion5.126 AU
Perihelion1.051 AU
Semi-major axis3.088 AU
Eccentricity0.65981
Orbital period5.428 years
Inclination9.219°
140.99°
Argument of
periapsis
62.227°
Mean anomaly66.147°
Last perihelion12 September 2022
Next perihelion15 February 2028[1]
TJupiter2.827
Earth MOID0.134 AU
Jupiter MOID0.488 AU
Physical characteristics[2]
Mean radius
0.44–0.56 km (0.27–0.35 mi)[4]
Comet total
magnitude
(M1)
16.9

41P/Tuttle–Giacobini–Kresák is a Jupiter-family comet with a 5.43-year orbit around the Sun. Observations with the Hubble Space Telescope and dynamical modeling estimate an effective nucleus radius of 440–560 m (1,440–1,840 ft), corresponding to a diameter of roughly 0.88–1.12 km (0.55–0.70 mi),[4] smaller than earlier ground-based estimates.[5]

Observational history

Discovery

Discovered by Horace Parnell Tuttle on May 3, 1858, and re-discovered independently by Michel Giacobini and Ľubor Kresák in 1907 and 1951 respectively, it is a member of the Jupiter family of comets.

2006 apparition

As of June 1, 2006, Comet 41P was a 10th magnitude object for telescopes, located on the Cancer-Leo border, with a predicted maximum of about 10 at perihelion on June 11. This comet is of interest as it has been noted to flare dramatically. In 1973 the flare was 10 magnitudes brighter than predicted, reaching easy naked-eye visibility at apparent magnitude 4.[6] However, by June 22, the comet had diminished to about magnitude 11, having produced no flare of note.

2011 apparition

The comet was not observed during the 2011 unfavorable apparition[7] since the perihelion passage occurred when the comet was on the far side of the Sun.

2017 apparition

41P was recovered on November 10, 2016, at apparent magnitude 21 by Pan-STARRS.[3] On April 1, 2017, the comet passed 0.142 AU (21.2 million km; 13.2 million mi) from the Earth.[8] The comet was expected to brighten to around magnitude 7 and be visible in binoculars.[9][10]

Observations during the apparition revealed rapid changes in the nucleus rotation rate, interpreted as being caused by strong outgassing torques near perihelion.[4]

Physical characteristics

High-resolution observations with the Hubble Space Telescope indicate that the nucleus of 41P has an effective radius between 440 and 560 m, based on photometry corrected for coma contamination and estimates from non-gravitational acceleration.[4]

Photometric observations show a lightcurve amplitude of about 0.4 magnitudes, implying an elongated nucleus with an axis ratio of at least 1.4:1. Period analysis gives a likely double-peaked rotation period of 0.599 days (14.4 hours). The comet exhibited rapid rotational deceleration near perihelion in 2017, attributed to asymmetric outgassing torques.

Modeling suggests that continued torques could lead to rotational instability on timescales of decades, potentially much shorter than the comet’s dynamical lifetime (~1,000 years). The nucleus may therefore be susceptible to rotational breakup.

Proposed exploration

In the 1960s, the European Space Research Organisation (ESRO) investigated about sending a probe to the comet by 1973, however this proposal was later rejected.[11]

References

  1. ^ "Horizons Batch for 41P/Tuttle-Giacobini-Kresak (90000489) on 2028-Feb-15" (Perihelion occurs when rdot flips from negative to positive). JPL Horizons. Retrieved July 6, 2023. (JPL#K171/19 Soln.date: 2023-May-04)
  2. ^ a b "41P/Tuttle–Giacobini–Kresák – JPL Small-Body Database Lookup". ssd.jpl.nasa.gov. Jet Propulsion Laboratory. Retrieved February 28, 2010.
  3. ^ a b "41P/Tuttle–Giacobini–Kresák Orbit". Minor Planet Center. Retrieved June 16, 2014.
  4. ^ a b c d D. C. Jewitt (2026). "Reversal of Spin: Comet 41P/Tuttle–Giacobini–Kresak". arXiv:2602.06403 [astro-ph.EP]. PDF
  5. ^ P. L. Lamy; I. Toth; Y. R. Fernández; H. A. Weaver (2004). "The Sizes, Shapes, Albedos, and Colors of Cometary Nuclei" (PDF). Comets II. University of Arizona Press. pp. 223–264. doi:10.2307/j.ctv1v7zdq5.22. ISBN 978-0-8165-2450-1. JSTOR j.ctv1v7zdq5.22.
  6. ^ G. W. Kronk. "41P/Tuttle–Giacobini–Kresák". Cometography.com. Retrieved April 23, 2025.
  7. ^ Seiichi Yoshida (July 22, 2011). "41P/Tuttle-Giacobini-Kresak (2011)". Seiichi Yoshida's Comet Catalog. Retrieved February 18, 2012.
  8. ^ "JPL Close-Approach Data: 41P/Tuttle-Giacobini-Kresak" (August 27, 2006 last obs). Retrieved February 22, 2012.{{cite web}}: CS1 maint: deprecated archival service (link)
  9. ^ Seiichi Yoshida (December 31, 2006). "41P/Tuttle-Giacobini-Kresak". Seiichi Yoshida's Comet Catalog. Retrieved February 28, 2010.
  10. ^ Bob King (January 4, 2017). "Bright Comet Prospects for 2017". Sky & Telescope. Retrieved March 2, 2017.
  11. ^ P. Ulivi; D. M. Harland (2007). Robotic Exploration of the Solar System Part I: The Golden Age 1957–1982. Springer. p. 89. ISBN 978-0-387-49326-8.