Juno's Close Encounter With Ganymede—An Overview
Abstract
The Juno spacecraft has been in orbit around Jupiter since 2016. Two flybys of Ganymede were executed in 2021, opportunities realized by evolution of Juno's polar orbit over the intervening 5 years. The geometry of the close flyby just prior to the 34th perijove pass by Jupiter brought the spacecraft inside Ganymede's unique magnetosphere. Juno's payload, designed to study Jupiter's magnetosphere, had ample dynamic range to study Ganymede's magnetosphere. The Juno radio system was used both for gravity measurements and for study of Ganymede's ionosphere. Remote sensing of Ganymede returned new results on geology, surface composition, and thermal properties of the surface and subsurface.
Key Points
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Juno passed Ganymede on 7 June 2021 at an altitude of approximately 1,000 km, the closest any spacecraft has come since the Galileo mission ended in 2003
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The path of Juno's trajectory allowed the spacecraft to pierce Ganymede's unique magnetosphere and map a swath of its surface and subsurface
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The geometry of the flyby is described for the close pass in June and a more distant pass (approximately 50,000 km) on 20 July 2021
Plain Language Summary
The evolution of Juno's orbit around Jupiter made it possible to execute a close and a distant flyby of Ganymede in 2021. The geometry of the close pass allowed Juno to enter Ganymede's unique magnetosphere. Juno's remote sensing instruments observed a significant area of Ganymede's surface and subsurface with higher resolution than Voyager or Galileo.
1 Introduction
Jupiter's moon Ganymede is the largest moon in the solar system and the only moon with its own intrinsic, permanent magnetic field that extends far beyond its surface to form a magnetosphere (Gurnett et al., 1996; Kivelson et al., 1996, 2002). The first missions to investigate Ganymede in detail were the Voyager flybys of Jupiter in 1979, and the Galileo mission, which orbited Jupiter from 1995 to 2003 and executed a series of six close Ganymede flybys (summarized by Volwerk et al., 2022). Key findings of these missions, combined with Earth-based observations from facilities such as Hubble and ALMA, are as follows.
Ganymede has a fully differentiated interior including a metallic core (Anderson et al., 1996; Hussmann et al., 2022). A subsurface liquid salt-water ocean forms a global layer, the top of which can be no more than 330 km below the icy surface (Kivelson et al., 1999; Saur et al., 2015, 2018). Ganymede is slightly larger and denser than, and forms a class with, the two other large solar system moons Callisto and Saturn's Titan. However, Ganymede's complex geologic history, which includes tectonic and/or volcanic production of grooved terrain well after the moon's formation, cutting through ancient heavily cratered terrain, shows a very different formation and evolution history than the other large moons (Schenk et al., 2022).
Ganymede's neutral molecular oxygen exosphere (Hall et al., 1998), sourced from sputtering, radiolysis, and sublimation of surface ice, is ionized by photo-ionization and electron impact on open field lines. O, H, and H2O have also been detected (Barth et al., 1997; Hall et al., 1998; Roth et al., 2021, respectively). Hubble Space Telescope (HST) spectral images suggest oxygen auroral emissions are generated at or near the polar boundary between open and closed magnetic field lines (McGrath et al., 2013). The ionosphere is weak and transient—detected in some but not all of the earth occultations observed by the Galileo mission (Kliore, 1998).
Galileo near-infrared spectra showed that the composition of the satellite's surface is dominated by a mixture of water ice, trapped carbon dioxide and other species (Carlson et al., 1996). The ice particles form a thin layer of frost which, in the polar regions, shows a higher albedo in the visible part of the spectrum. It has been suggested (G. B. Hansen and McCord, 2004; Khurana et al., 2007) and bolstered by more recent datasets (Ligier et al., 2019; Mura et al., 2020) that this albedo difference may be due to the interaction of the magnetic field of Ganymede with the Jovian magnetosphere, which at least partially protects the surface regions between ±40° latitude from the impact of Jovian magnetospheric particles, while leaving the polar regions exposed to plasma bombardment (Paranicas et al., 2021).
Our understanding of Ganymede's magnetosphere prior to Juno's flyby is summarized in Jia and Kivelson (2021). Ganymede's magnetic field interacts dynamically with the ambient Jovian plasma and magnetic field. The opportunity to investigate Ganymede's unique magnetosphere in situ and its interaction with the Jovian magnetosphere with the modern Juno payload, has given us the most comprehensive close-range data set since those acquired by Galileo and Voyager (Table 1). Juno's close flyby of Ganymede occurred on 7 June 2021 with a more distant flyby on 20 July 2021.
Instrument name | Description | Ganymede science |
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Gravity | Doppler Radio Science (Asmar et al., 2017) | Ganymede gravity field and ionosphere |
Mag | Dual Fluxgate Magnetometers (Connerney et al., 2017) | Ganymede's dynamo field and magnetic field structure in Ganymede's magnetosphere |
MWR | Microwave Radiometer (Janssen et al., 2017) | Subsurface properties |
JEDI | Energetic Particle Detectors (Mauk et al., 2017) | Energetic charged particle flux and composition in Ganymede's magnetosphere |
JADE | Plasma Particle Detectors (McComas et al., 2017) | Plasma electron and ion distributions; ion composition in Ganymede's magnetosphere |
Waves | Radio and Plasma Waves (Kurth et al., 2017) | Radio emissions from, and plasma waves in, Ganymede's magnetosphere |
UVS | Ultraviolet Imaging Spectrograph (Gladstone et al., 2017) | Ganymede's aurora and surface albedo |
JIRAM | Infrared Imaging Spectrometer (Adriani et al., 2017) | High resolution surface composition |
JunoCam | Visible Color Imager (C. J. Hansen et al., 2017) | Day-side images for surface geomorphology |
SRU | Stellar Reference Unit (Becker et al., 2017) | Night-side image illuminated by Jupiter-shine for surface geomorphology |
ASC | Advanced Stellar Compass (Connerney et al., 2017) | Energetic electron detection in the Jovian environment |
2 Juno's Orbit Evolution
The Juno spacecraft, launched in 2011, went into orbit around Jupiter on 4 July 2016. The initial 53-day orbit was polar and elliptical, with apojove at an altitude of approximately 8,032,760 km and perijove at an altitude of 4,163 km (Bolton et al., 2017). The perijove (PJ) latitude at PJ1 was at approximately 3.8°N latitude. The orientation of the orbit ellipse was such that apojove was over the dawn terminator, perijove over the dusk terminator, and both nearly in the plane of the ecliptic. Jupiter's obliquity is just over 3°, thus the high inclination of Juno's orbit precluded any close flybys of the Galilean moons for almost the entire prime mission.
Juno's prime mission was designed to achieve 35 PJ passes, to map the Jovian magnetosphere with 11.25° longitudinal spacing. Over the 5 years of the primary mission, orbit evolution due to Jupiter's oblateness moved perijove northward and apojove southward as shown in Figure 1. Once the orbital distance of Juno at the equatorial plane crossing on the inbound leg of its orbit evolved inwards to the point that it reached the orbital distances of the Galilean satellites, opportunities became available to observe the moons up close. Trajectory timing was designed to encounter Ganymede when Juno crossed its orbit on PJ34 and PJ35. There are no more close Ganymede flybys in the remainder of the extended mission (EM) as the orbit continues to evolve.
3 Geometry of the Ganymede Flybys
3.1 PJ34 Ganymede Flyby
Juno flew by Ganymede on 7 June 2021 at a closest-approach (CA) altitude of 1,046 km over the leading hemisphere, about 14.8 hr before PJ34. The spacecraft approached Ganymede from the night side, went behind Ganymede as seen from the earth (achieving an earth occultation), passed through the moon's magnetosphere, then departed on the sunlit ∼sub-Jovian side. The trajectory with respect to Ganymede's magnetosphere is illustrated in Figure 2 and events are listed in Table 2.
2021 June 7 hh:mm UTC | Altitude | Event |
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16:40 | 15,636 | Earth occultation ingress |
Approximately 16:42 | 13,474 | Entry into wake region |
16:50 | 5,115 | Magnetosphere entry: Transition from field lines connected Jupiter-Jupiter to Jupiter-Ganymede field lines |
16:53 | 2,439 | Earth occultation egress |
16:56 | 1,049 | Closest approach |
16:57 | 1,166 | Night–day boundary crossing (radial projection from surface) |
Approximately 17:01 | 3,890 | Outbound magnetopause boundary crossing |
As shown in Figure 3 remote sensing coverage began with an SRU image taken of territory lit by Jupiter-shine, on the night side of the terminator. UVS detected the aurora on both the nightside and dayside. MWR scanned the subsurface. JunoCam imaged the surface on the dayside. JIRAM collected five very high spatial resolution samples of different terrain types.
Table 3 lists the geometric parameters for the flyby.
PJ34 Ganymede encounter | |
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Time of closest approach | 7 June 2021 16:56 UTC |
Altitude | 1,046 km |
Subspacecraft latitude | 23.6°N |
Subspacecraft longitude | 56.8°W |
Subsolar latitude | 0.06°N |
Subsolar longitude | 318°W |
Phase angle | 98° |
Sun-Jupiter-Ganymede angle | 136° |
Juno speed with respect to Ganymede | 18.57 km/s |
Jupiter centrifugal latitude (Phipps & Bagenal, 2021)a | 1.8°S |
Jupiter System III west longitude | 302°W |
- Note. All parameters are with respect to Ganymede unless otherwise noted.
- a The centrifugal equator is the plane to which the magnetospheric plasma is confined, geometrically defined as the loci of points where each magnetic field line is at its farthest distance from Jupiter's spin axis.
3.2 PJ35 Ganymede Flyby
Juno made another more distant pass by Ganymede at approximately 50,000 km altitude on 20 July 2021, 15.4 hr before PJ35. At this distance the fields and particles instruments could study the environment at Ganymede's range from Jupiter, thus providing a point of reference for magnetospheric conditions without the presence of Ganymede. Comparisons to magnetospheric conditions on the PJ34 observations close to Ganymede help to establish how Ganymede affects conditions in Jupiter's magnetosphere.
The JIRAM, UVS and JunoCam imagers were able to gather data over territory not imaged in PJ34. Table 4 lists the flyby geometric parameters.
PJ35 Ganymede encounter | |
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Time of c/a | 20 July 2021 16:48 UTC |
Altitude | 50,109 km |
Subspacecraft latitude | 22.5°S |
Subspacecraft longitude | 237.4°W |
Phase angle | 80.9° |
Jupiter centrifugal latitude | 0.4°N |
Juno speed with respect to Ganymede | 17.9 km/s |
- Note. All parameters are with respect to Ganymede unless otherwise noted.
4 Science Results Summary
4.1 Interior Structure
Tracking data from Juno's radio subsystem are combined with datasets from the Galileo mission, allowing an update to the gravity field of Ganymede. The degree-2 gravity field is consistent with a body in hydrostatic equilibrium, while degree >2 signal hints at localized nonhydrostatic features (Palguta et al., 2006). Including explicitly the effect of nonhydrostatic gravity provides a more realistic assessment of the error in Ganymede's moment of inertia. The larger derived error allows for a larger variation in the densities of internal layers as compared to Anderson et al. (1996) (Gomez Casajus et al., 2022).
4.2 Surface and Subsurface Properties
Juno examined the surface of Ganymede from microwave to ultraviolet wavelengths. The subsurface mapped by MWR shows variation vertically and horizontally in thermophysical properties, from warmer ancient dark terrain to the very cold crater Tros (Brown, 2022). JIRAM data were obtained with pixel resolution <1 km/px on both the leading and trailing side, sampling grooved terrain, dark terrains, and fresh crater ejecta. Spectroscopic data show a wealth of information, with variable distribution of specific categories of mineral salts and possibly organic compounds. The analysis of JIRAM spectroscopic data suggests that Ganymede's surface composition at low latitudes is complex and likely endogenous in nature, with perhaps limited alteration by space weathering. Visible images from the SRU and JunoCam reveal detail at higher resolution, in stereo, and with better quality in the imaged region than the best of the existing Voyager and Galileo coverage, enabling improvements to the geologic and topographic maps (Becker et al., 2022; Ravine et al., 2022). Albedo mapped at ultraviolet wavelengths shows latitudinal trends in composition and ice grain size (Molyneux et al., 2022). Sputtering rates to evaluate energetic particle weathering of Ganymede's surface have been computed (Paranicas et al., 2022).
4.3 Exosphere, Ionosphere, Aurora
The ionosphere was probed by observing Juno's radio signal as the spacecraft disappeared behind Ganymede as seen from the Earth, and electron density in the ionosphere was determined (Buccino et al., 2022). The UVS mapped emissions from Ganymede's aurora that mark the boundary of the open and closed field lines of Ganymede's magnetosphere. This data set constrains models of Ganymede's magnetosphere (Greathouse et al., 2022). Data obtained from Hubble Space Telescope at the time of Juno's encounter reveal the coupling of the brightness of the aurora to Jupiter's plasma sheet (Saur et al., 2022).
4.4 Ganymede's Magnetosphere Structure and Dynamics
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Plasma ions and electrons: The ion composition near Ganymede is very different from the local plasma environment. H2+ and H3+ ions were detected inside Ganymede's magnetosphere and outside in the wake region. The presence of H2+ and H3+ is a strong indicator that the composition is dominated by water products from Ganymede's surface (Allegrini et al., 2022). Observation of heated, streaming electrons near Ganymede's magnetopause was consistent with magnetic reconnection (Ebert et al., 2022; Valek et al., 2022).
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Energetic charged particles: Similar flux levels on polar Ganymede field lines to those in the surrounding region were found (Paranicas et al., 2022). Ganymede causes a relative decrease in high energy electron flux that is central to and symmetrical about Ganymede's position (Clark et al., 2022; Kollman et al., 2022).
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Radio and plasma wave: Radio emissions were detected, likely originating from Ganymede's magnetosphere. Various plasma wave modes and instabilities have been identified, namely, whistler modes, electron cyclotron harmonics, and upper hybrid bands. The latter emissions allowed for the inference of the local electron density profile, revealing a day-night asymmetry in variability (Kurth et al., 2022).
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Magnetic field: Updated best-fit spherical harmonics of Ganymede's internal magnetic field reveal a very dominant dipole moment, with quadrupole moments that are over an order of magnitude weaker (Weber et al., 2022). The detection of flux ropes and non-zero magnetic field normal component across the ram-side magnetopause was consistent with magnetic reconnection (Duling et al., 2022; Romanelli et al., 2022).
5 Conclusions
Important new observations have clarified long-standing puzzles from the Galileo epoch and generated new questions to guide the upcoming JUICE and Clipper missions. Juno will continue its program of comparative studies of the Galilean satellites with close flybys of Europa on 29 September 2022 (PJ45), and Io on 30 December 2023 (PJ57) and 3 February 2024 (PJ58), which will further advance our understanding of Jupiter's diverse retinue of large satellites.
Acknowledgments
Support from the Juno project through a subcontract from the Southwest Research Institute is acknowledged. Stefan Duling has received funding from the European Research Council (ERC) under the European Union's Horizon 2020 research and innovation program (Grant agreement No. 884711). The authors thank the Juno project flight team for their design and execution of a unique Ganymede flyby.
Conflict of Interest
The authors declare no conflicts of interest relevant to this study.
Open Research
Data Availability Statement
All Juno data are archived in the NASA Planetary Data System (PDS) at https://pds-atmospheres.nmsu.edu/data_and_services/atmospheres_data/JUNO and https://pds-ppi.igpp.ucla.edu/mission/JUNO.