Volume 45, Issue 16 p. 8111-8120
Research Letter
Free Access

Great Expectations: Plans and Predictions for New Horizons Encounter With Kuiper Belt Object 2014 MU69 (“Ultima Thule”)

Jeffrey M. Moore

Corresponding Author

Jeffrey M. Moore

Space Science Division, National Aeronautics and Space Administration (NASA) Ames Research Center, Moffett Field, CA, USA

Correspondence to: J. M. Moore,

[email protected]

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William B. McKinnon

William B. McKinnon

Department of Earth and Planetary Sciences, Washington University, St. Louis, MO, USA

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Dale P. Cruikshank

Dale P. Cruikshank

Space Science Division, National Aeronautics and Space Administration (NASA) Ames Research Center, Moffett Field, CA, USA

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G. Randall Gladstone

G. Randall Gladstone

Southwest Research Institute, San Antonio, TX, USA

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John R. Spencer

John R. Spencer

Southwest Research Institute, Boulder, CO, USA

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S. Alan Stern

S. Alan Stern

Southwest Research Institute, Boulder, CO, USA

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Harold A. Weaver

Harold A. Weaver

Johns Hopkins University Applied Physics Laboratory, Laurel, MD, USA

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Kelsi N. Singer

Kelsi N. Singer

Southwest Research Institute, Boulder, CO, USA

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Mark R. Showalter

Mark R. Showalter

The SETI Institute, Mountain View, CA, USA

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William M. Grundy

William M. Grundy

Lowell Observatory, Flagstaff, AZ, USA

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Ross A. Beyer

Ross A. Beyer

Space Science Division, National Aeronautics and Space Administration (NASA) Ames Research Center, Moffett Field, CA, USA

The SETI Institute, Mountain View, CA, USA

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Oliver L. White

Oliver L. White

Space Science Division, National Aeronautics and Space Administration (NASA) Ames Research Center, Moffett Field, CA, USA

The SETI Institute, Mountain View, CA, USA

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Richard P. Binzel

Richard P. Binzel

Massachusetts Institute of Technology, Cambridge, MA, USA

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Marc W. Buie

Marc W. Buie

Southwest Research Institute, Boulder, CO, USA

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Bonnie J. Buratti

Bonnie J. Buratti

NASA Jet Propulsion Laboratory, California Institute of Technology, Pasadena, CA, USA

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Andrew F. Cheng

Andrew F. Cheng

Johns Hopkins University Applied Physics Laboratory, Laurel, MD, USA

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Carly Howett

Carly Howett

Southwest Research Institute, Boulder, CO, USA

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Cathy B. Olkin

Cathy B. Olkin

Southwest Research Institute, Boulder, CO, USA

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Alex H. Parker

Alex H. Parker

Southwest Research Institute, Boulder, CO, USA

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Simon B. Porter

Simon B. Porter

Southwest Research Institute, Boulder, CO, USA

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Paul M. Schenk

Paul M. Schenk

Lunar and Planetary Institute, Houston, TX, USA

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Henry B. Throop

Henry B. Throop

Planetary Science Institute, Tucson, AZ, USA

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Anne J. Verbiscer

Anne J. Verbiscer

Department of Astronomy, University of Virginia, Charlottesville, VA, USA

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Leslie A. Young

Leslie A. Young

Southwest Research Institute, Boulder, CO, USA

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Susan D. Benecchi

Susan D. Benecchi

Planetary Science Institute, Tucson, AZ, USA

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Veronica J. Bray

Veronica J. Bray

Lunar and Planetary Laboratory, University of Arizona, Tucson, AZ, USA

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Carrie L. Chavez

Carrie L. Chavez

Space Science Division, National Aeronautics and Space Administration (NASA) Ames Research Center, Moffett Field, CA, USA

The SETI Institute, Mountain View, CA, USA

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Rajani D. Dhingra

Rajani D. Dhingra

Department of Physics, University of Idaho, Moscow, ID, USA

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Alan D. Howard

Alan D. Howard

Department of Environmental Sciences, University of Virginia, Charlottesville, VA, USA

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Tod R. Lauer

Tod R. Lauer

National Optical Astronomy Observatory, Tucson, AZ, USA

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C. M. Lisse

C. M. Lisse

Johns Hopkins University Applied Physics Laboratory, Laurel, MD, USA

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Stuart J. Robbins

Stuart J. Robbins

Southwest Research Institute, Boulder, CO, USA

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Kirby D. Runyon

Kirby D. Runyon

Johns Hopkins University Applied Physics Laboratory, Laurel, MD, USA

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Orkan M. Umurhan

Orkan M. Umurhan

Space Science Division, National Aeronautics and Space Administration (NASA) Ames Research Center, Moffett Field, CA, USA

The SETI Institute, Mountain View, CA, USA

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First published: 02 August 2018
Citations: 14
This article has been contributed to by US Government employees and their work is in the public domain in the USA.

Abstract

The New Horizons encounter with the cold classical Kuiper Belt object 2014 MU69 (informally named “Ultima Thule,” hereafter Ultima) on 1 January 2019 will be the first time a spacecraft has ever closely observed one of the free-orbiting small denizens of the Kuiper Belt. Related to but not thought to have formed in the same region of the solar system as the comets that been explored so far, it will also be the most distant, and most primitive body yet visited by spacecraft. In this letter we begin with a brief overview of cold classical Kuiper Belt objects, of which Ultima is a prime example. We give a short preview of our encounter plans. We note what is currently known about Ultima from Earth-based observations. We then review our expectations and capabilities to evaluate Ultima's composition, surface geology, structure, near space environment, small moons, rings, and the search for activity.

Key Points

  • New Horizons will fly to within 3,500 km of 2014 MU69, acquiring images with pixel scale resolutions significantly better than 100 m/pixel
  • Our spectroscopic observations potentially could detect H2O, CH4, N2, CH3OH, and NH3, depending on their brightness and abundance
  • We will evaluate Ultima's composition, surface geology, structure, near space environment, and the search for small moons, rings, and activity

Plain Language Summary

The letter discusses the current state-of-knowledge for the cold classical Kuiper Belt object 2014 MU69, the target of a close encounter by NASA's New Horizon spacecraft on 1 January 2019. We also review our encounter plans and make broad speculative predictions as to might be revealed by our observations. New Horizons will fly to within 3,500 km of 2014 MU69 (informally named “Ultima Thule”), acquiring images with pixel scale resolutions significantly better than 100 m/pixel). We plan to obtain topography derived from stereo imaging and body shape. Our spectroscopic observations potentially could detect H2O, CH4, N2, CH3OH, and NH3, depending on their brightness and abundance on the surface. We will also search for evidence of outgassing, small moons, and rings. This exploration will transform Kuiper Belt and Kuiper Belt object science from a purely astronomical regime, to a geological and geophysical regime, which radically changed paradigms when the same happened to asteroids and comets in past decades.

1 2014 MU69 in the Context of the Cold Classical Kuiper Belt

The cold classical Kuiper Belt object (CCKBO) 2014 MU69 (“Ultima”) is the flyby primary target for NASA's New Horizons first Kuiper Belt Extended Mission (Stern, Weaver, et al., 2018). The cold classical Kuiper Belt consists of objects on nonresonant, low-eccentricity (e), low-inclination orbits (typically i < 5° to the invariable plane of the solar system), that is, dynamically cold (relatively unexcited) orbits, with heliocentric semimajor axes (a) between about 40 and 50 AU. The cold classical objects likely formed in-place and escaped perturbation from their initial orbits by giant planet migration (Batygin et al., 2011; Dawson & Murray-Clay, 2012; Fraser et al., 2017; Parker & Kavelaars, 2010), making them the most distant known remnants of the original protoplanetary disk. Ultima's orbital elements (a = 44.2 AU, i = 2.4°, e = 0.03; Porter et al., 2018) are fully consistent with it being a CCKBO, as is its visible color (discussed below).

The CCKBOs are on average physically smaller, that is, lacking in large bodies (dwarf planets), as well as following a steep power law size-frequency distribution at the bright, or large end (Fraser et al., 2014; Petit et al., 2011), and they are spectrally redder in the visible and near-infrared than the dynamically hot KBO populations (e.g., Doressoundiram et al., 2008; Tegler & Romanishin, 2000). The dynamically hot KBO populations (hot classicals, bodies in mean-motion resonances with Neptune such as Pluto, scattered disk bodies, etc.) are thought to have formed closer in to the Sun and have been scattered and emplaced in their present orbital configurations by giant planet migration (principally, that of Neptune; Nesvorný & Vokrouhlický, 2016, and references therein). A much larger fraction of the cold classicals are wide binaries as well (at least 30%), compared with the hot classicals (Fraser et al., 2017; Noll et al., 2008; Parker et al., 2011). The steep size distribution and preponderance of binaries suggest that the cold classical population has never been subjected to a period of intense collisional comminution (Nesvorný et al., 2011; Parker & Kavelaars, 2012), unlike other KB subpopulations. The cold classicals thus appear to be a physically and dynamically distinct and likely a more pristinely preserved population.

The upcoming New Horizons flyby of Ultima on 1 January 2019 is a unique opportunity to explore the disk processes and original chemistry of the primordial solar nebula, as well as the nature of CCKBO bodies themselves. Naturally, compositional measurements during the flyby are of paramount importance, as is high-resolution imaging of shape and structure, because the intermediate size of Ultima (much smaller than Pluto but ~103× more massive than a typical comet) may show signs of its accretion from much smaller bodies (layers, aggregates, lobes, etc., in the manner of comet 67P/Churyumov-Gerasimenk; Davidsson et al., 2016; Jutzi & Benz, 2017; Massironi et al., 2015; Nesvorný et al., 2018; Rickman et al., 2015), or alternatively, derivation via the collisional fragmentation of a larger body if KBOs are “born big” (cf. Johansen et al., 2015; Morbidelli & Rickman, 2015; Nesvorný et al., 2010; Schwartz et al., 2018). Ultima is also large enough (of order 20 km × 35 km and possibly a binary; Buie et al., 2018) that it may show some signs of internal evolution driven by radiogenic heat from 26Al decay, if it accreted early enough and fast enough (McKinnon et al., 2008; Prialnik et al., 2007).

2 Highlights of the Planned Observations by New Horizons

A detailed account of this subject is given in Stern, Weaver, et al. (2018); here we briefly summarize: The major science goals of the New Horizons encounter with Ultima are to (1) characterize its global geology, morphology, and rotational characteristics; (2) map its surface composition; (3) search for any satellites and rings and study them as feasible; (4) characterize or constrain its composition and magnitude of any volatile or dust escape from Ultima; (5) characterize the physical properties of its surface; (6) determine its crater size/frequency distribution; (7) constrain its bulk parameters (mass and density); and (8) evaluate evidence of interaction with solar wind. At closest approach New Horizons should pass Ultima at a nominal distance of 3,500 km and at a relative velocity of 14.16 km/s.

On board New Horizons is a suite of remote sensing imagers and fields and particle detectors (see Weaver et al., 2008 for overview). The instruments most relevant to geological and compositional investigations are the Long-Range Reconnaissance Imager (LORRI), Linear Etalon Imaging Spectral Array (LEISA), and Multispectral Visible Imaging Camera (MVIC), the specifications of which are described in detail elsewhere (Cheng et al., 2008; Reuter et al., 2008; Stern, Weaver, et al., 2018). Because the rotational period, shape, and rotation axis orientation of Ultima are not known, it is unclear how much of the object will be seen at high resolution. As described in more detail in Stern, Weaver, et al. (2018), resolved observations of Ultima will begin about 2.5–3 days from the closest approach time (~5:33 UTC). Starting at 39 days to closest approach, unresolved images taken by LORRI will be used to search for rings and satellites, especially in regards to potential navigational hazards to the spacecraft. For ~22 hr preceding the encounter an alternating series of LORRI, MVIC, and LEISA observations will be taken with an increasing cadence designed to be robust to observing different longitudes on the object given different rotation periods. For example, at ~12 hr out, the cadence of observations is every 60 min, while at ~3.5 hr out the cadence is tightened to observations every 20 min. During the 24 hr before closest approach there will also be satellite and ring searches of a broader region of space around Ultima.

Beginning approximately 80 min before closest approach, a series of LORRI images will be taken as ride-along observations during LEISA and MVIC scans of the nominal position of Ultima and the downtrack error ellipse around Ultima, derived from the uncertainty in Ultima's orbit. These observations will provide the highest resolution panchromatic, color, and spectral data on Ultima (Figure 1). LORRI images may be as good as ~35 m/px (with some degradation from smear in one direction) but will generally have lower signal-to-noise than the panchromatic MVIC observations, which reach pixel scales as high as ~135 m/px (and should have little-to-no smear). The nominal phase angle of ~32° for the highest resolution observations should allow for reasonable visual analysis of topographic features (Figure 2).

Details are in the caption following the image
Shown here are the relative fields of view (but not the actual boresights) of the principal remote sensing instruments on New Horizons at the time of closest approach (~05:33 UTC). The model representing Ultima is 30 km across. Best (highest resolution) encounter imaging will take place a few minutes before closest approach in order to optimize surface coverage and lighting (phase angle). Although all three instrument fields-of-view are shown here for reference, only MVIC and LORRI will operate during the final observation before closest approach.
Details are in the caption following the image
The best images of Ultima are planned to have an effective resolution between 42 and 78 m/pixel (as a consequence of smear and signal-to-noise ratio [SNR] effects) at a phase angle between 27 and 55°. What this might resemble can be demonstrated using this High Resolution Imaging Science Experiment image of Phobos (mean diameter 22.5 km), obtained at a phase angle of 26.4° and with resolution degraded to 78 m/pixel, with expected smear and SNR simulated.

Stereo observations are constrained by the close flyby nature of the encounter. Optimal stereo parallax angles are 20 to 30°. The best convergence angle under the nominal flyby plan is approximately 21° (combining the closest approach image at 32° phase and images from the incoming trajectory at 11° phase), but these images also have—at best—a factor of four difference in ground scale (which will make feature correlation difficult). There are observations that provide more similar ground scales, but at the cost of poorer parallax angles (~15°). The best terrain model we expect to be able to make will be approximately 1 km/pixel in ground scale and will have a stereo height accuracy around 300 m. These estimates are based on the assumption that Ultima will not have rotated much in the 20 min to an hour between these observations. If Ultima is a fast rotator, such that these planned observations do not capture the same portion of the surface, then stereo correlation will be significantly more challenging. Shape from shadows and shading will have to suffice.

3 Compositional Knowledge and Speculations

Ices detected on planetary satellites, Centaurs, Pluto, and KBOs in the outer solar system (OSS) include H2O, CH4, N2, CO, CO2, CH3OH (methanol), HCN (hydrogen cyanide), NH3 • nH2O (ammonia hydrate), and C2H6 (ethane; Clark et al., 2013). Most of these represent the inventory expected for low-temperature condensation in the outer parts of the solar nebula (e.g., Lewis, 1972), and a few can be synthesized by chemical processing of the others. At the low temperatures in the OSS the volatility of these ices ranges over many orders of magnitude from the most volatile (N2 and CO) to the least (H2O). Watson et al. (1963) and Lebofsky (1975) calculated the lifetimes against evaporation of icy bodies in the OSS, finding that H2O, CO2, NH3, and NH3 hydrates are highly stable for the age of the solar system, while CH4 evaporation is slow but not negligible. Methane is readily processed by ultraviolet light with charged particles forming a refractory colored solid, so the original CH4 inventory of a small icy body such as Ultima Thule may be locked up in such a material. Ar, Xe, O2, CO, and N2, where exposed at the surface, are expected to have evaporated from Ultima Thule long ago.

The ability of the LEISA imaging spectrometer on New Horizons to detect ices on Ultima depends on the presence of suitably strong spectral absorption bands in its operational wavelength range of 1.25–2.5 μm and native spectral resolution λ/Δλ = 240 (Reuter et al., 2008). H2O, CH4, CH3OH, and NH3 meet these criteria; in data of high signal precision (signal/noise ratio), NH3 hydrates can also be detected, as they were on Pluto's satellites Charon, Nix, and Hydra (Cook et al., 2018). The highest spatial resolution LEISA observation of Ultima will be ~1.8 km px−1, and the highest resolution MVIC color observation will be ~0.3 km px−1.

Ultima has an estimated albedo pV = 0.068 ± 0.006 calculated from mV ≈ 27.5 ± 0.1 (Benecchi et al., 2017; Porter et al., 2018) and an equivalent radius of 15 km; occultation results suggest that Ultima could be a binary or bilobate object of 20 × 35 km size (Buie et al., 2018), implying a somewhat higher pV = 0.087 ± 0.008. Unpublished measurements with the Hubble Space Telescope show that MU69 is red in color, a property shared with many small bodies in the OSS (S. Benecchi, personal communication, 2018; Benecchi et al., 2017). In contrast, Pluto's small satellites Nix and Hydra have much higher visible albedos (0.56 and 0.83, respectively) and generally neutral colors, although Nix has a large red-colored region that may be indicative of an organic component derived from radiation processing of a native hydrocarbon such as CH4 (Weaver et al., 2016). The presumed original CH4 is not, however, detected in the near-infrared spectrum of Nix, which instead is dominated by H2O ice absorption bands plus a band at 2.21 μm attributed to an ammonia hydrate (Cook et al., 2018).

Ultima Thule's low albedo may preclude the detection of any spectral bands attributable to ferro-magnesian silicates or ices, although bands of H2O ice could be observed; in models of mixtures of H2O with dark particles, the absorption bands of water ice at 1.55, 2.0, and 2.3 μm are visible. For example, Phobos has an albedo of 0.07 and no ice bands are seen, while the extremely red-colored Centaur (5145) Pholus has a similarly low albedo at 0.5 μm and clearly detected absorption bands of H2O (2.0 μm) and CH3OH (2.27 μm) ices (Cruikshank et al., 1998). The best fitting model of the Pholus spectrum included magnesium-rich olivine (Fo82) and suggests that ferro-magnesian silicates might occur together with ices on Ultima Thule's surface. In the inner solar system, nanophase neutral iron sputtered from Fe-bearing minerals and deposited on surface grains accounts at least in part for the red colors seen on the Moon and some asteroids, while larger Fe particles contribute to an overall darkening of their surfaces (Pieters & Noble, 2016). The mechanism, efficiency, and long-term effects of this or a similar space weathering process at 44 AU are unknown. Saturn's irregular satellite Phoebe, thought to be a captured object from the Kuiper Belt (Johnson & Lunine, 2005), has a visible albedo pV = 0.0856 ± 0.0023 (Miller et al., 2011) and also has clearly detected absorption bands of H2O (Buratti et al., 2008). Localized exposures richer in ice may also exist. Ultima, however, is much closer in size to Phobos (mean radius 11.3 km) than either Phoebe (mean radius 106.5 km) or (5145) Pholus (mean radius 50–85 km).

As a summary prediction for the properties of Ultima detected with LEISA and MVIC, we might expect to find the H2O ice band at 2 μm, plus possible detections of CO2, or CH3OH bands if they are sufficiently abundant, but probably no CH4, and an overall reddish color suggestive of processed hydrocarbons. Alternatively, there may be red-colored regions superimposed on the otherwise more neutral-colored surface, suggestive of processed hydrocarbons exposed in the subsurface by impact (s), and/or fragmentation, perhaps indicating an irregular early history of accretion from an inhomogeneous source in the solar nebula. There may be outgassing pits or fissures indicative of an original component of N2 or CO that has since been lost. In detail, Ultima is unlikely to look much like comet 67P/CG, which has significantly outgassed by passages close to the Sun and residence time in the inner solar system (possibly losing ~400 m of surface material; Nesvorný et al., 2018), thus affecting the texture, composition, and shape of its surface as revealed by Rosetta.

4 Inferences for Ultima's Gas and Particle Environment

As noted above, it is likely that any highly volatile species (e.g., Ar, Xe, O2, N2, CO, and CH4) that might have once been present on the surface of Ultima are now gone from its surface. However, it is possible that some less volatile ices (e.g., CH3OH, C2H2, C2H6, HCN, and NH3) remain (e.g., Lebofsky, 1975; Schaller & Brown, 2007). Although these species are stable on the surface at their current temperature, ongoing radiation processing and occasional impacts provide a possible source for a transient atmosphere. Although unlikely, such a transient atmosphere will be searched for by the Alice ultraviolet spectrograph (Stern, Weaver, et al., 2018), for example, in absorption, using (i) stellar and (ii) solar appulses, and (iii) in emission, using resonantly scattered solar emissions. Dust coma or material otherwise associated with Ultima will be searched for with high phase angle LORRI and MVIC imaging, and with in situ SDC dust detector observations. In addition, the particle and plasma environment of KBOs is largely unknown. New Horizons fields and particle instruments SWAP and PEPSSI observations will establish the interaction of the interplanetary medium with Ultima, for example, by looking for pickup ions resulting from sputtering of surface materials. Finally, New Horizons Alice, SWAP, and PEPSSI observations will characterize the fluxes of UV, solar wind, interstellar pickup ions, and energetic particles, that is, space weather, that modify KBO surfaces.

5 Geological Outlook and Speculations

The only other KBOs of comparable size to Ultima that have been imaged at pixel scales comparable to what New Horizons will achieve at Ultima are Pluto's small moons Nix and Hydra. Those moons are ~43 and ~45 km in diameter and were imaged by New Horizons at 0.3 and 1.14 km/pixel, respectively (Weaver et al., 2016). New Horizons identified 11 craterlike features identified on Nix and 3 on Hydra. The rims of 3 km diameter craters on Nix have a softened appearance at 0.3 km/pixel, suggesting the possible presence of a mantling material (possibly impact ejecta) covering its surface (see below). Additionally, a faint linear fabric was observed on Nix, probably imparted by the surface expression of internal structure.

The presence of impact craters, a ubiquitous feature on most solar system bodies, is almost certain on Ultima. However, solar system objects that attain sizes comparable to that of Ultima (~30 km across) also have the potential to harbor unusual, and in some cases, possibly active, surface geological processes: several small satellites of Saturn, including Helene and Epimetheus, and Methone (in the extreme) display what appears to be fine-grained material covering large portions of their surfaces. These may be related to the dynamic ring- and midsize moon region of the Saturn system of course (Umurhan et al., 2015). The surface of Phobos, the largest satellite of Mars, displays an unusual system of parallel grooves, as do many asteroids observed in this size range (Figure 2).

Although there have been no detailed predictions published of the collisional rate between Ultima and each of the Kuiper Belt subpopulations as was done for Pluto in advance of flyby (Greenstreet et al., 2015), we expect a cratering rate per km2 of the same order as on Pluto and Charon (JeongAhn et al., 2018). Impact velocities should be somewhat lower than at Pluto and extend down to the escape speed from Ultima (~10 m s−1 for a mean density of 500–1,000 kg m−3). The low velocity tail could be more accretional than erosive, and such events may be efficient at producing ejecta that remains gravitationally bound, reaccreting onto the main body as a mantle. Such a mantle can modify and remove existing craters, altering apparent crater density. Additionally, if a substantial mantle forms, it might become mobile and be transported across large portions of the body's surface by the seismic energy of later impacts.

Sublimation-modified landforms, commonly seen on comets and a number of other solar system objects including Pluto, could have developed on Ultima even if it has never spent any time closer to the Sun than theory suggests for CCKBOs. The volatiles most able to sublimate and form erosional landforms would be surface exposures of N2 and CO and other volatiles as delineated above. If exposed at the surface, CH4 will also sublimate, though much more slowly than N2 and CO. The loss of these volatiles, if present in sufficient quantities and concentrations and susceptible to exposure at the surface, might form distinctive and diagnostic scarps, pits, and perhaps lags (e.g., Moore et al., 1999; Spencer, 1987). By corollary one can speculate that crater rim structures, if initially formed from deposits of volatile-rich material excavated from the interior, could show a unique range of pits, scarps, and lags surrounding the central depression of the original crater. Volatile loss may also mobilize grains in saltation or reptation, the principal grain motions in eolian geology (e.g., Bridges et al., 2012), and these motions may manifest as large eolian ripples as on 67P (Jia et al., 2017; Thomas et al., 2015). The scale of these ripples (low 10s of m wavelength) will be at the limit of the pixel scale of the LORRI camera, though location near the terminator would improve the chances of their detection.

Tectonic features might be reasonably anticipated on Ultima. Many small objects exhibit them, usually in the form of parallel scarps, troughs, or coalescing strings of pits. On objects like the Martian moon Phobos (Figure 2), these features are thought to be the consequence of Martian tides and impact-induced seismic fracturing of the interior (e.g., Buczkowski et al., 2008; Hurford et al., 2016; Morrison et al., 2009; Prockter et al., 2002). The appearance of such features on Ultima would provide insight into the interior strength and coherence.

Finally, the scattering properties of particles on Ultima's surface should become the prototype for those of other CCKBOs. From the disk-resolved analyses of spatially resolved New Horizons LORRI and MVIC images, the surface of Ultima will be the only CCKBO surface whose microphysical structure (macroscopic roughness and single particle phase function) has been characterized by disk-resolved photometric analyses. Furthermore, the disk-integrated solar phase curve derived from New Horizons observations of Ultima will provide context for the interpretation of the disk-integrated phase curves measured by New Horizons of other, distant CCKBOs (Verbiscer et al., 2017; Stern, Weaver, et al., 2018), and enable comparisons between the physical characteristics of particles on their surfaces with those on Ultima's. Comparing Ultima's disk-integrated phase curve with those of other objects in the OSS should reveal whether particles on its surface preferentially scatter incident visible sunlight in the forward direction like those on both Nix and Hydra (Verbiscer et al., 2018) and Phoebe (Buratti et al., 2008).

6 Shape and Structure

Results of the 17 July 2017 stellar occultation by Ultima indicate that this object displays a very irregular shape and could even be a close or contact binary (Buie et al., 2017, 2018; Zangari et al., 2017). Binaries are common in the Kuiper Belt (Noll et al., 2008), including contact binaries (Lacerda, 2011; Lacerda et al., 2014; Thirouin et al., 2017; Thirouin & Sheppard, 2017), and it has been argued that many short period comets, such as 67P/Churyumov-Gerasimenko, 8P/Tuttle, and 103P/Hartley 2, and even 19P/Borrely and 1P/Halley, were formed as or evolved to be contact binaries (or more generally, bilobate bodies; Harmon et al., 2010; Nesvorný et al., 2018; Rickman et al., 2015), albeit from smaller components than the ostensible components of Ultima. Gravitational collapse of “pebble clouds” in the solar nebula is predicted to have naturally and efficiently formed binaries in the Kuiper belt, and with subequal mass ratios (Nesvorný et al., 2010). Some contact and near-contact binary bodies may form by rotational fission (e.g., Walsh et al., 2008), though this relies on a thermal YORP mechanism (effective for small asteroids but relatively ineffective in the Kuiper Belt and for larger bodies) and generally yields small secondary/primary mass ratios.

Close binaries can also form from wider binaries and contact binaries from close binaries, through tidal dissipation of orbital energy, though angular momentum must be removed as well, such as by collisional diffusion, shedding material from the system, or by modifying the spin states of the bodies (e.g., Nesvorný et al., 2018; Porter & Grundy, 2012). Three-body systems can evolve such that the third body is ejected, carrying off energy and angular momentum and allowing the remaining two to become more tightly bound. Even a single body, if elongated and rotating, can become bilobate as the result of a subcatastrophic collision, and at impact velocities well under 1 km s−1 (Jutzi & Benz, 2017; Schwartz et al., 2018). A virtue of being a true binary, as opposed to a contact binary or bilobate body, is that the mass of the system can be estimated (and thus the mean density of Ultima constrained from its total volume) from the size and period of their mutual orbit; determination of the system barycenter from New Horizons images would give the densities of the individual components.

Our current lack of information prevents us from knowing whether or not objects like Ultima entirely form from the low velocity accretion of small (1-mm to 1-m scale) building blocks, variously referred to as spherules or pebbles in the astrophysical literature (e.g., Blum et al., 2017; Johansen et al., 2015; Johansen & Lacerda, 2010). If this is the case, then it might contribute the appearance of a mantle at the best resolution New Horizons will image Ultima (several tens of meters). Conversely, if Ultima's overall appearance is strongly faceted, this would imply that it is a coherent fragment from disruption of a larger parent body, though it has also been argued that catastrophic disruption of a porous, low-strength body may also yield a body similar to 67P (Jutzi et al., 2017; Jutzi & Benz, 2017; Morbidelli & Rickman, 2015).

One of the more remarkable structural features of 67P was the pervasive layering at the surface discovered in Rosetta imaging (Massironi et al., 2015). Though layering had been seen or suspected in other comets, the level of detail provided by Rosetta high-resolution imaging was unprecedented. An approximately 650-m-thick stack of layers, individually between 50 and 200 m thick, envelops both lobes of 67P. The origin of these layers is enigmatic and not agreed upon but is clearly a major clue to the assembly of the comet (cf. Jutzi et al., 2017; Massironi et al., 2015; Schwartz et al., 2018). The best LORRI images of Ultima (~35 m px−1) might just be able to detect layering of the thicknesses seen at 67P, and more easily if layer thicknesses scale with the size the body. Detection and characterization of such layers and other surface and structural features of Ultima is a major goal of the upcoming New Horizons encounter and should advance our understanding of accretion and catastrophic disruption in the Kuiper Belt and thus our overall understanding of early solar system evolution.

7 Moons and Rings

During the approach to Ultima, we will conduct a deep search for small satellites and rings with the LORRI camera. Small satellites have previously been detected around several KBOs (e.g., Brown et al., 2006; Kiss et al., 2017; Parker et al., 2016; Stephens & Noll, 2006), Centaurs (10199) Chariklo and (2060) Chiron, and dwarf planet Haumea have rings (Braga-Ribas et al., 2014; Ortiz et al., 2015, 2017), and the moderately sized (47171) Lempo is a hierarchical triple system (Benecchi et al., 2010).

This search is not just of scientific interest; it is needed to assess any potential hazards to the spacecraft during the flyby. Based on the probable size of Ultima's Hill sphere, satellite orbits could be stable out to distances of ~100,000 km. Simulations of approach phase images indicate that a moon as small as 1 km could be detected, assuming a geometric albedo ~0.1. However, because orbital periods can be very long—decades—it will be difficult to determine the precise orbit of a moon unless it orbits within a few thousand kilometers of Ultima. Narrow rings could potentially be detected in the existing stellar occultation data (Young et al., 2017). Detecting an optically thin dust ring requires LORRI or MVIC. Simulations show that most dust is orbitally unstable near Ultima because solar radiation pressure, although weak, is still stronger than Ultima's gravity. However, Hamilton (2018) has shown that dust can be stable in a “sunflower” configuration, where the orbits are oriented perpendicular to the Sun. Solar radiation pressure keeps the dust in this configuration as Ultima orbits the Sun. Our studies using simulated ring images indicate that LORRI imaging on approach will be capable of detecting broad rings of width 1,000 km to an I/F (reflected/incident solar radiation) of ~3e-8. This limit is deeper than observed at Pluto, due to the reduced stray light of the central body, and the use of longer LORRI exposures than were taken at Pluto (Lauer et al., 2018). Additional high-phase imaging with MVIC may be able to search to even lower optical depth limits.

8 Final Comments

Just as with our encounter with the Pluto system, The New Horizons encounter with Ultima will completely revolutionize our understanding of the small denizens of the Kuiper Belt. Ultima, being a cold classical object, is a particularly exciting opportunity for a close-up investigation of an object probably resident in the OSS since the time of its formation. The story it should tell of solar system origins and the subsequent environment along the solar system's edge since its formation may well place end member values on such topics as impact flux rates and volatile compositions. The encounter with Ultima fills a critical gap in our knowledge about KBOs in its size range: Pluto represents the largest KBO, which underwent substantial differentiation (Stern, Grundy, et al., 2018), while Rosetta's close scrutiny of 67P/Churymov-Gerasimenko revealed the primitive nature of a small (~7-km long by 4-km wide) object from the Kuiper Belt (Taylor et al., 2017). Pluto's moon Charon and Saturn's Phoebe, the latter of which appears undifferentiated and quite possibly originated in the Kuiper Belt (Castillo-Rogez et al., 2012; Johnson & Lunine, 2005), represent medium-sized KBOs, while Ultima fills a critical gap in size between these objects and 67P.

Ultima's exploration—the furthest robotically-visited world in the solar system—has important implications for better understanding the original context of cometary nuclei, the origin of small planets, the solar system as a whole, the solar nebula, and extrasolar disks, as well as studying thermally primitive material from the planet formation era. This exploration will transform Kuiper Belt and KBO science from a purely astronomical regime, to a geological and geophysical regime, which radically changed paradigms when the same happened to asteroids and comets in past decades.

Acknowledgments

We thank the many people, especially the New Horizons Science Team and Engineering Team, who have worked very hard in myriad ways to make the New Horizons mission and the plans for the encounter described here possible. Special thanks to the anonymous reviewer whose suggestions improved the content and clarity of the manuscript. This work was funded by NASA's New Horizons Project. All data from the Ultima Thule encounter, once losslessly received and calibrated, will “ultimately” be posted on the NASA Planetary Data System.