Pluto's Ocean Is Capped and Insulated by Gas Hydrates

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Pluto's Ocean Is Capped and Insulated by Gas Hydrates ARTICLES https://doi.org/10.1038/s41561-019-0369-8 Pluto’s ocean is capped and insulated by gas hydrates Shunichi Kamata 1,8*, Francis Nimmo 2, Yasuhito Sekine 3, Kiyoshi Kuramoto 4, Naoki Noguchi 5, Jun Kimura 6 and Atsushi Tani 7 Many icy Solar System bodies possess subsurface oceans. On Pluto, Sputnik Planitia’s location near the equator suggests the presence of a subsurface ocean and a locally thinned ice shell. To maintain an ocean, Pluto needs to retain heat inside. On the other hand, to maintain large variations in its thickness, Pluto’s ice shell needs to be cold. Here we show, by thermal evolu- tion and viscous relaxation calculations, that the presence of a thin layer of clathrate hydrates (gas hydrates) at the base of the ice shell can explain both the long-term survival of the ocean and the maintenance of shell thickness contrasts. Clathrate hydrates act as a thermal insulator, preventing the ocean from completely freezing while keeping the ice shell cold and immo- bile. The most likely clathrate guest gas is methane, derived from precursor bodies and/or cracking of organic materials in the hot rocky core. Nitrogen molecules initially contained and/or produced later in the core would probably not be trapped as clath- rate hydrates, instead supplying the nitrogen-rich surface and atmosphere. The formation of a thin clathrate hydrate layer cap to a subsurface ocean may be an important generic mechanism to maintain long-lived subsurface oceans in relatively large but minimally heated icy satellites and Kuiper belt objects. iquid water oceans are thought to exist inside icy satellites of Another possibility is that the viscosity of the ice shell is high due gas giants such as Europa and Enceladus and the icy dwarf to the presence of high-strength material, such as salts12 or silicate planet Pluto1. Understanding the survival of subsurface oceans particles13. However, in a multiphase system, the weaker phase L 12,13 is of fundamental importance not only to planetary science but also (that is, water ice) dominates the flow . Consequently, inhibiting to astrobiology. One indication of a subsurface ocean on Pluto is substantial viscous relaxation requires the stronger phase (that is, Sputnik Planitia, a ~1,000-km-wide basin. It is a topographical low salts) to be the dominant component. Such an ice shell would have −3 and is located near the equator, indicating that it is a positive gravity a high density (for example, ~1.3 g cm for a mixture of 50% H2O anomaly. To make this basin a positive gravity anomaly, a subsurface ice and 50% epsomite). While the density of the ocean might also be ocean beneath a locally thinned ice shell (by ~90 km) is inferred2. high due to the presence of salts in the ocean11, their concentrations The presence of an ocean suggests a ‘warm’ (that is, not com- would be largely controlled by the formation of clay minerals and pletely frozen) Pluto. However, unlike icy satellites, tides do not play evaporates in the rocky core, keeping the ocean salinity <4–5 mol l−1 3 14 an important role in heating the dwarf planet , and radiogenic heat- or <10 mol% relative to H2O (ref. ) and, thus, the ocean density ing is insufficient to avoid complete freezing unless the ice shell is <1.3 g cm−3. For the ice shell to float on the ocean and for Sputnik highly viscous (greater than ~1016 Pa s (ref. 4)). Heat may be retained Planitia to be a positive gravity anomaly, the ice shell has a density inside Pluto owing to a thick surface thermal insulating layer much lower than the ocean (at least by ~0.2 g cm−3 (ref. 11)), and its resulting from high porosity and a high concentration of nitrogen major constituent needs to be water ice. ice5. However, if the ice shell is warm, its viscosity should be low6. Instead, we propose that the ice shell has a thin layer of clath- Substantial viscous flow of ice would then occur, eliminating any rate hydrates at its base (Fig. 1). Clathrate hydrates, or gas hydrates, local thickness contrasts7. Consequently, a locally thinned shell sug- are solids in which water molecules create cages trapping gas mol- gests a ‘cold’ Pluto (lower than ~200 K at the base of the ice shell2). ecules15. As the formation temperatures of clathrate hydrates are One way to reconcile these contradictory requirements is to depress higher than the melting point of pure water ice15 and the subsurface the freezing point of water by contaminating the ocean with anti- ocean is sufficiently pressurized by the overlying ice shell, a freezing freeze molecules, such as ammonia2. However, to avoid substantial ocean would form clathrate hydrates rather than water ice if dis- viscous relaxation of the ice shell, the ammonia concentration needs solved gas concentrations are sufficiently high16. The thermal con- to be ~30 wt% (Supplementary Fig. 1). Such a high concentration is ductivity of clathrate hydrates is about a factor of 5–10 smaller than hard to justify; the ammonia concentration in comets, whose chem- that of water ice17 and the viscosity of clathrate hydrates is about an ical composition should be representative of Kuiper belt objects order of magnitude higher than that of water ice18. As a result of including Pluto8, is mostly less than 1% with respect to water9. In these physical properties, a cap of clathrate hydrates would act as addition, an ammonia concentration >20 wt% leads to an ocean a highly viscous thermal insulator between a subsurface ocean and density <1,000 kg m−3 (Supplementary Fig. 2, ref. 10), which makes an ice shell. The temperature difference across this layer allows the it difficult for Sputnik Planitia to be a positive gravity anomaly11. presence of a subsurface ocean with a temperature near the melting 1Creative Research Institution, Hokkaido University, Sapporo, Japan. 2Department of Earth and Planetary Sciences, University of California, Santa Cruz, Santa Cruz, CA, USA. 3Earth-Life Science Institute, Tokyo Institute of Technology, Tokyo, Japan. 4Department of Cosmosciences, Hokkaido University, Sapporo, Japan. 5Graduate School of Technology, Industrial and Social Sciences, Tokushima University, Tokushima, Japan. 6Department of Earth and Space Science, Osaka University, Toyonaka, Japan. 7Department of Human Environmental Science, Kobe University, Kobe, Japan. 8Present address: Department of Earth and Planetary Sciences, Hokkaido University, Sapporo, Japan. *e-mail: [email protected] NatURE GEOSCIENCE | www.nature.com/naturegeoscience ARTICLES NATURE GEOSCIENCE Nitrogen-rich ice Temperature of methane hydrates15,17,18 (Methods). The origin of the local inte- Without rior structure beneath Sputnik Planitia (a thin ice shell above a With Water-rich ice clathrate clathrate thick ocean) is considered to be associated with the large impact hydrates 2,11 hydrates that formed the Sputnik Planitia basin . Although the age of this Clathrate hydrate impact is unknown, the eroded rim of the basin suggests that it is 23 Subsurface ocean likely to be billions of years . Consequently, the timescale of viscous Depth relaxation should be at least one billion years. Rocky core If a clathrate hydrate layer does not exist, shell thickness contrasts can be maintained for only a few million years unless an extremely viscous ice shell and/or an extremely cold ocean is assumed (Fig. 3 and Supplementary Fig. 5). In contrast, if a clathrate hydrate layer of a few to 10 km in thickness exists at the base of the ice shell, the timescale of ice shell relaxation is increased even by 3 to 4 orders Fig. 1 | A schematic diagram of the interior structure of Pluto. The ice shell of magnitude and can exceed one billion years even if we assume has a thin clathrate hydrate layer at its base. The temperature changes typical pure-water properties both for the water ice layer and the substantially across this layer immediately above the subsurface ocean, ocean (Fig. 3). Such a large increase in the timescale results from the leading to a conductive shell rather than a convective shell. Nitrogen-rich combined effect of a low temperature in the water ice layer and the ice on the surface is the bright surface of Sputnik Planitia. high viscosity of clathrate hydrates (Supplementary Fig. 6). Thus, under the presence of a thin clathrate hydrate layer, an extremely ammonia- or salt-rich Pluto is no longer necessary to explain a long point of pure water ice while the overlying ice shell maintains a viscous relaxation timescale for the ice shell. much lower temperature at the same time. Its high viscosity would also maintain shell thickness contrasts for a long time. Implications for geochemical evolution Various gas species can form clathrate hydrates, although some Global thermal evolution of Pluto species (for example, CH4) occupy clathrate hydrates more read- 15,16 We first evaluate the effect of clathrate hydrates on the thermal evo- ily than others (for example, N2) (refs. ). This behaviour may lution of Pluto using the physical properties of methane hydrates explain the unique volatile composition observed on Pluto. Comets 15,17 9 (CH4 · nH2O, where n ≈ 6 (refs. )) (Methods). In the absence of contain ~1% of CH4 and a few percent of CO with respect to water , clathrate hydrates, a subsurface ocean is expected to freeze com- and even these low concentrations are sufficient to form a clath- pletely because thermal convection in the ice shell removes heat rate hydrate layer several tens of kilometres in thickness (Methods effectively from the deep interior4 (Fig. 2a,b). To maintain a thick and Supplementary Fig. 7). When Pluto formed, volatiles trapped in subsurface ocean, the ice shell needs to be conductive, requiring a precursor bodies would have been partitioned between the atmo- reference viscosity about one or two orders of magnitude higher sphere, the ice shell and the subsurface ocean.
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