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首页> 外文期刊>Journal of geophysical research. Planets >Mobile lid convection beneath Enceladus' south polar terrain
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Mobile lid convection beneath Enceladus' south polar terrain

机译:土卫二南极地形下的活动盖对流

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Enceladus' south polar region has a large heat flux, 55–110 mW m?2, that is spatially associated with cryovolcanic and tectonic activity. Tidal dissipation and vigorous convection in the underlying ice shell are possible sources of heat, however, prior predictions of the heat flux carried by stagnant lid convection range from F conv ~ 15 to 30 mW m?2, too low to explain the observed heat flux. The high heat flux and increased cryovolcanic and tectonic activity suggest that near-surface ice in the region has become rheologically and mechanically weakened enough to permit convective plumes to reach close to the surface. If the yield strength of Enceladus' lithosphere is less than ~1–10 kPa, convection may instead occur in the “mobile lid” regime, which is characterized by large heat fluxes and large horizontal velocities in the near-surface ice. I show that model ice shells with effective surface viscosities between 1016 and 1017 Pa s and basal viscosities between 1013 and 1015 Pa s have convective heat fluxes comparable to that observed by Composite Infrared Spectrometer. If this style of convection is occurring, the south polar terrain should be spreading horizontally with v ~1–10 mm a?1 (where a is years) and should be resurfaced in ~0.1–10 Ma. On the basis of Cassini imaging data, the south polar terrain is ~0.5 Ma old, consistent with the mobile lid hypothesis. Maxwell viscoelastic tidal dissipation in such ice shells is not capable of generating enough heat to balance convective heat transport. However, tidal heat may also be generated in the near-surface along faults as suggested by Nimmo et al. (2007) and/or viscous dissipation within the ice shell may occur by other processes not accounted for by the canonical Maxwell dissipation model.
机译:土卫二的南极地区具有较大的热通量,为55-110 mW m?2,在空间上与低温火山活动和构造活动有关。下层冰壳中的潮汐消散和剧烈对流可能是热源,但是,先前对停滞盖对流所携带的热通量的预测范围为F conv〜15至30 mW m?2,太低而无法解释观察到的热通量。高热通量和增强的低温火山活动和构造活动表明,该区域的近地表冰在流变学和机械上已变得足够弱,足以使对流羽流接近地表。如果土卫二岩石圈的屈服强度小于〜1-10 kPa,则在“活动盖”状态下可能会发生对流,其特征是近地表冰中的热通量大且水平速度大。我表明,有效表面粘度在1016和1017 Pa s之间且基础粘度在1013和1015 Pa s之间的模型冰壳具有与复合红外光谱仪观察到的对流热通量。如果发生这种形式的对流,则南极地形应以v〜1–10 mm a?1(其中a是年)的水平方向扩展,并应在〜0.1–10 Ma内重新出现。根据卡西尼号的影像资料,南极地形约〜0.5 Ma,与活动盖假说相符。这种冰壳中的麦克斯韦粘弹性潮汐耗散不能产生足够的热量来平衡对流传热。但是,如Nimmo等人的建议,沿断层在近地表也可能产生潮汐热。 (2007年)和/或冰壳内的粘性耗散可能由标准麦克斯韦耗散模型未考虑的其他过程发生。

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