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note
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A shape model using stereophotoclinometry (SPC) has also been generated. The SPC and SPG techniques are complementary, and detailed comparisons, outside the scope of this report, will be made at a later date. The exclusive use of SPG here is solely for internal consistency and simplicity and should not be interpreted as a choice of one approach over the other.
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note
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Although it is unusual for planetary geomorphology works, we do not use a latitude/longitude system for the nucleus at this time because of the ambiguity that would result when using a simple (latitude/longitude) system. An approach to solving the cartographic problem of the highly irregular shape is currently being formulated.
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84921733401
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note
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The sizes of the particles making up the surface layer are not known at this time and are formally constrained only by the resolution limit (∼1 m). The use of the word "dust" should not be interpreted as implying a specific size range.
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note
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Dust forms a thin veneer over the brittle material in the Ma'at and Ash regions. We here avoid the use of the word "mantle"because of the strong geological connotations and the implications of a compositionally different surface layer for which we have no evidence at this time. As noted in the text, layering is evident at several scales, but the origin (primordial or evolutionary) remains open.
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18
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84921821320
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note
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We use the term "brittle material" to imply a rock that breaks/fractures with a high ratio of fine to coarse fragments. It is a weakly consolidated material that displays fracturing but more readily crumbles and creates debris deposits. Fractures contained in more-consolidated material (e.g., in the Aker region) show no evidence of fine fragments.
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84921805689
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note
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2/h, where ρ is the density, g is the gravitational acceleration at the overhang, α is the angle between gravitational acceleration and the normal of the overhang, l is the length of the overhang, and h is its height. For larger, already collapsed, overhangs of ∼200 m in length (e.g., at the Ash-Imhotep interface), we estimate values of σ & le; 200 Pa. Smaller (∼10 m) overhangs are seen (with talus below in some cases where previous collapse has occurred), which suggest that collapse occurs at 10 to 20 Pa.
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20
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84921784699
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note
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We are aware of some work in this field by (35) and unpublished calculations by M. Jutzi, which may be of significance for the future.
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21
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84921728608
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note
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Although the morphology of many surfaces on 67P suggests a rock-like texture, we have avoided using that term here because of the expected very low density of the surfaces when compared to terrestrial rocks. We have adopted the term "consolidated cometary material" instead (CCM).
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Some smooth areas are also seen in the adjacent Khepry region (fig. S10), again at different gravitational heights. This argues against a single flow or a single source of fluidized material being responsible. More complex emplacement mechanisms seem to be required.
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AGU, San Francisco, CA, 2013
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Crack formation through a thermal contraction mechanism in frozen terrestrial soils is discussed in (36).
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A model for the breakup of Comet LINEAR (C/1999 S4)
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