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Additional file 1 of Variation of crater morphological parameters in the landing area of Tianwen-1: relationships with the geological environment and climate change

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posted on 2024-08-14, 20:09 authored by Yu Yang, Yi Wang, Bo Li, Zongcheng Ling, Yang Liu, Shaojie Qu, Shengbo Chen
Additional file 1: Fig. S1. Crater depth raster (1 m per pixel). Depth is calculated by fitting a 3D plain across the rim using the points shown. Each point is assigned an elevation value from the HiRISE DEM. The DEM is then subtracted from the overlying 3D surface. Note: (e) is the 3D representation of (d). Fig. S2. Crater rim height raster (1 m per pixel) with the 0.2D annular region that generally defines the majority of the rim structure for all craters. Rim height is calculated by fitting a plain across the continuous ejecta blanket (1D from crater rim). This 3D plane defines the pre‐ impact surface and is subtracted from the overlying DEM. Note: (g) is the 3D representation of (f). Fig. S3. (a) The low-frequency radar imaging profile, with the uppermost thick black line denoting the topography relative to the landing site. The dashed line above 10 m denotes the estimated bottom of the top layer presumably containing mainly regolith. The two solid lines at depths of around 30 and 80 m represent the contacts between the second and third layers and the base of the third layer, respectively. The two dashed lines at around 10 and 40 m deep roughly separate finer- and coarser-grained rocky blocks within the second and third layers, respectively. (b) The interpreted lithologic stratigraphy based on radar imaging. (c) The variation of dielectric permittivity with depth. (Image credit: Chao Li et al.; 2022, Nature).

Funding

the National Key Research and Development Program of China the Strategic Leading Science and Technology Special Project of Chinese Academy of Sciences the National Natural Science Foundation Natural Science Foundation of Shandong Province

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