Aerodynamic roughness of rippled beds under active saltation at Earth-to-Mars atmospheric pressures

As winds blow over sand, grains are mobilized and reorganized into bedforms such as ripples and dunes. In turn, sand transport and bedforms affect the winds themselves. These complex interactions between winds and sediment render modeling of windswept landscapes challenging. A critical parameter in such models is the aerodynamic roughness length, z<sub>0</sub>, defined as the height above the bed at which wind velocity predicted from the log law drops to zero. In aeolian environments, z<sub>0</sub> can variably be controlled by the laminar viscous sublayer, grain roughness, form drag from bedforms, or the saltation layer. Estimates of z<sub>0</sub> are used on Mars, notably, to predict wind speeds, sand fluxes, and global circulation patterns; yet, no robust measurements of z<sub>0</sub> have been performed over rippled sand on Mars to date. Here, we measure z<sub>0</sub> over equilibrated rippled sand beds with active saltation under atmospheric pressures intermediate between those of Earth and Mars. Extrapolated to Mars, our results suggest that z<sub>0</sub> over rippled beds and under active saltation may be dominated by form drag across a plausible range of wind velocities, reaching values up to 1 cm-two orders of magnitude larger than typically assumed for flat beds under similar sediment transport conditions.

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Publication Details

Journal
Nature Communications
Published
2025-06-02
DOI
https://doi.org/10.1038/s41467-025-60212-7
Citations
5
Primary Topic
Aeolian processes and effects
Type
article
Field-Weighted Citation Impact
8.35

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article

Aerodynamic roughness of rippled beds under active saltation at Earth-to-Mars atmospheric pressures

Philippe Claudin, Pan Jia, M. G. A. Lapôtre, Carlos A. Alvarez et al.
5 citations
Nature Communications
Aeolian processes and effects
8.35
article

Aerodynamic roughness of rippled beds under active saltation at Earth-to-Mars atmospheric pressures

Philippe Claudin, Pan Jia, M. G. A. Lapôtre, Carlos A. Alvarez, Christy Swann, R. C. Ewing
article en
5 citations

Abstract

As winds blow over sand, grains are mobilized and reorganized into bedforms such as ripples and dunes. In turn, sand transport and bedforms affect the winds themselves. These complex interactions between winds and sediment render modeling of windswept landscapes challenging. A critical parameter in such models is the aerodynamic roughness length, z<sub>0</sub>, defined as the height above the bed at which wind velocity predicted from the log law drops to zero. In aeolian environments, z<sub>0</sub> can variably be controlled by the laminar viscous sublayer, grain roughness, form drag from bedforms, or the saltation layer. Estimates of z<sub>0</sub> are used on Mars, notably, to predict wind speeds, sand fluxes, and global circulation patterns; yet, no robust measurements of z<sub>0</sub> have been performed over rippled sand on Mars to date. Here, we measure z<sub>0</sub> over equilibrated rippled sand beds with active saltation under atmospheric pressures intermediate between those of Earth and Mars. Extrapolated to Mars, our results suggest that z<sub>0</sub> over rippled beds and under active saltation may be dominated by form drag across a plausible range of wind velocities, reaching values up to 1 cm-two orders of magnitude larger than typically assumed for flat beds under similar sediment transport conditions.

Nature CommunicationsVol. 16(1)
Centre National de la Recherche Scientifique (FR), Planetary Science Institute (US), University of New Orleans (US), Université Paris Cité (FR), Harbin Institute of Technology (CN), Sorbonne Université (FR), Physique et Mécanique des Milieux Hétérogènes (FR), Johnson Space Center (US), Stanford University (US)
National Aeronautics and Space Administration, National Natural Science Foundation of China, Nuclear Safety and Security Commission, National Natural Science Foundation of China-Yunnan Joint Fund
Climate action
Openalex Percentile: Top 2%
Aeolian processes and effects
8.35
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