4 results on '"R. Lichtenheldt"'
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2. Stress Analysis of Soil Beneath Grouser Wheel for Planetary Rover by Using Discrete Element Method
- Author
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S. Ono, R. Lichtenheldt, and K. Yoshida
- Abstract
Modeling the interaction between rover's wheel and soft terrain is of great importance in predicting or evaluating wheel performance for lunar and planetary rovers. The current wheel-soil interaction models predict or evaluate wheel performance under certain conditions. However, most of them do not consider the soil flow and deformation, and thus, they cannot capture the physical phenomena of wheel-soil interaction. Developing a new model that includes such physical phenomena contributes to the improvement of prediction accuracy. To develop such a model, it is necessary to analyze soil flow and deformation beneath the wheel. This study analyzes the stress distributions in the soil and soil flow fields beneath the grouser wheel by performing experiments using the discrete element method (DEM) with the particle simulation tool "Sir partsival". In addition to the single wheel simulation, two simple test simulations - an angle of repose test and a shear test - are performed to confirm the soil flow fields and stress distributions in the soil. In the field of fluid dynamics, (shear) stress generally exists along high gradients of flow velocity. These two tests confirm if the soil stress shows the same trend. The wheel simulations are performed under several slip conditions to investigate their influences on soil flow characteristics. The shape of the soil flow region - the shape of the slip line - can be divided into two patterns depending on the slip conditions. The stress increases along the slip line in all simulations. The findings of this study contribute to understanding the relationship between soil velocity field and stress distribution in the soil.
- Published
- 2022
3. The InSight HP
- Author
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T, Spohn, T L, Hudson, E, Marteau, M, Golombek, M, Grott, T, Wippermann, K S, Ali, C, Schmelzbach, S, Kedar, K, Hurst, A, Trebi-Ollennu, V, Ansan, J, Garvin, J, Knollenberg, N, Müller, S, Piqueux, R, Lichtenheldt, C, Krause, C, Fantinati, N, Brinkman, D, Sollberger, P, Delage, C, Vrettos, S, Reershemius, L, Wisniewski, J, Grygorczuk, J, Robertsson, P, Edme, F, Andersson, O, Krömer, P, Lognonné, D, Giardini, S E, Smrekar, and W B, Banerdt
- Abstract
The NASA InSight Lander on Mars includes the Heat Flow and Physical Properties Package HPThe online version contains supplementary material available at 10.1007/s11214-022-00941-z.
- Published
- 2021
4. The InSight HP 3 Penetrator (Mole) on Mars: Soil Properties Derived from the Penetration Attempts and Related Activities.
- Author
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Spohn T, Hudson TL, Marteau E, Golombek M, Grott M, Wippermann T, Ali KS, Schmelzbach C, Kedar S, Hurst K, Trebi-Ollennu A, Ansan V, Garvin J, Knollenberg J, Müller N, Piqueux S, Lichtenheldt R, Krause C, Fantinati C, Brinkman N, Sollberger D, Delage P, Vrettos C, Reershemius S, Wisniewski L, Grygorczuk J, Robertsson J, Edme P, Andersson F, Krömer O, Lognonné P, Giardini D, Smrekar SE, and Banerdt WB
- Abstract
The NASA InSight Lander on Mars includes the Heat Flow and Physical Properties Package HP
3 to measure the surface heat flow of the planet. The package uses temperature sensors that would have been brought to the target depth of 3-5 m by a small penetrator, nicknamed the mole. The mole requiring friction on its hull to balance remaining recoil from its hammer mechanism did not penetrate to the targeted depth. Instead, by precessing about a point midway along its hull, it carved a 7 cm deep and 5-6 cm wide pit and reached a depth of initially 31 cm. The root cause of the failure - as was determined through an extensive, almost two years long campaign - was a lack of friction in an unexpectedly thick cohesive duricrust. During the campaign - described in detail in this paper - the mole penetrated further aided by friction applied using the scoop at the end of the robotic Instrument Deployment Arm and by direct support by the latter. The mole tip finally reached a depth of about 37 cm, bringing the mole back-end 1-2 cm below the surface. It reversed its downward motion twice during attempts to provide friction through pressure on the regolith instead of directly with the scoop to the mole hull. The penetration record of the mole was used to infer mechanical soil parameters such as the penetration resistance of the duricrust of 0.3-0.7 MPa and a penetration resistance of a deeper layer ( > 30 cm depth) of 4.9 ± 0.4 MPa . Using the mole's thermal sensors, thermal conductivity and diffusivity were measured. Applying cone penetration theory, the resistance of the duricrust was used to estimate a cohesion of the latter of 2-15 kPa depending on the internal friction angle of the duricrust. Pushing the scoop with its blade into the surface and chopping off a piece of duricrust provided another estimate of the cohesion of 5.8 kPa. The hammerings of the mole were recorded by the seismometer SEIS and the signals were used to derive P-wave and S-wave velocities representative of the topmost tens of cm of the regolith. Together with the density provided by a thermal conductivity and diffusivity measurement using the mole's thermal sensors, the elastic moduli were calculated from the seismic velocities. Using empirical correlations from terrestrial soil studies between the shear modulus and cohesion, the previous cohesion estimates were found to be consistent with the elastic moduli. The combined data were used to derive a model of the regolith that has an about 20 cm thick duricrust underneath a 1 cm thick unconsolidated layer of sand mixed with dust and above another 10 cm of unconsolidated sand. Underneath the latter, a layer more resistant to penetration and possibly containing debris from a small impact crater is inferred. The thermal conductivity increases from 14 mW/m K to 34 mW/m K through the 1 cm sand/dust layer, keeps the latter value in the duricrust and the sand layer underneath and then increases to 64 mW/m K in the sand/gravel layer below., Supplementary Information: The online version contains supplementary material available at 10.1007/s11214-022-00941-z., Competing Interests: Competing InterestsThe authors declare that they have no conflict of interest., (© The Author(s) 2022.)- Published
- 2022
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