Can Slope-Dependent Transport Explain Martian Crater Profiles

Slides:



Advertisements
Similar presentations
Guided Notes on Erosion and Deposition
Advertisements

Hillslope morphology Ch 8. Hillslope Types Soil-mantled Soil-mantled –Transport-limited –Shape: smooth, rounded Bare bedrock or thin soils Bare bedrock.
Martian Craters with Interior Deposits: Global Survey Results and Wind Model P21D-1875 Kristen A. Bennett 1 and Mark Schmeeckle 2 1 School of Earth and.
EROS (Crave & Davy, 2001) “Stochastic model of erosion– sedimentation processes, based on cellular automata, which mimics the natural variability of climatic.
Sam Coleman Northern Arizona University USGS-Flagstaff Mentor: Dr. Rosalyn Hayward.
The timing of, duration of, and wind patterns driving sand saltation on Mars are typically poorly constrained. The patterns of aeolian activity within.
A.Erosion – The transportation of weathered sediments 1. Agents of Erosion or Transport Systems: a. Running water b. Wind c. Glaciers d. Waves & Tidal.
Landscape Development
The Growth and Erosion of Cinder Cones An Article Summary Kelsii Dana.
Effect of Subsidence Styles and Fractional Diffusion Exponents on Depositional Fluvial Profiles Vaughan Voller: NCED, Civil Engineering, University of.
Alluvial Fan Science Potential Kelin X. Whipple and Kelli Wakefield School of Earth and Space Exploration Arizona State University.
Conclusions of small-scale geomorphology Off road vehicles have lasting affects on desert environment Channels in walkway plots are bimodal and follow.
National Center for Earth-surface Dynamics Modeling physical and ecological dynamics of channel systems that shape Earth’s surface Moving boundary problems.
Flood Mapping and Sediment Transport in Otsego County Streams, New York By Les Hasbargen, Tyson Robb, Anthony Grimes, and Roy Widrig Earth Sciences Department,
Ancient Glaciation on Mars By J. Kargel, R. Strom presented by Megan Simpson.
Contour lines. Contour lines: curved lines drawn on the map, connecting points having the same elevation.
Erosion By Water and Wind.
National Aeronautics and Space Administration Jet Propulsion Laboratory California Institute of Technology NASA Exoplanet Science Institute Group Projects:
Earth’s History Section 4.1
Gradation Landforms are continuously changing: Tectonic and Volcanic activity builds up the earth and gradation forces try to level the earth If Gradational.
SPECIFICATION TARGET: to be able to explain the impact of weathering, erosion and mass movement on river landscapes.
Nicole Gasparini Arizona State University Landscape Modeling.
Landscape Evolution Modeling ERODE Irina Overeem, February 2013.
Numerical Analysis of Flow and Mixing Phenomena of Municipal Solid Waste Particles on a Reverse Acting Grate Masato R. Nakamura, Marco J. Castaldi, and.
The Impact of Orographic Precipitation on the Form of Mountain Ranges Alison Anders Earth and Space Sciences Dale Durran Atmospheric Sciences Gerard Roe.
Numerical models of landscape evolution Mikaël ATTAL Marsyandi valley, Himalayas, Nepal Acknowledgements: Jérôme Lavé, Peter van der Beek and other scientists.
Searching for Columnar Jointing on Mars Brittany Meucci Mentor- Dr. Moses Milazzo Northern Arizona University-NASA Space Grant 25 cm/pixel.
Identifying Ancient Glacial Features in The Circum-Argyre Region, Mars, Using HiRISE, CTX, and MOC Imagery Alexander Prescott Mentor: Victor R. Baker Department.
Gravity Physical Science Section 3.2. Gravity All objects have a gravitational attraction for all other objects Law of Gravitation- Any two masses exert.
If the sum of all the forces acting on a moving object is zero, the object will (1) slow down and stop (2) change the direction of its motion (3) accelerate.
1 Volatile Exchange on Mars Maria T. Zuber MIT David E. Smith NASA/GSFC 16 th International Workshop on Laser Ranging Poznan, Poland 13 October 2008 NASA/MRO/HiRISE.
Partnership for AiR Transportation Noise and Emission Reduction An FAA/NASA/TC-sponsored Center of Excellence Matthew Woody and Saravanan Arunachalam Institute.
Lava Flows of Arsia Mons, Mars Ruben Rivas College of Engineering University of Arizona (Tucson, Az) Space Grant Mentor: David Crown Planetary Science.
Software used: ArcMap , MatLab R2015b, Google Earth 7.1.5
Bradley Central High School
1 INTRODUCTION TO “Stratigrafia” The code in the workbook “stratigrafia” computes - longitudinal profiles; - water surface elevation; - sediment transport.
BACKGROUND MARS Research Presentation By Bradley Central Chemistry 3 rd Period Dr. Buckner.
Section 4: Earth’s Moon. What are we learning about today? 1. What features are found on the moon’s surface? 2. What are some characteristics of the moon?
Lunar Orbit Anomaly and GM=tc 3 Cosmology L. Riofrio, University of Houston, Clear Lake, Texas European Planetary Science Conference, Madrid September.
Earth Science Notes Wind Erosion. Objectives I can… Explain how wind changes the Earths surface Describe the different types of Wind Erosion Describe.
Impact craters are geologic structures formed when a large meteoroid, asteroid or comet smashes into a planet or a satellite.Impact craters are geologic.
Modeling the impact of vegetation changes on erosion rates and landscape evolution Jon D. Pelletier, University of Arizona.

of Temperature in the San Francisco Bay Area
EROSION: The force that shapes the Earth!
Topic 14 – Landscape Development and Environmental Change
Landscape Development
Accuracy of Cosmogenic Ages for Moraines
Mass Movements, Wind, and Glaciers
Landscape Development
Science Jeopardy!.
11.1 The Active River.
Nathan White Mentor: Dr. Nadine Barlow Northern Arizona University
Morphodynamic and Sediment Tracers in One-Dimension
of Temperature in the San Francisco Bay Area
Clark R. Chapman Southwest Research Inst. Boulder, CO USA
Warm-up What 3 particles are used to determine soil texture?
Craters on Mars DRAFT Google Earth.
Estimating the Age of Lava Flows on Mars
Gradual, Incremental Hillslope Transport:
Aeolian dune sediment flux heterogeneity in Meridiani Planum, Mars
Biogenic transport—slope dependent
Dept. of Earth and Atmospheric Sciences
Arizona Space Grant Consortium
Rivers and Running Water
AIM: What is a stream/river?
Dune-Yardang Interactions in Becquerel Crater, Mars
Mass Movements.
The Role of Stretching in Slow Axonal Transport
From the Convection Zone to the Heliosphere
Presentation transcript:

Can Slope-Dependent Transport Explain Martian Crater Profiles 12 km 6 km 15 km 18 km 21 km 3 km 9 km 0 km -9 km -6 km -3 km Can Slope-Dependent Transport Explain Martian Crater Profiles Sara Goldenbaum and Les Hasbargen Dept. of Earth and Atmospheric Sciences , SUNY Oneonta, NY, 13820 Saragoldenbaum@gmail.com Session 227 : “T206. Geomorphology and Landscape Evolution of Mars : The GK Gilbert Award Session (Posters)” Tuesday, 24 October 2017 9 AM – 6:30 PM Booth Number : 353 Martian impact craters have rims and walls that have been modified by surface processes. Indeed, the craters on Mars vary drastically in age as well as size and degree of degradation. Of the many mechanisms of mass transport, we chose a simple model of downslope gravity driven transport as a testable hypothesis. We constructed a numerical model in a spreadsheet of how a crater profile would change over time. We assume that sediment transport rate varies according to slope magnitude, and this results in a diffusive-like model. The mathematical elevation profile evolves through time based on spatial changes of sediment transport rate.The model has seven variables that must be specified including initial elevation; diffusivity; time step size; spacing between nodes in the solution; two boundary flux conditions; and duration of a simulation. We performed sensitivity tests in order to see how each variable affected the mathematical profile. We found a moderate range in forms can develop in the model, with the dominant control exerted by boundary flux conditions. Old craters, if they evolve according to a slope-dependent transport model, should smoothly fill from the edges inward, relief and slope should decline over time, and the point on the profile which divides the eroding section from the depositing section should very slowly migrate toward the crater center over time. The profile evolves toward a constant boundary between erosion-deposition areas early in the evolution, coincident with ~0.5 crater relief. Thus, no bedrock should be visible below that height. We test these predictions against a cohort of Martian crater profiles extracted from Mars Orbiter Laser Altimeter data that range in degree of degradation. Relief and slope covary for the craters, with lower slope coinciding with lower crater relief, consistent with the model. We are initiating a search of HiRise imagery to test the erosion-deposition transition location. Conclusions The main sediment transportation process that our model takes into account is gravity driven transport. The older craters are less steep and have lower slopes then younger ones Older craters show less relief Parabolic crater floors are not obvious in old craters in our data set Example of the crater selection process in the JMARS interface. Individual profiles can be exported to csv files and compiled in a spreadsheet (see below). Acknowledgements We thank NASA, Arizona State University and JMARS team for providing access to Mars elevation data in a very user friendly software Attendance at the conference was made possible in part by a grant from the D’Antonio Travel for Excellence Fund, SUNY Oneonta At left is a numeric evolution of a Mars crater profile showing how it evolves over time. The crater slopes decrease in steepness Crater relief declines Crater floors aggrade in a parabolic form The boundary between erosion and deposition remains constant over time At left we plot several profiles of Mars craters. Each of these craters are of different ages but approximately the same size. We chose craters that were between 10 and 40 km wide. It appears older profiles are less steep with lower relief and possibly the valley floors became more rounded overtime in Martian craters.