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Discrete Modeling Research

Snow

Picture showing snow drifting over the trunda.

       More than 40% of the northern hemisphere is affected by seasonal snow, including the U.S., Canada, most of Europe, and northern Asia (Turkey, Iran, Afghanistan, and Russia). The presence of snow strongly affects vehicle mobility, sensors, and the ground state in winter and in mountains. Our goal is to develop an accurate snow model that can be used to solve problems that depend on the ability to realistically simulate snow deformation, metamorphosis, and electromagnetic and radiative interaction. We have developed a three-dimensional discrete-element-based (DEM) snow model that differs from all other snow models in having an explicit geometric structure composed of a large aggregate of discrete, individual snow grains. The model contains the fundamental grain-scale processes that underlie snow deformation. Interactions between grains are governed by contact algorithms for sintering, deformation, and failure. Consequently, this model can be used to investigate problems in which knowledge of the microstructure of the snow is important, such as dynamic simulations of the interaction of tires and tracks with snow and calculations of snow grain surface-to-volume ratios important in electromagnetic and radiative processes. These processes are impossible to simulate using continuum models. We have used the model to perform simulations of snow settlement, shear, and micro-penetration that qualitatively reproduce experimental results.

Below are links to two Power Point Presentations
on Discrete Element (DEM) snow modeling:

Picture of man standing in fresh snow.  Click here to view powerpoint presentation: A Discrete Element Method for Snow Mechanics I.
Click on Picture above for Power Point presentation:

A Discrete Element Method for
Snow Mechanics I

Picture of tire pressing on simulated snow.  Click here to see Powerpoint presentation: A Descrete Element Method for Snow Mechanics II.
Click on Picture above for Power Point presentation:

A Discrete Element Method for
Snow Mechanics II

 

        The DEM technique is a logical tool to use to simulate snow because, in addition to employing the grain-scale process models, it has an explicit geometric structure that is composed of individual ice grains and grain clusters and that evolves with deformation and metamorphosis. The DEM model snow consists of a large assembly of grains with an arbitrary mixture of axisymmetric particle shapes, including spheres, tapered cylinders, and elongated or oblate spheroids and ellipsoids. Grains translate and rotate in space in response to contact and body forces. Over the past several years we have determined the important microscale processes that affect snow sintering and the micromechanical properties of snow from the literature on laboratory and field tests. We have developed dynamic constitutive models that simulate grain boundary sliding, power law creep, grain rotation, and viscous-elastic bond deformation and failure in tension, compression, bending, and twisting, and grain-to-grain sintering.

The contact force model has the following structure. Pairs of grains interact through unfrozen and frozen viscous-elastic contacts. Forces are calculated with respect to a plane of contact tangent to the surface of each grain. At unfrozen contacts there are compressive forces normal to the plane of contact and frictional sliding forces in the plane of contact. At frozen contacts there are tensile and compressive forces in the direction normal to the plane of contact, tensile forces in the plane of contact, a twisting moment about the normal to the plane of contact, and a bending moment about an axis in the plane of contact. Each component of the force and moment at a frozen contact has an associated failure mechanism based on tensile strength and an associated viscous creep mechanism that acts to relax stress. The frozen contact is circular. The growth of the circular contact area is governed by the sintering model and depends on time, temperature, and contact pressure.


Model Snow Samples

Currently, model snow samples are created by populating a cubic lattice with randomly sized and oriented particles, giving them small random velocities, and contracting them to the desired density. (Click on Figure 1 to see the building of a model snow sample.) Frozen bonds are generated on contact. Initial bond areas are uniformly distributed. Values for the micromechanical parameters were taken from macroscale test data for snow and ice, as microscale test data is not yet available. We use empirical sintering data because the controlling physical mechanisms for sintering in snow are not well defined. Figure 2 shows a stereographic slice through the model snow sample. We have used the model to perform simulations of a micro-penetrometer in snow (Figure 3) and a snow-filled shear box (Figures 4 and 5) that qualitatively reproduce experimental results. This is a severe test of the snow model since either dilation or contraction and either strain hardening or softening can occur, depending on strain rate and temperature. We are able to replicate these behaviors in simulations, which cannot be done using previous methods. Currently, the snow model does not use a metamorphosed microstructure or grain shape for lack of information. In addition, the parameters for the micromechanical processes and sintering are not accurately known since the necessary experiments have not been performed. However, we have started an experiment to determine grain scale parameters by measuring the micromechanical properties of snow. Our-long term goal is to develop a virtual snow that can simulate metamorphosis, fluid and vapor flow, heat conduction, and electromagnetic properties.

Figure 1. Model snow sample creation. Click 

                here to watch snow sample creation by populating 

                a lattice with random Particles.

Figure 1. Model snow sample creation. Click on the image above to watch snow sample creation by populating a lattice with random Particles (14.3 MBytes).

Click here
to see a rotation of the completed model snow sample (8.6 MBytes).

Figure 

                2. A stereographic slice through

                a model snow sample. (The porosity is 70%.)

                Click on the figure above to see the slice

                move through the model snow sample.

Figure 2. A stereographic slice through a model snow sample. (The porosity is 70%.) Click on the figure above to see the slice move through the model snow sample (4.6 MBytes).

Figure 3. A large model snow 

                sample with a

                1 cm diameter micro-penetrometer.

Figure 3. A large model snow sample with a
1 cm diameter micro-penetrometer.

Figure 4. A model snow sample after settlement. The box is 20 mm wide. The grains are 1 mm in diameter. During settlement, porosity decreased from 70% to 61%, while the coordination number increased from 3.21 to 4.71. Click here to view a movie of the settling process.

Figure 4. A model snow sample after settlement. The box is 20 mm wide. The grains are 1 mm in diameter. During settlement, porosity decreased from 70% to 61%, while the coordination number increased from 3.21 to 4.71. Click on the figure above to view a movie of the settling process (3.2 MBytes).

Figure 5. The sample in Figure 4 after 20% shear. The coordination number further increased to 4.98. Click here to view a movie of the shear process.

Figure 5. The sample in Figure 4 after 20% shear. The coordination number further increased to 4.98. Click on the figure above to view a movie of the shear process (3.3 MBytes).


Principal Investigators:

Dr. Jerome Johnson has worked at the Cold Regions Research and Engineering Laboratory (CRREL) since 1983 and is a member of the Snow and Ice Branch. His research focuses on solving applied problems relating to ice, frozen ground, snow, and other granular materials. Dr. Johnson is a scientific editor for the Journal of Glaciology, a science team member for the Mars CryoScout project, a former participating scientist on the Mars Polar Lander Mission, and a consultant on the upcoming Mars Rover mission.

Dr. Mark Hopkins works in the Snow and Ice Branch at CRREL. His research is focused on the development of discrete element modeling techniques and the application of those techniques to simulate problems in sea ice, river ice, and snow mechanics.


Collaborators:

Dr. Dave Cole (CRREL) designs and conducts the small-scale laboratory experiments for the snow modeling project and is an expert on the mechanical and physical properties of ice and mechanical testing methods. He has extensive experience conducting multi-scale mechanical and structural tests on ice. He holds patents on test apparatus design.

Dr. Randall German is Brush Chair Professor in Materials and Director for the Center for Innovative Sintered Products, Pennsylvania State University. He has authored numerous articles and books on the sintering of powders.

Dr. Martin Schneebeli is a research scientist from the Swiss Institute for Snow and Avalanche Research and is an expert in characterizing snow microstructure and microstructural testing techniques.


References:

Hopkins, M.A. (in press) Discrete Element Modeling With Dilated Particles, to appear in the Journal of Engineering Computations.

Johnson, J.B. and M.A. Hopkins (in prep.) A discrete element method model of deformation for dry seasonal snow. Draft ERDC Technical Report.

Johnson, J.B. and M. Schneebeli (1999) Characterizing the microstructural and micromechanical properties of snow. Cold Regions Science and Technology, 30: 91-100.

Johnson, J.B. (1998) A preliminary numerical investigation of the micromechanics of snow compaction. Annals of Glaciology, 26: 51-54.

Shapiro, L.H., J.B. Johnson, M. Sturm, G.L. Blaisdell (1997) Snow Mechanics: Review of the state of knowledge and applications, United States Army Corps of Engineers Cold Regions Research and Engineering Laboratory (USACRREL), Report CR 97-03.


Discrete Element Research Page                                           Snow and Ice Branch


Contact Information

Dr. Mark A. Hopkins
Phone: 603-646-4249
Fax: 603-646-4644
E-mail: Mark.A.Hopkins@erdc.usace.army.mil

(Postal address below.)

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Updated: August 2004 (dbh)