tweel traction modeling presentation

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Numerical Simulation of the new generation Non-Pneumatic Tweel™ and sand Jianfeng Ma Avinash Kolla Joshua D. Summers Paul F. Joseph Vincent Y. Blouin Sherrill Biggers 1/20 http://aid.ces.clemson.edu 3/6/2009

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Page 1: Tweel Traction Modeling Presentation

Numerical Simulation of the new generation Non-Pneumatic Tweel™ and sand

Jianfeng MaAvinash Kolla

Joshua D. SummersPaul F. Joseph

Vincent Y. BlouinSherrill Biggers

1/20

http://aid.ces.clemson.edu

3/6/2009

Page 2: Tweel Traction Modeling Presentation

Objectives of the project

• To Improve the performance of tire on sand.

– In other words traction

• To develop a full computational model for tire-sand interaction with an acceptable accuracy.

• To search for novel tread concepts that can avoid slip.

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Page 3: Tweel Traction Modeling Presentation

Mechanics of tire-terrain interaction

• Output energy = Input energy – Energy losses(losses due to motion resistance)

• Traction forces = Drawbar-pull + Work energy/unit travel distance

Energy dissipated in the distorting the tractive element

Energy dissipated in terms of compacting the soil

Energy loss associated with slip

VInput EnergyUseful output

energy

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Page 4: Tweel Traction Modeling Presentation

Modeling Techniques

• Analytical models (Bekker, 1969)

• Empirical models (Yong and Fattah, 1986)

• Computational models

– FEM (Fervers, 1996)

– DEM (Nakasimha et al., 2003)

• FEM is employed for the simulation due to less computational effort and acceptable levels of accuracy

• Soil is treated as Elasto-plastic solid. Tweel™ is treated as a deformable body.

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Page 5: Tweel Traction Modeling Presentation

Segmented cylinder Tweel™

• Typical properties of pneumatic tires carried to Tweel™:

• Low contact pressure

• low stiffness

• high load carrying efficiency

• low energy loss from obstacle impact

• In addition to being non-pneumatic makes it flexible enough to withstand extreme temperatures on both terrains.

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Page 6: Tweel Traction Modeling Presentation

2D Tweel™ Model

• 2-D FEM Model of tire replicating the prototype is shown in figure.

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Page 7: Tweel Traction Modeling Presentation

Soil Modeling

• Soil can be modeled using four elasto plastic models:1. Drucker-Prager model (Classical, Drucker-prager/cap model)

2. Mohr-Coloumb model

3. Critical state theory

4. Lade’s single hardening model

• For the analysis, sand is represented by elastoplastic Drucker-prager/Cap model that uses the results obtained from triaxialtests and consolidation test.

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Page 8: Tweel Traction Modeling Presentation

Soil properties

• By using Drucker-prager/cap plasticity constitutive law.

Properties of soil used for ABAQUS:Drucker-Prager/Cap model*

* Taken from literature for the Lebanon sand found in NH.

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Material parameters Value

Young’s modulus, E 8500 kPaPoisson’s ratio, ν 0.32

Angle of friction, β 55.8˚Material cohesion, d 10.0 kPaCap eccentricity, R 0.45

Initial value of volumetric plastic strain 0

Flow stress ratio 1

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Page 9: Tweel Traction Modeling Presentation

Interaction model

• From the simulation model, soil deformation, distributions of different stresses in both sand and Tweel™ and distributions of contact pressure along the contact patch at all instances are expected.

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Page 10: Tweel Traction Modeling Presentation

Numerical results (1)

• Two loading steps:

•Initial loading to deform Tweel™

•Final step for displacing the Tweel™

• Deformation in Tweel™ is more because the spokes can’t withstand compression.

Sand bed

Tweel™ model

Displacement (0.4m, -0.04m)

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Page 11: Tweel Traction Modeling Presentation

Numerical results(2)

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von Mises stress distribution

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Page 12: Tweel Traction Modeling Presentation

Numerical results (3)

• The deformations in sand are permanent after the Tweel™ passes by, since sand is treated as elasto- plastic solid indicating that the residual stresses are permanent.

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Page 13: Tweel Traction Modeling Presentation

• This low contact pressure can cause less deformation of sand reducing the bulldozing effect.

• Long contact path accounts for low contact pressure i.e. relatively uniform contact pressure.

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Numerical results(4) 13/203/6/2009

Page 14: Tweel Traction Modeling Presentation

• σ11 distribution in Tweel™ at final instant

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Numerical results (5) 14/203/6/2009

Page 15: Tweel Traction Modeling Presentation

Numerical results (6)

• σ11 distribution in sand at final instant

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Page 16: Tweel Traction Modeling Presentation

• σ22 distribution in sand at final instant

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Numerical results (7) 16/203/6/2009

Page 17: Tweel Traction Modeling Presentation

• σ33 distribution in sand at final instant

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Numerical results (8) 17/203/6/2009

Page 18: Tweel Traction Modeling Presentation

Conclusions

• FEM code-ABAQUS is used to perform the simulation.

• Soil is modeled using elasto-plastic Drucker-Prager/cap model.

• The Numerical results show that there is a relatively low contact pressure observed for this Tweel™ model.

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Page 19: Tweel Traction Modeling Presentation

• The work presented will be used as a basis for improving the performance of the Tweel™ on sand.

• Several Tweel™ that can give better tractive performance will be investigated.

• Ways to induct Tweel™’s pressure profile into another wheel model needs to be explored.

• After developing tire-model that have better traction based on pressure profiles, influence of tread profiles will be studied to find ways to improve traction further.

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Future Work 19/203/6/2009

Page 20: Tweel Traction Modeling Presentation

Thank you for your Attention!!

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Questions?? 20/203/6/2009