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Continuum Mechanics for Hillslopes: Part III

Continuum Mechanics for Hillslopes: Part III. Today we will f ocus on Deformation and Strain. Conservation Laws and Constitutive Relations on Thursday. Deformation. Driven by both body forces and stresses

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Continuum Mechanics for Hillslopes: Part III

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  1. Continuum Mechanics for Hillslopes: Part III • Today we will focus on Deformation and Strain. • Conservation Laws and Constitutive Relations on Thursday.

  2. Deformation • Driven by both body forces and stresses • Style and rate of deformation differs based on material properties (liquids, solids, etc.) • Deformation described by a ‘displacement field’ • Vectors connect positions before and after deformation • Rigid-body translation • Rigid-body rotation • Distortion (strain)

  3. Normal Strain Elongation of contraction of a displacement vector.

  4. Normal Strain • Displacement of point b can be described as: • Displacement of point a PLUS • Product of the gradient of displacement and the original line length PLUS • An expansion series of higher order terms • (using Taylor’s Theorem)

  5. Normal Strain

  6. Normal Strain (by definition: the normal component of strain is a change in line length) (note: strain is a dimensionless quantity)

  7. Normal Strain • For infinitesimal strains, can assume only linear relationships matter. • Assumption good for strains as large as 0.1% or even 1%. • Works for large strains, if considered over short periods of time.

  8. Normal Strain • By definition: positive in elongation. • Relates infinitesimal normal strain to the gradient of displacement, along a coordinate direction. • Note subscripts: • If related: normal • If unequal: shear

  9. Normal Strain (Area) Fractional change in area

  10. Normal Strain (Area) Calculating the area Of the final region, A1 Substituting the expression last into:

  11. Normal Strain (Area) and because are <<1, their product is very small. Thus, and in 3 dimensions, dilation is:

  12. Shear Strain The change in angle between lines that were originally perpendicular. Rotation α1 is positive in ccw direction because produces a displacement in the + y direction. Same for α2. When α1 = α2, this is pure shear

  13. Shear Strain By the small angle approximation where:

  14. Shear Strain DEFINING: The average angular change from the original right angle of the elemental area (average shear strain): Plugging in from above: Or: Finding components as symmetric:

  15. Shear Strain Same derivations can be done for: Many engineering applications use the total shear strain (the sum of the angular changes, α1 + α2), But most geological analyses use the average shear strain.

  16. Combined normal strain and average shear strain give a strain tensor: Total shear strain would remove the ½’s from the off-diagonal terms.

  17. Application: Debris Flows

  18. Rotation

  19. Rotation

  20. Rotation

  21. Strain in Alternate Coordinate Systems

  22. Strain in Alternate Coordinate Systems

  23. Rate of Deformation

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