1.033/1.57 Mechanics of Material Systems (Mechanics and Durability of Solids I) Franz-Josef Ulm Lecture: MWF1 // Recitation: F3:00-4:30 1.033/1.57 Mechanics.

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1.033/1.57 Mechanics of Material Systems (Mechanics and Durability of Solids I) Franz-Josef Ulm Lecture: MWF1 // Recitation: F 3:00-4: /1.57 Mechanics.
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1.033/1.57 Mechanics of Material Systems (Mechanics and Durability of Solids I) Franz-Josef Ulm Lecture: MWF1 // Recitation: F3:00-4: /1.57 Mechanics of Material Systems

Part II: Momentum Balance, Stresses and Stress States 4. Stress States / Failure Criteria 1.033/1.57 Mechanics of Material Systems

Content 1.033/1.57 Part I. Deformation and Strain 1 Description of Finite Deformation 2 Infinitesimal Deformation Part II. Momentum Balance and Stresses 3 Momentum Balance 4 Stress States / Failure Criterion Part III. Elasticity and Elasticity Bounds 5 Thermoelasticity, 6 Variational Methods Part IV. Plasticity and Yield Design 7 1D-Plasticity – An Energy Approac 8 Plasticity Models 9 Limit Analysis and Yield Design 1.033/1.57 Mechanics of Material Systems

Stress Vector and Stress Components Stress components on a material surface oriented by unit normal n Stress components on a material surface oriented in the principal stress direction n = u I 1.033/1.57 Mechanics of Material Systems

Stress Vector in the Principal Stress Space (Illustration of Stress Invariants) = Orientation of hydrostatic axis T( − u 3 ) 1.033/1.57 Mechanics of Material Systems

Stress Vector in the Mohr Plane 1.033/1.57 Mechanics of Material Systems

Mohr Circles and The Mohr Circle The Mohr Circle 1.033/1.57 Mechanics of Material Systems

Selected Stress States: Hydrostatic Pressure σ = −p1 Material Plane Mohr Stress Plane 1.033/1.57 Mechanics of Material Systems

Selected Stress States: Uniaxial Tension σ = σ I e z ⊗ e z Material Plane Mohr Stress Plane 1.033/1.57 Mechanics of Material Systems

Selected Stress States: Pure Shear σ = τ (e x ⊗ e y +e y ⊗ e x ) Material Plane Mohr Stress Plane 1.033/1.57 Mechanics of Material Systems

Selected Stress States: Plane Stress T(n=e z ) = σ ⋅ e z = 0 Material Plane Mohr Stress Plane 1.033/1.57 Mechanics of Material Systems

Tension Cut-Off Direct Tension Shear 1.033/1.57 Mechanics of Material Systems − τ max

Tresca Criterion

Tresca Criterion: Application 1.033/1.57 Mechanics of Material Systems

Mohr- Coulomb 1.033/1.57 Mechanics of Material Systems

Mohr- Coulomb Direct Tension Shear Uniaxial Compression 1.033/1.57 Mechanics of Material Systems

Training Set: Excavation Set 1.033/1.57 Mechanics of Material Systems

Max. Excavation Depth of Tresca Material 1.033/1.57 Mechanics of Material Systems

Homework Set #2 Part I: Triaxial Test Part II: Circular Foundation