CRITICAL STATE SOIL MECHANICS
TRESCA MODEL (MAX. SHEAR STRESS THEORY)
1. Rameez Riyaz (2021MCIVGT006)
2. Eiqan Shafi (2021MCIVGT017)
3. Shahid Manzoor Bhat (2021MCIVGT002)
INTRODUCTION
Failure occurs when material starts exhibiting inelastic behavior
Brittle and Ductile materials have different modes of failure
Ductile materials exhibit yielding or plastic deformation before failure
Yield stree is the property of the material
No yielding occurs in Brittle materials.There is a sudden failure
FAILURE THEORY MODELS
 Mohr – Coulomb Model
 Hardening Soil Model / Hardening Mohr – Coulomb Model
 Modified Cam – Clay Model
 Drucker – Prager Model
 Tresca Model
 Hoek – Brown Model
 Duncan – Chang Model
TRESCA MODEL (MAX. SHEAR STRESSTHEORY)
Failure occurs when maximum shear stress in a complex stress system equals to the
maximum shear stress at yield point under uniaxial loading.
No failure occurs if maximum shear <Y/2
PURE SHEAR CASE
ShearYield = 0.5x TensileYield
3D STRESS STATE
In 3D stress state, principal stresses are =>
• Maximum shear stress:
• Yield
function:
Yield function in Principal stress space
Tresca hexagon
2D STRESS
STATE
EACH EQUATION REPRESENTS
TWO LINES IN 2D STRESS SPACE
CONCLUSION
 This theory is suitable for ductile materials
 For pure shear case it is oversafe
Limitations
 Not applicable for materials subjected to hydrostatic
loading as it says shear stress will be zero and material
will never fail which is practically impossible
 Not applicable for brittle materials as they have
different yield stress in tension and compression
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Tresca Model for Geotechnical Engineering

  • 1.
    CRITICAL STATE SOILMECHANICS TRESCA MODEL (MAX. SHEAR STRESS THEORY) 1. Rameez Riyaz (2021MCIVGT006) 2. Eiqan Shafi (2021MCIVGT017) 3. Shahid Manzoor Bhat (2021MCIVGT002)
  • 2.
    INTRODUCTION Failure occurs whenmaterial starts exhibiting inelastic behavior Brittle and Ductile materials have different modes of failure Ductile materials exhibit yielding or plastic deformation before failure Yield stree is the property of the material No yielding occurs in Brittle materials.There is a sudden failure
  • 3.
    FAILURE THEORY MODELS Mohr – Coulomb Model  Hardening Soil Model / Hardening Mohr – Coulomb Model  Modified Cam – Clay Model  Drucker – Prager Model  Tresca Model  Hoek – Brown Model  Duncan – Chang Model
  • 4.
    TRESCA MODEL (MAX.SHEAR STRESSTHEORY) Failure occurs when maximum shear stress in a complex stress system equals to the maximum shear stress at yield point under uniaxial loading. No failure occurs if maximum shear <Y/2
  • 5.
    PURE SHEAR CASE ShearYield= 0.5x TensileYield
  • 6.
    3D STRESS STATE In3D stress state, principal stresses are => • Maximum shear stress: • Yield function:
  • 7.
    Yield function inPrincipal stress space
  • 8.
  • 9.
    2D STRESS STATE EACH EQUATIONREPRESENTS TWO LINES IN 2D STRESS SPACE
  • 10.
    CONCLUSION  This theoryis suitable for ductile materials  For pure shear case it is oversafe Limitations  Not applicable for materials subjected to hydrostatic loading as it says shear stress will be zero and material will never fail which is practically impossible  Not applicable for brittle materials as they have different yield stress in tension and compression
  • 11.