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Constitutive Modelling of Soil
(Duncan-Chang Model)
Mostafa Abedi
‫رحیم‬ ‫یا‬ ‫رحمان‬ ‫یا‬
1
Constitutive Modelling of Soil (Duncan-Chang Model)
Mostafa Abedi
/15
Comparison Duncan-Chang with other hyperbolic
models
Shear Modulus (G):
Determination G (Shear Modulus) relative to  (shear starin)
2
Ramberg-Osgood Model (1992)
Hardin-Drnevich Model (1972)
Davidenkov Model (1953)
and etc.
Constitutive Modelling of Soil (Duncan-Chang Model)
Mostafa Abedi
/15
Comparison Duncan-Chang with other hyperbolic
models
Tangent Modulus (Et):
Determination Et (tangent Modulus) relative to - (axial stress-strain)
3
Duncan-Chang(1960)
Constitutive Modelling of Soil (Duncan-Chang Model)
Mostafa Abedi
/15
Duncan-Chang constitutive equations
Kondner and et al. (1963) have shown that the nonlinear stress-strain
curves of both clay and sand may be approximated by hyperbolae with a
high degrss of accuracy.
The hyperbolic equation propose by Kondner was:
𝜎1 − 𝜎3 =
𝜀
𝑎 + 𝑏. 𝜀
4
Constitutive Modelling of Soil (Duncan-Chang Model)
Mostafa Abedi
/15
Duncan-Chang constitutive equations
5
E0 or Ei Et
Esec
Constitutive Modelling of Soil (Duncan-Chang Model)
Mostafa Abedi
/15
Duncan-Chang constitutive equations
𝑞 = 𝜎1 − 𝜎3 =
𝜀𝑎
𝑎 + 𝑏. 𝜀𝑎
→ lim
𝜀𝑎→∞
𝜀𝑎
𝑎 + 𝑏. 𝜀𝑎
=
1
𝑏
= 𝑞𝑢𝑙𝑡 = (𝜎1 − 𝜎3) 𝑢𝑙𝑡
𝐸 =
𝜕𝑞
𝜕𝜀𝑎
=
𝜕(𝜎1 − 𝜎3)
𝜕𝜀𝑎
=
𝑎
𝑎 + 𝑏. 𝜀𝑎
2
→ lim
𝜀𝑎→0
𝑎
𝑎 + 𝑏. 𝜀𝑎
2
=
1
𝑎
= 𝐸𝑖 = 𝐸0
6
Constitutive Modelling of Soil (Duncan-Chang Model)
Mostafa Abedi
/15
Duncan-Chang constitutive equations
7
Constitutive Modelling of Soil (Duncan-Chang Model)
Mostafa Abedi
/15
8
The a and b values
should be calculate
in 70% to 95%
( - /1-3) chart
Constitutive Modelling of Soil (Duncan-Chang Model)
Mostafa Abedi
/15
Duncan-Chang constitutive equations
Failure ratio (Rf):
𝑅𝑓 =
𝜎1 − 𝜎3 𝑓
𝜎1 − 𝜎3 𝑢𝑙𝑡
≤ 1.0
independent of confining pressure
Rf = 0.75  1.0
9
Constitutive Modelling of Soil (Duncan-Chang Model)
Mostafa Abedi
/15
Duncan-Chang constitutive equations
If the parameters a and b are expressed in terms of E0, Rf, and (1-3):
𝜎1 − 𝜎3 =
𝜀
1
𝐸0
+
𝜀. 𝑅𝑓
𝜎1 − 𝜎3 𝑓
10
Constitutive Modelling of Soil (Duncan-Chang Model)
Mostafa Abedi
/15
Duncan-Chang constitutive equations
Janbu (1963):
𝐸0 = 𝑘. 𝑝𝑎
𝜎3
𝑝𝑎
𝑛
11
Constitutive Modelling of Soil (Duncan-Chang Model)
Mostafa Abedi
/15
Duncan-Chang constitutive equations
Mohr-Coulomb failure criterion:
𝜎1 − 𝜎3 𝑓 =
2𝑐. 𝑐𝑜𝑠𝜑 + 2𝜎3. 𝑠𝑖𝑛𝜑
1 − 𝑠𝑖𝑛𝜑
12
Constitutive Modelling of Soil (Duncan-Chang Model)
Mostafa Abedi
/15
Duncan-Chang constitutive equations
• Tangent modulus values (Et):
𝐸𝑡 = 1 − 𝑅𝑓
(1 − 𝑠𝑖𝑛𝜑)(𝜎1 − 𝜎3)
2(𝑐. 𝑐𝑜𝑠𝜑 + 𝜎3. 𝑠𝑖𝑛𝜑)
2
𝑘.
𝜎3
𝑝𝑎
𝑛
13
Constitutive Modelling of Soil (Duncan-Chang Model)
Mostafa Abedi
/15
Duncan-Chang constitutive equations
• Tangent modulus values (Et):
𝐸𝑡 = 1 − 𝑅𝑓
(1 − 𝑠𝑖𝑛𝜑)(𝜎1 − 𝜎3)
2(𝑐. 𝑐𝑜𝑠𝜑 + 𝜎3. 𝑠𝑖𝑛𝜑)
2
𝑘.
𝜎3
𝑝𝑎
𝑛
14
Constitutive Modelling of Soil (Duncan-Chang Model)
Mostafa Abedi
/15
Duncan-Chang constitutive equations
15
The incremental models described
cannot account for the strain
softening behavior after peak
strength (e.g., for dense sands and
overconsolidated clays).

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Constitutive modelling of soil (Duncan-chang Model)

  • 1. Constitutive Modelling of Soil (Duncan-Chang Model) Mostafa Abedi ‫رحیم‬ ‫یا‬ ‫رحمان‬ ‫یا‬ 1
  • 2. Constitutive Modelling of Soil (Duncan-Chang Model) Mostafa Abedi /15 Comparison Duncan-Chang with other hyperbolic models Shear Modulus (G): Determination G (Shear Modulus) relative to  (shear starin) 2 Ramberg-Osgood Model (1992) Hardin-Drnevich Model (1972) Davidenkov Model (1953) and etc.
  • 3. Constitutive Modelling of Soil (Duncan-Chang Model) Mostafa Abedi /15 Comparison Duncan-Chang with other hyperbolic models Tangent Modulus (Et): Determination Et (tangent Modulus) relative to - (axial stress-strain) 3 Duncan-Chang(1960)
  • 4. Constitutive Modelling of Soil (Duncan-Chang Model) Mostafa Abedi /15 Duncan-Chang constitutive equations Kondner and et al. (1963) have shown that the nonlinear stress-strain curves of both clay and sand may be approximated by hyperbolae with a high degrss of accuracy. The hyperbolic equation propose by Kondner was: 𝜎1 − 𝜎3 = 𝜀 𝑎 + 𝑏. 𝜀 4
  • 5. Constitutive Modelling of Soil (Duncan-Chang Model) Mostafa Abedi /15 Duncan-Chang constitutive equations 5 E0 or Ei Et Esec
  • 6. Constitutive Modelling of Soil (Duncan-Chang Model) Mostafa Abedi /15 Duncan-Chang constitutive equations 𝑞 = 𝜎1 − 𝜎3 = 𝜀𝑎 𝑎 + 𝑏. 𝜀𝑎 → lim 𝜀𝑎→∞ 𝜀𝑎 𝑎 + 𝑏. 𝜀𝑎 = 1 𝑏 = 𝑞𝑢𝑙𝑡 = (𝜎1 − 𝜎3) 𝑢𝑙𝑡 𝐸 = 𝜕𝑞 𝜕𝜀𝑎 = 𝜕(𝜎1 − 𝜎3) 𝜕𝜀𝑎 = 𝑎 𝑎 + 𝑏. 𝜀𝑎 2 → lim 𝜀𝑎→0 𝑎 𝑎 + 𝑏. 𝜀𝑎 2 = 1 𝑎 = 𝐸𝑖 = 𝐸0 6
  • 7. Constitutive Modelling of Soil (Duncan-Chang Model) Mostafa Abedi /15 Duncan-Chang constitutive equations 7
  • 8. Constitutive Modelling of Soil (Duncan-Chang Model) Mostafa Abedi /15 8 The a and b values should be calculate in 70% to 95% ( - /1-3) chart
  • 9. Constitutive Modelling of Soil (Duncan-Chang Model) Mostafa Abedi /15 Duncan-Chang constitutive equations Failure ratio (Rf): 𝑅𝑓 = 𝜎1 − 𝜎3 𝑓 𝜎1 − 𝜎3 𝑢𝑙𝑡 ≤ 1.0 independent of confining pressure Rf = 0.75  1.0 9
  • 10. Constitutive Modelling of Soil (Duncan-Chang Model) Mostafa Abedi /15 Duncan-Chang constitutive equations If the parameters a and b are expressed in terms of E0, Rf, and (1-3): 𝜎1 − 𝜎3 = 𝜀 1 𝐸0 + 𝜀. 𝑅𝑓 𝜎1 − 𝜎3 𝑓 10
  • 11. Constitutive Modelling of Soil (Duncan-Chang Model) Mostafa Abedi /15 Duncan-Chang constitutive equations Janbu (1963): 𝐸0 = 𝑘. 𝑝𝑎 𝜎3 𝑝𝑎 𝑛 11
  • 12. Constitutive Modelling of Soil (Duncan-Chang Model) Mostafa Abedi /15 Duncan-Chang constitutive equations Mohr-Coulomb failure criterion: 𝜎1 − 𝜎3 𝑓 = 2𝑐. 𝑐𝑜𝑠𝜑 + 2𝜎3. 𝑠𝑖𝑛𝜑 1 − 𝑠𝑖𝑛𝜑 12
  • 13. Constitutive Modelling of Soil (Duncan-Chang Model) Mostafa Abedi /15 Duncan-Chang constitutive equations • Tangent modulus values (Et): 𝐸𝑡 = 1 − 𝑅𝑓 (1 − 𝑠𝑖𝑛𝜑)(𝜎1 − 𝜎3) 2(𝑐. 𝑐𝑜𝑠𝜑 + 𝜎3. 𝑠𝑖𝑛𝜑) 2 𝑘. 𝜎3 𝑝𝑎 𝑛 13
  • 14. Constitutive Modelling of Soil (Duncan-Chang Model) Mostafa Abedi /15 Duncan-Chang constitutive equations • Tangent modulus values (Et): 𝐸𝑡 = 1 − 𝑅𝑓 (1 − 𝑠𝑖𝑛𝜑)(𝜎1 − 𝜎3) 2(𝑐. 𝑐𝑜𝑠𝜑 + 𝜎3. 𝑠𝑖𝑛𝜑) 2 𝑘. 𝜎3 𝑝𝑎 𝑛 14
  • 15. Constitutive Modelling of Soil (Duncan-Chang Model) Mostafa Abedi /15 Duncan-Chang constitutive equations 15 The incremental models described cannot account for the strain softening behavior after peak strength (e.g., for dense sands and overconsolidated clays).