2016
DOI: 10.1007/s11043-016-9319-7
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Nonlinear creep damage constitutive model for soft rocks

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Cited by 103 publications
(47 citation statements)
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“…As shown in Figure 4, the traditional Nishihara model is composed of a Hooke body, a Kelvin body, and an ideal visco-plastic body in series, 45 where E 0 stands for the elastic modulus, E 1 denotes the viscoelastic modulus, and η 1 and η 2 are the viscosity coefficients of the dashpot.…”
Section: One-dimensional Nonlinear Creep Model For Coal or Rockmentioning
confidence: 99%
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“…As shown in Figure 4, the traditional Nishihara model is composed of a Hooke body, a Kelvin body, and an ideal visco-plastic body in series, 45 where E 0 stands for the elastic modulus, E 1 denotes the viscoelastic modulus, and η 1 and η 2 are the viscosity coefficients of the dashpot.…”
Section: One-dimensional Nonlinear Creep Model For Coal or Rockmentioning
confidence: 99%
“…27,29,36,37,45 For 3-D problems, the total strain can be given by. 27,29,36,37,45 For 3-D problems, the total strain can be given by.…”
Section: Three-dimensional Creep Equations For Coal Containing Gasmentioning
confidence: 99%
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“…Previous studies have shown that the viscosity coe cient of rock will decrease when stress exceeds the long-term ultimate strength [17][18][19]; since an exponential function can better re ect the relationship between the damage variables and the strain (Figure 10), we assume that the damage variables in the cycle creep stage can be expressed as an exponential function (as shown in (4)), and based on the characteristic of the Burgers creep model [20], a new viscoelastic-plastic creep model was proposed, as shown in Figure 13.…”
Section: Creep Model and Parameter Identi Cation Formmentioning
confidence: 99%
“…However, the parameters 2 and Shock and Vibration Figure 11 that the axial and the lateral creep curves show obvious nonlinear behavior; the instantaneous strain, decay creep, and steady creep reveal a trend of increase with the cycle number and cycle loading, indicating that both the cycle number and the level of the stress are the primary reason for the nonlinear behavior of the red stone under uniaxial cyclic loading. In order to better describe the creep behavior of red sandstone material under cyclic incremental uniaxial compressive and tensile stress, by adopting the decreasing hypothesis of viscosity coefficient [21][22][23], an improved Burgers creep model of rock material can be proposed, as shown in Figure 13.…”
Section: Creep Model and Parameter Identificationmentioning
confidence: 99%