Abstract
A triaxial creep model for deep coal considering temperature effect based on fractional derivative is proposed for the condition of triaxial stress state. In order to study the temperature effect on creep deformation of deep coal, the thermal damage variable is established based on the Weibull distribution and continuum damage mechanics theory. The thermal damage variable is assigned to the Hooke body and Abel dashpot in order to characterize the effect of temperature on elastic modulus and viscosity coefficient. The temperature-dependent mechanical elements are connected to the creep model, and a three-dimensional creep constitutive equation based on fractional derivative is established. A creep experimental study for deep coal under the constant axial pressure and unloading confining pressure at different temperatures is carried out to characterize the creep deformation of deep coal during mining. The experimental results show that the coal sample with higher temperature has greater axial deformation, but the radial deformation does not change monotonically with the change of temperature. Moreover, the proposed triaxial creep model is validated by experimental data and the nonlinear least square method is used to determine the model parameters. It is indicated that the triaxial creep model can better describe the time-dependent deformation under the effect of temperature, especially the accelerated creep stage of creep. In addition, the sensitivity analysis of key parameters of the proposed model, especially axial stress level and creep temperature, is carried out to further verify the accuracy of the triaxial creep model.
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Abbreviations
- a :
-
Temperature effect constant
- \(\alpha\) :
-
Parameter of Mittag–Leffler function
- \(\alpha _{1}\) :
-
Thermal expansion coefficient (K−1)
- b :
-
Temperature effect constant
- \(\beta\) :
-
Parameter of Mittag–Leffler function
- \(\beta _{1}\) :
-
Biot coefficient
- \(D^{\gamma }\) :
-
Fractional differential operator
- \(D_{{\text{T}}}\) :
-
Thermal damage variable
- \(D_{{\text{M}}}\) :
-
Mechanical damage variable
- \(D_{{{\text{TM}}}}\) :
-
Thermal–mechanical damage variable
- \(\varepsilon\) :
-
Strain of the Hooke body
- \(\varepsilon _{1}\) :
-
Axial strain of microunit
- \(\varepsilon (t)\) :
-
Strain of the Abel dashpot
- \(\varepsilon _{{\text{e}}}\) :
-
Strain of the Hooke body
- \(\varepsilon _{{{\text{ve}}}}\) :
-
Strain of the viscoelastic body
- \(\varepsilon _{{{\text{vp}}}}\) :
-
Strain of the viscoplastic body
- \(\varepsilon _{{\text{H}}}\) :
-
Strain of the Hooke body
- \(\varepsilon _{{\text{A}}}\) :
-
Strain of the Abel dashpot
- \(\varepsilon _{{ij}}^{'} \left( t \right)\) :
-
Total effective deviatoric strain tensor
- \(\varepsilon _{{ij}}^{e}\) :
-
Effective deviatoric strain tensor of elastic body
- \(\varepsilon _{{ij}}^{{ve}}\) :
-
Effective deviatoric strain tensor of viscoelastic body
- \(\varepsilon _{{ij}}^{{vp}}\) :
-
Effective deviatoric strain tensor of viscoplastic body
- E (T):
-
Elastic modulus at temperature T (GPa)
- \(E_{0} (T)\) :
-
Elastic modulus at temperature T (GPa)
- \(E_{1} (T)\) :
-
Elastic modulus at temperature T (GPa)
- \(E_{{\alpha ,\beta }} (z)\) :
-
Mittag–Leffler function
- \(F\) :
-
Yield function
- \(F_{0}\) :
-
Initial reference value of the yield function
- \(G_{0} (T)\) :
-
Shear modulus at temperature T (GPa)
- \(G_{1} (T)\) :
-
Shear modulus at temperature T (GPa)
- \(J_{2}\) :
-
Second invariant of deviatoric stress (MPa)
- \(K(T)\) :
-
Bulk modulus at temperature T (GPa)
- μ:
-
Poisson’s ratio
- m :
-
Shape parameter
- \(\eta _{0}^{\gamma }\) :
-
Viscosity coefficient at room temperature (GPa·hγ)
- \(\eta _{{}}^{\gamma } (T)\) :
-
Viscosity coefficient at temperature T (GPa·hγ)
- \(\eta _{1}^{\gamma } (T)\) :
-
Viscosity coefficient of the Abel dashpot at temperature T (GPa·hγ)
- \(\eta _{2}^{\gamma } (T)\) :
-
Viscosity coefficient of the Abel dashpot at temperature T (GPa·hγ)
- P :
-
Pore pressure (MPa)
- \(\gamma\) :
-
Fractional derivative order
- \(s_{{ij}}^{'}\) :
-
Effective deviatoric stress tensor
- \(\Delta T\) :
-
Change from room temperature (oC)
- \(T_{0}\) :
-
Room temperature (oC)
- \(\omega\) :
-
Parameter of viscosity coefficient (h−1)
- \(\psi\) :
-
Scale parameter
- \(\delta _{{ij}}\) :
-
Kronecker symbol
- \(\phi ( \cdot )\) :
-
Power function form
- \(\sigma\) :
-
Stress of the Hooke body (MPa)
- \(\sigma (t)\) :
-
Stress of the Abel dashpot (MPa)
- \(\sigma _{1}\) :
-
Axial stress (MPa)
- \(\sigma _{2}\) :
-
Radial stress (MPa)
- \(\sigma _{3}\) :
-
Confining pressure (MPa)
- \((\sigma _{s} )_{{\text{T}}}\) :
-
Yield limit with the temperature effect (MPa)
- \(\sigma _{{\text{d}}}\) :
-
Stress of the Abel dashpot (MPa)
- \(\sigma _{{\text{p}}}\) :
-
Stress of the fractional element (MPa)
- \(\sigma _{{\text{m}}}^{'}\) :
-
Effective spherical stress tensor
- \(\sigma _{{ij}}^{'}\) :
-
Effective stress tensor
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Acknowledgements
The present work is supported by the National Natural Science Foundation of China (51674266, 51827901, 51904309) and the Yueqi Outstanding Scholar Program of CUMTB (2017A03). The financial supports are gratefully acknowledged.
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Zhang, L., Zhou, H., Wang, X. et al. A triaxial creep model for deep coal considering temperature effect based on fractional derivative. Acta Geotech. 17, 1739–1751 (2022). https://doi.org/10.1007/s11440-021-01302-w
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DOI: https://doi.org/10.1007/s11440-021-01302-w