Issue 53
Y.D. Shou et alii, Frattura ed Integrità Strutturale, 53 (2020) 434-445; DOI: 10.3221/IGF-ESIS.53.34 439 damage variable d and the cumulative inverse strain p . The total strain are divided into two parts, namely the elastic strain e and the plastic strain p . e p = + and e p d d d = + (1) where d is the incremental total strain, e d is the incremental elastic strain e d is the incremental plastic strain. As stated by Shao et al. [9], the damage process is coupled with plastic deformation and plastic hardening. Therefore, the thermodynamic potential can be expressed as ( ) ( ) 1 : ( ) : ( , ) 2 p p p p C d d = − − + (2) where ( ) C d is the fourth-order elastic stiffness tensor of the damaged coal-rock and ( , ) p p d is the closed plastic potential of the damaged coal-rock related to plastic hardening. Then, the equation of state can be obtained by deriving the elastic strain e from the thermodynamic potential as [9] ( ) ( ) : p e C d = = − (3) According to works by Nemat-Nasser and Hori [26], the fourth-order elastic stiffness tensor can be expressed as ( ) 3 ( ) 2 ( ) C d k d J d K = + (4) where ( ) k d is the bulk modulus of damaged materials and ( ) d is shear modulus of damaged materials. The other two symmetric four-order tensors J and K are 1 3 J = and K I J = − (5) where is the two-order unit tensor, I is the symmetric four-order unit tensors. The thermal forces related to the damage variable is expressed as [9] ( ) ( ) ( , ) ( ) 1 : : 2 p p p p d d C d Y d d d = − = − − − − (6) According to the non-negativity of the internal energy dissipation, the following expression can be obtained [9] : 0 p d Y d + (7) where is the stress tensor of coal-rock, p is the derivation of p to time t and d is the derivation of d to time t . Then, the derivative form of the constitutive equation of coal-rock can be obtained as [9] ( ) ( ) : : ( ) ( ) : ( ) : ( ) e e p p C d C d d d C d C d d d = + = − + − (8) where is the derivation of to time t .
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