“…As depicted in work [24], we have [ ( , , 0)] = 0, [ ( , , 0)] = 0, [ ( , , 0)] = 0 and [ ( , , 0)] = 0. Therefore, Equations ( 9)-( 12…”
Section: Basic Equationsmentioning
confidence: 99%
“…Recently, 3D fracture behaviors of piezoelectric materials have received concerned under different electrical boundary condition (such as electrically permeable crack condition [10][11][12], the electrically impermeable crack condition [13][14][15] and the electrically semi-permeable condition [3,[16][17][18]). In order to acquire analytical solutions to 3D problems, the shape of crack was generally considered to be rectangular crack [12,[19][20][21], penny crack [22][23][24], elliptical crack [25][26][27]. In previous article, the material properties are considered to be general isotropic or transversely isotropic.…”
The paper presents the non-local stress and electric displacement solution of a 3D semi-permeable rectangular crack in infinite orthotropic piezoelectric materials (OPMs). With the help of the generalized Almansi's theorem and 2D Fourier transform, the boundary problem is formulated by three pairs of dual integral equations, and the displacement jumps across the crack surfaces are defined. The Schmidt method is used to solve the dual integral equations. The non-local stress field (NSF) and the non-local electric displacement field (NEDF) along the crack edges are deduced. Numerical results are reported to explain the influence of the size of the rectangular crack, the lattice parameter and the electric permittivity of the air inside the crack on the NSF and the NEDF at the crack edges in OPMs in detail. The present non-local solutions exhibit no stress and electric displacement singularities along the crack edges, and may be benefit future works.
“…As depicted in work [24], we have [ ( , , 0)] = 0, [ ( , , 0)] = 0, [ ( , , 0)] = 0 and [ ( , , 0)] = 0. Therefore, Equations ( 9)-( 12…”
Section: Basic Equationsmentioning
confidence: 99%
“…Recently, 3D fracture behaviors of piezoelectric materials have received concerned under different electrical boundary condition (such as electrically permeable crack condition [10][11][12], the electrically impermeable crack condition [13][14][15] and the electrically semi-permeable condition [3,[16][17][18]). In order to acquire analytical solutions to 3D problems, the shape of crack was generally considered to be rectangular crack [12,[19][20][21], penny crack [22][23][24], elliptical crack [25][26][27]. In previous article, the material properties are considered to be general isotropic or transversely isotropic.…”
The paper presents the non-local stress and electric displacement solution of a 3D semi-permeable rectangular crack in infinite orthotropic piezoelectric materials (OPMs). With the help of the generalized Almansi's theorem and 2D Fourier transform, the boundary problem is formulated by three pairs of dual integral equations, and the displacement jumps across the crack surfaces are defined. The Schmidt method is used to solve the dual integral equations. The non-local stress field (NSF) and the non-local electric displacement field (NEDF) along the crack edges are deduced. Numerical results are reported to explain the influence of the size of the rectangular crack, the lattice parameter and the electric permittivity of the air inside the crack on the NSF and the NEDF at the crack edges in OPMs in detail. The present non-local solutions exhibit no stress and electric displacement singularities along the crack edges, and may be benefit future works.
“…Nejati et al [7] gauged the relationship between T-stress and material properties. Chen et al [8] has shown that Graded Poisson's ratio affects the T-stress. Additionally, Toshio et al [9] concluded that the Poison's ratio influences the T-stress on a three-dimensional edge-cracked plate.…”
The work investigates the importance of the K-T approach in the modelling of pressure cracked structures. T-stress is the constant in the second term of the Williams expression; it is often negligible, but recent literature has shown that there are cases where T-stress plays the role of opening the crack, also T-stress improves elastic modeling at the point of crack. In this research study, the most important effects of the T-stress are collected and analyzed. A numerical analysis was carried out by the extended finite element method (X-FEM) to analyze T-stress in an arc with external notch under internal pressure. The different stress method (SDM) is employed to calculate T-stress. Moreover, the influence of the geometry of the notch on the biaxiality is also examined. The biaxiality gave us a view on the initiation of the crack. The results are extended with a comparison to previous literature to validate the promising investigations.
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