2016
DOI: 10.3233/asy-161369
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Heat distribution in a plane with a crack with a variable coefficient of thermal conductivity

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Cited by 4 publications
(5 citation statements)
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“…Two different criteria for cracking (face conductivity change from finite value to zero) are tested -the emergence of spatially random cracks, and the emergence of cracks at faces with maximal heat flux density. It should be noted, that the problem of thermal conduction in cracked solids has been a subject of analytical studies with associated constraints on domain and crack geometries and spatial distributions: an infinitely large plate with a single crack [21,22], a plate with isotropic distribution of identical cracks [23], cracks with specific geometries [24,25,26], and cracks in domains with specific geometry [27,28,29]. The proposed formulation avoids all constraints and allows for analysis of heterogeneous, anisotropic materials with an arbitrary criterion for the evolution of properties.…”
Section: Introductionmentioning
confidence: 99%
“…Two different criteria for cracking (face conductivity change from finite value to zero) are tested -the emergence of spatially random cracks, and the emergence of cracks at faces with maximal heat flux density. It should be noted, that the problem of thermal conduction in cracked solids has been a subject of analytical studies with associated constraints on domain and crack geometries and spatial distributions: an infinitely large plate with a single crack [21,22], a plate with isotropic distribution of identical cracks [23], cracks with specific geometries [24,25,26], and cracks in domains with specific geometry [27,28,29]. The proposed formulation avoids all constraints and allows for analysis of heterogeneous, anisotropic materials with an arbitrary criterion for the evolution of properties.…”
Section: Introductionmentioning
confidence: 99%
“…Different models (or different values of the gradation parameter λ in the rule of mixtures model) provided different profiles of material change, which meant different K Ic values near the crack tip. As can be seen from Equation (10), p cr /p 0 depended on K Ic .…”
Section: Resultsmentioning
confidence: 91%
“…Different models (or different values of the gradation parameter λ in the rule of mixtures model) provided different profiles of material change, which meant different KIc values near the crack tip. As can be seen from Equation (10), pcr/p0 depended on KIc. Different values of the critical load for different material models (as seen in Figure 3) but the same crack showed a difference in the fracture toughness values determined by these models, which in turn showed different concentrations of ceramic (metal) near the crack tip.…”
Section: Resultsmentioning
confidence: 91%
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“…Two different criteria for cracking (face conductivity change from finite value to zero) are tested -the emergence of spatially random cracks, and the emergence of cracks at faces with maximal heat flux density. It should be noted, that the problem of thermal conduction in cracked solids has been a subject of analytical studies with associated constraints on domain and crack geometries and spatial distributions: an infinitely large plate with a single crack [22,23], a plate with isotropic distribution of identical cracks [24], cracks with specific geometries [25][26][27], and cracks in domains with specific geometry [28][29][30]. The proposed formula-tion avoids all constraints and allows for analysis of heterogeneous, anisotropic materials with an arbitrary criterion for the evolution of properties.…”
Section: Introductionmentioning
confidence: 99%