1971
DOI: 10.1016/0020-7225(71)90055-3
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A crack between dissimilar anisotropic media

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Cited by 175 publications
(55 citation statements)
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“…In the following derivations, we will replace the complex variables 1 z x i y η = + by the common complex variable z x iy = + due to the fact that 1 z z = on the real axis (y = 0) [17]. When the analysis is finished, the complex variable z x iy = + for 1 ( ) f z shall be changed back to the corresponding complex variable 1 z .…”
Section: Basic Formationmentioning
confidence: 98%
“…In the following derivations, we will replace the complex variables 1 z x i y η = + by the common complex variable z x iy = + due to the fact that 1 z z = on the real axis (y = 0) [17]. When the analysis is finished, the complex variable z x iy = + for 1 ( ) f z shall be changed back to the corresponding complex variable 1 z .…”
Section: Basic Formationmentioning
confidence: 98%
“…The crack length is 5 cm, from (−5, 0) to (0, 0) and the crack-tip is located at (0, 0) and the plane stress state is presumed. The following material properties are used: (Norway spruce; Piceaabies) [41]: E 1 = 11.84 GPa, E 2 = 0.81 GPa, G 12 = 0.63 GPa, 12 = 0.38…”
Section: S Esna Ashari and S Mohammadimentioning
confidence: 99%
“…Clements [2] studied cracks between dissimilar anisotropic linear elastic materials. These early studies have been clarified and extended by Rice [3] and Hutchinson et al [4].…”
Section: Introductionmentioning
confidence: 99%