Interaction between elastic longitudinal shear waves and radially distributed cracks (Q2714556)
From MaRDI portal
| This is the item page for this Wikibase entity, intended for internal use and editing purposes. Please use this page instead for the normal view: Interaction between elastic longitudinal shear waves and radially distributed cracks |
scientific article; zbMATH DE number 1606992
| Language | Label | Description | Also known as |
|---|---|---|---|
| English | Interaction between elastic longitudinal shear waves and radially distributed cracks |
scientific article; zbMATH DE number 1606992 |
Statements
20 June 2001
0 references
medium with cracks
0 references
solution to the Helmholtz equation
0 references
Interaction between elastic longitudinal shear waves and radially distributed cracks (English)
0 references
An elastic medium is considered under the conditions of antiplane deformation with \(N\) cracks occupying the segments \(\,\theta=\theta_l\), \(\,r\in[a_l,b_l]\), \(\,l=1,2,\dots,N\,\) in the plane \(\,(r,\theta)r>0\), \(\,-\pi<\theta<\pi\). The cracks are affected by the longitudinal shear wave propagating in the medium and causing the transpositions NEWLINE\[NEWLINE w_0(r,\theta_l) = A\,\exp@,(ik_2r\,\cos@,(\theta-\theta_0)),\quad\,\, k_2^2 = \frac{\rho\omega^2}{G}, NEWLINE\]NEWLINE where \(\,\rho\) is the medium density, \(G\) is the shear modulus and \(\omega\) is the oscillation frequency.\flushpar The author applies the discontinuous solutions to the Helmholtz equation. This allows an efficient investigation of the peculiarities of the appearing dynamical stress state.
0 references