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Statements

Subject Item
n2:RIV%2F00216208%3A11320%2F11%3A10100730%21RIV12-GA0-11320___
rdf:type
n6:Vysledek skos:Concept
dcterms:description
Time-harmonic, homogeneous and inhomogeneous plane waves propagating in isotropic and anisotropic viscoelastic media are investigated. The componental specification of the slowness vector p is used, in which the slowness vector p is computed from its known projection pΣ to an arbitrarily chosen plane Σ. The vectors p and pΣ are, in general, complex-valued. The most important step in the procedure consists in the determination of the component σ of the slowness vector p to the normal nΣ to Σ. For general anisotropic viscoelastic media, the component σ is a root of an algebraic equation of the sixth degree, with complex-valued coefficients. For isotropic viscoelastic media, the algebraic equation of the sixth degree factorizes to simple quadratic equations. For SH plane waves propagating in the plane of symmetry of a monoclinic (orthorhombic, hexagonal) viscoelastic medium it also factorizes providing a quadratic equation for SH waves. Time-harmonic, homogeneous and inhomogeneous plane waves propagating in isotropic and anisotropic viscoelastic media are investigated. The componental specification of the slowness vector p is used, in which the slowness vector p is computed from its known projection pΣ to an arbitrarily chosen plane Σ. The vectors p and pΣ are, in general, complex-valued. The most important step in the procedure consists in the determination of the component σ of the slowness vector p to the normal nΣ to Σ. For general anisotropic viscoelastic media, the component σ is a root of an algebraic equation of the sixth degree, with complex-valued coefficients. For isotropic viscoelastic media, the algebraic equation of the sixth degree factorizes to simple quadratic equations. For SH plane waves propagating in the plane of symmetry of a monoclinic (orthorhombic, hexagonal) viscoelastic medium it also factorizes providing a quadratic equation for SH waves.
dcterms:title
Componental specification of plane waves in isotropic and anisotropic viscoelastic media Componental specification of plane waves in isotropic and anisotropic viscoelastic media
skos:prefLabel
Componental specification of plane waves in isotropic and anisotropic viscoelastic media Componental specification of plane waves in isotropic and anisotropic viscoelastic media
skos:notation
RIV/00216208:11320/11:10100730!RIV12-GA0-11320___
n6:predkladatel
n7:orjk%3A11320
n3:aktivita
n17:P
n3:aktivity
P(GAP210/11/0117)
n3:dodaniDat
n9:2012
n3:domaciTvurceVysledku
n13:8515360
n3:druhVysledku
n15:O
n3:duvernostUdaju
n12:S
n3:entitaPredkladatele
n10:predkladatel
n3:idSjednocenehoVysledku
191423
n3:idVysledku
RIV/00216208:11320/11:10100730
n3:jazykVysledku
n4:eng
n3:klicovaSlova
media; viscoelastic; anisotropic; isotropic; waves; plane; specification; Componental
n3:klicoveSlovo
n8:viscoelastic n8:anisotropic n8:media n8:specification n8:isotropic n8:Componental n8:plane n8:waves
n3:kontrolniKodProRIV
[C4C5449C65B4]
n3:obor
n16:DC
n3:pocetDomacichTvurcuVysledku
1
n3:pocetTvurcuVysledku
2
n3:projekt
n14:GAP210%2F11%2F0117
n3:rokUplatneniVysledku
n9:2011
n3:tvurceVysledku
Pšenčík, Ivan Červený, Vlastislav
n18:organizacniJednotka
11320