LEADER 03780nam 22006495 450 001 9910299706903321 005 20200630130712.0 010 $a3-642-40945-8 024 7 $a10.1007/978-3-642-40945-5 035 $a(CKB)2550000001152824 035 $a(EBL)1698211 035 $a(OCoLC)864755111 035 $a(SSID)ssj0001049312 035 $a(PQKBManifestationID)11592854 035 $a(PQKBTitleCode)TC0001049312 035 $a(PQKBWorkID)11019134 035 $a(PQKB)10022764 035 $a(MiAaPQ)EBC1698211 035 $a(DE-He213)978-3-642-40945-5 035 $a(PPN)176115463 035 $a(EXLCZ)992550000001152824 100 $a20131025d2014 u| 0 101 0 $aeng 135 $aur|n|---||||| 181 $ctxt 182 $cc 183 $acr 200 10$aPlasticity of Pressure-Sensitive Materials$b[electronic resource] /$fedited by Holm Altenbach, Andreas Öchsner 205 $a1st ed. 2014. 210 1$aBerlin, Heidelberg :$cSpringer Berlin Heidelberg :$cImprint: Springer,$d2014. 215 $a1 online resource (383 p.) 225 1 $aEngineering Materials,$x1612-1317 300 $aDescription based upon print version of record. 311 $a3-642-40944-X 320 $aIncludes bibliographical references. 327 $aPart I:Experimental Observations -- Part II: Theoretical Foundation -- Summary of Continuum mechanics -- Yield Criteria -- Theory of Plasticity -- Part III: Applications -- Metal Forming -- Powder -- Concrete -- Soil and Rock -- Porous Metals -- Cellular -- Human -- Adhesives and Polymers -- Part IV: Some Mathematics. 330 $aClassical plasticity theory of metals is independent of the hydrostatic pressure. However, if the metal contains voids or pores or if the structure is composed of cells, this classical assumption is no more valid and the influence of the hydrostatic pressure must be incorporated in the constitutive description. Looking at the microlevel, metal plasticity is connected with the uniform planes of atoms organized with long-range order. Planes may slip past each other along their close-packed directions. The result is a permanent change of shape within the crystal and plastic deformation. The presence of dislocations increases the likelihood of planes slipping. Nowadays, the theory of pressure sensitive plasticity is successfully applied to many other important classes of materials (polymers, concrete, bones etc.) even if the phenomena on the micro-level are different to classical plasticity of metals. The theoretical background of this phenomenological approach based on observations on the macro-level is described in detail in this monograph and applied to a wide range of different important materials in the last part of this book. 410 0$aEngineering Materials,$x1612-1317 606 $aMechanics 606 $aMechanics, Applied 606 $aMaterials science 606 $aSolid Mechanics$3https://scigraph.springernature.com/ontologies/product-market-codes/T15010 606 $aMaterials Science, general$3https://scigraph.springernature.com/ontologies/product-market-codes/Z00000 606 $aClassical Mechanics$3https://scigraph.springernature.com/ontologies/product-market-codes/P21018 615 0$aMechanics. 615 0$aMechanics, Applied. 615 0$aMaterials science. 615 14$aSolid Mechanics. 615 24$aMaterials Science, general. 615 24$aClassical Mechanics. 676 $a531.385 702 $aAltenbach$b Holm$4edt$4http://id.loc.gov/vocabulary/relators/edt 702 $aÖchsner$b Andreas$4edt$4http://id.loc.gov/vocabulary/relators/edt 906 $aBOOK 912 $a9910299706903321 996 $aPlasticity of Pressure-Sensitive Materials$91979668 997 $aUNINA