1972
DOI: 10.1007/bf00284326
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A continuum theory for granular materials

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Cited by 668 publications
(286 citation statements)
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“…In the microdilatation model described in [41,57,58] The proposed more specific form of the free energy potential is 15) where the relative strain measure e := ε eq − χ involves the equivalent strain measure, ε eq , function of the three invariants of the strain tensor ε 16) where ψ α related to hardening is left unspecified and can be non-quadratic. Accordingly,…”
Section: (B) Scalar Microstrainmentioning
confidence: 99%
“…In the microdilatation model described in [41,57,58] The proposed more specific form of the free energy potential is 15) where the relative strain measure e := ε eq − χ involves the equivalent strain measure, ε eq , function of the three invariants of the strain tensor ε 16) where ψ α related to hardening is left unspecified and can be non-quadratic. Accordingly,…”
Section: (B) Scalar Microstrainmentioning
confidence: 99%
“…Eringen (1970) and Nowacki (1966)developed the linear theory of micropolar thermoelasticity which are known as micropolar coupled thermoelasticity to include thermal effects. Goodman and Cowin (1972) established a continuum theory for granular materials, whose matrix material (or skeletal) is elastic and interstices are voids and they introduced the concept of distributed body, which represents a continuum model for granular materials (sand, grain, powder, etc) as well as porous materials (rock, soil, sponge, pressed powder, cork, etc.). Nunziato and Cowin (1979), developed the non-linear theory of elastic materials with void, underlying the basic concept that the bulk density of the material is written as the product of two fields, the density field of the matrix material and the volume fraction field (the ratio of volume occupied by grains to the bulk volume at a point of the material) Kumar and Gupta (2010)].…”
Section: Latin American Journal Of Solids and Structures 12 (2015) 14mentioning
confidence: 99%
“…Our approach is close to that of the volume fraction concept as the latter reduces to the former once a suitable constraint among the enlarged set of state parameters is assumed [34]. For example, for an incompressible solid constituent, it is easy to see [25] how a mixture model endowed with the volume fraction concept transforms into a binary mixture whose solid constituent has second gradient constitutive relations. After formulating a general problem, we study deformations of a porous hollow linear elastic cylinder filled with a perfect fluid.…”
Section: Introductionmentioning
confidence: 95%