1962
DOI: 10.1115/1.3640581
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Introduction of Mechanics of Continua

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Cited by 65 publications
(95 citation statements)
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“…Bingham's equation for a viscoplastic material under uniaxial stress was generalized by Hohenemser and Prager (1932), Prager (1937Prager ( , 1961 and Oldroyd (1947) for a multiaxial state of stress. Our derivation follows that of Prager (1937) and standard treatments of plasticity (Hill, 1950).…”
Section: Constitutive Relationsmentioning
confidence: 99%
“…Bingham's equation for a viscoplastic material under uniaxial stress was generalized by Hohenemser and Prager (1932), Prager (1937Prager ( , 1961 and Oldroyd (1947) for a multiaxial state of stress. Our derivation follows that of Prager (1937) and standard treatments of plasticity (Hill, 1950).…”
Section: Constitutive Relationsmentioning
confidence: 99%
“…Our purpose is to outline the basic structure of the theory and to use it as the basis of a natural rate-dependent extension, in the manner of the conventional extensions of classical rate-independent theory [22] to model viscoplastic behavior.…”
Section: Rate-independent Theory and A Natural Viscoplastic Extensionmentioning
confidence: 99%
“…Bingham ([104], p. 215) proposed a constitutive relation for a visco-plastic material in a simple shear flow where the relationship between the shear stress (or stress T in general), and the rate of shear (or the symmetric part of the velocity gradient D) is given by the following (see Prager [105], p. 137):…”
Section: Yield Stressmentioning
confidence: 99%