A Locke Dictionary (The Blackwell Philosopher Dictionaries) by John W. Yolton

By John W. Yolton

This dictionary provides and explains the foremost phrases and ideas in Locke's proposal and books. Over one hundred thirty entries comprise debts of his quite a few books, his position in technological know-how and faith and his writings on schooling, theology and economics. The dictionary may still make Locke's proposal obtainable to expert and non-specialist readers alike. The ideas and phrases are taken from the total variety of his guides and the dictionary is predicated on all that he released, together with his correspondence. each one "Blackwell thinker Dictionary" offers the existence and paintings of someone thinker in a scholarly but obtainable demeanour. Entries conceal key rules and recommendations, in addition to the most issues of the philosopher's paintings. A accomplished biographical cartoon is additionally incorporated. it's geared toward undergraduates in philosophy.

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Computational fracture mechanics, Proc. Symp. Numer. Comp. Methods in Struct. 585 (1973). Rudnicki, J . W . : Condition for the localization of deforma­ tion in pressure-sensitive dilatant materials, J. Mech. Phys. Solids, 2 3 , 371 (1975). , 2 1 , 19 (1973). , 469 (1974). , 2 3 , 421 (1975). S. : Deformation beha­ vior of elastic-plastic tubes under extended pressure and axial loads, Int. J. Mech. , 20, 263 (1986). Κ. : A five constant model unifying well-established concepts, Int. 175 (1984).

Solids, 6, 236 (1958). : On the classical constitutive relations for elastic-plastic solids, Re­ cent Progress in Appl. , 241 (1967). Iwan, W . D . Appl. , 3 4 , 612 (1967). Koiter, W . T . : Stress-strain relations, uniqueness and variational theories for elastic-plastic materials with a singular yield surface, Quart. Appl. , 10, 157 (1953). : A practical two surface plasticity theory, J. AppL Mech. ( A S M E ) , 4 2 , 641 (1975). D. : Accuracies of numerical solution methods for the elastic-perfectly plastic models, J.

In the initial loading process t h e stress reaches the yield surface moving along a stress p a t h t h e length of which corresponds to the radius of yield t h e surface. On t h e other h a n d , in t h e unloading - reverse loading process t h e stress reaches t h a t surface moving along a stress path t h e length of which corresponds to t h e diameter of the yield surface while t h e plastic deformation proceeds gradually even in the unloading process. Therefore, t h e plastic modulus m a y change more gradually in the unioading-reverse loading process than in t h e initial loading process.

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