Strength Analysis in Geomechanics ,_5YaX:<4
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by lN][xnP
S. Elsoufiev E<98ahZ?l
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Springer, 2007 O[5_9W
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Foundations of Engineering Mechanics 1b
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Series Editors: V.I. Babitsky, J. Wittenburg D~i@. k
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It is hardly possible to find a single rheological law for all the soils. However, 9FIe W[
they have mechanical properties (elasticity, plasticity, creep, damage, etc.) g~$GE},,
that are met in some special sciences, and basic equations of these disciplines U||w6:W5
can be applied to earth structures. This way is taken in this book. It represents ` + n
the results that can be used as a base for computations in many fields of the h.}t${1ZC
Geomechanics in its wide sense. Deformation and fracture of many objects -KU)7V
include a row of important effects that must be taken into account. Some of b[&,%Sm+6
them can be considered in the rheological law that, however, must be simple >TY5ZRB
enough to solve the problems for real objects. JPoK\-9NT
On the base of experiments and some theoretical investigations the constitutive I[cV"BDa
equations that take into account large strains, a non-linear unsteady SCt=OdP=
creep, an influence of a stress state type, an initial anisotropy and a damage [Q.4]K2
are introduced. The test results show that they can be used first of all to s&QBFyKtJ
finding ultimate state of structures – for a wide variety of monotonous loadings NP<F==,
when equivalent strain does not diminish, and include some interrupted, 3Q!J9t5dc
step-wise and even cycling changes of stresses. When the influence of time &[2Ej|o
is negligible the basic expressions become the constitutive equations of the 8KL_PwRX_f
plasticity theory generalized here. At limit values of the exponent of a hardening 4,*^QK
law the last ones give the Hooke’s and the Prandtl’s diagrams. Together U_
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with the basic relations of continuum mechanics they are used to describe the bVAgul=__
deformation of many objects. Any of its stage can be taken as maximum Fv7%TK{oe
allowable one but it is more convenient to predict a failure according to the H2FFw-xW
criterion of infinite strains rate at the beginning of unstable deformation. The zb~MF_ &gE
method reveals the influence of the form and dimensions of the structure on CL@h!h554_
its ultimate state that are not considered by classical approaches. +DbWMm
Certainly it is hardly possible to solve any real problem without some GJ^]ER-K
assumptions of geometrical type. Here the tasks are distinguished as antiplane !=h|&Vta
(longitudinal shear), plane and axisymmetric problems. This allows ~y-vKCp|
to consider a fracture of many real structures. The results are represented _WjETyh
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by relations that can be applied directly and a computer is used (if necessary) _w5~/PbWt
on a final stage of calculations. The method can be realized not only in HC;I0&v>
Geomechanics but also in other branches of industry and science. The whole @7[.>I(
approach takes into account five types of non-linearity (three physical and SJ WP8+
two geometrical) and contains some new ideas, for example, the consideration R6WgA@Z|r
of the fracture as a process, the difference between the body and the element N|Cy!E=d
of a material which only deforms and fails because it is in a structure, the l3Bxi1k[C
simplicity of some non-linear computations against linear ones (ideal plasticity *|gs-<[#X
versus the Hooke’s law, unsteady creep instead of a steady one, etc.), the XnI
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independence of maximum critical strain for brittle materials on the types of k1$2a8ja
structure and stress state, an advantage of deformation theories before flow %&=(,;d
ones and others. D@4&@>
All this does not deny the classical methods that are also used in the book r~D~7MNl
which is addressed to students, scientists and engineers who are busy with %Dr4~7=7a
strength problems.