Page 220 - Analysis and Design of Energy Geostructures
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Deformation in the context of energy geostructures  193


                     gg. The yield function of hardening materials only depends the stress state:
                         a. True
                         b. False
                    hh. Write the general mathematical formulation of the yield function of materials
                         characterised by hardening and an elastic limit that is considered to be sensitive
                         to temperature variations.
                      ii. Write the condition of consistency for materials characterised by hardening and
                         an elastic limit that is considered to be sensitive to temperature variations.
                      jj. Describe the concept of critical state.
                     kk. The critical state theory can be employed to describe the mechanical behaviour
                         of both coarse- and fine-grained materials.
                      ll. Write the mathematical expressions of the CSL in relevant planes.
                   mm. Describe the main features of multisurface and bounding surface plasticity.

                   Solutions

                    a. The variable that characterises most problems involved in mechanics is
                       the displacement vector.
                    b. The infinitesimal strain tensor is a symmetric tensor characterised by
                       nine components that in three-dimensional rectangular Cartesian coordi-
                       nates reads:

                                                      2              3
                                                        ε xx  ε xy  ε xz
                                                 ε ij 5  4  ε yx  ε yy  ε yz  5
                                                        ε zx  ε zy  ε zz
                       where the diagonal components ε kk [-] are called normal strains and repre-
                       sent stretching of an element and the off-diagonal components ε kl [-] are
                       called infinitesimal shear strains and measure angular distortion. The infini-
                                                                                         1
                       tesimal shear strains are one half of the engineering shear strains, ε kl 5 γ .
                                                                                         2  kl
                    c. The normal strains are the diagonal components ε kk of the infinitesimal
                       strain tensor. They represent the stretching of an element. In a two-
                       dimensional rectangular Cartesian coordinate system ðx;yÞ, the normal
                       strains read:

                                                               @u
                                                      ε xx 52
                                                               @x

                                                               @v
                                                       ε yy 52
                                                               @y
                       where u and v [m] are the horizontal and vertical displacements,
                       respectively.
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