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158   Analysis and Design of Energy Geostructures















                Figure 4.11 Concept of perfect elasticity.

                   In many situations, the reversible mechanical behaviour of materials is associated
                with linear stress strain relations, while their irreversible behaviour (typically achieved
                when the applied loads exceed the aforementioned limit) with nonlinear stress strain
                relations. However, the reversibility of the mechanical behaviour of materials does not
                imply linearity and various materials are characterised by a reversible behaviour follow-
                ing nonlinear stress strain relations, especially at small strain levels. Elasticity can be
                linear or nonlinear. In the following, reference is made to a linear thermoelastic
                behaviour of materials.


                4.9.2 Thermoelastic stress strain relations

                The total strain at each point of a material characterised by a thermoelastic behaviour
                is generally given by the sum of two contributions. The first contribution comprises
                the strains induced by the application of a force (or displacement) field that is required
                to maintain the continuity of the material by means of the generalised Hooke’s law.
                The second contribution comprises the strains induced by the application of a temper-
                ature change to the material.
                   The previous considerations can be mathematically expressed in compact form as

                                          ε ij 5 C ijkl σ kl 2 β ðT 2 T 0 Þ           ð4:48Þ
                                                        kl
                where C ijkl is the elastic compliance matrix (i.e. inverse of the elastic stiffness tensor,
                D ijkl ), β  is a vector that comprises the linear thermal expansion coefficient of the
                       kl
                material, α,and T 2 T 0 5 ΔT is the applied temperature variation. Strains induced
                by thermal loads are proportional to the applied temperature variation, ΔT, and to
                the linear thermal expansion coefficient of the material, α. Table 4.1 summarises the
                values of linear thermal expansion coefficient for many materials of practical interest
                in the context of energy geostructures. The temperature variations associated with
                the geothermal operation of energy geostructures should range, at worst, between
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