Page 100 - Analysis and Design of Energy Geostructures
P. 100

72    Analysis and Design of Energy Geostructures


                   The hypothesis for geomaterials to be characterised by only one fluid phase of
                water or air, which involves completely dry or fully saturated conditions with water,
                may be approximate to describe practical problems. While theories and modelling
                approaches are available to address this problem (see, e.g. Fredlund et al., 1993), they
                currently remain out of the scope of this book. Table 3.1 reports a summary of so-
                called index properties that relate the phases, masses M i (or weights W i ) and volumes
                V i of geomaterials.
                   In addition to the previous hypotheses, unless otherwise specified, reference is
                made in the following to materials that are isotropic, that is characterised by properties
                that are the same in all directions in space. When dealing with soil, rock and concrete,
                the hypothesis of isotropy may be approximate in some cases. However, when applied
                with judgement, the considered assumption has been largely proven to be effective in
                modelling the behaviour of materials and the related physical phenomena, and for this
                reason it is employed in the following.
                   Once effective properties are defined for continua, interest may lie in determining
                equivalent properties of composite materials, such as reinforced concrete. In those situations
                it is assumed that the equivalent property @ of a composite material can be determined
                from the average of the effective properties @ i of thesinglematerials i over representative
                dimensions x i (lengths, surfaces, volumes) characterising the composite material of interest
                with reference to the total reference dimension x. This approach involves

                                                    X
                                                @ 5     @ i x i                        ð3:1Þ
                                                         x
                                                     i

                3.3 Principles of heat transfer

                Heat transfer is the physical phenomenon for which energy is transferred between any two
                particles of matter that are at different temperatures. There are three modes of heat transfer
                considered in the following: conduction, convection and radiation. Additional heat transfer
                phenomena caused, for example by latent processes thatresultfromphase variations of
                material constituents exist. However, from an engineering perspective, latent heat transfer
                processes are considered negligible for the analysis and design of energy geostructures.

                   Heat transfer phenomena can be quantified and analysed in terms of suitable rate
                equations. These equations express the amount of thermal energy transferred per unit
                time. Heat transfer cannot be measured directly. However, its occurrence can be
                quantified through a measurable scalar quantity, that is the temperature, T.
                Temperature is the variable governing heat transfer. Knowledge of the temperature
                distribution within a region allows calculating the heat flow within this region
                (Hermansson et al., 2009). The analysis of the heat transfer in any medium is therefore
                strictly related to the determination of the temperature distribution within the medium
                that is subjected to certain boundary and initial conditions.
   95   96   97   98   99   100   101   102   103   104   105