Page 155 - Analysis and Design of Energy Geostructures
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Heat and mass transfers in the context of energy geostructures  127



                                                    ð
                                          λ 5 nλ a 1 1 2 nÞλ s 5 0:25 W=ðm CÞ
                          The thermal conductivity of water at ambient temperature is

                       λ w 5 0:58 W/(m C). Hence, for the case in which the sand is saturated
                       with water the effective thermal conductivity reads


                                         λ sat 5 nλ w 1 1 2 nÞλ s 5 0:48 W=ðm CÞ
                                                     ð
                          The above explains why a thermal conductor present in soil pores,
                       such as water, strongly increases the heat exchange between, for example
                       an energy pile and the surrounding soil, in contrast to what happens with
                       a thermal insulator like air.
                    n. The effective thermal conductivity can be defined as

                                                  λ 5 nλ a 1 1 2 nð  Þλ s

                          The thermal conductivity of air at ambient temperature is

                       λ a 5 0:025 W/(m C), hence λ 5 nλ a 1 1 2 nð  Þλ s 5 0:1 W/(m C), which is
                       five times less than the value obtained for the saturated sand. Therefore
                       in general, the heat exchange is less favourable for an energy geostructure
                       adjacent to a saturated clayey deposit than to a saturated sandy deposit.
                    o. Thermal conductivity for concrete goes from about 0.15 to about 2 W/
                       (m C), depending, for example on its structure and mix design.

                    p. Energy is transferred by the macroscopic motion of the fluid, in addition
                       to energy transfer due to random molecular motion (diffusion). The fluid
                       motion is associated with the fact that large numbers of molecules are
                       moving collectively or as aggregates. This motion, in the presence of a
                       temperature gradient, contributes to heat transfer. Since the molecules in
                       the aggregate retain their random motion, the total heat transfer is then
                       due to a superposition of energy transport by the random motion of the
                       molecules and by the bulk motion of the fluid. The term convection is
                       usually used when referring to this cumulative transport, and the term
                       advection usually refers to transport due to bulk fluid motion.
                    q. Convection heat transfer can be classified according to the nature of the
                       flow. Forced convection characterises heat flows caused by external means,
                       such as a pump, a fan or atmospheric winds. In contrast, free (or natural)
                       convection characterises heat flows induced by buoyancy forces, which are
                       due to density differences caused by temperature variations in the fluid.
                    r. Thermal radiation is energy emitted by matter that is at a nonzero tem-
                       perature. Radiation that is emitted by the surface originates from the
                       thermal energy of matter bounded by the surface and the rate at which
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