2017
DOI: 10.1016/j.applthermaleng.2017.05.131
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Effects of different parameters on the discharging of double-layer PCM through the porous channel

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Cited by 20 publications
(3 citation statements)
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“…(5) Thermal resistance of aluminum walls cannot be ignored because their thickness is considerable, and conductive heat transfers through walls; (6) The Rayleigh number, defined as Ra = (gβ(∆T)r 3 )⁄αυ, is set at a fixed value of 10 6 . ∆T stands for the amplitude of bulk HHTF temperature, g is the gravitational acceleration, r is the radius of PCM container, β is thermal expansion coefficient, and υ and α are the kinematic viscosity and thermal diffusivity, respectively; (7) Super-cooling effects and viscous dissipation are negligible; (8) Volume change in PCMs due to phase change is insignificant; (9) In annulus walls, no slip boundary conditions are employed; (10) To simulate the phase change process, the enthalpy method is employed; (11) In order to evaluate the flow within the porous matrix, Brinkman-Forchheimerextended Darcy model is used [23]; (12) The PCM is saturated in homogeneous and isotropic porous matrix.…”
Section: Physical Model and Boundary Conditionsmentioning
confidence: 99%
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“…(5) Thermal resistance of aluminum walls cannot be ignored because their thickness is considerable, and conductive heat transfers through walls; (6) The Rayleigh number, defined as Ra = (gβ(∆T)r 3 )⁄αυ, is set at a fixed value of 10 6 . ∆T stands for the amplitude of bulk HHTF temperature, g is the gravitational acceleration, r is the radius of PCM container, β is thermal expansion coefficient, and υ and α are the kinematic viscosity and thermal diffusivity, respectively; (7) Super-cooling effects and viscous dissipation are negligible; (8) Volume change in PCMs due to phase change is insignificant; (9) In annulus walls, no slip boundary conditions are employed; (10) To simulate the phase change process, the enthalpy method is employed; (11) In order to evaluate the flow within the porous matrix, Brinkman-Forchheimerextended Darcy model is used [23]; (12) The PCM is saturated in homogeneous and isotropic porous matrix.…”
Section: Physical Model and Boundary Conditionsmentioning
confidence: 99%
“…Likewise, Zhao et al [22] investigated the phase transition of RT58 through a porous matrix and reported enhancements of 3-10-fold in heat transfer rate for various metal foam structures and materials. Sefidan et al [23] numerically investigated the effects of various parameters on the solidification process of a double-layer PCM inside a rectangular porous channel. The effects of medium porosity, eccentricity of inner and outer sections, wall temperature and various arrangements of PCMs were reported.…”
Section: Introductionmentioning
confidence: 99%
“…There are three schemes for conserving thermal energy, the sensible, the latent, and the thermochemical TES 3 . The latent heat energy storage scheme (LHESS) is superior to the other forms of storing thermal energy due to these reasons 4 : (a) thermal energy is held at a constant temperature, 5 (b) the energy storage density of LHESS is higher than that of the others, 6 and (c) LHESS can operate in a large number of cycles without any significant limitation 7 . LHESS is mostly recommended in applications with space limitations since thermal energy can be stored 5–14 times greater than that of sensible heat storage materials 8,9 .…”
Section: Introductionmentioning
confidence: 99%