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Gas-Solid Flow in a Fluidized-Particle Tubular Solar Receiver: Off-Sun Experimental Flow Regimes Characterization

Author

Listed:
  • Ronny Gueguen

    (Processes, Materials and Solar Energy Laboratory, PROMES-CNRS, 7, Rue du Four Solaire, 66120 Font-Romeu, France)

  • Guillaume Sahuquet

    (Processes, Materials and Solar Energy Laboratory, PROMES-CNRS, 7, Rue du Four Solaire, 66120 Font-Romeu, France)

  • Samuel Mer

    (PROMES-CNRS Laboratory, Engineering Science Department, University of Perpignan (UPVD), Tecnosud, Rambla de la Thermodynamique, 66100 Perpignan, France)

  • Adrien Toutant

    (PROMES-CNRS Laboratory, Engineering Science Department, University of Perpignan (UPVD), Tecnosud, Rambla de la Thermodynamique, 66100 Perpignan, France)

  • Françoise Bataille

    (PROMES-CNRS Laboratory, Engineering Science Department, University of Perpignan (UPVD), Tecnosud, Rambla de la Thermodynamique, 66100 Perpignan, France)

  • Gilles Flamant

    (Processes, Materials and Solar Energy Laboratory, PROMES-CNRS, 7, Rue du Four Solaire, 66120 Font-Romeu, France)

Abstract

The fluidized particle-in-tube solar receiver concept is promoted as an attractive solution for heating particles at high temperature in the context of the next generation of solar power tower. Similar to most existing central solar receivers, the irradiated part of the system, the absorber, is composed of tubes in which circulate the fluidized particles. In this concept, the bottom tip of the tubes is immersed in a fluidized bed generated in a vessel named the dispenser. A secondary air injection, called aeration, is added at the bottom of the tube to stabilize the flow. Contrary to risers, the particle mass flow rate is controlled by a combination of the overpressure in the dispenser and the aeration air velocity in the tube. This is an originality of the system that justifies a specific study of the fluidization regimes in a wide range of operating parameters. Moreover, due to the high value of the aspect ratio, the particle flow structure varies along the tube. Experiments were conducted with Geldart Group A particles at ambient temperature with a 0.045 m internal diameter and 3 m long tube. Various temporal pressure signal processing methods, applied in the case of classical risers, are applied. Over a short acquisition time, a cross-reference of the results is necessary to identify and characterize the fluidization regimes. Bubbling, slugging, turbulent and fast fluidization regimes are encountered and the two operation modes, without and with particle circulation, are compared.

Suggested Citation

  • Ronny Gueguen & Guillaume Sahuquet & Samuel Mer & Adrien Toutant & Françoise Bataille & Gilles Flamant, 2021. "Gas-Solid Flow in a Fluidized-Particle Tubular Solar Receiver: Off-Sun Experimental Flow Regimes Characterization," Energies, MDPI, vol. 14(21), pages 1-25, November.
    • Handle: RePEc:gam:jeners:v:14:y:2021:i:21:p:7392-:d:673183
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    References listed on IDEAS

    as
    1. Zhang, Huili & Kong, Weibin & Tan, Tianwei & Baeyens, Jan, 2017. "High-efficiency concentrated solar power plants need appropriate materials for high-temperature heat capture, conveying and storage," Energy, Elsevier, vol. 139(C), pages 52-64.
    2. Ronny Gueguen & Benjamin Grange & Françoise Bataille & Samuel Mer & Gilles Flamant, 2020. "Shaping High Efficiency, High Temperature Cavity Tubular Solar Central Receivers," Energies, MDPI, vol. 13(18), pages 1-24, September.
    3. Benoit, H. & Spreafico, L. & Gauthier, D. & Flamant, G., 2016. "Review of heat transfer fluids in tube-receivers used in concentrating solar thermal systems: Properties and heat transfer coefficients," Renewable and Sustainable Energy Reviews, Elsevier, vol. 55(C), pages 298-315.
    4. Jacob, Rhys & Belusko, Martin & Inés Fernández, A. & Cabeza, Luisa F. & Saman, Wasim & Bruno, Frank, 2016. "Embodied energy and cost of high temperature thermal energy storage systems for use with concentrated solar power plants," Applied Energy, Elsevier, vol. 180(C), pages 586-597.
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