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Narrow-Channel, Fluidized Beds for Effective Particle Thermal Energy Transport and Storage

Technical Report ·
DOI:https://doi.org/10.2172/2007141· OSTI ID:2007141
Colorado School of Mines (Mines) led this program in collaboration with Sandia National Laboratories (Sandia) to characterize narrow-channel fluidized beds of aluminosilicate particles – supplied by Carbo Ceramics – as a means for releasing high-temperature thermal energy in particle heat exchangers and for capturing concentrated solar energy in indirect particle receivers. Single-channel, heat transfer experiments at Mines and reduced-order 1-D models and 3-D two-fluid, CFD models explored many aspects of counterflow, bubbling fluidized beds (net downward particle flow and upward gas flow) for enhancing particle-wall heat transfer at elevated temperatures. Results at Mines on single-channel test sections consistently showed that mild bubbling fluidization increases particle-wall heat transfer coefficients (hT,w) regularly by more than 4.0x over hT,w values without fluidization at similar conditions (mean particle diameter dp, bed depth Δzb, and bed particle temperatures Tp). Insights from lab-scale tests and modeling studies provided Nusselt number correlations for hT,w and informed the design and fabrication (by Vacuum Process Engineering) of a nominal 40-kWth, particle-sCO2 plate heat exchanger (HX) with 12 parallel narrow-channel, fluidized beds bounded by stainless-steel walls with embedded microchannels for high-pressure sCO2 flows. Tests of the 40-kWth HX at the particle-sCO2 HX test stand at Sandia's National Solar Thermal Test Facility (NSTTF) were limited, due to HX design, to particle inlet temperatures Tp,in≤ 520°C with maximum sCO2 outlet temperatures TsCO2,out ≈ 440°C, which are well below design conditions for a primary HX in a sCO2 power cycle for a Gen-3 concentrating solar power (CSP) plant. Total heat transfer $$\dot{Q}_{HX}$$ remains relatively constant with increased fluidization for fixed particle and sCO2 inlet conditions because higher hT,w due to fluidization is offset by increased axial dispersion, which suppresses temperature differences between the particles and sCO2 in the counterflow configuration. The axial dispersion reduces the effective overall heat transfer coefficient U based on Tp,in to values around 200 W m-2 K-1.
Research Organization:
Colorado School of Mines, Golden, CO (United States)
Sponsoring Organization:
USDOE Office of Energy Efficiency and Renewable Energy (EERE), Renewable Power Office. Solar Energy Technologies Office
Contributing Organization:
CARBO Ceramics
DOE Contract Number:
EE0008538
OSTI ID:
2007141
Report Number(s):
ColoradoSchoolOfMines--EE0008538
Country of Publication:
United States
Language:
English

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