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1-D Heat Conduction in Porous Layers...
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Villatoro Pineda, Walther.
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1-D Heat Conduction in Porous Layers for Electrochemical Energy Conversion.
紀錄類型:
書目-電子資源 : Monograph/item
正題名/作者:
1-D Heat Conduction in Porous Layers for Electrochemical Energy Conversion./
作者:
Villatoro Pineda, Walther.
出版者:
Ann Arbor : ProQuest Dissertations & Theses, : 2020,
面頁冊數:
54 p.
附註:
Source: Masters Abstracts International, Volume: 82-02.
Contained By:
Masters Abstracts International82-02.
標題:
Chemical engineering. -
電子資源:
https://pqdd.sinica.edu.tw/twdaoapp/servlet/advanced?query=27998187
ISBN:
9798662428058
1-D Heat Conduction in Porous Layers for Electrochemical Energy Conversion.
Villatoro Pineda, Walther.
1-D Heat Conduction in Porous Layers for Electrochemical Energy Conversion.
- Ann Arbor : ProQuest Dissertations & Theses, 2020 - 54 p.
Source: Masters Abstracts International, Volume: 82-02.
Thesis (M.S.)--University of California, Irvine, 2020.
This item must not be sold to any third party vendors.
Polymer electrolyte fuel cells (PEFCs) and electrolyzers show promise in enabling renewable energy source technologies such as solar and wind. Thermal management is an important aspect in the operation of these devices because it can have adverse effects on performance and durability. The porous transport layers (PTLs)/gas diffusion layers (GDLs) are porous thin layers that have many functions in both electrolyzers and fuel cells. One of their functions is to uniformly distribute heat, whereas the function of the porous flow fieldsis to distribute fluids. Knowledge of the thermal conductivity of these components is necessary when optimizing heat transport and modeling thermal distributions in PEFCs and electrolyzers. To this end, the through-plane effective thermal conductivity of a sintered and fiber titanium PTL, carbon based GDL, and nickel chromium flow field mesh is investigated ex-situ for the first time through experimental work for all the materials and computed tomography for the PTLs.Fourier's law was used to calculate thermal conductivity through a steady-state method. An apparatus was built and designed to measure the heat flux through layers of an individual sample and temperatures at designated points. The effective thermal conductivity of the dry, wet, and tomography calculated sintered Ti PTL is 0.46 ± 0.21 Wm−1K−1, 0.91 ± 0.10 Wm−1K−1, 7.66 Wm−1K−1, respectively. For the fiber Ti PTL, measured values are 0.41 ± 0.07 Wm−1K−1, 0.78 ± 0.46 Wm−1K−1, and 5.22 Wm−1K−1. The effective thermal conductivity of the GDL is 0.32 ± 0.05 Wm−1K−1 and 0.17 ± 0.03 Wm−1K−1 for the NiCr porous flow field mesh. It is shown that the thermal conductivity of the PTLs increases by a larger amount than expected when water is present. The studies presented here illustrate the importance of continued work in thermal characterization of the porous materials used in electrochemical energy conversion and storage.
ISBN: 9798662428058Subjects--Topical Terms:
560457
Chemical engineering.
Subjects--Index Terms:
1-D heat conduction
1-D Heat Conduction in Porous Layers for Electrochemical Energy Conversion.
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Polymer electrolyte fuel cells (PEFCs) and electrolyzers show promise in enabling renewable energy source technologies such as solar and wind. Thermal management is an important aspect in the operation of these devices because it can have adverse effects on performance and durability. The porous transport layers (PTLs)/gas diffusion layers (GDLs) are porous thin layers that have many functions in both electrolyzers and fuel cells. One of their functions is to uniformly distribute heat, whereas the function of the porous flow fieldsis to distribute fluids. Knowledge of the thermal conductivity of these components is necessary when optimizing heat transport and modeling thermal distributions in PEFCs and electrolyzers. To this end, the through-plane effective thermal conductivity of a sintered and fiber titanium PTL, carbon based GDL, and nickel chromium flow field mesh is investigated ex-situ for the first time through experimental work for all the materials and computed tomography for the PTLs.Fourier's law was used to calculate thermal conductivity through a steady-state method. An apparatus was built and designed to measure the heat flux through layers of an individual sample and temperatures at designated points. The effective thermal conductivity of the dry, wet, and tomography calculated sintered Ti PTL is 0.46 ± 0.21 Wm−1K−1, 0.91 ± 0.10 Wm−1K−1, 7.66 Wm−1K−1, respectively. For the fiber Ti PTL, measured values are 0.41 ± 0.07 Wm−1K−1, 0.78 ± 0.46 Wm−1K−1, and 5.22 Wm−1K−1. The effective thermal conductivity of the GDL is 0.32 ± 0.05 Wm−1K−1 and 0.17 ± 0.03 Wm−1K−1 for the NiCr porous flow field mesh. It is shown that the thermal conductivity of the PTLs increases by a larger amount than expected when water is present. The studies presented here illustrate the importance of continued work in thermal characterization of the porous materials used in electrochemical energy conversion and storage.
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