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    Hydrogen storage properties of nanoconfined LiBH4–Ca(BH4)2

    Access Status
    Fulltext not available
    Authors
    Javadian, Payam
    Sheppard, Drew
    Buckley, Craig
    Jensen, T.
    Date
    2015
    Type
    Journal Article
    
    Metadata
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    Citation
    Javadian, P. and Sheppard, D. and Buckley, C. and Jensen, T. 2015. Hydrogen storage properties of nanoconfined LiBH4–Ca(BH4)2. Nano Energy. 11: pp. 96-103.
    Source Title
    Nano Energy
    DOI
    10.1016/j.nanoen.2014.09.035
    ISSN
    2211-2855
    School
    Department of Physics and Astronomy
    URI
    http://hdl.handle.net/20.500.11937/44163
    Collection
    • Curtin Research Publications
    Abstract

    The hydrogen storage properties of the eutectic melting metal borohydrides, 0.7LiBH4–0.3Ca(BH4)2, nanoconfined in two carbon aerogel scaffolds with different surface areas and pore volumes (pristine and CO2-activated) are presented and compared to the bulk properties. The temperature of hydrogen release investigated by temperature programmed desorption mass spectroscopy is reduced by 83 °C for nanoconfined LiBH4–Ca(BH4)2 in the pristine scaffold and by 95 °C in the CO2-activated scaffold, compared to that of the bulk. This corresponds to apparent activation energies, EA, of 204, 156 and 130 kJ/mol. Several cycles of reversible, continuous release and uptake of hydrogen is investigated by the Sieverts' method. Nanoconfined LiBH4–Ca(BH4)2 in the CO2-activated scaffolds demonstrate high degree of stability, releasing 80% and 73% of the original hydrogen content in the second and third hydrogen release cycle, respectively. However most importantly, this study shows that CO2-activated carbon aerogel, CA-6, is more stabile against reaction with the metal hydride and a lower amount of borates and oxides are formed during melt infiltration and hydrogen release and uptake cycling. We conclude that the CO2-activated scaffold is more inert, provides faster kinetics and higher stability over several cycles of hydrogen release and uptake and has the potential to provide useful hydrogen storage densities in the range ~12 wt% H2.

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