The hydrogen storage properties of
eutectic melting 0.68LiBH4–0.32Ca(BH4)2 (LiCa) as bulk
and nanoconfined into a high surface area, S
BET = 2421 ± 189 m2/g, carbon aerogel scaffold,
with an average pore size of 13 nm and pore volume of V
tot = 2.46 ± 0.46 mL/g, is investigated. Hydrogen
desorption and absorption data were collected in the temperature range
of RT to 500 °C (ΔT/Δt = 5 °C/min) with the temperature then kept constant at 500
°C for 10 h at hydrogen pressures in the range of 1–8
and 134–144 bar, respectively. The difference in the maximum
H2 release rate temperature, T
max, between bulk and nanoconfined LiCa during the second cycle is ΔT
max ≈ 40 °C, which over five cycles
becomes smaller, ΔT
max ≈
10 °C. The high temperature, T
max ≈ 455 °C, explains the need for high temperatures for
rehydrogenation in order to obtain sufficiently fast reaction kinetics.
This work also reveals that nanoconfinement has little effect on the
later cycles and that nanoconfinement of pure LiBH4 has
a strong effect in only the first cycle of H2 release.
The hydrogen storage capacity is stable for bulk and nanoconfined
LiCa in the second to the fifth cycle, which contrasts to nanoconfined
LiBH4 where the H2 storage capacity continuously
decreases. Bulk and nanoconfined LiCa have hydrogen storage capacities
of 5.4 and 3.7 wt % H2 in the fifth H2 release,
which compare well with the calculated hydrogen contents of LiBH4 only and in LiCa, which are 5.43 and 3.69 wt % H2, respectively. Thus, decomposition products of Ca(BH4)2 appear to facilitate the full reversibility of the
LiBH4, and this approach may lead to new hydrogen storage
systems with stable energy storage capacity over multiple cycles of
hydrogen release and uptake.