Search for a command to run...
The present work focuses on the studies of influence of yttrium on the crystal structure, hydrogenation properties and electrochemical behaviors of the PuNi<sub>3</sub>-type La<sub>2-<i>x</i></sub>Y<sub><i>x</i></sub>MgNi<sub>9</sub> (<i>x</i> = 0.25; 0.50; 0.75; and 1.00) intermetallic alloys used as anodes of the Ni-MH batteries where up to 1/2 part of lanthanum was replaced by yttrium. X-ray diffraction studies revealed that all studied alloys are two-phase and contain PuNi<sub>3</sub>-type AB<sub>3</sub> intermetallics (major phase) and Gd<sub>2</sub>Co<sub>7</sub>-type A<sub>2</sub>B<sub>7</sub>-3R compounds (secondary phase). Unit cell constants and cell volumes for the crystal structures of the AB<sub>3</sub> intermetallics linearly decrease following an increase in Y content. Interestingly, in the LaMgNi<sub>4</sub> Laves type structure layer yttrium occupies not only the 6<i>c</i> site, but also partially fills the 3<i>a</i> site in the LaNi<sub>5</sub> layer. Neutron diffraction studies confirmed that the saturated La<sub>1.5</sub>Y<sub>0.5</sub>MgNi<sub>9</sub>D<sub>12.4</sub> hydride containing approximately 1 at. H/at. Me, crystallizes with a trigonal unit cell (space group <i>R</i>3̄<i>m</i>; <i>a</i> = 5.3681(2) Å, <i>c</i> = 26.437(4) Å) and is formed <i>via</i> an anisotropic expansion of the original intermetallic lattice. The studied hybrid structure is composed of LaNi<sub>5</sub>D<sub>5.2</sub> and LaMgNi<sub>4</sub>D<sub>7.2</sub> slabs with a similar hydrogen content. Interestingly, the H-caused expansion of the AB<sub>2</sub> and AB<sub>5</sub> layers is slightly uneven (23.2% and 27.7%, respectively). In the whole broad substitution range of yttrium for lanthanum, La<sub>2-<i>x</i></sub>Y<sub><i>x</i></sub>MgNi<sub>9</sub> alloys, independent on the content of Y, form intermetallic hydrides with a high reversible hydrogen storage capacity of ∼1.5 wt% H, while the properties of the obtained hydrides are directly related to the substitution extent Y → La. Indeed, the most rich in yttrium LaYMgNi<sub>9</sub> alloy at 20 °C shows a more than 10 times higher equilibrium pressure of hydrogen desorption as compared to the alloy with the smallest Y content, La<sub>1.75</sub>Y<sub>0.25</sub>MgNi<sub>9</sub>. A partial substitution of Y for La increases the electrochemical discharge capacity of La<sub>2.25</sub>Y<sub>0.75</sub>MgNi<sub>9</sub> alloy to reach ∼450 mA h g<sup>-1</sup> at a discharge current density of 10 mA g<sup>-1</sup>. The addition of Y greatly improves the electrochemical cycling performance, with remaining electrochemical capacity of up to 60% of the initial value, after performing 500 cycles, and is much superior as compared to the Y-free La<sub>2</sub>MgNi<sub>9</sub>-type anode. Thus, tailoring yttrium content in the alloys allows improvements of the performance of the studied alloys used as hydrogen storage and battery electrode materials.