Page 278 - Handbook of Battery Materials
P. 278

248  9 Metal Hydride Electrodes



                                                            atom    site
                                                                    occ.
                                                               La   1
                                                               Ni (1,2) 1
                                                               Ni (3)  1
                                                               D (1)  1/3
                                                               D (2)  2/3
                                                               D (3)  1/3
                                                               D (4)  2/3
                                                               D (5)  1




                    Figure 9.5  Structure of LaNi 5 D 7 . The unit cell is doubled
                    along the c axis; space group P6 3 mc [27].


                      However, disproportionation on the surface of polycrystalline LaNi 5 occurs
                    readily at room temperature and constitutes the alloy activation process described
                    in Section 9.3.1.
                      The kinetics of the formation and decomposition of LaNi 5 hydride have been
                    widely studied with just as widely varying results [30]. In most cases the investiga-
                    tions were done using static beds of metal/MH particles in contact with gaseous
                    hydrogen. Such systems have inherently poor heat transport and exchange char-
                    acteristics and, since reaction rates are high, isothermal conditions are difficult if
                    not impossible to maintain. Consequently the data are difficult to interpret, which
                    is the likely cause of the disparity in reported results. When kinetic experiments
                    were carried out isothermally or nearly so, the kinetics was well described by
                    a shrinking core model [31, 32]. In this model the rate-limiting process is the
                    solid-state transformation taking place at the interface between the α and β phases.
                    In hydride formation a growing product layer of ß LaNi 5 H x proceeds inward from
                    the surface while in hydride decomposition the reaction also proceeds inward from
                    the surface but now the growing product layer is α LaNi 5 as illustrated in Figure 9.6
                    [33].
                      A particular advantage of the AB 5 hydride family is that the properties of the
                    alloy–hydrogen system can be varied almost at will by substituting, in whole
                    or in part, other metals for lanthanum and Ni. For example, mischmetal when
                    substituted for La in LaNi 5 forms a hydride having about the same hydrogen content
                    but is much more unstable [34]. Lundin et al. [13] carried out a systematic study
                    of such substitutional alloys and correlated the free energy of formation (plateau
                    region) with the change of the interstitial hole size caused by the substituted metal
                    component. Gruen et al. [8] have taken a similar approach, but rather correlate the
                    cell volume with ln P plateau , as shown in Figure 9.7.
   273   274   275   276   277   278   279   280   281   282   283