Page 490 - Handbook of Battery Materials
P. 490

15.3 Lithiated Carbons vs Competing Anode Materials  463


                  400                                   STALION
                                                        Li-lon cell
                                                        (TOC-anode)

                  300                               common Li-lon cell
                 Energy density / Wh·L -1  200  Ni-MH cell
                                                    (carbon anode)







                  100
                                Ni-Cd cell

                    0
                     0           50          100         150
                               Specific energy / Wh·kg -1
               Figure 15.17  Specific energies and energy densities of
               rechargeable cells. Prepared from data kindly provided by
               Fujifilm Celltech Co., Ltd. (Idota, Y. Fujifilm Celltech Co.
               Ltd., personal communication).
               metals Mo [32, 337], W [21, 32, 338–342], and Ti [343–345]. Fujifilm Celltech claims
               that only the Sn(II) compounds in the composite oxide form the electrochemically
               active centers for Li insertion, whereas the oxides of B, P, or Al are electrochemically
               inactive. In order to explain the high specific charge, a mechanism is suggested in
               which the tin oxide reacts to Li 2 O and metallic Sn [29, 333–336]. This reaction is
               associated with large charge losses due to the irreversible formation of Li 2 Oduring
               the first charge (Figure 15.18). In a second step the Sn then alloys with lithium
               reversibly. Though Fuji Celltec Co. has stopped its R&D activities on the TCO
               recently, the idea that the high specific charge of the TCO is due to the alloying of
               metallic tin has led to a revival of research and development of Li alloys and related
               materials [135, 334–336, 346–348].
                The good cycling stability of the tin in TCO is quite unusual, because the
               electrochemical cycling of Li x Sn and also of other Li alloy electrodes is commonly
               associated with large volume changes in the order of 100–300% (Figure 15.19) [2,
               7, 22, 24, 26, 349–351]. Moreover, lithium alloys Li x M have a highly ionic character
                                x−
                            x+
               (‘Zintl-Phases,’ Li M ). For this reason they are usually fairly brittle. Mechanical
                            x
               stresses related to the volume changes induce a rapid decay in mechanical properties
               and, finally, a ‘pulverization’ of the electrode (see Part III, Chapter 15). In the TCO,
               however, the Sn is finely distributed within the matrix of the oxides of B, P, and
               Al. The matrix compounds have glass-forming properties, form a network, and
               thus stabilize the composite microstructure during charge–discharge cycling [332].
               The strategy for the improvement of cycle life by using a composite comprising
   485   486   487   488   489   490   491   492   493   494   495