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408  14 Lithium Alloy Anodes

                    on the use of these alloys started in 1983 [10], and they became commercially
                    available somewhat later.
                      It was also shown in 1983 [11] that lithium can be reversibly inserted into graphite
                    at room temperatures when a polymeric electrolyte is used. Prior experiments with
                    liquid electrolytes were unsuccessful due to co-intercalation of species from the
                    organic electrolytes that were used at that time. This problem has been subsequently
                    solved by the use of other electrolytes.
                      There has been a large amount of work on the development of graphites and
                    related carbon-containing materials for use as negative electrode materials in
                    lithium batteries in recent years, due in large part to the successful development
                    by Sony of commercial rechargeable batteries containing negative electrodes based
                    upon materials of this family.
                      Lithium–carbon materials are, in principle, no different from other lithium-
                    containing alloys. However, since this topic is treated in more detail in Part II,
                    Chapter 13, only a few points will be briefly discussed here.
                      One is that the behavior of these materials is very dependent upon the details
                    of both the nanostructure and the microstructure. Therefore, the composition,
                    as well as thermal and mechanical treatments, play especially important roles
                    in determining the resulting thermodynamic and kinetic properties. Materials
                    with a more graphitic structure have more negative potentials, whereas those
                    with less well-organized structures typically operate over much wider potential
                    ranges, resulting in a cell voltage that is both lower and more dependent on the
                    state-of-charge.
                      Another important consideration in the use of carbonaceous materials as negative
                    electrodes in lithium cells is the common observation of a considerable loss
                    of capacity during the first charge–discharge cycle due to irreversible lithium
                    absorption into the structure. This has the distinct disadvantage that it requires an
                    additional amount of lithium to be initially present in the cell. If this irreversible
                    lithium is supplied by the positive electrode, this means that an extra amount
                    of the positive electrode reactant material must be put into the cell during its
                    fabrication. As the positive electrode reactant materials often have relatively low
                                                            −1
                    specific capacities, for example, around 140 mAh g , this irreversible capacity in
                    the negative electrode leads to a requirement for an appreciable amount of extra
                    material weight and volume in the total cell.
                      There are some other matters that should be considered when comparing
                    metallic lithium alloys with the lithium–carbons. The specific volume of some
                    of the metallic alloys can be considerably lower than that of the carbonaceous
                    materials. As will be seen later, it is possible by selection among the metallic
                    materials to find good kinetics and electrode potentials that are sufficiently far
                    from that of pure lithium for there to be a much lower possibility of the potentially
                    dangerous formation of dendrites or filamentary deposits under rapid recharge
                    conditions.
                      It has been shown that there is a significant advantage in the use of very small
                    particles in cases in which there is a substantial change in specific volume upon
                    charging and discharging electrode reactants [12]. Since the absolute magnitude
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