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16.3 SEI Formation on Carbonaceous Electrodes  499

               molecules that form large and stable solvated lithium cations will have a smaller
               tendency for co-intercalation into the graphite.
                In conclusion, it seems that solvents appropriate for lithium-ion batteries em-
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               ploying a graphite anode must have high solvation energy, high E , and high
               i 0 for reduction in order to slow the co-intercalation of the solvated ion, and to
               enhance the formation of the SEI at the most positive potential (far from the Li/Li +
               potential).
                Another phenomenon which has practical importance, especially for large pris-
               matic cells, is gas production during the first charge [95, 96]. There are two
               sources of gas: (i) the reduction of the electrolyte with the formation of methane
               or ethane, CO, and hydrogen and (ii) replacement of gases adsorbed on the carbon
               by SEI-building materials during the formation of the SEI. Gases such as H 2 ,O 2 ,
               CO 2 ,N 2 , and small organic molecules are released from the micropores of the
               carbon. The second source of gases is very significant if the carbons being used are
               disordered, but less so if the carbons are graphite-like.
                It was concluded [97, 98] that, on long cycling of the lithium-ion battery, the
               passivating layer on the carbon anode becomes thicker and more resistive, and is
               responsible, in part, for capacity loss.
               16.3.3
               Parameters Affecting Q IR

               It has been shown [8, 72, 75] that Q IR is consumed mainly in the building of the
               SEI. However, for a variety of carbons and graphites, Q IR may have other sources
               [6, 72] (Equation 16.6):

                    Q IR = Q SEI + Q SP + Q U + Q T                       (16.6)
               where Q SEI is the capacity needed for the formation of the SEI, Q U is the unused
               capacity under specified experimental conditions (it is usable at low rates and high
               potentials), Q SP is the capacity associated with the formation of soluble reduction
               products [6, 72], and Q T is the capacity associated with the trapping of lithium
               inside the structure of the carbon, generally as a result of irreversible reaction with
               heteroatoms present on the inner surface of closed pores [68].
                Q IR depends on the electrolyte type (solvent and salts), the impurity level of
               the carbon and the electrolyte, the real surface area of the carbon including
               inner pores which the electrolyte can enter, the surface morphology, and the
               chemical composition of the carbon. It typically decreases in the order: powders >
               microbeads > fibers. Impurities such as acids and alcohols, water, or heavy metals
               may contaminate the SEI, causing side-reactions [1, 2] such as hydrogen evolution
               and electrolyte reduction; this results in larger Q IR values [99, 100].
                Since in many publications the impurity level in the carbons and electrolytes is
               not specified, it is difficult to correlate Q IR reliably with the type of solvent or salt.
               However, it seems that in cases where the electrolyte reduction products are Li 2 CO 3
               and LiF (as in the cases when EC, CO 2 , and fluorinated anions are used), Q IR is
               lowest. We believe that controlled reduction-induced formation of nonconducting
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