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               362                                                                                    Dielectric Gases


                                                                 V s  of the constituent component gases. In Fig. 4b, exam-
                                                                 ples are given of binary mixtures of a buffer gas that slows
                                                                 down electrons efficiently (CO, N 2 , or CO 2 ) and the elec-
                                                                 tronegative gas SF 6 . At all gas compositions, the measured
                                                                 (V s ) mix  exceedsthepartial-pressure-weightedvaluesofthe
                                                                 individual components. This has been referred to as syn-
                                                                 ergism. Similar results are shown in Fig. 4c for mixtures
                                                                 of the strongly electronegative gas c-C 4 F 8  and the nonpo-
                                                                 lar weakly electron-attaching buffer gas CF 4  or the polar
                                                                 buffer gases CHF 3  or 1,1,1-CH 3 CF 3 , which slow down
                                                                 electrons efficiently via dipole scattering. The (V s ) mix  for
                                                                 the polar gas-containing mixtures far exceeds the partial-
                                                                 pressure-weighted V s , especially for small percentages of
                                                                 the electronegative gases.
                                                                   In  Fig.  4c  the  behavior  of  curve  1  is  interesting  in
               FIGURE 2  Effective ionization coefficient (α −η)/N as a function
                                                                 that  for  certain  gas  compositions  the  (V s ) mix exceeds
               of the density-reduced electric field E /N. Curves are for the fol-
                                           2
               lowing gases and (E /N) lim (10 −17  V cm ):   N 2 , 130; ∇ 1% SF 6 ,  the V s  of either component. This has been observed for
                                                                 other binary mixtures (e.g., 1-C 3 F 6 /c-C 4 F 8 ; 1-C 3 F 6 /SO 2 ;
               160; +10% SF 6 , 235;   20% SF 6 , 269;   50% SF 6 , 323; and •
               100% SF 6 , 361. [Data from Aschwanden, T. (1984). In “Gaseous  SO 2 /SF 6 ; C 3 F 8 /SF 6 ; and OCS/SF 6 ) for which the electron-
               Dielectrics IV” (L. G. Christophorou and M. O. Pace, eds.), p. 30,  attachment properties of one or both of the constituent
               Pergamon Press, New York.]
                                                                 gases depend on the total gas pressure and the mixture
                                                                 composition. This is clearly seen by the data in Fig. 4d,
               constant,  as  a  function  of  the  mean  electron  energy  which show the variation of (V s ) mix  for SF 6 /1-C 3 F 6  with
                                                            R
                ε , k a ( ε ), increases, so does the breakdown voltage V  s  relative composition and total gas number density.
               relative to SF 6 . Knowledge of k a ( ε ) or σ a (ε) led to the  Many studies on gas mixtures identified binary gas mix-
               identification of many excellent unary gas dielectrics such  tures [e.g., SF 6 /N 2 , perfluorocarbon/SF 6 , and perfluoro-
               as the perfluorocarbons (see Table II, which is discussed  carbon/N 2  (or CHF 3 )] that can be useful for applications.
               in Section III).
                 It  is  thus  apparent  that  the  dielectric  properties  of
               gases can be optimized by a combination of two or more
               gases (i.e., by tailoring multicomponent gas mixtures) de-
               signed, for example, to provide the best effective com-
               bination of electron-attaching and electron slowing-down
               components. Basic knowledge on the processes in Table
               I offers several ways to the systematic development of
               dielectric gas mixtures. Thus knowledge on the electron-
               attachment cross section guided the choice of unary gas di-
               electrics or electronegative components for dielectric gas
               mixtures, and knowledge on electron scattering at low en-
               ergies guided the choice of buffer gases for mixtures con-
               taining electronegative additives. Of practical significance
               are mixtures of the strongly electron-attaching gases in
               Table II with abundant, inert, and inexpensive buffer gases
               (e.g., N 2 ), with which they act synergistically: the buffer
               gas(es) scatter electrons into the energy range in which the
               electronegative gas(es) capture electrons most efficiently.
                 Examples of the various types of observed uniform field
               behavior of the breakdown voltage (V s ) mix  of binary gas
               mixtures with respect to those (V s ) A,B  of the individual
               components A, B as a function of gas composition are
                                                                 FIGURE 3 Total electron-attachment rate constant k a as a func-
               shown in Fig. 4. Figure 4a shows the behavior of (V s ) mix
                                                                 tion of the mean electron energy  ε  for the perfluoroalkanes
               for binary mixtures of electronegative gases whose k a ( ε )
                                                                 C N F 2N+2 (N = 1–6) and their dc uniform field breakdown voltages
               is independent of gas number density  N. The (V s ) mix  is  relative to SF 6 . [From Christophorou, L. G., et al. (1984), IEEE
               nearly equal to the sum of the partial-pressure-weighted  Trans. Elect. Insul. El-19, 550–566.]
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