By Dr. Loucas G. Christophorou
Read Online or Download Gaseous Dielectrics II. Proceedings of the Second International Symposium on Gaseous Dielectrics, Knoxville, Tennessee, U.S.A., March 9–13, 1980 PDF
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Additional info for Gaseous Dielectrics II. Proceedings of the Second International Symposium on Gaseous Dielectrics, Knoxville, Tennessee, U.S.A., March 9–13, 1980
That is to say, the gas mixture may 6 33 exhibit a dielectric strength in excess of that expected from the properties of the separate gases. Clearly, the presence or absence of synergism, as broadly defined in the preceding sentence, depends not only on the gas properties but also on the approach taken to decide what to expect of the mixture, from the properties of the individual gases. In a certain extreme sense, "synergism" is solely the product of the inadequacies of the theory used to predict the mixture behavior.
If condition (i) is not satisfied, then (ii) is unlikely to be satisfied, and we expect the Wieland assumption to be best satisfied by gases which individually have similar energy distributions. This is illustrated by the data of Fig. 2 viewed in the light of Fig. 3. In Fig. 3a the normalized energy distributions computed (ref. 52 x 1 0 " V c m for He and S F separately, and for an S F ( 4 0 ) | He(60) mixture are plotted. Individually the gases have dramatically different distributions, and we note that when mixed the S F has a dominating effect.
Symp. on electrical insulation (Montreal, 1 9 7 6 ) , 282 (6) J. R. Hollahan and A. T, Bell (1974) Chemistry, Wiley, New York. (7) E.
Gaseous Dielectrics II. Proceedings of the Second International Symposium on Gaseous Dielectrics, Knoxville, Tennessee, U.S.A., March 9–13, 1980 by Dr. Loucas G. Christophorou