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Electrification of toluene flowing in large-diameter metal pipes

, and . Journal of Physics D (Applied Physics), 3 (4): 563--573 (April 1970)
DOI: http://dx.doi.org/10.1088/0022-3727/3/4/313

Abstract

Data are given on the electric currents generated by the flow of toluene ($=2 10^11$ Ømega cm) and toluene containing Shell Anti-static Additive No.3 ($=5 10^11$ Ømega cm and $5 10^10$ Ømega cm) in large stainless-steel pipes (length 29 m, diameters 1.62, 2.88, 5.39, 8.35 and 10.90 cm). It is shown that the effect of changes in flow velocity and pipe diameter on charging current can be calculated using empirical equations of the form $i_infinity =KV^md^n$ when $>10^11$ Ømega cm and V=100 to 1000 cm s$^-1$. The data are also used to test the validity of the Koszman and Gavis (1962) equation for the electrification of liquids during pipeline flow. The evidence suggests that, when $G<10^-6$, the power dependence of $i_infinity$ on d for large-diameter pipes differs from the value 0.88, predicted and found to be true for small-diameter pipes. After modification to have a diameter power of 1.4, the equation could be used to calculate the order of magnitude of i$_infinity$.

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