1997
DOI: 10.1088/0022-3727/30/8/008
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The simulation of short-term streaming electrification dynamics

Abstract: In an effort to understand the dynamic behaviour of the streaming electrification phenomenon better, a computational model has been prepared. This paper describes the development and behaviour of the simulation for the development of charge-density profiles in space and time subsequent to the initiation of flow in a channel. Results are provided to demonstrate the functionality of the model and its effectiveness in clarifying the nature of the phenomenon.

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Cited by 12 publications
(2 citation statements)
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“…The space between the cylinders is filled with transformer oil, which for the defined temperature T=293 K has the following parameters: dynamic viscosity: 0.02 Pa*s; heat capacity: 1720 J/(kg*K); density: 879 kg/m 3 ; thermal conductivity: 0.1107 W/(m*K). In the available literature, the values of diffusion coefficient D vary in the range of approximately 10 ˗9 -10 ˗12 (Bauer 2012;El-Adawy et al 2011;Palmer and Nelson 1997) but previous numerical studies led to the conclusion that the value may be much higher for transformer oils. Therefore, D was varied from 10 ˗6 to 10 ˗12 in the present study.…”
Section: Methodsmentioning
confidence: 99%
“…The space between the cylinders is filled with transformer oil, which for the defined temperature T=293 K has the following parameters: dynamic viscosity: 0.02 Pa*s; heat capacity: 1720 J/(kg*K); density: 879 kg/m 3 ; thermal conductivity: 0.1107 W/(m*K). In the available literature, the values of diffusion coefficient D vary in the range of approximately 10 ˗9 -10 ˗12 (Bauer 2012;El-Adawy et al 2011;Palmer and Nelson 1997) but previous numerical studies led to the conclusion that the value may be much higher for transformer oils. Therefore, D was varied from 10 ˗6 to 10 ˗12 in the present study.…”
Section: Methodsmentioning
confidence: 99%
“…However, in order to obtain analytical solutions some simplifications are needed. For instance, some authors assume the reactions' kinetics to be too slow [20][21][22][23][24], or too fast [25][26][27] when compared to charge relaxation time. In this work, we present and solve the differential equation that governs the transient formation of an EDL when a liquid at rest is put in contact with a solid wall, in the case of weak space charge density (which allows for the linearization of the equation).…”
Section: Introductionmentioning
confidence: 99%