Proceedings of the Royal Society of London A Mathematical and Physical Sciences · 1973 · 14 citations · 3 references
EngineeringPhysicsElectromagnetismHeat TransferTransport PhenomenaBoiling Heat TransferElectrical ConductivityHeat ConductionHeat Transfer FundamentalsHeat Transfer In FluidsConduction In FluidsConvectionDielectrophoresisDielectrophoretic TransportIon TransportIonic LiquidsIonic Polarity EffectPolarity Effects
Abstract Heat transfer by convection from a thin wire to a liquid was very appreciably increased by the application of a non-uniform electric field of several hundred kilovolts per centimetre which was confocal with the temperature field. This enhancement of the heat flux was much larger in a polar, slightly conducting liquid than in a practically ion-free liquid; the behaviour of a non-polar liquid which contained traces of a polar impurity was intermediate between the two. The polarity of the electric field affected the magnitude of the enhancement of the heat flux in the polar liquid and to a lesser extent also in the non-polar liquid which had a slight content of a polar contamination, but the direction of the field had no influence what-soever on the enhancement of the heat flux in the ion-free liquid. With each of these three liquids the electrostatic field delayed and even suppressed the transition to nucleate boiling and therefore reduced the risk of ‘burn-out'. It appears that dielectrophoresis is primarily responsible for the increased convection, but that an ion transport phenomenon can make a further significant contribution. The observed polarity effects, in the presence of a minute concentration of ions, suggest that this could be an ion wind. For large values of the electrical number (El) the incremental increase of the Nusselt number (Nu) by dielectrophoresis can be of the order of one hundred.
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