Contents lists available at ScienceDirect International Journal of Thermal Sciences journal homepage: www.elsevier.com/locate/ijts Eect of n and electrodes on electro-hydrodynamic enhanced heat transfer in enclosures F. Fazlollahi * , A.A. Alemrajabi Department of Mechanical Engineering, Isfahan University of Technology, Isfahan 84156-83111, Iran ARTICLE INFO Keywords: EHD Enhanced heat transfer Fin Corona Enclosure ABSTRACT In this work, enhancement of heat transfer in partially open nned enclosures with single n and multiple ns was investigated experimentally. Five faces of the enclosure were insulated thermally and electrically; while one face was copper nned plate with an aperture located at its opposite face. Various parameters were considered like supplied current, electrode arrangement, number of ns, and dierent types of corona discharge. It was concluded that the heat transfer is enhanced while the supplied current is increased. Moreover, higher number of ns can lead to more enhancement of the ratio of heat transfer caused by electrohydrodynamic (EHD) technique. Finally, it was observed that the best location for electrodes is in front of the ns. 1. Introduction In electrohydrodynamic (EHD) improvement technique, a large electric eld can be used to increase the heat transfer in a dielectric uid continuum by inducing a secondary ow. This secondary ow may reduce the thickness of the thermal boundary layer which leads to re- duction of convective heat transfer resistance. The momentum ex- change between the imposed electric eld and the molecules in the dielectric uid is responsible for the deterioration of this layer. This inuence causes reducing of the thickness of the thermal boundary layer and decaying the convective thermal resistance; by which, the heat transfer is augmented. Yonggang et al. [1] studied the eect of the ionic wind on the heat transfer rate from a heated vertical at plate and have concluded that the convective heat transfer coecients increase by several times with the help of the ionic wind. Bhattacharyya and Peterson [2] examined the inuence of the corona wind on the augmentation of the natural convection heat transfer from a vertical copper plate. They investigated the eects of varying a series of parameters coupled with a range of electrode voltages and its polarity. They have concluded that electric eld strength had a direct and signicant inuence on the enhancement scale, whereas polarity change of the applied eld did not produce much signicant inuence on the enhancement ratio. Grassi et al. [3] examined the heat transfer enhancement on the upper surface of a horizontal heated plate in a pool by employing an electro- hydrodynamically induced impinging liquid ow in a point-plane geometry and managed to augment heat transfer coecients more than 200% by varying the high voltage and the point-to-plane spacing. Some numerical modeling were developed to study the eect of imposing the electric eld in the absence of the external force ow inside two dimensional cavities [46]. Using computational uid dy- namic, the eect of electrohydrodynamic on heat transfer within an external force ow was studied by Kasayapanand [7,8]. An experi- mental research was carried out to investigate the EHD enhanced heat transfer in a vertical annulus by Grassi [9]. They managed to obtain local heat transfer improvement by inserting appropriate points on the inner surface of the annulus which generally acted as the positive electrode, while the surrounding pipe was grounded. Enhanced heat transfer techniques are classied into two main ca- tegories: active and passive methods. However, it is more advantageous to implement a combination of both methods to augment the heat transfer. For this purpose, we used EHD (an active method) in a n attached enclosure (passive technique) in the present study. Several numerical researches are reported by Kasayapanand [1012] which show the eect of the imposing electric eld on the partially open or closed nned enclosures. In this paper, contrary to other similar works which applied computational uid dynamics (CFD), we employed ex- perimental investigation to study heat transfer enhancement [13]. Three dierent nned enclosures including single n and multiple ns (3 and 7 ns) were constructed and used for the experiments. Both the positive and negative coronas were considered in this study. One of the shortcomings of the numerical methods is that they cannot predict the breakdown or spark over voltage correctly. A corona discharge is an electrical discharge brought on by the ionization of a uid surrounding a conductor that is electrically energized. The discharge will occur when the strength (potential gradient) of the electric eld around the https://doi.org/10.1016/j.ijthermalsci.2018.01.003 Received 31 December 2016; Received in revised form 30 December 2017; Accepted 4 January 2018 * Corresponding author. E-mail address: farid.fazlollahi@yahoo.com (F. Fazlollahi). International Journal of Thermal Sciences 127 (2018) 194–200 1290-0729/ © 2018 Published by Elsevier Masson SAS. T