An index error in the numerical procedure calculating the ion density and the electric field was discovered. While the general concepts, the numerical method, and the main conclusions presented in the paper remain valid, the index error resulted in incorrect figures. The rectified plots and results are presented below.The calculations are run for different values of applied voltage ranging from 3500 V to 5000 V. The solution for the electric field and the free charge density is presented in Figs. 1 and 2, respectively, for an applied voltage of 5000 V.The body force applied on the fluid is the product of the electric field and the ion density. The magnitude of the body force in horizontal and vertical directions is shown in Figs. 3 and 4. The velocity profile at the entrance of the heat exchanger channel is shown in Fig. 5 for different applied voltages. The channel Reynolds number did not exceed 1150, which is well below the critical Reynolds number of 2300, therefore justifying the assumption of laminar flow (Fig. 6).The average heat flux across the wall of the channel at different voltages is presented in Table 1. Utilizing ionic wind heat transfer enhancement, a maximum heat flux of 502.9 W/m2 was found at an applied voltage of 5000 V.Finally, the heat flux obtained with ionic wind heat transfer enhancement is compared to the case with natural convection calculated according to Bar-Cohen and Rohsenow [2] as shown in Eqs. (1) and (2). Thereby, the constants C1 and C2 take value of 576 and 287, respectively. At a voltage of 5000 V, an increase in the heat flux of a factor four as compared to natural convection only was calculated (Fig. 7)(1)Nu¯S=[C1(RaSS/L)2+C2(RaSS/L)1/2]−1/2=h¯Sk(2)q″=h¯(Ts−T∞)A novel passive cooling enhancement method for grid-scale power routers was presented. A numerical scheme based on finite difference approximation was developed to solve the electrodynamics problem. It is shown that the velocity profile at the exit of the ionic wind generator is proportional to the applied corona voltage. Consequently, the heat flux increases with increasing applied voltages. The total heat rejected to the ambient can be increased by a factor four as compared to natural convection only at an applied voltage of 5000 V. Given the described geometry of the power routers, this corresponds to a total cooling power of up to 2860 W. The active power input required by the ionic wind generator is less than 5.6 W. It is therefore demonstrated that corona electrodes combined with bonded fin arrays could potentially replace more costly and complex cooling systems such as thermosiphons and heat pipes. In future work, effort will be directed at the experimental validation of the presented numerical model.
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