“…Because the ionic charge layer emerges as a result of the applied AC electric field, both the induced free charge and tangential field component are sinusoidal functions of the time variable under Debye-Huckel limit, resulting in time-averaged electroosmosis flow even in a harmonically oscillating field [ 23 , 24 , 25 ]. Later, Bazant and Squires [ 26 , 27 ] indicated that a background electric field can act on its own induced free charge within the Debye layer at a polarizable phase interface, which is genuinely a more accurate physical description of nonlinear electrokinetic phenomena, and they coined the term ‘Induced-Charge Electroosmosis (ICEO)’ to delineate electroosmotic streaming on polarizable or highly-charged solid surfaces immersed in saline solutions, which has incorporated the physical concepts of AC electroosmosis/traveling-wave electroosmosis (ACEO/TWEO) on driving electrodes in standing-wave [ 28 , 29 ]/traveling-wave [ 30 , 31 , 32 , 33 , 34 , 35 ] electric fields, ICEO on bipolar conducting [ 15 , 36 , 37 , 38 , 39 , 40 , 41 , 42 ]/semiconducting [ 43 , 44 ]/dielectric [ 16 , 45 , 46 , 47 , 48 ] materials, and electroosmosis of second kind due to surface-conduction-induced bulk concentration polarization [ 49 , 50 , 51 , 52 ]. This new category of electrohydrodynamic flow shows great advantages in suppressing electrode reactions and bubble productions, as well as actuating faster fluid flows than conventional linear electroosmosis, by virtue of its second-order voltage dependence in time-varying electric fields [ 14 , 53 , 54 ,…”