The bubble coverage of vertical gas-evolving electrodes with forced upward electrolyte flow is studied systematically in laboratory experiments. A substantial decrease with increasing flow velocity past the electrode is found for various electrode materials of anodes and cathodes. A theoretical analysis explains the action of mechanical forces on the break-off diameter of bubbles exposed to flowing electrolytes. A simplified design equation for practical estimates is proposed.Reliable knowledge of the electrode area covered by adhering bubbles is of utmost importance for assessing the operational behavior of gas-evolving electrodes. The value is not only relevant to the ohmic voltage drop of the so-called bubble curtain before the electrode, but also for the extent of mass and heat transfer. The bubble coverage controls the actual current density and thus both the overpotential and the limiting current density. 1 A variation of the bubble coverage with distance from the leading edge contributes to the current distribution over the electrode.It is not astonishing that numerous experimental investigations were conducted to get information on the value of the bubble coverage, particularly its dependence on the current density. Nearly all of these investigations refer to stagnant electrolyte, i.e., liquids without forced flow, mostly in experimental devices where substantial flow past the electrode cannot develop. However, industrial cells are commonly operated with forced upward flow or designed in such a way that substantial free flow induced by gas bubbles develops. Owing to experimental difficulties, data under these conditions are rare. A few data were published by Sillen obtained at a cell with vertical electrodes. 2,3 More detailed data were obtained at horizontal electrodes facing upward. 4 However, industrial gas-evolving electrodes are in a vertical position, wherever possible, to enhance gas release from the interelectrode space. It is the object of the present paper to study the conditions at vertical electrodes of various electrode materials operated as anodes and cathodes with forced flow of varying rates.
Bubble Coverage in Stagnant LiquidsTo distinguish the active electrode surface area from the geometrical one, the ͑fractional͒ bubble coverage was introduced by Ibl and Venczel 5 in 1961. It was defined as the fraction of the electrode area covered on the average by bubbles sitting on it. A stricter definition was given in 1980 defining the covered area as that obtained by perpendicular projection of the bubble contours to the electrode, referred to the electrode mean area pertinent to each adhering bubble. 6 This definition is superior in that it considers that the current density on the shadowed area below adhering bubbles with contact angles smaller than 90°͑which is a common case in aqueous electrolytes͒ is small, 7-9 and may approximately be neglected for the present purpose.The value of the bubble coverage is controlled by the bubble population density on the electrode surface, i.e., the number ...