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Behaviour of a tall vertical gas-evolving cell Part II: Distribution of current
Authors:L J J Janssen  G J Visser
Affiliation:(1) Faculty of Chemical Technology, Eindhoven University of Technology, P. O. Box 513, 5600 MB Eindhoven, The Netherlands;(2) Computing Centre, Eindhoven University of Technology, P. O. Box 513, 5600 MB Eindhoven, The Netherlands
Abstract:Vertical electrolysers with a narrow electrode gap are used to produce gases, for example, chlorine, hydrogen and oxygen. The gas voidage in the solution increases with increasing height in the electrolyser and consequently the current density is expected to decrease with increasing height. Current distribution experiments were carried out in an undivided cell with two electrodes each consisting of 20 equal segments or with a segmented electrode and a one-plate electrode. It was found that for a bubbly flow the current density decreases linearly with increasing height in the cell. The current distribution factor increases with increasing average current density, decreasing volumetric flow rate of liquid and decreasing distance between the anode and the cathode. Moreover, it is concluded that the change in the electrode surface area remaining free of bubbles with increasing height has practically no effect on the current distribution factor.Notation A e electrode surface area (m2) - A e,s surface area of an electrode segment (m2) - A e, 1–19 total electrode surface area for the segments from 1 to 19 inclusive (m2) - A e,a anode surface area (m2) - A e,a,h A e,a remaining free of bubbles (m2) - A e,e cathode surface area (m2) - A e,c,h A e,c remaining free of bubbles (m2) - a 1 parameter in Equation 7 (A–1) - B current distribution factor - B r B in reverse position of the cell - B s B in standard position of cell - b a Tafel slope for the anodic reaction (V) - b c Tafel slope for the cathodic reaction (V) - d distance (m) - d ac distance between the anode and the cathode (m) - d wm distance between the working electrode and an imaginary membrane (m) (d wm=0.5d wt=0.5d ac) - d wt distance between the working and the counter electrode (m) - F Faraday constant (C mol–1) - h height from the leading edge of the working electrode corresponding to height in the cell (m) - h e distance from the bottom to the top of the working electrode (m) - I current (A) - I s current for a segment (A) - I 20 current for segment pair 20 (A) - I 1–19 total current for the segment pairs from 1 to 19 inclusive (A) - i current density (A m–2) - i av average current density of working electrode (A m–2) - i b current density at the bottom edge of the working electrode (A m–2) - i 0 exchange current density (A m–2) - i 0,a i 0 for anode reaction (A m–2) - i l current density at the top edge of the working electrode (A m–2) - n 1 parameter in Equation 15 - n s number of a pair of segments of the segmented electrodes from their leading edges - Q g volumetric rate of gas saturated with water vapour (m3 s–1) - Q 1 volumetric rate of liquid (m3 s–1) - R resistance of solution (OHgr) - R 20 resistance of solution between the top segments of the working and the counter electrode (OHgr) - R p resistance of bubble-free solution (OHgr) - R p,20 R p for segment pair 20 (OHgr) - r s reduced specific surface resistivity - r s,0 r s ath=0 - r s,20 r s for segment pair 20 - r s,infin r s for uniform distribution of bubbles between both the segments of a pair - r s,infin,20 r s,infin for segment pair 20 - T temperature (K) - U cell voltage (V) - U r reversible cell voltage (V) - v 1 linear velocity of liquid (m s–1) - v 1,0 v 1 through interelectrode gap at the leading edges of both electrodes (m s–1) - x distance from the electrode surface (m) - beta gas volumetric flow ratio - beta20 beta at segment pair 20 - gamma specific surface resistivity (OHgr m2) - gammat gamma at top of electrode (OHgr m2) - gammap gamma for bubble-free solution (OHgr m2) - gammab gamma at bottom of electrode (OHgr m2) - delta thickness of Nernst bubble layer (m) - delta0 delta ath=0 (m) - delta0,i delta0 ati - epsi voidage - epsix,0 epsi atx andh=0 - epsi0,0 voidage at the leading edge of electrode wherex=0 andh=0 - 
$$\varepsilon _{0,0,i_b } $$
epsi0,0 ati b - 
$$\varepsilon _{0,0,i_t } $$
epsi0,0 ati=i t - epsiinfin,h voidage in bulk of solution at heighth - epsiinfin,20 voidage in bubble of solution at the leading edge of segment pair 20 - epsilim maximum value of epsi0,0 - eegr overpotential (V) - eegra anodic overpotential (V) - eegrc cathodic overpotential (V) - eegrh hyper overpotential (V) - eegrh,a anodic hyper overpotential (V) - eegrh,c cathodic hyper overpotential (V) - theta fraction of electrode surface area covered by of bubbles - thetaa theta for anode - thetac theta for cathode - rgr resistivity of solution (OHgr m) - rgrp resistivity of bubble-free solution (OHgr m)
Keywords:
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