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A bubble curtain model applied in chlorate electrolysis

A bubble curtain model applied in chlorate electrolysis

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voltages are given for the <strong>model</strong> with <strong>bubble</strong> <strong>curta<strong>in</strong></strong> compared to the <strong>model</strong> without. For lower current<br />

densities, the differences <strong>in</strong> cell voltages are gett<strong>in</strong>g smaller.<br />

The implementation of a <strong>bubble</strong> <strong>curta<strong>in</strong></strong> or high liquid velocity will almost have no effect on the cell voltage<br />

for low current densities. The biggest change <strong>in</strong> cell voltage occurs when <strong>bubble</strong> coverage on the cathode<br />

is taken <strong>in</strong>to account. Of course this depends on the value of the coverage on the cathode which was<br />

taken as 0,5 here. Keep<strong>in</strong>g the cathode surface free from <strong>bubble</strong>s has a higher impact on the total cell<br />

voltage than <strong>in</strong>creas<strong>in</strong>g the liquid velocity to reduce the voidage.<br />

In reality, the voidage, <strong>bubble</strong> <strong>curta<strong>in</strong></strong> and <strong>bubble</strong> coverage are all effect<strong>in</strong>g the cell voltage together. The<br />

developed Equations serve to figure out their mutual importance. Different values can be used for the<br />

parameters <strong>in</strong> the Equations to see their <strong>in</strong>fluence. Learn<strong>in</strong>g more about how the cell voltage is <strong>in</strong>fluenced<br />

by different parameters will help to f<strong>in</strong>d a way to reduce the cell voltage or at least po<strong>in</strong>t out where the<br />

biggest changes can be made.<br />

4.10 Dissolv<strong>in</strong>g time of a small <strong>bubble</strong><br />

Close the cathode only small <strong>bubble</strong> appears as seen <strong>in</strong> Bollens work.[1] Further away from the cathode<br />

the <strong>bubble</strong>s are larger (see Figure 10). S<strong>in</strong>ce coalescence does not occur, there must be another<br />

explanation on how those larger <strong>bubble</strong>s of the size of 0,1 mm can exist and where they come from.<br />

Once a <strong>bubble</strong> is formed, it gets bigger by diffusion and absorption of hydrogen from the liquid <strong>in</strong>to the<br />

<strong>bubble</strong> [13]. The larger a <strong>bubble</strong> becomes, the slower it can grow because the area/volume ratio is gett<strong>in</strong>g<br />

smaller with a larger volume. The larger a <strong>bubble</strong>, the lower its <strong>in</strong>side pressure (see Eq.(4.10)). A large<br />

<strong>bubble</strong> will absorb the hydrogen from a smaller <strong>bubble</strong> through the electrolyte because of the difference<br />

of Laplace pressure of two <strong>bubble</strong>s of different size. The pressure gradient can be seen as the driv<strong>in</strong>g<br />

force of the mechanism where a larger <strong>bubble</strong> will absorb the hydrogen from a smaller <strong>bubble</strong>. This<br />

expla<strong>in</strong>s why larger <strong>bubble</strong>s only appear further away from the cathode s<strong>in</strong>ce then they already had time<br />

to grow. The speed at which the diameter of a dissolv<strong>in</strong>g <strong>bubble</strong> decreases is calculated. Together with<br />

the diameter of the <strong>bubble</strong>, this speed will result <strong>in</strong> a certa<strong>in</strong> time it takes for a big <strong>bubble</strong> to fully dissolve<br />

a smaller <strong>bubble</strong>. Of course this way of reason<strong>in</strong>g is only acceptable if there is a large <strong>bubble</strong> near the<br />

cathode and close enough to the small <strong>bubble</strong>.<br />

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