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Electrolysis : Migration Of The Ions |
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The bodily transfer of the ions under the influence of an electric field can be demonstrated, and its speed measured, by the apparatus shown in
Expt. 4. - The U-tube is half-filled with a solution containing 0.3 gm. of KNO3 in a litre of water. By connecting a funnel with the capillary tap below the U-tube, a solution containing 0.5 gm. of KMnO4 per litre of water, to each 100 c.c. of which 5 gm. of urea have been added to increase its density, is slowly admitted. The surface of separation between the colourless liquid above and the purple permanganate solution below should be quite sharp. A current of 0.3 - 0.4 amp. Is now passed between the platinum electrodes, from the D.C. mains. The purple MnO4'-ions at once begin to move towards the anode, and the levels alter in the directions shown. If the former levels are marked by thin strips of gummed label, the change is quite apparent after 10-15 minutes. This experiment shows that the speed of the ions in bulk through the solution is very slow. It thus resembles the diffusion of dissolved substances. In both cases the moving particles enter repeatedly into collision with the molecules of the solvent. The actual ionic mobilities, under a potential gradient of 1 volt per cm., in cm. per sec. (for very dilute solutions, where the influence of ions on one another, or on the un-ionised salt molecules, may be neglected) are given below: K˙ 0.00067 Ag˙ 0.0057 Cl' 0.00068 NO3' 0.00064 H˙ 0.00326 Na˙ 0.00045 OH' 0.00181 I' 0.00069 NH4˙ 0.00066 SO4'' 0.00071 The ions in their motion are under the influence of two forces: (i) the driving force of the potential gradient; (ii) the viscous resistance of the solvent. The latter frictional resistance is enormous. In order to pull 1 gm. mol of potassium ions through the solution with a speed of 1 cm. per sec. it would be necessary to apply to them an aggregate force of no less than 1,500,000 tons (Kohlrausch). |
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