Electrolytic Assay

lyte is situated. The following short study is an account of such a magnet and of some results obtained with it. The magnet was of the four-clawpot ty...
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AUGUST 15, 1939

ANALYTICAL EDITlON

denser moved onto the vacant position, the temperature raised a little, and a new fraction collected. This process is repeated a number of times until a series of bands has been formed. The effect is particularly striking when colored substances are distilled. Apart from its value for distilling small quantities of material, the apparatus is excellent for testing the purity of a compound, since the first and last bands should have identical melting points. It is also good for observing the approximate sublimation temperatures when it is

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desired to obtain data preliminary to handling a large batch. Passage of the sublimate through the long tube has little effect on raising the temperature of sublimation if the heating is not too rapid.

Literature Cited (1) Burch, .Vatwe, 122, 729 (1928).

(2) M

~ “Laboratory ~ ~ Technique ~ in~ Organic , Chemistry,” p. 120, New York, McGraw-Hill Book Co., 1938.

Electrolytic Assay J

4

G . L. JONES, Sir John Cass Technical Institute, Aldgate, E. C. 3, England

I

T IS customary to carry out the electrolytic assay of copper, nickel, and other solutions with the aid of rotating cathodes or anodes, but where their use is inconvenient the electrolyte may be made to rotate instead. This is usually done b y placing an electromagnet beneath the electrolyte, thus producing a vertical field, which, in the presence of a current moving radially gives rise t o a stirring motion. Several workers have adopted this method of agitating the solution (1-4). When the employment of a n electromagnet is impracticable, the same result may be obtained b y means of a permanent magnet, within the air gap of which the electrolyte is situated. The following short study is a n account of such a magnet and of some results obtained with it. The magnet was of the four-claw pot type used in loud speakers, but the center pole was truncated and the annular pole enlarged, as depicted in Figure 1. The field produced was substantially vertical at the center pole, becoming almost radial towards the outer one. A pot magnet of the size shown is capable of accommodating beakers of 400-ml. capacity. The magnet was of 15 per cent cobalt steel, having the following approximate percentage analysis: carbon, 1; cobalt, 15; chromium 9 to 10; molybdenum, 1. The steel was cruciblemelted and sand-cast. The casting was sand-blasted, machined, and heat-treated by annealing and hardening. The magnet used for the experiments was devoid of pole pieces; these, when fitted, gave a gap 38 mm. in inside diameter, 41 mm. in outside diameter, and 0.6 cm. (0.25 inch) dee and an associated flux density of 8500 to 9000 lines, the total f k x being 64,000 to 68,000 lines. Solutions of electrolytic copper were electrolyzed under various conditions of acidity and current density, and for three different times. The volume in each case was 100 ml. The cathode consisted of a circular cylinder of platinum gauze, 2.4 cm. in diameter by 3 cm. high, attached to a central stem by means of cruciform

cross pieces. The anode was arranged to surround the cathode, and was composed of four angle strips attached to a side stem by hoops top and bottom. The cylinder so formed was 4.5 cm. in diameter by 3 cm. high. Since the stirring effect would clearly be weak at low current densities, experiments under these conditions were not carried out. In the case of mixed acid solutions 1 gram of urea was added to the electrolyte towards the end of the assay. Good, firm deposits were obtained, particularly in the instance of mixed acid solutions. TABLE

Time Hours 0.5 1.0

1.5 0.5 1.0 1.5 0.6 1.0 1.5

0.5

1.0

1.5 0.5

1.0 1.5 0.5 1.0

1.5 0.5 1.0 1.5

I. DEPOSITIONO F

Acidity HsSOd “ 0 3

% 6 5

%

COPPER

Copper

Copper Deposited

Current

Present

Amp.

Gram

Gram

0,4995 0.4995 0.4995 0.4995 0.4995 0,4995 0,4995 0.4995 0.4995 0.4995 0.4995 0.4995 0.4995 0.4996 0.4995 0,9990 0.9990 0.9990 0,9990 0,9990 0,9990

0.4783 0.4993 0.499s 0 4757 0.4993 0,4994 0,4698 0.4982 0.4995 0.4914 0.4993 0.4995 0.4814 0.4979 0.4996 0.9879 0.9954 0.9986 0.9940 0.9979 0 9983

I .

7.5 7.; i. 3

5 3

3

7.5 7.5 7.5 J

5 5 7.5 7.6 7.5 10 10 10

The results (Table I) indicate that, although most of t h e copper is deposited within half an hour, complete removal of the copper from solution does not take place until electrolysis has proceeded for a further hour. At the end of every experiment the electrolyte was tested for copper b y means of potassium ferrocyanide; those solutions which had been electrolyzed for the full period (90 minutes) gave a negative reaction. Assays carried out in nitric acid solution yielded poor deposits, and deposition of the metal was incomplete. The stirring effect of the magnet is appreciable at moderate current densities, and becomes vigorous at high densities. A more powerful magnet than that used in the present study would, of course, enhance the action. Since the magnet is working a t a large air gap, it is possible t h a t loss of magnetism may occur in the course of time, although this is unlikely to be serious. Literature Cited

FIGURE 1. PLASAND SECTIOKAL ELEVATION OF MAGNET

(1) Ashcroft, Electrochem. Met. Rev., 4, 145 (1906). (2) Frary, J . Am. Chem. Soc., 29, 1692 (1907). (3) Hurmuzescu, Elec. Reu., 42, 322 (1898). (4) Knot and Work, J. IND. ENG.CHEM.,4,534 (1912).