20,000 l/s = 1/10,000

_l_ expressing the thickness of the voltameter expressed in meters,

and _s_ being the section in square millimeters. For example: For l =

1/10, s = 20,000,000, say 20 square meters. It will be seen from this

example what should be the proportions of apparatus designed for a

production on a large scale.

The new principles that permit of the construction of such voltameters

are as follows: (1) the substitution of an alkaline for the acid

solution, thus affording a possibility of employing iron electrodes;

(2) the introduction of a porous partition between the electrodes, for

the purpose of separating the gases.

_Electrolytic Liquid._--Commandant Renard's experiments were made with

15 per cent, solution of caustic soda and water containing 27 per

cent. of acid. These are the proportions that give the maximum of

conductivity. Experiments made with a voltameter having platinum

electrodes separated by an interval of 3 or 4 centimeters showed that

for a determinate E.M.F. the alkaline solution allows of the passage

of a slighter intenser current than the acidulated water, that is to

say, it is less resistant and more advantageous from the standpoint of

the consumption of energy.

_Porous Partition._--Let us suppose that the two parts of the trough

are separated by a partition containing small channels at right angles

with its direction. It is these channels alone that must conduct the

electricity. Their conductivity (inverse of resistance) is

proportional to their total section, and inversely proportional to

their common length, whatever be their individual section. It is,

therefore, advantageous to employ partitions that contain as many

openings as possible.

The separating effect of these partitions for the gas is wholly due to

capillary phenomena. We know, in fact, that water tends to expel gas

from a narrow tube with a pressure inversely proportional to the

tube's radius. In order to traverse the tube, the gaseous mass will

have to exert a counter-pressure greater than this capillary pressure.

As long as the pressure of one part and another of the wet wall

differs to a degree less than the capillary pressure of the largest

channel, the gases disengaged in the two parts of the trough will

remain entirely separate. In order that the mixing may not take place

through the partition above the level of the liquid (dry partition),

the latter will have to be impenetrable in every part that emerges.

The study of the partitions should be directed to their separating

effect on the gases, and to their electric resistance. In order to

study the first of these properties, the porous partition, fixed by a

hermetical joint to a glass tube, is immersed in the water (Fig. 2).

An increasing pressure is exerted from the interior until the passage

of bubbles is observed. The pressure read at this moment on the

manometer indicates (transformed above the electrolytic solution) the

changes of level that the bath may undergo. The different porcelains

and earths behave, from this point of view, in a very unequal manner.

For example, an earthen vessel from the Pillivayt establishment

supports some decimeters of water, while the porcelain of Boulanger,

at Choisy-le-Roi, allows of the passage of the gas only at pressures

greater than one atmosphere, which is much more than is necessary.

Wire gauze, canvas, and asbestos cloth resist a few centimeters of

water. It might be feared, however, that the gases, violently

projected against these partitions, would not pass, owing to the

velocity acquired. Upon this point experiment is very reassuring.

After filling with water a canvas bag fixed to the extremity of a

rubber tube, it is possible to produce in the interior a tumultuous

disengagement of gas without any bubbles passing through.

[Illustration: FIG. 2.--ARRANGEMENT FOR THE STUDY OF CAPILLARY

REACTION IN POROUS VESSELS.]

From an electrical point of view, partitions are of very unequal

quality. Various partitions having been placed between electrodes

spaced three centimeters apart, currents were obtained which indicated

that, with the best of porcelains, the rendering of the apparatus is

diminished by one-half. Asbestos cloth introduces but an insignificant

resistance.

To this inconvenience of porous vessels is added their fragility,

their high price, and the impossibility of obtaining them of the

dimensions that large apparatus would call for. The selection of

asbestos cloth is therefore clearly indicated; but, as it does not

entirely separate the gases, except at a pressure that does not exceed

a few centimeters of water, it was always necessary to bring back the

variation of the level to these narrow limits by a special

arrangement. We cannot, in fact, expect that the entire piping shall

be always in such conditions that no difference in pressure can occur.

The levels are brought back to equality within the effective limits by

interposing between the voltameter and the piping an apparatus called

a compensator, which consists of two vessels that communicate in the

interior part through a large tube. The gases enter each vessel

through a pipe that debouches beneath the level of the water. If a

momentary stoppage occurs in one of the conduits, the water changes

level in the compensator, but the pressure remains constant at the

orifice of the tubes. The compensator is, as may be seen, nothing more

than a double Mariotte flask. When it is desired to obtain pure gases,

there is introduced into the compensator a solution of tartaric acid,

which retains the traces of alkalies carried along by the current of

gas. The alkaline solution, moreover, destroys the ozone at the moment

of its formation.

It will be seen that laboratory studies have furnished all the

elements of a problem which is now capable of entering the domain of

practice. The cheapness of the raw materials permits of constructing

apparatus whose dimensions will no longer be limited except by reasons

of another nature. The electrodes may be placed in proximity at will,

owing to the use of the porous partition. It may be seen, then, that

the apparatus will have a considerable useful effect without its being

necessary to waste the electric energy beyond measure.

_Industrial Apparatus._--We have shown how the very concise researches

of Commandant Renard have fixed the best conditions for the

construction of an industrial voltameter. It remains for us to

describe this voltameter itself, and to show the rendering of it.

[Illustration: FIG. 3.--PLANT FOR THE INDUSTRIAL ELECTROLYSIS OF

WATER.]

The industrial voltameter consists of a large iron cylinder. A battery

of such voltameters is shown to the left of Fig. 3, and one of the

apparatus, isolated, is represented in Fig. 4. The interior electrode

is placed in an asbestos cloth bag, which is closed below and tied at

its upper part. It is provided with apertures which permit of the

ascent of the gases in the interior of the cylinder. The apparatus is

hermetically sealed at the top, the two electrodes being naturally

insulated with rubber. Above the level of the liquid the interior

electrode is continuous and forms a channel for the gas. The hydrogen

and oxygen, escaping through the upper orifices, flow to the

compensator. The apparatus is provided with an emptying cock or a cock

for filling with distilled water, coming from a reservoir situated

above the apparatus.

[Illustration: FIG. 4.--DETAILS OF AN INDUSTRIAL VOLTAMETER.]

The constants of the voltameter established by Commandant Renard are

as follows:

Height of external electrode 3.405 m.

" internal " 3.290 "

Diameter of external " 0.300 "

" internal " 0.174 "

The iron plate employed is 2 millimeters in thickness. The electric

resistance is about 0.0075 ohm. The apparatus gives 365 amperes under

2.7 volts, and consequently nearly 1 kilowatt. Its production in

hydrogen is 158 liters per hour.

It is clear that, in an industrial exploitation, a dynamo working

under 3 volts is never employed. In order to properly utilize the

power of the dynamo, several voltameters will be put in series--a

dozen, for example, if the generating machine is in proximity to the

apparatus, or a larger number if the voltameters are actuated by a

dynamo situated at a distance, say in the vicinity of a waterfall.

Fig. 3 will give an idea of a plant for the electrolysis of water.

It remains for us to say a few words as to the net cost of the

hydrogen and oxygen gases produced by the process that we have just

described. We may estimate the value of a voltameter at a hundred

francs. If the apparatus operates without appreciable wear, the

amortizement should be calculated at a very low figure, say 10 per

cent., which is large. In continuous operation it would produce more

than 1,500 cubic meters of gas a year, say a little less than one

centime per cubic meter. The caustic soda is constantly recuperated

and is never destroyed. The sole product that disappears is the

distilled water. Now one cubic meter of water produces more than 2,000

cubic meters of gas. The expense in water, then, does not amount to a

centime per cubic meter. The great factor of the expense resides in

the electric energy. The cost of surveillance will be minimum and the

general expenses _ad libitum_.

Let us take the case in which the energy has to be borrowed from a

steam engine. Supposing very small losses in the dynamo and piping, we

may count upon a production of one cubic meter of hydrogen and 500

cubic decimeters of oxygen for 10 horse-power taken upon the main

shaft, say an expenditure of 10 kilogrammes of coal or of about 25

centimes--a little more in Paris, and less in coal districts. If,

consequently, we fix the price of the cubic meter of gas at 50

centimes, we shall preserve a sufficient margin. In localities where a

natural motive power is at our disposal, this estimate will have to be

greatly reduced. We may, therefore, expect to see hydrogen and oxygen

take an important place in ordinary usages. From the standpoint alone

of preservation of fuel, that is to say, of potential energy upon the

earth, this new conquest of electricity is very pleasing. Waterfalls

furnish utilizable energy in every locality, and, in the future, will

perhaps console our great-grandchildren for the unsparing waste that

we are making of coal.--_La Nature._

* * * * *

[Continued from SUPPLEMENT, No. 818, page 13066.]

Scientific American Supplement No. 819, September 12, 1891 · 第 5 / 45 题