FOOTNOTES:

[1] See J.A. Fleming, _The Alternate Current Transformer_, vol. i. p.

519.

[2] See Maxwell, _Electricity and Magnetism_, vol. ii. chap. ii.

[3] See Maxwell, _Electricity and Magnetism_, vol. ii. 642.

[4] _Experimental Researches_, vol. i. ser. 1.

[5] See Maxwell, _Electricity and Magnetism_, vol. ii. S 542, p. 178.

[6] See W.G. Rhodes, _An Elementary Treatise on Alternating Currents_

(London, 1902), chap. vii.

[7] See J.A. Fleming, "Problems on the Distribution of Electric

Currents in Networks of Conductors," _Phil. Mag_. (1885), or Proc.

Phys. Soc. Lond. (1885), 7; also Maxwell, _Electricity and Magnetism_

(2nd ed.), vol. i. p. 374, S 280, 282b.

[8] See _Berl. Acad. Ber._, 1876, p. 211; also H.A. Rowland and C.T.

Hutchinson, "On the Electromagnetic Effect of Convection Currents,"

_Phil. Mag._, 1889, 27, p. 445.

ELECTROLIER, a fixture, usually pendent from the ceiling, for holding

electric lamps. The word is analogous to chandelier, from which indeed

it was formed.

ELECTROLYSIS (formed from Gr. [Greek: lyein], to loosen). When the

passage of an electric current through a substance is accompanied by

definite chemical changes which are independent of the heating effects

of the current, the process is known as _electrolysis_, and the

substance is called an _electrolyte_. As an example we may take the case

of a solution of a salt such as copper sulphate in water, through which

an electric current is passed between copper plates. We shall then

observe the following phenomena. (1) The bulk of the solution is

unaltered, except that its temperature may be raised owing to the usual

heating effect which is proportional to the square of the strength of

the current. (2) The copper plate by which the current is said to enter

the solution, i.e. the plate attached to the so-called positive terminal

of the battery or other source of current, dissolves away, the copper

going into solution as copper sulphate. (3) Copper is deposited on the

surface of the other plate, being obtained from the solution. (4)

Changes in concentration are produced in the neighbourhood of the two

plates or electrodes. In the case we have chosen, the solution becomes

stronger near the anode, or electrode at which the current enters, and

weaker near the cathode, or electrode at which it leaves the solution.

If, instead of using copper electrodes, we take plates of platinum,

copper is still deposited on the cathode; but, instead of the anode

dissolving, free sulphuric acid appears in the neighbouring solution,

and oxygen gas is evolved at the surface of the platinum plate.

With other electrolytes similar phenomena appear, though the primary

chemical changes may be masked by secondary actions. Thus, with a dilute

solution of sulphuric acid and platinum electrodes, hydrogen gas is

evolved at the cathode, while, as the result of a secondary action on

the anode, sulphuric acid is there re-formed, and oxygen gas evolved.

Again, with the solution of a salt such as sodium chloride, the sodium,

which is primarily liberated at the cathode, decomposes the water and

evolves hydrogen, while the chlorine may be evolved as such, may

dissolve the anode, or may liberate oxygen from the water, according to

the nature of the plate and the concentration of the solution.

_Early History of Electrolysis._--Alessandro Volta of Pavia discovered

the electric battery in the year 1800, and thus placed the means of

maintaining a steady electric current in the hands of investigators,

who, before that date, had been restricted to the study of the isolated

electric charges given by frictional electric machines. Volta's cell

consists essentially of two plates of different metals, such as zinc and

copper, connected by an electrolyte such as a solution of salt or acid.

Immediately on its discovery intense interest was aroused in the new

invention, and the chemical effects of electric currents were speedily

detected. W. Nicholson and Sir A. Carlisle found that hydrogen and

oxygen were evolved at the surfaces of gold and platinum wires connected

with the terminals of a battery and dipped in water. The volume of the

hydrogen was about double that of the oxygen, and, since this is the

ratio in which these elements are combined in water, it was concluded

that the process consisted essentially in the decomposition of water.

They also noticed that a similar kind of chemical action went on in the

battery itself. Soon afterwards, William Cruickshank decomposed the

magnesium, sodium and ammonium chlorides, and precipitated silver and

copper from their solutions--an observation which led to the process of

electroplating. He also found that the liquid round the anode became

acid, and that round the cathode alkaline. In 1804 W. Hisinger and J.J.

Berzelius stated that neutral salt solutions could be decomposed by

electricity, the acid appearing at one pole and the metal at the other.

This observation showed that nascent hydrogen was not, as had been

supposed, the primary cause of the separation of metals from their

solutions, but that the action consisted in a direct decomposition into

metal and acid. During the earliest investigation of the subject it was

thought that, since hydrogen and oxygen were usually evolved, the

electrolysis of solutions of acids and alkalis was to be regarded as a

direct decomposition of water. In 1806 Sir Humphry Davy proved that the

formation of acid and alkali when water was electrolysed was due to

saline impurities in the water. He had shown previously that

decomposition of water could be effected although the two poles were

placed in separate vessels connected by moistened threads. In 1807 he

decomposed potash and soda, previously considered to be elements, by

passing the current from a powerful battery through the moistened

solids, and thus isolated the metals potassium and sodium.

The electromotive force of Volta's simple cell falls off rapidly when

the cell is used, and this phenomenon was shown to be due to the

accumulation at the metal plates of the products of chemical changes in

the cell itself. This reverse electromotive force of polarization is

produced in all electrolytes when the passage of the current changes the

nature of the electrodes. In batteries which use acids as the

electrolyte, a film of hydrogen tends to be deposited on the copper or

platinum electrode; but, to obtain a constant electromotive force,

several means were soon devised of preventing the formation of the film.

Constant cells may be divided into two groups, according as their action

is chemical (as in the bichromate cell, where the hydrogen is converted

into water by an oxidizing agent placed in a porous pot round the carbon

plate) or electrochemical (as in Daniell's cell, where a copper plate is

surrounded by a solution of copper sulphate, and the hydrogen, instead

of being liberated, replaces copper, which is deposited on the plate

from the solution).

[Illustration: FIG. 1.]

_Faraday's Laws._--The first exact quantitative study of electrolytic

phenomena was made about 1830 by Michael Faraday (_Experimental

Researches_, 1833). When an electric current flows round a circuit,

there is no accumulation of electricity anywhere in the circuit, hence

the current strength is everywhere the same, and we may picture the

current as analogous to the flow of an incompressible fluid. Acting on

this view, Faraday set himself to examine the relation between the flow

of electricity round the circuit and the amount of chemical

decomposition. He passed the current driven by a voltaic battery ZnPt

(fig. 1) through two branches containing the two electrolytic cells A

and B. The reunited current was then led through another cell C, in

which the strength of the current must be the sum of those in the arms A

and B. Faraday found that the mass of substance liberated at the

electrodes in the cell C was equal to the sum of the masses liberated in

the cells A and B. He also found that, for the same current, the amount

of chemical action was independent of the size of the electrodes and

proportional to the time that the current flowed. Regarding the current

as the passage of a certain amount of electricity per second, it will be

seen that the results of all these experiments may be summed up in the

statement that the amount of chemical action is proportional to the

quantity of electricity which passes through the cell.

Faraday's next step was to pass the same current through different

electrolytes in series. He found that the amounts of the substances

liberated in each cell were proportional to the chemical equivalent

weights of those substances. Thus, if the current be passed through

dilute sulphuric acid between hydrogen electrodes, and through a

solution of copper sulphate, it will be found that the mass of hydrogen

evolved in the first cell is to the mass of copper deposited in the

second as 1 is to 31.8. Now this ratio is the same as that which gives

the relative chemical equivalents of hydrogen and copper, for 1 gramme

of hydrogen and 31.8 grammes of copper unite chemically with the same

weight of any acid radicle such as chlorine or the sulphuric group, SO4.

Faraday examined also the electrolysis of certain fused salts such as

lead chloride and silver chloride. Similar relations were found to hold

and the amounts of chemical change to be the same for the same electric

transfer as in the case of solutions.

We may sum up the chief results of Faraday's work in the statements

known as Faraday's laws: The mass of substance liberated from an

electrolyte by the passage of a current is proportional (1) to the total

quantity of electricity which passes through the electrolyte, and (2) to

the chemical equivalent weight of the substance liberated.

Since Faraday's time his laws have been confirmed by modern research,

and in favourable cases have been shown to hold good with an accuracy of

at least one part in a thousand. The principal object of this more

recent research has been the determination of the quantitative amount of

chemical change associated with the passage for a given time of a

current of strength known in electromagnetic units. It is found that the

most accurate and convenient apparatus to use is a platinum bowl filled

with a solution of silver nitrate containing about fifteen parts of the

salt to one hundred of water. Into the solution dips a silver plate

wrapped in filter paper, and the current is passed from the silver plate

as anode to the bowl as cathode. The bowl is weighed before and after

the passage of the current, and the increase gives the mass of silver

deposited. The mean result of the best determinations shows that when a

current of one ampere is passed for one second, a mass of silver is

deposited equal to 0.001118 gramme. So accurate and convenient is this

determination that it is now used conversely as a practical definition

of the ampere, which (defined theoretically in terms of magnetic force)

is defined practically as the current which in one second deposits 1.118

milligramme of silver.

Taking the chemical equivalent weight of silver, as determined by

chemical experiments, to be 107.92, the result described gives as the

electrochemical equivalent of an ion of unit chemical equivalent the

value 1.036 X 10^(-5). If, as is now usual, we take the equivalent

weight of oxygen as our standard and call it 16, the equivalent weight

of hydrogen is 1.008, and its electrochemical equivalent is 1.044 X

10^(-5). The electrochemical equivalent of any other substance, whether

element or compound, may be found by multiplying its chemical equivalent

by 1.036 X 10^(-5). If, instead of the ampere, we take the C.G.S.

electromagnetic unit of current, this number becomes 1.036 X 10^(-4).

_Chemical Nature of the Ions._--A study of the products of decomposition

does not necessarily lead directly to a knowledge of the ions actually

employed in carrying the current through the electrolyte. Since the

electric forces are active throughout the whole solution, all the ions

must come under its influence and therefore move, but their separation

from the electrodes is determined by the electromotive force needed to

liberate them. Thus, as long as every ion of the solution is present in

the layer of liquid next the electrode, the one which responds to the

least electromotive force will alone be set free. When the amount of

this ion in the surface layer becomes too small to carry all the current

across the junction, other ions must also be used, and either they or

their secondary products will appear also at the electrode. In aqueous

solutions, for instance, a few hydrogen (H) and hydroxyl (OH) ions

derived from the water are always present, and will be liberated if the

other ions require a higher decomposition voltage and the current be

kept so small that hydrogen and hydroxyl ions can be formed fast enough

to carry all the current across the junction between solution and

electrode.

The issue is also obscured in another way. When the ions are set free at

the electrodes, they may unite with the substance of the electrode or

with some constituent of the solution to form secondary products. Thus

the hydroxyl mentioned above decomposes into water and oxygen, and the

chlorine produced by the electrolysis of a chloride may attack the metal

of the anode. This leads us to examine more closely the part played by

water in the electrolysis of aqueous solutions. Distilled water is a

very bad conductor, though, even when great care is taken to remove all

dissolved bodies, there is evidence to show that some part of the trace

of conductivity remaining is due to the water itself. By careful

redistillation F. Kohlrausch has prepared water of which the

conductivity compared with that of mercury was only 0.40 X 10^(-11) at

18 deg. C. Even here some little impurity was present, and the

conductivity of chemically pure water was estimated by thermodynamic

reasoning as 0.36 X 10^(-11) at 18 deg. C. As we shall see later, the

conductivity of very dilute salt solutions is proportional to the

concentration, so that it is probable that, in most cases, practically

all the current is carried by the salt. At the electrodes, however, the

small quantity of hydrogen and hydroxyl ions from the water are

liberated first in cases where the ions of the salt have a higher

decomposition voltage. The water being present in excess, the hydrogen

and hydroxyl are re-formed at once and therefore are set free

continuously. If the current be so strong that new hydrogen and hydroxyl

ions cannot be formed in time, other substances are liberated; in a

solution of sulphuric acid a strong current will evolve sulphur dioxide,

the more readily as the concentration of the solution is increased.

Similar phenomena are seen in the case of a solution of hydrochloric

acid. When the solution is weak, hydrogen and oxygen are evolved; but,

as the concentration is increased, and the current raised, more and more

chlorine is liberated.

An interesting example of secondary action is shown by the common

technical process of electroplating with silver from a bath of

potassium silver cyanide. Here the ions are potassium and the group

Ag(CN)2.[1] Each potassium ion as it reaches the cathode precipitates

silver by reacting with the solution in accordance with the chemical

equation

K + KAg(CN)2 = 2KCN + Ag,

while the anion Ag(CN)2 dissolves an atom of silver from the anode,

and re-forms the complex cyanide KAg(CN)2 by combining with the 2KCN

produced in the reaction described in the equation. If the anode

consist of platinum, cyanogen gas is evolved thereat from the anion

Ag(CN)2, and the platinum becomes covered with the insoluble silver

cyanide, AgCN, which soon stops the current. The coating of silver

obtained by this process is coherent and homogeneous, while that

deposited from a solution of silver nitrate, as the result of the

primary action of the current, is crystalline and easily detached.

In the electrolysis of a concentrated solution of sodium acetate,

hydrogen is evolved at the cathode and a mixture of ethane and carbon

dioxide at the anode. According to H. Jahn,[2] the processes at the

anode can be represented by the equations

Encyclopaedia Britannica, 11th Edition, "Ehud" to "Electroscope" Volume 9, Slice 2 · 第 31 / 43 题