I have now to revert to a point of apparently small moment, but which

really constitutes an important step in the development of this

subject. I refer to the form given in 1857 to the rotating armature

by Dr. Werner Siemens, of Berlin. Instead of employing coils wound

transversely round cores of iron, as in the machine of Saxton,

Siemens, after giving a bar of iron the proper shape, wound his wire

longitudinally round it, and obtained thereby greatly augmented

effects between suitably placed magnetic poles. Such an armature is

employed in the small magneto-electric machine which I now introduce

to your notice, and for which the institution is indebted to Mr. Henry

Wilde, of Manchester. There are here sixteen permanent horse-shoe

magnets placed parallel to each other, and between their poles a

Siemens armature. The two ends of the wire which surrounds the

armature are now disconnected. In turning the handle and causing the

armature to rotate, I simply overcome ordinary mechanical friction.

But the two ends of the armature coil can be united in a moment, and

when this is done I immediately experience a greatly increased

resistance to rotation. Something over and above the ordinary

friction of the machine is now to be overcome, and by the expenditure

of an additional amount of muscular force I am able to overcome it.

The excess of labour thus thrown upon my arm has its exact equivalent

in the electric currents generated, and the heat produced by their

subsidence in the coil of the armature. A portion of this heat may be

rendered visible by connecting the two ends of the coil with a thin

platinum wire. When the handle of the machine is rapidly turned the

wire glows, first with a red heat, then with a white heat, and finally

with the heat of fusion. The moment the wire melts, the circuit round

the armature is broken, an instant relief from the labour thrown upon

the arm being the consequence. Clearly realise the equivalent of the

heat here developed. During the period of turning the machine a

certain amount of combustible substance was oxidised or burnt in the

muscles of my arm. Had it done no external work, the matter consumed

would have produced a definite amount of heat. Now, the muscular heat

actually developed during the rotation of the machine fell short of

this definite amount, the missing heat being reproduced to the last

fraction in the glowing platinum wire and the other parts of the

machine. Here, then, the electric current intervenes between my

muscles and the generated heat, exactly as it did a moment ago between

the voltaic battery and its generated heat. The electric current is

to all intents and purposes a vehicle which transports the heat both

of muscle and battery to any distance from the hearth where the fuel

is consumed. Not only is the current a messenger, but it is also an

intensifier of magical power. The temperature of my arm is, in round

numbers, 100° Fahr, and it is by the intensification of this heat that

one of the most refractory of metals, which requires a heat of 3,600°

Fahr. to fuse it, has been reduced to the molten condition.

Zinc, as I have said, is a fuel far too expensive to permit of the

electric light produced by its combustion being used for the common

purposes of life, and you will readily perceive that the human

muscles, or even the muscles of a horse, would be more expensive

still. Here, however, we can employ the force of burning coal to turn

our machine, and it is this employment of our cheapest fuel, rendered

possible by Faraday's discovery, which opens out to us the prospect of

being able to apply the electric light to public use.

In 1866 a great step in the intensification of induced currents, and

the consequent augmentation of the magneto-electric light, was taken

by Mr. Henry Wilde. It fell to my lot to report upon them to the

Royal Society, but before doing so I took the trouble of going to

Manchester to witness Mr. Wilde's experiments. He operated in this

way: starting from a small machine like that worked in your presence a

moment ago, he employed its current to excite an electro-magnet of a

peculiar shape, between whose poles rotated a Siemens armature;

[Footnote: Page and Moigno had previously shown that the

magneto-electric current could produce powerful electro-magnets.] from

this armature currents were obtained vastly stronger than those

generated by the small magneto-electric machine. These currents might

have been immediately employed to produce the electric light; but

instead of this they were conducted round a second electro-magnet of

vast size, between whose poles rotated a Siemens armature of

corresponding dimensions. Three armatures therefore were involved in

this series of operations: first, the armature of the small

magneto-electric machine; secondly, the armature of the first

electro-magnet, which was of considerable size; and, thirdly, the

armature of the second electro-magnet, which was of vast dimensions.

With the currents drawn from this third armature, Mr. Wilde obtained

effects, both as regards heat and light, enormously transcending those

previously known. [Footnote: Mr. Wilde's paper is published in the

'Philosophical Transactions 'for 1867, p. 89. My opinion regarding

Wilde's machine was briefly expressed in a report to the Elder

Brethren of the Trinity House on May 17, 1866: 'It gives me pleasure

to state that the machine is exceedingly effective, and that it far

transcends in power all other apparatus of the kind.']

But the discovery which, above all others, brought the practical

question to the front is now to be considered. On the 4th of

February, 1867, a paper was received by the Royal Society from Dr.

William Siemens bearing the title, 'On the Conversion of Dynamic into

Electrical Force without the use of Permanent Magnetism.' [Footnote: A

paper on the same subject, by Dr. Werner Siemens, was read on January

17, 1867, before the Academy of Sciences in Berlin. In a letter to

'Engineering,' No. 622, p. 45, Mr. Robert Sabine states that

Professor Wheatstone's machines were constructed by Mr. Stroh in the

months of July and August, 1866. I do not doubt Mr. Sabine's

statement; still it would be dangerous in the highest degree to depart

from the canon, in asserting which Faraday was specially strenuous,

that the date of a discovery is the date of its publication. Towards

the end of December, 1866, Mr. Alfred Varley' also lodged a

provisional specification (which, I believe, is a sealed document)

embodying the principles of the dynamo-electric machine, but some

years elapsed before he made anything public. His brother, Mr.

Cromwell varlet', when writing on this subject in 1867, does not

mention him (Proc. Roy. Soc, March 14, 1867). It probably marks a

national trait, that sealed communications, though allowed in France,

have never been recognised by the scientific societies of England.] On

the 14th of February a paper from Sir Charles Wheatstone was received,

bearing the title, 'On the Augmentation of the Power of a Magnet by

the reaction thereon of Currents induced by the Magnet itself.' Both

papers, which dealt with the same discovery, and which were

illustrated by experiments, were read upon the same night, viz. the

14th of February. It would be difficult to find in the whole field of

science a more beautiful example of the interaction of natural forces

than that set forth in these two papers. You can hardly find a bit of

iron--you can hardly pick up an old horse-shoe, for example--that does

not possess a trace of permanent magnetism; and from such a small

beginning Siemens and Wheatstone have taught us to rise by a series of

interactions between magnet and armature to a magnetic intensity

previously unapproached. Conceive the Siemens armature placed between

the poles of a suitable electro-magnet. Suppose this latter to possess

at starting the faintest, trace of magnetism; when the armature

rotates, currents of infinitesimal strength are generated in its coil.

Let the ends of that coil be connected with the wire surrounding the

electro-magnet. The infinitesimal current generated in the armature

will then circulate round the magnet, augmenting its intensity by an

infinitesimal amount. The strengthened magnet instantly reacts upon

the coil which feeds it, producing a current of greater strength.

This current again passes round the magnet, which immediately brings

its enhanced power to bear upon the coil. By this play of mutual give

and take between magnet and armature, the strength of the former is

raised in a very brief interval from almost nothing to complete

magnetic saturation. Such a magnet and armature are able to produce

currents of extraordinary power, and if an electric lamp be introduced

into the common circuit of magnet and armature, we can readily obtain

a most powerful light. [Footnote: In 1867 Mr. Ladd introduced the

modification of dividing the armature into two separate coils, one of

which fed the electro-magnets, while the other yielded the induced

currents.] By this discovery, then, we are enabled to avoid the

trouble and expense involved in the employment of permanent magnets;

we are also enabled to drop the exciting magneto-electric machine, and

the duplication of the electro-magnets. By it, in short, the electric

generator is so far simplified, and reduced in cost, as to enable

electricity to enter the lists as the rival of our present means of

illumination.

Soon after the announcement of their discovery by Siemens and

Wheatstone, Mr. Holmes, at the instance of the Elder Brethren of the

Trinity House, endeavoured to turn this discovery to account for

lighthouse purposes. Already, in the spring of 1869, he had

constructed a machine which, though hampered with defects, exhibited

extraordinary power. The light was developed in the focus of a

dioptric apparatus placed on the Trinity Wharf at Blackwall, and

witnessed by the Elder Brethren, Mr. Douglass, and myself, from an

observatory at Charlton, on the opposite side of the Thames. Falling

upon the suspended haze, the light illuminated the atmosphere for

miles all round. Anything so sunlike in splendour had not, I imagine,

been previously witnessed. The apparatus of Holmes, however, was

rapidly distanced by the safer and more powerful machines of Siemens

and Gramme.

As regards lighthouse illumination, the next step forward was taken by

the Elder Brethren of the Trinity House in 1876-77. Having previously

decided on the establishment of the electric light at the Lizard in

Cornwall, they instituted, at the time referred to, an elaborate

series of comparative experiments wherein the machines of Holmes, of

the Alliance Company, of Siemens, and of Gramme, were pitted against

each other. The Siemens and the Gramme machines delivered direct

currents, while those of Holmes and the Alliance Company delivered

alternating currents. The light of the latter was of the same

intensity in all azimuths; that of the former was different in

different azimuths, the discharge being so regulated as to yield a

gush of light of special intensity in one direction. The following

table gives in standard candles the performance of the respective

machines:

Name of Machines. Maximum. Minimum.

Holmes 1,523 1,523

Alliance 1,953 1,953

Gramme (No. 1). 6,663 4,016

Gramme (No. 2). 6,663 4,016

Siemens (Large) 14,818 8,932

Siemens (Small, No. 1) 5,539 3,339

Siemens (Small, No. 2) 6,864 4,138

Two Holmes's coupled 2,811 2,811

Two Gramme's (Nos. 1 and 2) 11,396 6,869

Two Siemens' (Nos. 1 and 2) 14,134 8,520

[Footnote: Observations from the sea on the night of November 21,

1876, made the Gramme and small Siemens practically equal to the

Alliance. But the photometric observations, in which the external

resistance was abolished, and previous to which the light-keepers had

become more skilled in the management of the direct current, showed

the differences recorded in the table. A close inspection of these

powerful lights at the South Foreland caused my face to peel, as if it

had been irritated by an Alpine sun.]

These determinations were made with extreme care and accuracy by Mr.

Douglass, the engineer-in-chief, and Mr. Ayres, the assistant engineer

of the Trinity House. It is practically impossible to compare

photo-metrically and directly the flame of the candle with these

sun-like lights. A light of intermediate intensity--that of the

six-wick Trinity oil lamp--was therefore in the first instance

compared with the electric light. The candle power of the oil lamp

being afterwards determined, the intensity of the electric light

became known. The numbers given in the table prove the superiority of

the Alliance machine over that of Holmes. They prove the great

superiority both of the Gramme machine and of the small Siemens

machine over the Alliance. The large Siemens machine is shown to

yield a light far exceeding all the others, while the coupling of two

Grammes, or of two Siemens together, here effected for the first time,

was followed by a very great augmentation of the light, rising in the

one case from 6663 candles to 11,396, and in the other case from 6864

candles to 14,134. Where the arc is single and the external

resistance small, great advantages attach to the Siemens light. After

this contest, which was conducted throughout in the most amicable

manner, Siemens machines of type No. 2 were chosen for the Lizard.

[Footnote: As the result of a recent trial by Mr. Schwendler, they

have been also chosen for India.]

*****

We have machines capable of sustaining a single light, and also

machines capable of sustaining several lights. The Gramme machine,

for example, which ignites the Jablochkoff candles on the Thames

Embankment and at the Holborn Viaduct, delivers four currents, each

passing through its own circuit. In each circuit are five lamps

through which the current belonging to the circuit passes in

succession. The lights correspond to so many resisting spaces, over

which, as already explained, the current has to leap; the force which

accomplishes the leap being that which produces the light. Whether

the current is to be competent to pass through five lamps in

succession, or to sustain only a single lamp, depends entirely upon

the will and skill of the maker of the machine. He has, to guide him,

definite laws laid down by Ohm half a century ago, by which he must

abide.

Ohm has taught us how to arrange the elements of a Voltaic battery so

as to augment indefinitely its electromotive force--that force,

namely, which urges the current forward and enables it to surmount

external obstacles. We have only to link the cells together so that

the current generated by each cell shall pass through all the others,

and add its electro-motive force to that of all the others. We

increase, it is true, at the same time the resistance of the battery,

diminishing thereby the quantity of the current from each cell, but we

augment the power of the integrated current to overcome external

hindrances. The resistance of the battery itself may, indeed, be

rendered so great, that the external resistance shall vanish in

comparison. What is here said regarding the voltaic battery is

equally true of magneto-electric machines. If we wish our current to

leap over five intervals, and produce five lights in succession, we

must invoke a sufficient electromotive force. This is done through

multiplying, by the use of thin wires, the convolutions of the

rotating armature as, a moment ago, we augmented the cells of our

voltaic battery. Each additional convolution, like each additional

cell, adds its electro-motive force to that of all the others; and

though it also adds its resistance, thereby diminishing the quantity

of current contributed by each convolution, the integrated current

becomes endowed with the power of leaping across the successive spaces

necessary for the production of a series of lights in its course. The

current is, as it were, rendered at once thinner and more piercing by

the simultaneous addition of internal resistance and electro-motive

power. The machines, on the other hand, which produce only a single

light have a small internal resistance associated with a small

electro-motive force. In such machines the wire of the rotating

armature is comparatively short and thick, copper riband instead of

wire being commonly employed. Such machines deliver a large quantity

of electricity of low tension--in other words, of low leaping power.

Hence, though competent when their power is converged upon a single

interval, to produce one splendid light, their currents are unable to

force a passage when the number of intervals is increased. Thus, by

augmenting the convolutions of our machines we sacrifice quantity and

gain electro-motive force; while by lessening the number of the

convolutions, we sacrifice electro-motive force and gain quantity.

Whether we ought to choose the one form of machine or the other

depends entirely upon the external work the machine has to perform. If

the object be to obtain a single light of great splendour, machines of

low resistance and large quantity must be employed. If we want to

obtain in the same circuit several lights of moderate intensity,

machines of high internal resistance and of correspondingly high

electro-motive power must be invoked.

When a coil of covered wire surrounds a bar of iron, the two ends of

the coil being connected together, every alteration of the magnetism

of the bar is accompanied by the development of an induced current in

the coil. The current is only excited during the period of magnetic

change. No matter how strong or how weak the magnetism of the bar may

be, as long as its condition remains permanent no current is

developed. Conceive, then, the pole of a magnet placed near one end

of the bar to be moved along it towards the other end. During the

time of the pole's motion there will be an incessant change in the

magnetism of the bar, and accompanying this change we shall have an

induced current in the surrounding coil. If, instead of moving the

magnet, we move the bar and its surrounding coil past the magnetic

pole, a similar alteration of the magnetism of the bar will occur, and

a similar current will be induced in the coil. You have here the

fundamental conception which led M. Gramme to the construction of his

beautiful machine. [Footnote: 'Comptes Rendus,' 1871, p. 176. See

also Gaugain on the Gramme machine, 'Ann. de Chem. et de Phys,'

vol. xxviii. p. 324] He aimed at giving continuous motion to such

a bar as we have here described; and for this purpose he bent it into

a continuous ring, which, by a suitable mechanism, he caused to rotate

rapidly close to the poles of a horse-shoe magnet. The direction of

the current varied with the motion and with the character of the

influencing pole. The result was that the currents in the two

semicircles of the coil surrounding the ring flowed in opposite

directions. But it was easy, by the mechanical arrangement called a

commutator, to gather up the currents and cause them to flow in the

same direction. The first machines of Gramme, therefore, furnished

direct currents, similar to those yielded by the voltaic pile. M.

Gramme subsequently so modified his machine as to produce alternating

currents. Such alternating machines are employed to produce the

lights now exhibited on the Holborn Viaduct and the Thames Embankment.

Another machine of great alleged merit is that of M. Lontin. It

resembles in shape a toothed iron wheel, the teeth being used as

cores, round which are wound coils of copper wire. The wheel is

caused to rotate between the opposite poles of powerful

electromagnets. On passing each pole the core or tooth is strongly

magnetised, and instantly evokes in its surrounding coil an induced

current of corresponding strength. The currents excited in

approaching to and retreating from a pole, and in passing different

poles, move in opposite directions, but by means of a commutator these

conflicting electric streams are gathered up and caused to flow in a

common bed. The bobbins, in which the currents are induced, can be so

increased in number as to augment indefinitely the power of the

machine. To excite his electro-magnets, M. Lontin applies the

principle of Mr. Wilde. A small machine furnishes a direct current,

which is carried round the electro-magnets of a second and larger

machine. Wilde's principle, it may be added, is also applied on the

Thames Embankment and the Holborn Viaduct; a small Gramme machine

being used in each case to excite the electro-magnets of the large

one.

The Farmer-Wallace machine is also an apparatus of great power. It

consists of a combination of bobbins for induced currents, and of

inducing electro-magnets, the latter being excited by the method

discovered by Siemens and Wheatstone. In the machines intended for

the production of the electric light, the electromotive force is so

great as to permit of the introduction of several lights in the same

circuit. A peculiarly novel feature of the Farmer-Wallace system is

the shape of the carbons. Instead of rods, two large plates of

carbons with bevelled edges are employed, one above the other. The

electric discharge passes from edge to edge, and shifts its position

according as the carbon is dissipated. The duration of the light in

this case far exceeds that obtainable with rods. I have myself seen

four of these lights in the same circuit in Mr. Ladd's workshop in the

City, and they are now, I believe, employed at the Liverpool Street

Station of the Metropolitan Railway. The Farmer-Wallace 'quantity

machine' pours forth a flood of electricity of low tension. It is

unable to cross the interval necessary for the production of the

electric light, but it can fuse thick copper wires. When sent through

a short bar of iridium, this refractory metal emits a light of

extraordinary splendour. [Footnote: The iridium light was shown by Mr.

Ladd. It brilliantly illuminated the theatre of the Royal

Institution.]

The machine of M. de Méritens, which he has generously brought over

from Paris for our instruction, is the newest of all. In its

construction he falls back upon the principle of the magneto-electric

machine, employing permanent magnets as the exciters of the induced

currents. Using the magnets of the Alliance Company, by a skilful

disposition of his bobbins, M. de Méritens produces with eight magnets

a light equal to that produced by forty magnets in the Alliance

machines. While the space occupied is only one-fifth, the cost is

little more than one-fourth of the latter. In the de Méritens machine

the commutator is abolished. The internal heat is hardly sensible,

and the absorption of power, in relation to the effects produced, is

small. With his larger machines M. de Méritens maintains a

considerable number of lights in the same circuit. [Footnote: The

small machine transforms one-and-a-quarter horse-power into heat and

light, yielding about 1,900 candles; the large machine transforms

five-horse power, yielding about 9,000 candles.]

*****

In relation to this subject, inventors fall into two classes, the

contrivers of regulators and the constructors of machines. M. Rapieff

has hitherto belonged to inventors of the first class, but I have

reason to know that he is engaged on a machine which, when complete,

will place him in the other class also. Instead of two single carbon

rods, M. Rapieff employs two pairs of rods, each pair forming a V. The

light is produced at the common junction of the four carbons. The

device for regulating the light is of the simplest character. At the

bottom of the stand which supports the carbons are two small

electro-magnets. One of them, when the current passes, draws the

carbons together, and in so doing throws itself out of circuit,

leaving the control of the light to the other. The carbons are caused

to approach each other by a descending weight, which acts in

conjunction with the electro-magnet. Through the liberality of the

proprietors of the Times, every facility has been given to M. Rapieff

to develope and simplify his invention at Printing House Square. The

illumination of the press-room, which I had the pleasure of

witnessing, under the guidance of M. Rapieff himself, is extremely

effectual and agreeable to the eye. There are, I believe, five lamps

in the same circuit, and the regulators are so devised that the

extinction of any lamp does not compromise the action of the others.

M. Rapieff has lately improved his regulator.

Many other inventors might here be named, and fresh ones are daily

crowding in. Mr. Werdermann has been long known in connection with

this subject. Employing as negative carbon a disc, and as positive

carbon a rod, he has, I am assured, obtained very satisfactory

results. The small resistances brought into play by his minute arcs

enable Mr. Werdermann to introduce a number of lamps into a circuit

traversed by a current of only moderate electro-motive power. M.

Reynier is also the inventor of a very beautiful little lamp, in which

the point of a thin carbon rod, properly adjusted, is caused to touch

the circumference of a carbon wheel which rotates underneath the

point. The light is developed at the place of contact of rod and

wheel. One of the last steps, though I am informed not quite the

last, in the improvement of regulators is this: The positive carbon

wastes more profusely than the negative, and this is alleged to be due

to the greater heat of the former. It occurred to Mr. William Siemens

to chill the negative artificially, with the view of diminishing or

wholly preventing its waste. This he accomplishes by making the

negative pole a hollow cone of copper, and by ingeniously discharging

a small jet of cold water against the interior of the cone. His

negative copper is thus caused to remain fixed in space, for it is not

dissipated, the positive carbon only needing control. I have seen

this lamp in action, and can bear witness to its success.

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