The present civilization of Europe very properly began with the clock,

a machine which a monk, afterwards Pope Sylvester II, was supposed

to have borrowed from Satan, though he was probably indebted for it

to the Saracens. For nearly nine hundred years after his day, the

best ingenuity of Italian, German, Swiss, French, and English

mechanics was devoted to perfecting this noble creation, and it

became at last a part of the civilized man, a sort of additional or

supplementary sense. The savage may well be excused for mistaking

the watch for a living creature. It could not serve us better, if it

were. True, it does not perform its function by its own force, but by

a stock of extraneous force which is from time to time put into a

little store-house called a spring. Neither does the living creature

perform its functions by any other force than that which is developed

by the chemical action within it, or the _quasi_ combustion of its

food. Its will does but direct the application of its mechanical

power. It creates none. You may weigh the animal and all the food it

is to consume, and thence calculate the utmost ounce of work, of a

given kind, which it can thereafter perform. It may do less, but

cannot do more. Having consumed all of its food and part of itself,

it dies. Its chemical organs have oxydated or burned up all the

combustibles submitted to them, thus developing a definite amount of

heat, a part of which, at the dictation of the will, by the

mechanism of nerves and muscles, has been converted into mechanical

motion. When the chemical function ceases, for the want of materials

to act upon, the development of heat ceases. There is no more either

to be converted into motion or to maintain the temperature of the

body; and self-consumption having already taken the place of

self-repair, there is no article left but the _articulus mortis_.

But of all the force or motion produced by, or rather passing through,

a living animal, or any other organism, none is ever, so far as we

know, annihilated. The motion which has apparently ceased or been

destroyed has in reality passed into heat, light, electricity,

magnetism, or other effect,--itself, perhaps, nothing but motion, to

keep on, in one form or another, indefinitely. The fuel which we put

into the stomach of the horse, of iron or of flesh, first by its

oxydation raises heat, a part of which it is the function of the

individual to convert into motion, to be expended on friction and

resistance, or, in other words, to be reconverted into heat. What

becomes of this heat, then? If the fuel were to be replaced or

deoxydated, the heat that originally came from the oxydation would be

precisely reabsorbed. But this heat of itself cannot overcome the

stronger affinity which now chains the fuel to the oxygen. It must

go forward, not backward, about its business, forever and ever. It

may pass, but not cease. The sharp-eyed Faraday has been following

far away this Proteus, with a strong suspicion that it changes at

last into gravity, in which shape it returns straight to the sun,

carrying down with it, probably, those flinty showers of meteors

which, striking fire in the atmosphere of the prime luminary,

replenish its overflowing fountain of life. But we are not aware

that he has yet discovered the anastomosis of this conversion, or

quite established the fact. We are therefore not yet quite ready to

resolve the universe of physical forces into the similitude of the

mythical mill-stream, which, flowing round a little hill, came back

and fed its own pond. Nevertheless, we believe the physicists have

pretty generally agreed to assume as a law of Nature what they call

the conservation of force, the principle we have been endeavoring to

explain.

Under the lead of this law, theory, or assumption, discoveries have

been made that deeply and practically interest the most abject

mortal who anywhere swings a hoe or shoulders a hod, as well as the

lords of the land. For example, it has been ascertained that heat is

converted into motion, or motion into heat, according to a fixed or

constant ratio or equivalent. To be more particular, the heat which

will raise the temperature of a pound of water one degree of

Fahrenheit's scale, when converted into mechanical motion, is

equivalent to the force which a weight of seven hundred and

seventy-two pounds would exert by falling one foot. This is a

wonderfully small quantity of heat to balance so heavy a blow, but

the careful experiments of Mr. Joule of Manchester, the discoverer,

confirmed by Regnault, Thomson, Rankine, Clausius, Mayer, Rennie,

and others, have, we believe, satisfied scientific men that it is

not far from the correct measure. Were the same, or a far less

amount of heat, concentrated on a minute chip of steel struck off by

collision with a flint, it would be visible to the eye as a spark,

and show us how motion is converted into light as well as heat.

It is not our vocation to dive into the infinities, either upward or

downward, in search, on the one hand, of the ultimate atoms of the

rarest ether, by whose vibrations the luminous waves run through

space at the rate of more than ten millions of miles a minute, or,

on the other, of the nebulous systems, worlds in the gristle, so far

off that the light just now arriving from them tells only how they

looked two hundred thousand years ago. All we have to say is, that,

if we do not now absolutely know, we do reasonably suspect, that heat

and light are mere mechanical motions, alike in nature and

interconvertible in fact. The luminiference seems to behave itself,

not like infinitely small bullets projected from Sharpe's rifles of

proportionately small bore, as was once supposed, but rather after

the manner of the sound-waves, which we know travel through the air

from the sonorous body to the ear. They have also a resemblance, not

so close, to the waves which run in all directions along the surface

of a pond of water from the point where a stone falls into it. These

three classes of waves, differing so immensely in magnitude and

velocity, all agree in this,--that it is the wave that travels, and

not the fluid or medium. The rapidity of the luminous wave is about

nine hundred million times that of the sound-wave; hence we may

suppose that the ether in which it moves is about as many times

rarer or lighter than air, and the retina of the eye which it

impresses as many times more delicate and sensitive than the drum of

the ear. It can hardly be unreasonable to suppose that a fluid so

rare as this luminiferous ether will readily interflow the particles

of all other matter, gaseous, liquid, or solid, and that in such

abundance that its vibrations or agitations may be propagated through

them. Yet even the rarest gases must considerably obstruct and

modify the vibratory waves, while liquids and solids, according to

their density and structural arrangement of atoms, must do it far

more. The luminiferous ether, in which all systems are immersed,

kept hereabout in an incessant quiver through its complete and

perhaps three-fold gamut of vibrations by the sun, strikes the aërial

ocean of the earth about an average of five hundred million millions

of blows per second, for each of the seven colors, or luminous notes,

not to speak of the achromatic vibrations, whose effects are other

than vision or visionary. The aërial ocean is such open-work, that

these infinitesimal billows are not much, though somewhat, broken by

it; but when they reach the terraqueous globe itself, they dash into

foam which goes whirling and eddying down into solids and liquids,

among their wild caverns of ultra-microscopic littleness, and this

foam or whirl-storm of ethereal substance is heat, if we are not

much mistaken. According to its intensity, it expands by its own mere

motion all grosser material.

The quantity of this ethereal foam, yeast, whirlwind, hubbub, or

whatever else you please to call it, which is got up or given up by

the combustion of three pounds of good bituminous coal, according to

Mr. Joule's experiments, is more than equivalent to a day's labor

of a powerful horse. With our best stationary steam-engines, at

present, we get a day's horse-power from not less than twenty-four

pounds of coal. At this rate, the whole supply of mineral coal in

the world, as it may be roughly estimated, is equivalent only to the

labor of one thousand millions of horses for fifteen hundred years.

With the average performance of our present engines, it would

support that amount of horse-power for only one thousand years. But

could we obtain the full mechanical duty of the fuel by our engines,

it would be equal to the work of a thousand millions of horses for

sixteen thousand years, or of about fifteen times as many men for

the same time. This would materially postpone the exhaustion of the

coal, at which one so naturally shudders,--to say nothing of the

saving of having to dig but one eighth as much of the mineral to

produce the same effect. Hence some of the interest that attaches to

this discovery of Mr. Joule, which has given a new impulse to the

labor of inventors in pushing the steam-engine towards perfection.

But if the whole available mechanical power, laid in store in the

coal mines, in addition to all the unimproved wind and water power,

should seem to any one insufficient to work out this world's manifest

destiny, the doctrine of the essential unity or conservation of

force is not exhausted of consolation. All the coal of which we have

spoken is but the result of the action of sun-light in past ages,

decomposing carbonic acid in the vegetative process. The combustion

of the carbon reproduces a force exactly equivalent to that of the

sun-light which was absorbed or consumed in its vegetative separation.

Supposing the whole estimated stock of coal in the world to be

consumed at once, it would cover the entire globe with a stratum of

carbonic acid about seventy-two feet deep. And if all the energy of

sun-light which this globe receives or encounters in a year were to

be devoted to its decomposition, according to Pouillet's estimate of

the strength of sunshine,--and he probably knows, if any one does,--

deducting all that would be wasted on rock or water, there would be

enough to complete the task in a year or two. A marvellous growth of

forest, that would be! But the coal is not to be burned up at once.

When we get our steam-engines in motion to the amount of two or

three thousand millions of horse-power, and are running off the coal

at the rate of one tenth of one per cent per annum, the simple and

inevitable consequence will be that the wood will be growing enough

faster to keep good the general stock of fuel. Doubtless the forests

are now limited in their growth and stunted from their ante-Saurian

stature, not so much for want of soil, moisture, or sunshine as for

want of carbonic acid in the air, to be decomposed by the foliage,

the great deposition of coal in the primitive periods having

exhausted the supply. Our present havoc of wood only changes the

locality of wood-lots, and our present consumption of coal, rapid

enough to exhaust the entire supply in about seventy-seven thousand

years, is sure to increase the aggregate cordage of the forests. By

the time we have brought our locomotive steam-cultivators to such

perfection as to plough up and pulverize the great central deserts,

we may see trees flourish where it would have been useless to plant

the seed before we had converted so much of the earth's entrails

into smoke.

There was a time, before we had harnessed the powers of Nature to

found, forge, spin, weave, print, and drudge for us generally, that

in every civilized country the strong-headed men used their

strong-handed brethren as machines. Only he could be very knowing who

owned many scribes, or he very rich who owned many hewers of wood

and drawers of water. With our prodigious development of mechanical

inventions, iron and coal, our mighty steam-driven machinery for

making machines, the time for chattelizing men, or depending mainly

on animal power of any sort for the production of wealth, has passed

by. Abrogate the golden rule, if you will, and establish the creed

of caste,--let the strongest of human races have full license to

enslave the weakest, and let it have the pick of soil and staples,--

still, if you do not abolish the ground rules of arithmetic, and the

fact that a pound of carbon costs less than a pound of corn, and must

cost less for at least a thousand years to come, chattelism of man

will cease in another generation, and the next century will not dawn

on a human slave. At present, a pound of carbon does not cost so

much as a pound of corn in any part of the United States, and in no

place visited by steam-transportation does it cost one fifth as much.

We are already able to get as much work out of a pound of carbon as

can be got from a pound of corn fed to the faithfullest slave in the

world. Mr. Joule has shown us that there is really in a pound of

carbon more than twice as much work as there is in a pound of corn.

The human corn-consuming machine comes nearer getting the whole

mechanical duty or equivalent out of his fuel than our present

steam-engine does, but the former is all he ever will be, while the

latter is an infant and growing.

We shall doubtless soon see engines that will get the work of two

slaves out of the coal that just balances one slave's food in the

scales. Our iron-boned, coal-eating slave, with the advantage of

that peculiar and almost infinitely applicable mechanical element,

the wheel, may be made to go anywhere and do any sort of work, and,

as we have seen, he will do it for one tenth of the cost of any

brute or human slave.

But will not our artificial slave be more liable to insurrection?

Everybody admits that he already accomplishes incalculable drudgery

in the huge mill, on the ocean, and on the iron highway. But almost

everybody looks upon him as a sleeping volcano, which must sooner or

later flare up into irresistible wrath and do frightful mischief.

Underwriters shake their prudent heads at him. Coroners' inquests,

sitting solemnly over his frequent desolations, find only that some

of his ways are past finding out. Can such a creature be

domesticated so as to serve profitably and comfortably on by-roads

as well as high-roads, on farms, in gardens, in kitchens, in mines,

in private workshops, in all sorts of places where steady,

uncomplaining toil is wanted? Can we ever trust him as we trust

ourselves, or our humble friends, the horse and the ox? The law of

the conservation of force, now so nearly developed, will perhaps

throw some light on this inquiry.

Boiler explosions have a sort of family resemblance to the freaks of

lightning or the thunderbolt. Indeed, so striking is the similarity,

that people have been prone to think, that, previously to an

explosion, the steam in the boiler must have become in some

inexplicable way charged with electricity like a thunder-cloud, and

that the discharge must have occasioned the catastrophe. It is

needless to say to those who understand a Leyden jar, that nothing

of the sort takes place. The friction of the watery globules, carried

along by the steam in blowing off, is found to disturb the

electrical equilibrium, as any other friction does; but the

circumstances in the case of a boiler are always so favorable to its

restoration, that an electrical thunderbolt cannot possibly be

raised there that would damage a gnat. Yet a boiler explosion may,

after all, depend on the same immediate cause as the mechanical

effect which is frequently noticed after an electrical discharge in a

thunder-storm. Let us hypothetically analyze what takes place in a

thunder-storm. For the sake of illustration, and nothing more, we

will suppose the existence, throughout all otherwise void space, of

three interflowing ethers, the atoms of each of which are, in regard

to each other, repellant, negative, or the reverse of ponderable,

and that these ethers differ in a series by vast intervals as to

size and distance of atoms, that each neither repels nor attracts

the other, that only the rarest is everywhere, and that the denser

ones, while self-repellant, have affinities, more or less, which

draw them from the interplanetary spaces towards the ponderable

masses. Let the rarest of these ethers be that whose vibrations

cause the phenomena of light,--the next denser that which, either by

vibration or translatory motion, causes the electrical phenomena,--

and the most dense of the three that which by its motions, of

whatever sort, causes the phenomena of heat. The solar impulse

propagated through the luminiferous ether towards any mass encounters

in its neighborhood the electrical and calorific ethers, and sets

them into motions which may be communicated from one to the other,

but which are communicated to ponderable matter, or result in

mechanical action, only or chiefly by the impulse of the denser or

calorific ether. When the sun shines on land and water, as we have

already said, there is a violent ethereal commotion in the

interstices of the superficial matter, which we will now suppose to

be that of the calorific ether; and by virtue of this motion,

together with whatever affinities this ether may be supposed to have

for ponderable matter, we may account for evaporation, and the

production of those vast aërial currents by which the evaporated

water is diffused. In the production of aërial currents, heat is

converted into force, and hence vapor is converted into watery

globules mechanically suspended on clouds, which, by their friction,

sweep the electrical ether into excessive condensation in the great

Leyden-jar arrangement of the sky. Whatever it may be that gives

relief to this condensation, the relief itself consists in motion,

either translatory or vibratory, of the electrical ether or ethers.

As this motion, if it be such, often takes place through gases,

liquids, and solids, without any sensible mechanical effect, and at

other times is contemporary with phenomena of intense heat, we may,

till otherwise informed, suppose, that, whenever it produces a

mechanical effect, it is by so impinging on the calorific ether as

to produce the motion of heat, which is instantly thereafter

converted into mechanical force. It is not so much the greatness of

the amount of this mechanical force which gives it its peculiar

destructiveness, as the inequality of its strain; not so much the

quantity of matter projected, as the velocity of the blow. One may

have his brains blown out by a bullet of air as well as one of lead,

if the air only blows hard enough and to one point. Whatever its

material, the edge of the thunder-axe is almost infinitely sharp,

and its blow is as destructive as it is timeless. But it is always

heat, not electrical discharge, which only sometimes causes heat,

that strikes the blow.

Now in the case of a steam-boiler, when the water, having been

reduced too low, is allowed suddenly to foam up on the overheated

crown-sheet of the furnace, there must be just that sudden or

instantaneous conversion of heat into force which may take place

when the current of the electrical discharge passes through the

gnarled fibres of an oak. The boiler and the oak are blown to shivers

in equally quick time. The only difference seems to be, that in one

case electricity stood immediately, in point of time, behind the heat,

and in the other it stood away back beyond the crocodiles, playing

its _rôle_ more genially in the growth of the monster forests whose

remains we are now digging from the bowels of the earth as coal. In

the normal action of a steam-boiler, the steam-generating surfaces

being all under water, however unequally the fire may act in

different localities, the water, by its rapid circulation, if not by

its heat-absorbing power, diffuses the heat and constantly equalizes

the strain resulting from its conversion into mechanical force. The

increase of pressure takes place gradually and evenly, and may

easily be kept far within safe limits. It is quite otherwise when

the conductivity of the boiler-plate is not aided and controlled by

the distributiveness of the water, as it is not whenever the plate

is in contact with the fire on one side without being also in contact

with the water on the other. Everybody knows that boilers explode

under such circumstances, but everybody does not know why.

A cylinder of plate-iron will withstand a gradually applied, evenly

distributed, and constant pressure, one thousandth part of which,

acting at one spot, as a blow, would rend its way through, or

establish a crack. This slight rent, giving partial relief to the

sudden but comparatively small force that causes it, would be

nothing very serious in itself,--no more so than a rent produced by

the hydraulic press,--if the whole force, equal, perhaps, to that of

a thousand wild horses imprisoned within, did not take instant

advantage of it to enlarge the breach and blow the whole structure

to fragments, or, in other words, if it did not permit nearly the

whole of the accumulated heat in the boiler to be at once converted

into mechanical motion. For example, a boiler whose ordinary working

pressure is one hundred pounds to the square inch, which may give an

aggregate on the whole surface of five millions of pounds, would not

give way, perhaps, if that pressure were gradually and evenly

increased to thirty millions. But if the water is allowed to get so

low that some part of the plate exposed to the fire is no longer

covered with it, that part will directly become far hotter than the

water or the mass of the steam,--dry steam having no more power to

carry away the excess of heat than so much air. After that, when the

water rises again, the first wave or wallop that strikes the

overheated plate absorbs the excess of heat, and its conversion into

steam of higher pressure than that already existing is so sudden

that it may be regarded as instantaneous. It is to be remembered

that for every pound of water raised one degree, or heat to that

amount absorbed in generating steam, a force of seven hundred and

seventy-two pounds is created. In this case a new or additional

force is created, which, acting in all directions from one point,

first takes effect on the line which joins that point with the

nearest opposite point in the wall of the boiler. If it is not like

smiting with the edge of a ponderous battle-axe, it is at least as

dangerous as a cannon ball shot along that line. If the local heat

so suddenly absorbed be but enough to raise ten pounds of water ten

degrees, it is equivalent to the force acquired by seventy-seven

thousand two hundred pounds falling through a foot, or of a

cannon-ball of one hundred pounds flying at the rate of more than a

mile per second. If by any miracle the boiler should stand this

shock or series of shocks, the pressure becomes equalized, and the

overheated plate having parted with its excess of heat, safety is

restored. But if cohesion is anywhere overcome by the sudden blow,

the wild horses stampede in all directions. The boiler, minus the

water and boiler-head perhaps, goes through ceiling, roof, and brick

walls, as if they were cobwebs, and, surrounded with fragments of

men and things, is seen descending like a comet through the

neighboring air.

The Atlantic Monthly, Volume 02, No. 08, June 1858 A Magazine of Literature, Art, and Politics · 第 15 / 21 段