It may be thought impossible that vegetable matter should have so

changed as to become a dense, black, glistening, brittle mass, showing

no obvious forms of leaves or texture of wood. But no one who has seen

how a quantity of damp hay closely pressed together will, after a time,

become heated and change in colour to black, can have any difficulty in

comprehending how chemical and mechanical actions may completely alter

the aspect of vegetable matter. We have, however, the most direct

evidence of the vegetable origin of coal in the numberless

unquestionable forms of trees and plants met with in all coal strata.

Sometimes the trunks of the trees fossilized into stony matter are found

upright in the very situation in which they grew. Thus in Fig. 341 is

represented the appearance exhibited by the trunks and roots of some

fossil trees, which were exposed to view in the formation of a railway

cutting between Manchester and Bolton. In every coal-field also

beautiful impressions of the stems and leaves of plants are met with—one

common form of which is shown in Fig. 342. Most of the plants so found

belong to the flowerless division of the vegetable kingdom. Some are

closely allied to the ferns of the present day—to the common

“mare’s-tail” (_Equisetum_), to the club-moss, and to other well-known

plants. The firs and pines of the coal age are scarcely distinguishable

from existing species. If a fragment of ordinary coal be ground to a

very thin slice—so thin as to be transparent—and placed under the

microscope, it will show a number of minute rounded bodies, which are,

there is good reason to believe, nothing else than the spores or seeds

of plants, closely resembling the existing club-mosses. The spores of

the club-moss (_Lycopodium_) are so full of resinous matter, that they

are used for making fireworks and the flashes of lightning at theatres.

It is, therefore, extremely probable that the bitumen of coal is due to

the resin of similar spores, altered by the effects of subterranean

heat. The immense abundance of these little spores in the coal is a

proof that they accumulated in the ancient forests as the mosses grew,

and therefore the matter of coal was not accumulated under water or

washed down into the sea; for these little spores are extremely light,

and they cannot be wetted by water, and therefore they would have

floated on the surface, and would not have been found so diffused

throughout the coal. Fig. 343 is a picture of the possible aspect of the

ancient forests of the coal age. In the humid atmosphere which probably

prevailed at that period, the large tree-ferns and gigantic club-mosses,

which are conspicuous in the picture, must have flourished luxuriantly.

[Illustration:

FIG. 343.—_Possible Aspect of the Forests of the Coal Age._

]

The immense importance of coal for domestic purposes will be obvious

from the fact that it is estimated that in the United Kingdom alone no

less than 30,000,000 tons are annually consumed in house fires. Another

great use of coal is in the smelting, puddling, and working of iron, and

this probably consumes as much as our domestic fireplaces. Then there is

the vast consumption by steam engines, by locomotives, and by

steamboats. Another purpose for which coal is largely used is the making

of illuminating gas; and to the foregoing must also be added the

quantity which goes to feed the furnaces necessary in so many of the

arts—such as in the manufacturing of glass, porcelain, salt, chemicals,

&c. The quantity of coal raised in Great Britain was not accurately

known until 1854, when it was ordered that a register should be kept,

and an annual return made. The following figures, in round numbers, are

the returns published up to 1873. The table is continued in Note A.

Year. Coal raised, in Tons.

1854 64,661,000

1855 64,453,000

1856 66,645,000

1857 65,395,000

1858 65,008,000

1859 71,979,000

1860 83,208,000

1861 85,635,000

1862 83,638,000

1863 88,292,000

1864 92,787,000

1865 98,150,000

1866 101,630,000

1867 104,500,000

1868 103,141,000

1869 107,427,000

1870 110,289,000

1871 117,352,000

1872 123,497,000

1873 127,017,000

The first return showed our annual produce to be 64,661,000 tons. The

amount did not greatly vary until 1859, when there was an increased

production of nearly seven millions of tons; in 1860 a further increase

of eleven millions of tons more. Since then the quantity annually raised

has been increasing. Comparing the quantity which has been raised in any

year after 1863 with that raised ten years before, we see that the

increase in ten years is nearly half as much again; or, that at the

present rate of increase the amount annually raised doubles itself at

least every twenty years. Now, the question arises, How long can this go

on? However great may be the store of coal, it must sooner or later come

to an end. Is it possible to calculate how long our coals will last? and

what are the results of such calculations? These calculations have been

made; but there are great discrepancies in the results, for the

estimates of the amount of available coal still remaining vary greatly,

and different views are held regarding the rate of consumption in the

future. A very liberal estimate, by an excellent authority, of the

quantity of coal remaining under British soil, makes it 147,000 millions

of tons. With a consumption stationary at the present rate, this will

last 1,200 years; with an increase of consumption of 3,000,000 tons a

year, 276 years; but if the consumption continues to increase in the

same geometrical ratio it has hitherto followed, the supply will

scarcely last 100 years. It cannot be conceived, however, that this last

will be the real case, for the increasing depth to which it will be

necessary to go will soon cause a great increase in the cost, and thus

effectually check the consumption. Great Britain will, however, be

compelled to retire from the coal trade altogether, by the cheaper

supplies which other countries will yield, long before the absolute

exhaustion of her own coal-fields. It is calculated that the coal-fields

of North America contain thirteen times as much as those of all Europe

put together. Coal is also found abundantly in India, China, Borneo,

Eastern Australia, and South Africa; and it is believed that these

stores will supply the world for many thousand years.

[Illustration:

FIG. 344.—_The Fireside._

]

Seeing, then, that our supply of coal has a limit, and that at the

present increasing rate of consumption, the chief source of the wealth

of Great Britain must necessarily be exhausted in a few more centuries,

it behoves us to turn our mineral treasures to the best account, and to

adopt every possible means of obtaining from our coal its whole

available heat and force. The amount of avoidable waste of which we are

guilty in the consumption of coal is enormous. This is especially the

case in its domestic use, where probably nineteen-twentieths of the heat

produced is absolutely thrown away—sent off from the earth to warm the

stars. In England people look upon the wide open fireplace as the image

and type of home comfort. No doubt there are, from long use and habit,

many pleasing associations which cluster round the domestic hearth; but

we, to whom it is given to “look before and after,” must think what it

takes to feed that wide-throated chimney. All but a very small fraction

of the heat thus escapes, and is lost to man and the world for ever; and

surely we shall deserve the curses of our descendants if we continue

recklessly to throw away a treasure which, unlike the oil in the widow’s

cruse, is never renewed—for there is no contemporaneous formation of

coal. Thanks to the enhanced price of coal during the last few years,

some attention has been directed to contrivances for the economical

consumption of coal in its domestic, as well as in its manufacturing,

applications.

A time, however, will sooner or later come, when the whole available

coal shall have been consumed. What will then be the fuel of the

engines, and steamboats, and locomotives of the future? The reader may

think that then it will only be necessary to burn wood. But wood is

already being consumed from the face of the earth much more rapidly than

it is produced. How, then, can it be available when coal fails? The

truth is, we are now consuming not merely the wood which the sun-rays

are building up in our own time, but in hewing down the forests we are

using the sun-work of a century, while in coal we have the forests of

untold ages at our disposal—the accumulated combustible capital stored

up during an immense period of the earth’s existence. Upon this

stored-up capital we are now living, our current receipts of sun-force

being wholly inadequate to meet our expenditure. The coal is the

sun-force of former ages; and it is from this we are now deriving the

energy which performs most of our work. George Stephenson long ago

declared that his locomotives were driven by sunshine—by the sunshine of

former ages bottled up in the coal. And he was right. The mechanical

energy of our steam engines, and the chemical energy of our blast

furnaces, are derived from the combustion of vegetable matter, in which

the heat and light of the sun—our present sun or that of the coal

ages—are in some way stored up. The burning of wood or coal is,

chemically, the reverse action to that performed by the sunlight: by the

former carbon and oxygen are united, by the latter they are separated.

We foresee, then, a future period—however distant may be that future—in

which the world’s capital shall have been exhausted, and the energies

which are now employed in doing the world’s work will no longer be

available. But the reader will perhaps think that by improvements in the

steam engine, and in other ways, means will be found of getting more and

more work out of coal. It is true that we obtain from coal only a

_fraction_ of its available energy; but the whole work which could, by

any possible process, be done by the combustion of coal is _definite and

limited_, although its amount is large. A pound of coal burnt in one

minute sets free an amount of energy which would, if it could all be

made available, do as much as 300 horses working in the same time. But,

again, the reader may think, even if at some distant future the supplies

of fuel for the steam engines of our remote posterity should fail, that

before that time some other form of force than steam or heat engines

will have been discovered—some application of electricity, for example.

Now, it will appear, from principles which will be discussed in a

subsequent article, that not only is there no probability of such a

discovery, but that now, when the relations of the whole available

energies of the globe have been traced and defined, Science can find no

ground for admitting such a possibility under the present condition of

the universe.

_PETROLEUM._

When coal is heated in closed vessels, there are given off, as we shall

presently see, a number of gaseous and volatile products—many being

compounds of carbon and hydrogen—which condense to liquids or solids at

ordinary temperatures. Carbon is by far the largest constituent of coal,

which commonly contains only about 10 per cent. of other substances,

although the proportions vary very widely. Another important constituent

of coal is its hydrogen, and the value of coal as a source of heat

depends almost entirely upon the carbon and hydrogen it contains. Carbon

is one of the most remarkable of all the elements of the globe for its

power of entering into an enormous number of compounds. Thus, for

example, the compounds of carbon with only hydrogen are innumerable; but

they are all definite, and their composition is expressible by the

admirable system of chemical symbols, of which the reader has now, it is

hoped, some definite notion. Perhaps these hydro-carbons are among the

best evidences which could be adduced that modern science has obtained a

grasp of certain conceptions which have a real correspondence with the

actual facts of nature, even as regards the intimate constitution of

matter. This is not the place to enter into a complete exposition of

this subject. We may, however, invite the reader’s attention to a few

simple facts. A very large number of compounds of carbon and hydrogen

are known. If the percentage compositions of these be compared together,

it is only the eye of a most expert arithmetician which can detect any

relation between the proportions of the constituents in the various

compounds. The chemist, however, by associating such of these compounds

as resemble each other in their general properties, finds that they can

be arranged in series, in which the composition is accurately expressed

by multiples of the proportions: C = 12, H = 1. And not only so, the

different series themselves form a series of series, having a simple

relation to each other. Thus, confining ourselves to some of the known

hydro-carbons, we have the following:

┌──────────────────────┬──────────────────────┬──────────────────────┐

│ A │ B │ C │

├──────────────────────┼──────────────────────┼──────────────────────┤

│ C H_{4} │ C H_{2} │ │

│ C_{2}H_{6} │ C_{2}H_{4} │ C_{2}H_{2} │

│ C_{3}H_{8} │ C_{3}H_{6} │ C_{3}H_{4} │

│ C_{4}H_{10} │ C_{4}H_{8} │ C_{4}H_{6} │

│ C_{5}H_{12} │ C_{5}H_{10} │ C_{5}H_{8} │

│ C_{6}H_{14} │ C_{6}H_{12} │ C_{6}H_{10} │

│ &c. │ &c. │ &c. │

│ C_{_n_}H_{2_n_ + 2} │ C_{_n_}H_{2_n_} │ C_{_n_}H_{2_n_ – 2} │

└──────────────────────┴──────────────────────┴──────────────────────┘

┌──────────────────────┬──────────────────────┬──────────────────────┐

│ D │ E │ F │

├──────────────────────┼──────────────────────┼──────────────────────┤

│ │ │ │

│ │ │ │

│ C_{3}H_{2} │ │ │

│ C_{4}H_{4} │ C_{4}H_{2} │ │

│ C_{5}H_{6} │ C_{5}H_{4} │ C_{5}H_{2} │

│ C_{6}H_{8} │ C_{6}H_{6} │ C_{6}H_{4} │

│ &c. │ &c. │ &c. │

│ C_{_n_}H_{2_n_ – 4} │ C_{_n_}H_{2_n_ – 6} │ C_{_n_}H_{2_n_ – 8} │

└──────────────────────┴──────────────────────┴──────────────────────┘

This table might be indefinitely extended, but enough is given to enable

the intelligent reader to discover the laws connecting these formulæ.

The series headed B, it will be observed, have all the same percentage

composition. Why, then, one formula rather than another? The answer to

this question is the statement of a theoretical law upon which the whole

science of modern chemistry is based; for it has the same relation to

that science as gravitation has to astronomy. It is a matter of fact

that all gases, whatever their chemical nature, expand alike with the

same application of heat, and all obey the same law, which connects

volumes and pressures. These are very remarkable uniformities, for gases

in this respect exhibit the most decided contrast to liquids and solids.

The volume of each solid and of each liquid has its own special

relations to temperature and pressure: here there is endless diversity.

The volumes of all gases have one and the same relation to temperature

and pressure: here there is absolute uniformity. As an explanation of

these and other facts relating to gases, Amedeo Avogadro, in 1811, put

forward this hypothesis—_Equal volumes of all gases, under like

circumstances of temperature and pressure, contain the same number of

molecules_. This hypothesis was revived by Ampère a few years later, and

sometimes is called his. A necessary consequence of this law is that the

weights of the molecules of gases are proportional to their densities or

specific gravities. Hence when the percentage composition of a

hydro-carbon has been determined, by burning or oxidizing it in such a

manner as to obtain and weigh the products, carbonic acid and water, the

next thing the chemist does is to obtain the weight of a volume of the

gas. The number of times this exceeds the weight of hydrogen gas, under

the same conditions, expresses how many times the molecule is heavier

than the hydrogen molecule. Now, the chemist’s unit of weight in these

inquiries is the weight of a single _atom_ of hydrogen; and, as there

are grounds for believing that the _molecule_ of hydrogen consists of

two atoms of that substance, its weight = 2. Now, if the molecule of

marsh gas, the first hydro-carbon in the above list, has the composition

assigned, it will be 12 + 4 = 16 times heavier than the _atom_ of

hydrogen, and 16/2 = 8 times heavier than the _molecule_ of hydrogen.

Hence, if Avogadro’s law be correct, marsh gas should be just eight

times heavier than hydrogen gas; which is really the fact. The formula

expressing the composition of the molecule of a hydro-carbon, or of any

chemical compound whatever, is always so fixed that the same relations

may hold; and almost the first thing a chemist does in examining a new

body is to endeavour to obtain it in the state of gas.

The first four members of the series headed A are gases at ordinary

temperatures, the fifth is a gas at temperatures above the

freezing-point, and a liquid at lower temperatures; the next following

members are liquids which boil (that is, are converted into gases) at

temperatures rising with each additional carbon atom about 20° F. The

specific gravities and boiling-points of these liquids augment as we

pass from one hydro-carbon to the next, and the lower members of the

series are solids, fusing at temperatures higher and higher as the

number of carbon atoms is greater. Similar gradations of properties are

exhibited by the other series of hydro-carbons. Petroleum or rock-oil is

the name given to liquid hydro-carbons found in nature, and consisting

chiefly of compounds belonging to the series marked A in the above list.

Some varieties of petroleum hold in solution other hydro-carbons, and in

some cases paraffin is extracted from the oils by exposing the liquid to

cold, when the solid crystallizes out. Paraffin is a solid belonging to

the B series, and it is for the most part obtained by heating certain

minerals.

Deposits of liquid hydro-carbons, perhaps formed by a kind of natural

subterranean distillation from coal or other fossil organic matter,

exist in various localities. These deposits have long been known and

utilized at Rangoon, in Burmah, and on the shores of the Caspian Sea. At

Rangoon the mineral oil is obtained by sinking wells about 60 ft. deep

in a kind of clay soil, which is saturated with it. The oily clay rests

upon a bed of slate also containing oil, and underneath this is coal. It

may be supposed that subterranean heat, acting upon the coal, has

distilled off the petroleum, which has condensed in the upper strata.

This petroleum, when distilled in a current of steam, leaves about 4 per

cent of residue, and the volatile portion contains about one-tenth of

its weight of a substance (paraffin) which is solid at ordinary

temperatures. After an agitation with oil of vitriol, and another

distillation, _rock oil_ or _naphtha_ is obtained, which, however, is

still a mixture of several distinct chemical compounds. Mineral oils

have also been found in China, Japan, Hindostan, Persia, the West India

Islands, France, Italy, Bavaria, and England. In one of the Ionian

Islands there are oil-springs which have flowed, it is said, over 2,000

years.

But it is the recently discovered and extremely copious springs and

wells in Pennsylvania and Canada which have given a vastly extended

importance to the trade in mineral oil. Rock oil is now used in enormous

quantities as the cheapest illuminating oil, and that which furnishes

the most intense light. Its consumption as a lubricating oil for

machines has also been very large. Mineral oil was occasionally found at

various places in the United States, and sometimes used by the

inhabitants of the locality before the recent discoveries; but it was

not until August, 1859, that it was met with in large quantities. About

this time a boring which was made at Oil Creek, Pennsylvania, reached an

abundant source, for 1,000 gallons a day were drawn from it for many

weeks. The news of the discovery of this copious oil-spring spread

rapidly: thousands of persons flocked to the neighbourhood in hopes of

easily making a fortune by “striking oil.” Before the end of 1860 more

than a thousand wells had been bored, and some of these had yielded

largely. The regions of North America in which petroleum has been found

cover a large part of the States, and comprise Pennsylvania, New York,

Ohio, Michigan, Kentucky, Tennessee, Kansas, Illinois, Texas, and

California. In the vicinity of Oil Creek the bore-holes are usually

about 3 in. or 4 in. in diameter, and are often 500 ft. deep, and even

800 ft. is not uncommon. To make a bore-hole 900 ft. deep, and procure

all the requisites—steam engines, barrels, &c., for pumping the

oil—costs about $5,000. In 1869 many of these wells still yielded

regularly 300 barrels a day, but the supply has not continued with the

same abundance. One of the luckiest wells flowed at its first opening at

the rate of about 25,000 barrels a day. The apparatus used for working

the oil-wells is very simple—a rude derrick, a small steam engine, a

pump, and some barrels and tubs being all that is necessary. Fig. 345

will give the reader an idea of the scene presented by a cluster of

oil-wells in the Oil Creek region. Oil Creek received its name before

the petroleum trade was established, from the oil found floating on the

surface of the water. It is on the Alleghany River, about 150 miles

above Pittsburg, and here at its mouth is situated Oil City. There is a

wharf in Pittsburg for the oil traffic, and the barrels are brought down

the river in flats, or the oil is poured into very large flat boxes,

divided into compartments, which are then closed, and the boxes floated

down in groups of twenty or more. The refining process consists in

placing the crude oil into a large iron retort, connected with a

condenser formed of a coil of iron pipes, surrounded by cold water. Heat

is applied, and the lighter hydro-carbons (naphtha) come over first.

After the naphtha, the oils which are used for illuminating purposes

distil off. A current of steam is then forced into the retort, and this

brings over the heavy oils which are used for greasing machinery. A

black tarry oil yet remains; and, finally, after the separation of this,

a quantity of coke. The products are subjected to certain processes of

purification, which need not here be described. The magnitude of the

American oil trade may be inferred from the fact that in the second year

of its existence, from January to June, 1862, more than 4,500,000

gallons were exported from four seaports. This can hardly be wondered

at, considering the extremely low price at which this excellent

illuminating and lubricating agent can be produced. Refined petroleum

can be bought at Pittsburg for 16 cents. per gallon. It is believed by

some that the supplies of petroleum which exist in various localities

are so abundant that they will furnish illuminating oils to the whole

world for centuries.

[Illustration:

FIG. 345.—_View on Hyde and Egbert’s Farm, Oil Creek._

]

_PARAFFIN._

In the course of some researches on the substances contained in the tar,

which is obtained by heating wood in close vessels, Reichenbach found a

white translucent substance, to which he gave the above name, because it

was not acted upon by any of the ordinary chemical reagents, such as

sulphuric acid, nitric acid, &c. This substance, which is composed of

carbon and hydrogen only, is not unlike spermaceti; it is colourless,

translucent, and without smell or taste. But when slightly warmed, it

becomes very plastic, and may then be moulded with the greatest ease—and

in this respect it differs from spermaceti. Paraffin melts at from 88°

to 150° C., to a colourless liquid, which is so fluid that it may be

filtered through paper like water, and at a higher temperature it can be

distilled unchanged. Paraffin does not dissolve in water, and is but

slightly soluble in alcohol. In ether, naphtha, turpentine, benzol, and

sulphide of carbon, it dissolves very readily. When heated with sulphur,

it is decomposed: the sulphur seizes upon its hydrogen, sulphuretted

hydrogen is given off, and the carbon is separated; and this action has

been proposed as a ready means of obtaining pure sulphuretted hydrogen

for laboratory use. It is probable that paraffin is a mixture of various

hydro-carbons, having a composition expressible by the formula,

C_{_n_}H_{2_n_}; for different specimens fuse at different temperatures,

according as the paraffin has been obtained from one or the other

source.

Discoveries and Inventions of the Nineteenth Century · 第 85 / 93 段