THE SOLIDITY OF THE EARTH.

In his opening address to the Mathematical and Physical Section of the

British Association, Sir William Thomson affirmed, “with almost perfect

certainty, that, whatever may be the relative densities of rock, solid

and melted, or at about the temperature of liquefaction, it is, I

think, quite certain that cold solid rock is denser than hot melted

rock; and no possible degree of rigidity in the crust could prevent

it from breaking in pieces and sinking wholly below the liquid lava,”

and that “this process must go on until the sunk portions of the crust

build up from the bottom a sufficiently close-ribbed skeleton or frame,

to allow fresh incrustations to remain bridged across the now small

areas of lava-pools or lakes.”[11]

This would doubtless be the case if the material of the earth were

chemically homogeneous or of equal specific gravity throughout, and if

it were chemically inert in reference to its superficial or atmospheric

surroundings. But such is not the case. All we know of the earth shows

that it is composed of materials of varying specific gravities, and

that the range of this variation exceeds that which is due to the

difference between the theoretical internal heat of the earth and its

actual surface temperature.

We know by direct experiment that these materials, when fused together,

arrange themselves according to their specific gravities, with the

slight modification due to their mutual diffusibilities. If we take a

mixture of the solid elements of which the earth, so far as we know it,

is composed, fused them, and leave them exposed to atmospheric action,

what will occur?

The heavy metals will sink, the heaviest to the bottom, the lighter

metals (_i.e._, those that we call the metals of the earths, because

they form the basis of the earth’s superficial crust) will rise along

with the silicon, etc., to the surface; these and the silicon will

oxidize and combine, forming silicates, and with a sufficient supply

of carbonic acid, some of them, such as calcium, magnesium, etc.,

will form carbonates when the temperature sinks below that of the

dissociation of such compounds.

The scoria thus formed will float upon the heavy metals below and

protect them from cooling by resisting their radiation; but if in

the course of contraction of this crust some fissures are formed

reaching to the melted metals below, the pressure of the floating

solid will inject the fluid metal upwards into these fissures to a

height corresponding to the flotation depth of the solid, and thus

form metallic veins permeating the lower strata of the crust. I need

scarcely add that this would rudely but fairly represent what we know

of the earth.

But it may be objected that I only describe an imaginary experiment.

This is true as regards the whole of the materials united in a single

fusion. Nobody has yet produced a complete model with platinum and gold

in the centre, and all the other metals arranged in theoretical order

with the oxidized, silicated, and carbonated crust outside; but with a

limited number of elements this has been done, is being done daily, on

a scale of sufficient magnitude to amply refute Sir William Thomson’s

description of a fused earth solidifying from the centre outwards.

This refutation is to be seen in our blast furnaces, refining furnaces,

puddling furnaces, Bessemer ladles, steel melting-pots, cupels, foundry

crucibles; in fact, in almost every metallurgical operation down to the

simple fusion of lead or solder in a plumber’s ladle, with its familiar

floating crust of dross or oxide.

As an example I will, on account of its simplicity, take the open

hearth finery and the refining of pig-iron. Here a metallic mixture of

iron, silicon, carbon, sulphur, etc., is simply fused and exposed to

the superficial action of atmospheric air. What is the result?

Oxidation of the more oxidizable constituents takes place, and

these oxides at once arrange themselves according to their specific

gravities. The oxidized carbon forms atmospheric matter and rises above

all as carbonic acid, then the oxidized silicon, being lighter than

the iron, floats above that, and combines with aluminium or calcium

that may have been in the pig and with some of the iron; thus forming

a silicious crust closely resembling the predominating material of the

earth’s crust.

When the oxidation in the finery is carried far enough, the melted

material is tapped out into a rectangular basin or mould, usually

about 10 feet long and about 3 feet wide, where it settles and cools.

During this cooling the silica and silicates—_i.e._, the rock

matter—separate from the metallic matter and solidify on the surface

as a thin crust, which behaves in a very interesting and instructive

manner. At first a mere skin is formed. This gradually thickens, and

as it thickens and cools becomes corrugated into mountain chains and

valleys much higher and deeper, in proportion to the whole mass, than

the mountain chains and valleys of our planet. After this crust has

thickened to a certain extent volcanic action commences. Rifts, dykes,

and faults are formed by the shrinkage of the metal below, and streams

of lava are ejected. Here and there these lava streams accumulate

around their vent and form insulated conical volcanic mountains with

decided craters, from which the eruption continues for some time. These

volcanoes are relatively far higher than Chimborazo. The magnitude of

these actions varies with the quality of the pig-iron.

The open hearth finery is now but little used, but probably some are

to be seen at work occasionally in the neighborhood of Glasgow, and I

am sure that Sir William Thomson will find a visit to one of them very

interesting. Failing this, he may easily make an experiment by tapping

into a good-sized “cinder bogie” some melted pig-iron from a pudding

furnace (taking it just before the iron “comes to nature”), and leaving

the melted mixture to cool slowly and undisturbed.

The cinder of the blast furnace, which in like manner floats on the top

of the melted pig-iron, resembles still more closely the prevailing

rock-matter of the earth, on account of the larger proportion, and the

varied compounds, of earth-metals it contains.

For the volcanic phenomena alone he need simply watch what occurs

when in the ordinary course of puddling the cinder is run into a

large bogie, and the bogie is left to cool standing upright. I need

scarcely add that these phenomena strikingly illustrate and confirm Mr.

Mallett’s theory of earthquakes, volcanoes, and mountain-formation.

In merely passing through an iron-making district one may see the

results of what I have called the volcanic action, by simply observing

the form of those oyster-shaped or cubical blocks of cinder that are

heaped in the vicinity of every blast furnace that has been at work for

some time. Radial ridges or consolidated miniature lava-streams are

visible on the exposed face of nearly, if not quite all of these. They

were ejected or squeezed up from below while the mass was cooling, when

the outer crust had consolidated but the inner portion still remained

liquid. Many of these are large enough, and sufficiently well-marked,

to be visible from a railway carriage passing a cinder heap near the

road.[12]

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