CHAPTER II.

THE NATURE OF VOLCANIC ACTION.

The dose investigation of what goes on within a volcanic vent may

appear at first sight to be a task beset with so many difficulties and

dangers that we may be tempted to abandon it as altogether hopeless. At

the first recorded eruption of Vesuvius the elder Pliny lost his life

in an attempt to approach the mountain and examine the action which

was taking place there; and during the last great outburst of the same

volcano a band of Neapolitan students, whose curiosity was greater than

their prudence, shared the same fate.

But in both these cases the inquirers paid the penalty of having

adopted a wrong method. If we wish to examine the mode of working of a

complicated steam-engine, it will be of little avail for us to watch

the machinery when the full blast of steam is turned on, and the rapid

movements of levers, pinions, and slides baffle all attempts to follow

them, and render hopeless every effort to trace their connection with

one another. But if some friendly hand turn off the greater part of

the steam-supply, then, as the rods move slowly backwards and forwards,

as the wheels make their measured revolutions, and the valves axe

seen gradually opening and shutting, we may have an opportunity of

determining the relations of the several parts of the machine to one

another, and of arriving at just conclusions concerning the plan on

which it is constructed. Nor can we doubt that the parts of the machine

bear the same relation to one another, and that their movements take

place in precisely the same order, when the supply of steam is large as

when it is small.

Now, as we shall show in the sequel, a volcano is a kind of great

natural steam-engine, and our best method of investigating its action

is to watch it when a part of the steam-supply is cut off. It is

true that we cannot at will control the source of supply of steam to

a volcano, as we can in a steam-engine, but as some volcanoes have

usually only a small steam-supply, and nearly all volcanoes vary

greatly in the intensity of their action at different periods, we can,

by a careful selection of the object or the time of our study, gain all

those advantages which would be obtained by regulating its action for

ourselves.

Spallanzani appears to have been the first to perceive the important

fact, that the nature of volcanic action remains the same, however

its intensity may vary. Taking advantage of the circumstance that

there exists in the Mediterranean Sea a volcano--Stromboli--which

for at least 2,000 years has been in a constant and regular, but not

in a violent or dangerous, state of activity, he visited the spot,

and made the series of careful observations which laid the foundation

of our knowledge of the 'physiology of volcanoes.' Since the time

of Spallanzani, many other investigators have visited the crater

of Stromboli, and they have been able to confirm and extend the

observations of the great Italian naturalist, as to the character of

the action which is constantly taking place within it. We cannot better

illustrate the nature of volcanic action than by describing what has

been witnessed by numerous observers within the crater of Stromboli,

where it is possible to watch the series of operations going on by the

hour together, and to do so without having our judgment warped either

by an excited imagination or the sense of danger.

[Sidenote: APPEARANCE OF STROMBOLI FROM A DISTANCE.]

In the sketch, fig. 1, which was made on April 20, 1874, I have shown

the appearance which this interesting volcano usually presents, when

viewed from a distance. The island is of rudely circular outline, and

conical form, and rises to the height of 3,090 feet above the level of

the Mediterranean. From a point on the side of the mountain, masses

of vapour are seen to issue, and these unite to form a cloud over

the mountain, the outline of this vapour-cloud varying continually

according to the hygrometric state of the atmosphere, and the direction

and force of the wind. At the time when this sketch was made, the

vapour-cloud was spread in a great horizontal stratum overshadowing

the whole island, but it was clearly seen to be made up of a number

of globular masses, each of which, as we shall hereafter see, is the

product of a distinct outburst of the volcanic forces.

Viewed at night-time, Stromboli presents a far more striking and

singular spectacle. The mountain, with its vapour canopy, is visible

over an area having a radius of more than 100 miles. When watched from

the deck of a vessel anywhere within this area, a glow of red light is

seen to make its appearance from time to time above the summit of the

mountain; this glow of light may be observed to increase gradually in

intensity, and then as gradually to die away. After a short interval

the same appearances are repeated, and this goes on till the increasing

light of the dawn causes the phenomenon to be no longer visible. The

resemblance presented by Stromboli to a 'flashing light' on a most

gigantic scale is very striking, and the mountain has long been known

as 'the lighthouse of the Mediterranean.'

It must be pointed out, however, that in two very important particulars

the appearances presented by Stromboli differ markedly from those

rhythmical gleams exhibited by the 'flashing-lights' of our coasts.

In the first place, the intervals between successive flashes are very

unequal, varying from less than one minute to twenty minutes, or even

more; and in the second place, the duration and intensity of the red

glow above the mountain are subject to like variation, being sometimes

a momentary scarcely visible gleam, and at others a vivid burst of

light which illuminates the sky to a considerable distance round.

[Illustration: Fig. 1.--Stromboli, viewed from the North-west, April

1874.]

[Illustration: Fig. 2.--Map of tub Island of Stromboli. (Scale about

two inches to a mile.)]

[Sidenote: GENERAL FEATURES OF THE MOUNTAIN.]

Let us now draw near and examine this wonderful phenomenon of a

mountain which seemingly ever burns with fire, and yet is not consumed.

The general form of the Island of Stromboli will be gathered from an

inspection of the plan, fig. 2, which is copied from a map published by

the Italian Government. When we land upon the island, we find that it

is entirely built up of such materials as we know to be ejected from

volcanoes; indeed, it resembles on a gigantic scale the surroundings

of an iron furnace, with its heaps of cinders and masses of slag. The

irregularity in the form of the island is at once seen to be due to the

action of the wind, the rain, and the waves of the surrounding sea,

which have removed the loose, cindery materials at some points, and

left the hard, slaggy masses standing up prominently at others.

This great heap of cindery and slaggy materials rises, as we have said,

to a height of more than 3,000 feet above the sea-level, but even this

measurement does not give a just idea of its vast bulk. Soundings in

the sea surrounding the island show that the bottom gradually shelves

around the shores to the depth of nearly 600 fathoms, so that Stromboli

is a great conical mass of cinders and slaggy materials, having a

height of over 6,000 feet, and a base whose diameter exceeds four miles.

The general form and proportions of this mass will be better understood

by an examination of the section, fig. 3, which is also constructed

from the materials furnished by the map of the island issued by the

Italian Government. The same section, and the map, fig. 2, will serve

to make clear the position and relations of the point on the mountain

at which the volcanic activity takes place. At a spot on the north-west

slope of the mountain, about 1,000 feet below its summit, and 2,000

feet above the level of the sea, there exists a circular depression,

the present active 'crater' of the volcano; and leading down from this

to the sea there is a flat slope making an angle of about 35° with the

horizon, and known as the 'Sciarra.' The Sciarra is bounded by steep

cliffs, as shown in the sketch fig. 1, and the plan fig. 2.

[Illustration: Fig. 3.--Section through the Island of Stromboli from

n.w. to s.e.

_a._ Highest summit of the mountain, _c._ Cratère del Fossa, _b._ Point

overlooking the crater, _d._ Steep slope known as the Sciarra del

Fuoco. _e._ Continuation of the same slope beneath the level of the

sea. _f._ Steep cliffs of the Punta dell' Omo.]

[Sidenote: FORM AND FUNCTION OF THE CRATER.]

If we climb up to this scene of volcanic activity, we shall be able to

watch narrowly the operations which are going on there. On the morning

of the 24th of April, 1874, I paid a visit to this interesting spot in

order to get a near view of what was taking place. On reaching a point

upon the side of the Sciarra, from which the crater was in full view

before me, I witnessed, and made a sketch of, an outburst which then

took place, and this sketch has been reproduced in fig. 4. Before the

outburst, numerous light curling wreaths of vapour were seen ascending

from fissures on the sides and bottom of the crater. Suddenly, and

without the slightest warning, a sound was heard like that produced

when a locomotive blows off its steam at a railway-station; a great

volume of watery vapour was at the same time thrown violently into

the atmosphere, and with it there were hurled upwards a number of

dark fragments, which rose to the height of 400 or 500 feet above the

crater, describing curves in their course, and then falling back upon

the mountain. Most of these fragments tumbled into the crater with a

loud, rattling noise, but some of them fell outside the crater, and a

few rolled down the steep slope of the Sciarra into the sea. Some of

these falling fragments were found to be still hot and glowing, and in

a semi-molten condition, so that they readily received the impression

of a coin thrust into them.

[Illustration: Fig. 4.--The Crates of Stromboli as viewed from the side

of the Sciarra during an eruption on the morning of April 24, 1874.]

[Sidenote: APERTURES AT THE BOTTOM OF THE CRATER.]

But on the upper side of the crater, at the point marked 6, on the

section fig. 3, there exists a spot from which we can look down upon

the bottom of the crater, and view the operations taking place there.

This is the place where Spallanzani and other later investigators have

carried on their observations, and, when the wind is blowing from

the spectator towards the crater, he may sit for hours watching the

wonderful scene displayed before him. The black slaggy bottom of the

crater is seen to be traversed by many fissures or cracks, from most

of which curling jets of vapour issue quietly, and gradually mingle

with and disappear in the atmosphere. But besides these smaller cracks

at the bottom of the crater, several larger openings are seen, which

vary in number and position at different periods; sometimes only one of

these apertures is visible, at others as many as six or seven, and the

phenomena presented at these larger apertures are especially worthy of

careful investigation.

These larger apertures, if we study the nature of the action taking

place at them, may be divided into three classes. From those of the

first class, steam is emitted with loud, snorting puffs, like those

produced by a locomotive-engine, but far less regular and rhythmical

in their succession. In the second class of apertures masses of molten

material are seen welling out, and, if the position of the aperture

be favourable, flowing outside the crater; from this liquid molten

mass steam is seen to escape, sometimes in considerable quantities.

The openings of the third class present still more interesting

appearances. Within the walls of the aperture a viscid or semi-liquid

substance is seen slowly heaving up and down. As we watch the seething

mass the agitation within it is observed to increase gradually, and at

last a gigantic bubble is formed which violently bursts, when a great

rush of steam takes place, carrying fragments of the scum-like surface

of the liquid high into the atmosphere.

If we visit the crater by night, the appearances presented are found to

be still more striking and suggestive. The smaller cracks and larger

openings glow with a ruddy light. The liquid matter is seen to be red-

or even white-hot, while the scum or crust which forms upon it is of a

dull red colour. Every time a bubble bursts and the crust is broken up

by the escape of steam, a fresh, glowing surface of the incandescent

material is exposed. If at these moments we look up at the vapour-cloud

covering the mountain, we shall at once understand the cause of the

singular appearances presented by Stromboli when viewed from a distance

at night, for the great masses of vapour are seen to be lit up with a

vivid, ruddy glow, like that produced when an engine-driver opens the

door of the furnace and illuminates the stream of vapour issuing from

the funnel of his locomotive.

Let us now endeavour to analyse the phenomena so admirably displayed

before us in the crater of Stromboli. The three essential conditions

on which the production of these phenomena seems to depend are the

following: first, the existence of certain apertures or cracks

communicating between the interior and the surface of the earth;

secondly, the presence of matter in a highly heated condition beneath

the surface; and thirdly, the existence of great quantities of water

imprisoned in the subterranean regions--which water, escaping as steam,

gives rise to all those active phenomena we have been describing.

[Sidenote: CAUSE OF THE GLOWING LIGHT.]

We have said, at the outset, that there exists no analogy whatever

between the action which takes place in volcanoes and the operation of

burning or combustion. Occasionally, it is true, certain inflammable

substances are formed by the action going on within the volcano, and

these inflammable substances, taking fire, produce real flames. Such

flames are, however, in almost all cases only feebly luminous, and do

not give rise to any conspicuous appearances. What is usually taken for

flame during volcanic eruptions is simply, as we have already pointed

out, the glowing red-hot surface of a mass of molten rock, reflected

from a vapour-cloud hanging over it. The red glow observed over a

volcano in eruption is indeed precisely similar in its nature and

origin to that which is seen above London during a night of heavy fog,

and which is produced by the reflection of the gas-lights of the city

from the innumerable particles of water-vapour diffused through the

atmosphere. Fires, of course, occur when the molten and incandescent

materials poured out from a volcano come in contact with inflammable

substances, such as forests and houses, but in these cases the

combustion is quite a secondary phenomenon.

There is another popular delusion concerning volcanic action, which it

may be necessary to refer to and to combat. From the well-known fact

that sulphur or brimstone is found abundantly in volcanic regions, the

popular belief has arisen that this highly inflammable substance has

something to do with the production of the eruptions of volcanoes. In

school-books which were, until comparatively recent years, in constant

use in this country, the statement may be found that by burying certain

quantities of sulphur, iron-pyrites, and charcoal in a hole in the

ground, we may form a miniature volcano, and produce all the essential

phenomena of a volcanic eruption. No greater mistake could possibly be

made. The chemical reactions which take place when sulphur and other

substances are made to act upon each other differ entirely from the

phenomena of volcanic action. The sulphur which is found in volcanic

regions is the result and not the cause of volcanic action. Among the

most common substances emitted from volcanic vents along with the steam

are the two gases, sulphurous acid and sulphuretted hydrogen. When

these two gases come into contact with one another, chemical action

takes place, and the elements contained in them--oxygen, hydrogen,

and sulphur--are free to group themselves together in an entirely new

fashion; the consequence of this is that water and sulphuric acid (oil

of vitriol) are formed, and a certain quantity of sulphur is set free.

The water escapes into the atmosphere, the sulphuric acid combines with

lime, iron, or other substances contained in the surrounding rocks,

and the sulphur builds up crystals in any cavities which may happen to

exist in these rocks.

[Sidenote: VOLCANIC ACTION RESEMBLES BOILING.]

If, however, careful and exact observations, like those carried on

at Stromboli, compel us to reject the popular notions concerning

the supposed resemblance between volcanic action and the combustion

of sulphur or other substances, they nevertheless suggest analogies

with certain other simple and well-known operations. And in pursuing

these analogies, we are led to the recognition of some admirable

illustrations both of the attendant phenomena and of the true cause of

volcanic outbursts.

No one can look down on the mass of seething material in violent

agitation within the fissures at the bottom of the crater of Stromboli,

without being forcibly reminded of the appearances presented by liquids

in a state of boiling or ebullition. The glowing material seems to be

agitated by two kinds of movements, the one whirling or rotatory, the

other vertical or up-and-down in its direction. The fluid mass in this

way appears to be gradually impelled upwards, till it approaches the

lips of the aperture, when vast bubbles are formed upon its surface,

and to the sudden bursting of these the phenomena of the eruption are

due.

Now if we take a tall narrow vessel and fill it with porridge or

some similar substance of imperfect fluidity, we shall be able, by

placing it over a fire, to imitate very closely indeed the appearances

presented in the crater of Stromboli. As the temperature of the mass

rises, steam is generated within it, and in the efforts of this steam

to escape, the substance is set in violent movement. These movements of

the mass are partly rotatory and partly vertical in their direction; as

fresh steam is generated in the mass its surface is gradually raised,

while an escape of the steam is immediately followed by a fall of the

surface. Thus an up-and-down movement of the liquid is maintained, but

as the generation of steam goes on faster than it can escape through

the viscid mass, there is a constant tendency in the latter to rise

towards the mouth of the vessel. At last, as we know, if heat continues

to be applied to the vessel, the fluid contents will be forced up to

its edge and a catastrophe will occur; the steam being suddenly and

violently liberated from the bubbles formed on the surface of the mass,

and a considerable quantity of the material forcibly expelled from

the vessel. The suddenness and violence of this catastrophe is easily

accounted for, if we bear in mind that the escaping steam acts after

the manner of a compressed spring which is suddenly released. Steam

is first formed at the bottom of the vessel which is in contact with

the fire; but here it is under the pressure of the whole mass of the

liquid, and moreover, the viscidity of the substance tends to retard

the union of the steam bubbles and their rise to the surface of the

mass. But when the pressure is relieved by the bursting of bubbles at

the surface, the whole of the generated steam tends to escape suddenly.

[Sidenote: ESCAPE OF STEAM-BUBBLES FROM LAVA.]

Now within the crater of Stromboli we have precisely the necessary

conditions for the display of the same series of operations. In the

apertures at the bottom there exists a quantity of imperfectly fluid

materials at a higher temperature, containing water entangled in its

mass. As this water passes into the state of steam it tends to escape,

and in so doing puts the whole mass into violent movement. When the

steam rises to the surface, bubbles are formed, and the formation of

these bubbles is promoted by the circumstance that the liquid mass,

where exposed to the atmosphere, becomes chilled, and thereby rendered

less perfectly fluid. By the bursting of these bubbles the pressure is

partially relieved, and a violent escape of the pent-up steam takes

place through the whole mass. Equilibrium being thus restored, there

follows a longer or shorter interval of quiescence, during which steam

is being generated and collected within the mass, and the series of

operations which we have described then recommences.

There is one other consideration which must be borne in mind in

connection with this subject. It is well known that if water be

subjected to sufficiently great pressure it may be raised to a very

high temperature and still retain its liquid condition. When this

pressure is removed, however, the whole mass passes at once into the

condition of steam or water-gas; and the gas thus formed at high

temperatures has a proportionably high tension. In a Papin's digester

water confined in a strong vessel is raised to temperatures far above

its ordinary boiling-point, and from any opening in such a vessel the

steam escapes with prodigious violence. Now, at considerable depths

beneath the earth's surface, and under the pressure of many hundreds

or thousands of feet of solid rock, water still retaining its liquid

condition may become intensely heated. When the pressure is relieved by

the formation of a crack or fissure in the superincumbent mass of rock,

the escape of the superheated steam will be of very violent character,

and may be attended with the most striking and destructive results. In

the existence of high temperatures beneath the earth's surface, and the

presence in the same regions of imprisoned water capable of passing

into the highly elastic gas which we call steam, we have a cause fully

competent to produce all the phenomena which we have described as

occurring at Stromboli.

It may at first sight appear that the grand and terrible displays

of violence witnessed during a great volcanic eruption differ

fundamentally in their character and their origin from those feeble

outbursts which we are able to examine closely and analyse rigorously

at Stromboli. But that such is not the case a few simple considerations

will soon convince us.

[Sidenote: STROMBOLI COMPARED WITH VESUVIUS.]

Although Stromboli usually displays the subdued and moderate activity

which we have been describing, yet the intensity of the action going

on within it is subject to considerable variation. Occasionally the

violence of the outbursts is greatly increased--the roaring of the

steam-jets may be heard for many miles around, considerable streams of

incandescent liquefied rock flow down the Sciarra into the sea, and the

explosions in the crater are far more frequent and energetic, cinders

and fragments of rock being scattered all over the island and the

surrounding seas.

On the other hand, volcanoes like Vesuvius, which are sometimes the

scene of eruptions on the very grandest scale, at others subside into a

temporary state of moderate activity quite similar in character to that

which is the normal condition of Stromboli. Thus, shortly before the

great eruption of Vesuvius in April 1872, a small cone was formed near

the edge of the crater, and during some months observers could watch,

in ease and safety, a series of small explosions taking place, quite

similar in their character and attendant phenomena to those which we

have described as occurring at Stromboli. French geologists are in the

habit of defining the condition of activity in a volcano by speaking

of the more quiet and, regular state as the 'Strombolian stage,' and

the more violent and paroxysmal as the 'Vesuvian stage'; but the two

conditions are, as we have seen, presented by the same volcano at

different periods, and pass into one another by the most insensible

gradations.

We must now proceed to compare the grand and terrible appearances

presented during a great eruption with those more feeble displays which

we have been describing, to show that in all their essential features

these different kinds of outbursts are identical with one another, and

must be referred to the action of similar causes.

The volcanic eruption which has been most carefully studied in recent

times is that which we have already referred to as occurring at

Vesuvius, in the month of April 1872. With the exception, perhaps, of

that which took place in October 1822, this eruption was the grandest

which has broken out at Vesuvius during the present century. Owing to

the circumstance of its proximity to the great city of Naples, Vesuvius

has always been the most carefully watched of all volcanoes, and in

recent years the erection of an observatory, provided with instruments

for recording the smallest subterranean tremors affecting the mountain,

has facilitated the carrying on of those continuous and minute

observations which are so necessary for exact scientific inquiry.

[Illustration: Fig 5. Vesuvius in Eruption, as seen from Naples, April

26, 1872. (_From a photograph_)]

[Sidenote: VESUVIUS ERUPTION OF 1872.]

On the occasion of this outburst, the aid of instantaneous photography

was first made available for obtaining a permanent record of the

appearances displayed at volcanic eruptions. In fig. 5 we have one of

these photographs, which was taken at 5 o'clock P.M. on April 26, 1872,

transferred to a wood-block and engraved. In examining it we feel sure

that we are not being misled by any exaggeration or error on the part

of the artist. Vesuvius rises to the height of nearly 4,000 feet above

the level of the sea, and an inspection of the photograph proves that

the vapours and rock-fragments were thrown to the enormous height of

20,000 feet, or nearly four miles, into the atmosphere.

The main features of this terrifying outburst were as follows. For

more than a twelvemonth before, the activity of the forces at work

within the mountain appeared to be gradually increasing, and the great

eruption commenced on April 24, attained its climax on the 26th, and

began to die out on the following day. During the eruption the bottom

of the crater was entirely broken up, and the sides of the mountain

were rent by fissures in all directions. So numerous were these

fissures and cracks that liquid matter appeared to be oozing from every

part of its surface, and, as Professor Palmieri, who witnessed the

outburst from the observatory, expressed it, 'Vesuvius sweated fire.'

One of the fissures was of enormous size, extending from the summit to

far beyond the base of the cone; the scar left by this gigantic rent

being plainly visible at the present day.

From the great opening or crater at the summit, and from some of the

fissures on the sides of the mountain, enormous volumes of steam rushed

out with a prodigious roaring sound, the noise being so terrific that

the inhabitants of Naples, five miles off, fled from their houses

and spent the night in the open streets. Although this roaring sound

appeared at a distance to be continuous, yet those upon the mountain

could perceive that it was produced by detonations or explosions

rapidly following one another. Each of these explosions was accompanied

by the formation of a great globe of white vapour, which, rising into

the atmosphere, swelled the bulk of the vast cloud overhanging the

mountain. An inspection of the photographs (see fig. 5) shows that the

great vapour-cloud over Vesuvius was made up of the globular masses

ejected at successive explosions. Each of these explosive upward

rushes of steam carried along with it a considerable quantity of solid

fragments, and these fell in great numbers all over the surface of

the mountain, breaking the windows of the observatory, and making it

dangerous to be out of doors.

We have said that lava, or molten rock, appeared to be issuing from

the very numerous cracks formed all over the flanks of the mountain.

But at three points this molten rock issued in such quantities as to

form great, fiery floods, which rushed down the sides of the mountain,

and flowed to a considerable distance beyond its base. The largest

of these lava-floods overwhelmed and destroyed the two villages of

Massa di Somma and San Sebastiano, besides many country houses in the

neighbourhood.

[Sidenote: STEAM EMITTED FROM LAVA-CURRENT.]

A very marked and interesting feature exhibited by these three

lava-floods was the quantity of watery vapour which they gave off

during their flow. All along their course, enormous volumes of steam

were evolved from them, as will be seen by an inspection of the

photograph. Indeed, such was the abundance and tension of the steam

thus escaping from the surfaces of the lava-currents that it forced

the congealing rock up into great bubbles and blisters, and gave rise

to the formation of innumerable miniature volcanoes, varying in size

from a beehive to a cottage, some of which remained in a state of

independent activity for a considerable time.

So far, what we have described as taking place at Vesuvius, in April

1872, has been only the repetition on a £Eur grander scale of the

three kinds of action which we have shown to be constantly taking

place at Stromboli; namely, the formation of cracks or fissures in the

earth's surface, the escape of steam with explosive violence from these

openings, often propelling rock-fragments into the atmosphere, and the

outwelling, under the influence of this compressed steam, of masses of

molten materials.

There were some other appearances presented at the great outburst at

Vesuvius, which do not seem at first sight to find any analogies in

the manifestations of the more feeble action continually going on at

Stromboli.

Before and during the great outbreak of April 1872, Vesuvius itself

and the whole country round were visited with earthquake-shocks, or

tremblings of the ground. The sensitive instruments in the Vesuvian

Observatory showed the mountain daring the eruption to be in a constant

state of tremor. These earthquakes are not, as is commonly supposed,

actual upheavings of the earth's surface, but are vibrations propagated

through the solid materials of which the earth is built up. We cannot

stamp our feet upon the ground without giving rise to such vibrations,

though our senses may not be sufficiently acute to perceive them.

The explosive escape of steam from a crack is a cause sufficiently

powerful to produce a shock which is propagated and may be felt for

a considerable distance round. Even on Stromboli an observer at the

edge of the crater may notice that each explosive outburst of steam

is accompanied by a perceptible tremor of the ground, and in the case

of Vesuvius the violent shocks produced by the escape of far larger

volumes of steam give rise to proportionately stronger vibrations. The

nature and origin of those far more terrible and destructive shocks

which sometimes accompany, and more frequently precede, great volcanic

eruptions, we shall consider in the sequel.

[Sidenote: CAUSE OF LIGHTNING DURING ERUPTIONS.]

Another striking phenomenon which was exhibited in the great eruption

of Vesuvius in 1872 was the vivid display of lightning accompanied

by thunder. The uprushing current of steam and rock-fragments forms

a vertical column, but as the steam condenses it spreads out into a

great horizontal cloud which is seen to be made up of the great globes

of vapour emitted at successive explosions. When there is little or

no wind the vertical column with a horizontal cloud above it bears a

striking resemblance to the stone-pine trees which form so conspicuous

a feature in every Neapolitan landscape. Around this column of vapour

the most vivid lightning constantly plays and adds not a little to the

grand and awful character of the spectacle of a volcanic eruption,

especially when it is viewed by night.

In the eruption of 1872 a strong wind blowing from the north-west

destroyed the usual regular appearance of this 'pine-tree appendage' to

the mountain, which is so well known to, and dreaded by the inhabitants

of Naples; the cloud, as will be seen from the photograph (fig. 5,

_facing_ p. 24), was blown on one side, and most of the falling

fragments took the same direction.

It is well known that when high-pressure steam is allowed to escape

through an orifice, electricity is abundantly generated by the

friction, and Sir William Armstrong's hydro-electric machine is

constructed on this principle. Every volcano in violent eruption is

a very efficient hydro-electric machine, and the uprushing column

is in a condition of intense electrical excitation. This result is

probably aided by the friction of the solid particles as they are

propelled upwards and fall back into the crater. The restoration of

the condition of electrical stability between this column and the

surrounding atmosphere is attended with the production of frequent

lightning-flashes and thunder-claps, the found of the latter being

usually, however, drowned in the still louder roar of the uprushing

steam-column.

The discharge of Buch large quantities of steam into the atmosphere

soon causes the latter to be saturated with watery vapour, and there

follows an excessive rainfall; long-continued rain and floods were an

accompaniment of the great Vesuvian outbreak of 1872, as they have

been of almost all great volcanic eruptions. The Italians, indeed,

dread the floods which follow an eruption more than the fiery streams

of lava which accompany it--for they have found the mud-streams (_lave

di fango_), formed by rain-water sweeping along the loose volcanic

materials, to be more widely destructive in their effects than the

currents of molten rock (_lave di fuoco_).

Besides the phenomena which we have now described as accompanying a

great volcanic outburst, many others have undoubtedly been recorded

by apparently trustworthy authorities. But, in dealing with the

descriptions of these grand and terrible events, we must always be on

our guard against accepting as literal facts, the statements made by

witnesses, often writing at some distance from the scene of action, and

almost always under the influence of violent excitement and terror.

The desire to administer to the universal love of the marvellous, and

the tendency to exaggeration, will usually account for many of the

wonderful statements contained in such records; and, even where the

witness is accurately relating events which he thinks passed before his

eyes, we must remember that it is probable he may have had neither the

opportunity nor the capacity for exact observation.

The more carefully we sift the accounts which have been preserved of

great volcanic outbursts, the more are we struck by the fact that the

appearances described can be resolved into a few simple operations, the

true character of which has been distorted or disguised by the want of

accurate observation on the part of the witnesses.

[Sidenote: SIMILARITY OF FEEBLE AND VIOLENT ERUPTIONS.]

We are thus led to the conclusion that the grand and terrible

appearances displayed at Vesuvius and other volcanoes in a state of

violent eruption do not differ in any essential respect from the

phenomena which we have witnessed accompanying the miniature outbursts

of Stromboli. And we are convinced, by the same considerations, that

the forces which give rise to the feeble displays in the latter case

would produce, if acting with greater intensity and violence, all the

magnificent spectacles presented in the former.

In Vesuvius and Stromboli alike, the active cause of all the phenomena

exhibited is found to be the escape of steam from the midst of

masses of incandescent liquefied rock. The violence, and therefore

the grandeur and destructive effects of an eruption, depend upon the

abundance and tension of this escaping steam.

There is one respect in which volcanic phenomena are especially

calculated to excite the fear and wonder of beholders--namely, in the

sudden and apparently spontaneous character of their manifestations.

Eclipses were regarded as equally portentous with volcanic eruptions

till astronomers learned not only to explain the causes which gave

rise to them, but even to predict to the second the times of their

occurrence. If we were able in like manner to warn the inhabitants of

volcanic regions of the approach of a grand eruption, the fear and

superstition with which these events are now regarded would doubtless

be in great part dispelled. The power of prediction is alike the

crucial test and the crowning triumph of a scientific theory.

But, although natural philosophers are able to assign the causes to

which the grand operations of volcanoes are due, and also to explain

all the varied appearances which accompany them, they have not as yet

so far mastered the laws which govern volcanic action as to be able to

predict the periods of their manifestation.

That these operations, like all others going on upon the globe, are

governed by great natural laws we cannot for a moment doubt. And that,

in all probability, more careful and exact observation and reasoning

will at some future time lead us to the recognition of these laws,

every student of nature is sanguine. But at the present time, it must

be confessed, we are very far indeed from being able to afford that

crowning proof of the truth of our theories of volcanic action which is

implied in the power of predicting the period and degree of intensity

of their manifestations.

[Sidenote: ERUPTIONS AND THE INTERVALS BETWEEN THEM.]

There are, however, some observations which lead us to hope that the

time may not be far distant when we shall have so £Eur obtained a

knowledge of the conditions on which volcanic action depends as to be

able to form some judgment as to its manifestations in the future at

any particular locality. But we must recollect that these conditions

axe very numerous and complicated, and that some of them may lie almost

entirely outside our sphere of observation; hence hasty attempts in

this direction, such as have recently been made, are to be deprecated

by every true lover of science.

Concerning the eruptions that have taken place at those volcanic

centres which have been known from a remote antiquity, we have records

from which we can determine the intervals separating these outbursts

and their relative violence. A critical examination of these records

leads to the following conclusions:--

(1.) A long period of quiescence is generally followed by an eruption

which is either of long duration or of great violence.

(2.) A long-continued, or very violent eruption is usually followed by

a prolonged period of repose.

(3.) Feeble and short eruptions usually succeed one another at brief

intervals.

(4.) As a general rule, the violence of a great eruption is inversely

proportional to its duration.

It will be seen that these general conclusions are in perfect harmony

with the theory that volcanic outbursts are due to the accumulation

of steam at volcanic centres, and that the tension of this imprisoned

gas eventually overcomes the repressing forces which tend to prevent

its manifestation. Before astronomers had learnt to determine all

the conditions on which the production of eclipses depends, they had

found that these phenomena succeed one another at regular intervals.

The discovery of such astronomical cycles was a great advance in our

knowledge of the heavenly bodies, and in the same way the determination

of these general relations between the intensity and duration of

volcanic outbursts and the intervals of time which separate them may

be regarded as the first step towards the discovery of the laws which

govern volcanic activity.

In the actual determination of the conditions upon which the occurrence

of volcanic eruptions depends, it must be confessed, however, that

very little has as yet been done. This is in part due to the fact that

some at least of these conditions lie beyond the limits of direct

observation. But it must also be admitted, on the other hand, that

little has been as yet accomplished towards the careful and systematic

observation of those phenomena which may, and probably do, exert an

influence in bringing about volcanic outbursts.

[Sidenote: INFLUENCE OF ATMOSPHERIC CONDITIONS.]

In the Lipari Islands there has prevailed a belief, from the very

earliest period of history, that the feeble eruptions of Stromboli

are in some way dependent upon the condition of the atmosphere.

These islands were known to the ancients as the Æolian Isles, from

the fact that they were once ruled over by a king of the name of

Æolus. It seems not improbable that Æolus was gifted with natural

powers of observation and reasoning far in advance of those of his

contemporaries. A careful study of the vapour-cloud which covers

Stromboli would certainly afford him information concerning the

hygrometric condition of the atmosphere; the form and position

assumed by this vapour-cloud would be a no less perfect index of the

direction and force of the wind; and, if the popular belief be well

founded, the frequence and violence of the explosions taking place

from the crater would indicate the barometric pressure. From these

data an acute observer would be able to issue 'storm-warnings' and

weather-prognostics of considerable value. In the vulgar mind, the

idea of the prediction of natural events is closely bound up with that

of their production; and the shrewd weather-prophet of Lipari was

after his death raised to the rank of a god, and invested with the

sovereignty of the winds.

Whether the popular idea that the outbursts of Stromboli are regulated

by atmospheric conditions has any foundation is still open to grave

doubt. It seems to be certain, however, that during autumn and winter

the more violent paroxysms of the volcano occur, and that in summer

the action which takes place is far more regular and equable. It would

be of the greatest benefit to science if an observatory were erected

beside the crater of Stromboli, where a careful record might be kept of

all atmospheric changes, and of the synchronous manifestations of the

volcanic forces.

A little consideration will show that it is a by no means unreasonable

supposition that variations in atmospheric pressure may exercise a very

important influence in bringing about volcanic outbursts. Changes in

the barometer to the extent of two inches within a very short period

are not uncommon occurrences. A very simple calculation will show that

the fall of the mercury in the barometer to the extent of two inches

indicates the removal of a weight of two millions of tons from each

square mile of the earth's surface where this change takes place. Now,

if we suppose, as we have good ground for doing, that under volcanic

areas vast quantities of superheated water are only prevented from

flashing into steam by the superincumbent pressure, a relief of this

pressure to the extent of two millions of tons on every square mile

could scarcely fail to produce very marked effects. The way in which

explosions in fiery coal-mines generally follow closely upon sudden

falls in the atmospheric pressure is now well known; and coal-mine

explosions and volcanic outbursts have this in common, that both

result from the sudden and violent liberation of subterranean gases.

There are not a few apparently well-authenticated accounts of volcanic

and earthquake phenomena following closely on peculiar atmospheric

conditions, and the whole question of the relation of the volcanic

forces to atmospheric pressure, as Spallanzani himself so long ago

pointed out, is deserving of a most careful and rigorous investigation.

[Sidenote: SUPPOSED TIDAL EFFECTS.]

There is one other consideration which has frequently been urged as

worthy of especial attention, in dealing with the question of the

exciting causes of volcanic outbursts. If volcanoes were, as was at one

time almost universally supposed, in direct communication with a great

central mass of liquefied materials, or even if any large reservoirs

of such liquids existed beneath volcanic districts, as others have

imagined, then the different mobility of the solid and liquid portions

of the earth's mass would give rise to tidal effects similar to those

occurring in the surface waters of the globe. Under such circumstances,

volcanic outbursts, like the tides, would be determined by the relative

positions of the sun and moon to our globe. It is certain, however,

that no very direct relation has yet been established between the

lunar periods and those of volcanic outbursts, though recent close

observations upon the crater of Vesuvius, by Professor Palmieri, do

seem to lend support to the view that such relations may exist.

At the present time, therefore, it must be admitted that vulcanologists

have only just commenced those series of exact and continuous

observations which are necessary to determine the conditions that

regulate the appearance of volcanic phenomena. The study of the laws

of volcanic action is yet in its infancy. But the establishment of

observatories on Vesuvius and Etna 18 fall of promise for the future,

and when we consider the advances which have been made, during the last

one hundred years, in our knowledge of the true nature of volcanic

action, we need not despair that the extension of the same methods

of inquiry will lead to equally important results concerning the

conditions which determine and the laws which govern it.

In the meanwhile, it is no small gain to have established the fact that

volcanic phenomena, divested of all those wonderful attributes with

which superstition and the love of the marvellous have surrounded them,

are operations of nature obeying definite laws, which laws we may hope

by careful observation and accurate reasoning to determine; and that

the varied appearances, presented alike in the grandest and feeblest

outbursts, can all be referred to one simple cause--namely, the escape,

from the midst of masses of molten materials, of imprisoned steam or

water-gas.

Volcanoes: What They are and What They Teach · 第 2 / 12 章