CHAPTER X

ON SOME OF THE PHENOMENA OF GLACIERS, WITH SPECIAL REGARD TO THOSE OF

NEW ZEALAND

_The cause of glaciers_—_Formation and

structure_—_Motion_—_Moraines_: _Lateral_, _medial_, _and

terminal_—_‘Surface’ moraines_—_Crevasses_—_Moulins_—_Glacier

cones_—_Glacier tables_—_Surface torrents_—_Avalanches_—_Cornices_

In a work of this nature it may not be out of place to briefly describe

some of those interesting features and phenomena which accompany the

world above the snow-line.

Here is a quotation from a recent review of Professor Heim’s work[2] by

a prominent member of the English Alpine Club:—

‘Some thirty years ago a systematic _résumé_ of all that was known up

to that date about existing glaciers appeared in the work of Professor

Albert Mousson, “Die Gletscher der Jetztzeit,” since which, with

perhaps the exception of Major Hüber’s “Les Glaciers,” no attempt

has been made to collect into a focus the light which numerous able

observers and theorists have subsequently thrown upon the question. The

intricacy of the problem has, indeed, increased almost in proportion to

our enlarged knowledge of its conditions; and in spite of the labours

of a large and very distinguished body of investigators, not only do

many important points remain matters of dispute, but the very materials

for a complete solution are still wanting.’

[Footnote 2: _Handbuch der Gletscherkunde_, von Dr. Albert Heim, Zürich

(Stuttgart: Verlag von J. Engelhorn, 1885, 18 francs.)]

CAUSE OF GLACIERS

The joint cause of glaciers is precipitation and cold. A low

temperature alone can do nothing without moisture, and this fact

quickly disposes of the popular notion that glaciers invariably exist

in cold countries. Thibet, for instance, and also some parts of Arctic

North America are destitute of ice streams, though eternal cold may be

said to reign supreme in these parts.

Imagine for a moment the higher mountains clear of snow and ice, and

then watch for the formation of a glacier. Snow falls and fills up all

the valleys and gullies, avalanches descend from the higher parts, and

a great accumulation gathers in all hollows. By constant repetition

of snow-falls (always provided a greater quantity is deposited than

can be melted by the sun’s rays and by the natural warmth of the

earth’s crust) great pressure is put upon the lower portions by the

superincumbent accumulation, and aided by the infiltration of water and

refreezing (or ‘regelation’ as the correct term is), a large body of

ice is formed which at once begins to move down the valleys containing

it.

GLACIER ICE

Glacier ice is not like the solid blue ice on the surface of water,

but consists of granules joined together by an intricate network of

capillary water-filled fissures.

In exposed sections and upon the surface of the ice can be observed

a ‘veined’ or ‘banded’ structure—veins of a denser blue colour

alternating with those of a lighter shade containing air bubbles.

The cause of this peculiar structure has been the subject of much

theorising amongst investigators, but hitherto I believe the greatest

authorities consider that the explanation of the phenomenon is yet

wanting.

GLACIER MOTION

The motion of glaciers is yet another bone of contention, but it

is generally admitted that the cause of it is to be found mainly

in gravitation, and is also partially accounted for by the strange

property of ‘viscosity’ in what appears to the casual observer to be

nothing more or less than a rigid solid.

Recently observations for ascertaining the rate of progress of the

Tasman, Murchison, Hooker, and Mueller Glaciers have been made by the

New Zealand Government Survey Department. Some of the results were

embodied in a paper by Mr. J. H. Baker, the Chief Surveyor of the

Provincial District of Canterbury, and will appear in the ‘Transactions

of the Australasian Association for the Advancement of Science’ for

1891. At the late meeting of that body a committee was appointed to

further these investigations, and a sum of 25_l._ voted for the aid of

the same.

Before long, therefore, there will be put before the scientific public

reliable measurements of the motion of several of the largest and

least-known glaciers in temperate regions.

MORAINES

There is a remarkable feature of the glaciers of this country which

stamps them as unique in one respect—I refer to the very extensive

moraines. I write feelingly of this, for my acquaintance with them has

been a very close one, and they have impressed me very deeply—in more

ways than one.

The large glaciers of which I have written in this work are completely

moraine-covered over their lower parts.

‘SURFACE’ MORAINES

Moraines may be divided into four sections: ‘Lateral’ moraines,

fringing the sides of the glaciers, their outlying portions often being

‘dead’—that is, at present unmoved by the action of the ice, and

forming banks, as it were, for the ice stream to flow between; ‘medial’

moraines, which begin at the junction of two streams of ice and often

continue for many miles to the terminal face; ‘terminal’ moraines,

formed by the depositing of detritus at the melting point or end of the

glacier; and, lastly, ‘surface’ moraines (so called by Professor Hutton

of Christchurch, N.Z.), which are the combined accumulations of the

first two divisions in the lower parts of the glacier.

It is these ‘surface’ moraines that are such a characteristic feature

of the glaciers situate on the eastern side of the chain in New

Zealand. Of those on the western side I am not able to speak with

authority, never having visited them myself; but I understand that

they do not carry such a large quantity of detritus as those of the

eastern slopes.

This disparity remains to be accounted for and awaits an explanation.

I have a theory of my own upon the subject, which, however, as yet I

would not like to put too strongly forward.

On both sides of Mount Cook, on Mount De la Bêche (ten miles further

along the chain), and on a peak just north of the Hochstetter Dome (ten

miles still further north) I have observed enormous exposed sections of

the rock strata, which in each case dip at a steep angle _from east to

west_, presenting slab faces, not easily disturbed by the action of the

frost, to the westward, but broken and fast denuding faces (‘basset’

faces, as they are geologically termed) to the eastward. I am hoping at

some future time to further investigate this interesting subject.

As the western glaciers, however, must descend steeper valleys than the

eastern, I make no doubt that their rate of progress will be eventually

ascertained to be greater than that of the latter, and this would

militate largely against an accumulation of moraine _upon the ice_.

THE SURFACE OF A GLACIER

All sorts of queer notions as to what the surface of a glacier is like

exist. Indeed I have often heard people inquire if it would be possible

_to skate upon it_!

Let us for a moment imagine ourselves at the head of the great Tasman

Glacier, 8,600 feet above sea-level. All around us is snow, either

freshly fallen or merging into _névé_. We begin to walk down, and

at first, upon the steeper slopes, cross a few large crevasses and

_bergschrunds_ by means of snow bridges; then, as the incline becomes

less steep, we walk for six miles or so upon a smooth surface of

_névé_, or perchance knee-deep in fresh snow, and scarcely a crevasse

exists. At the beginning of the great turn we gradually leave the

_névé_ and find ourselves upon hard, white ice, and soon transverse

crevasses appear; these are a little further on cut by longitudinal

crevasses forming the surface into huge squares, not flat on the top,

but hummocky. A perfect network of crevasses cuts up the whole of the

surface, but those parts on the outside of the curve are infinitely

more disturbed than those on the inside, owing to the tension put upon

them by the faster rate at which they have to move. After rounding the

turn the glacier again consolidates and few crevasses appear, only the

surface is covered with old wounds—if I may coin such a term—from the

rents which have occurred at the turn, and presents a very undulating

appearance. The little gullies are formed into watercourses and

intersect the glacier in all directions. On our right, now, is the

medial moraine formed by detritus from Mount De la Bêche, brought down

partly by the Tasman and partly by the Rudolf Glaciers, and it stands

up 100 feet or so above the surface of the clear ice on either side of

it, owing to the protection from the sun’s rays afforded by it to the

ice beneath, so preventing ‘ablation’ or waste going on so quickly. We

follow down for another four or five miles, and then cross this moraine

(which has in the meantime joined that on the northern side of the

Hochstetter Glacier) on to the Hochstetter on our right.

SURFACE TORRENTS AND MOULINS

We are now immediately below the great ice-fall, and the surface

of the glacier presents an appearance not unlike the back of some

enormous caterpillar wrinkled transversely by crevasses, which close

up as we proceed downwards, and furrowed longitudinally by two large

or main watercourses whose icy banks are in places 100 feet above

their respective torrents. These two small rivers are fed from

every direction by minor watercourses, and a mile or two further

down discharge all their contents into crevasses and _moulins_, or

water-shafts in the ice.

GLACIER TABLES AND CONES—THE ACTION OF WARMTH

The locality of the glacier on which we now are is very interesting,

for Nature’s mills are here seen at work day by day. Glacier

tables—blocks of rock perched upon pedestals of ice formed by the

protection from the action of the sun’s warmth—are of frequent

occurrence. Glacier cones—heaps of sand and small fragments of rock

raised by a similar agency (after having been washed to one spot by

water)—are in places all around us. Then, strange and contradictory

as it may seem, we see thousands of holes, each with a stone at the

bottom and filled with the bluest of blue water, formed also in the

first place by the rays of the sun warming the stone and causing it to

sink in the ice. It is well-known in physics that water at 39° Fahr.

is at its heaviest, and as soon as the warm stone—the dark colour of

the stone having absorbed more heat than the surrounding ice—begins

to sink the warmer water follows it, whilst that in the neighbouring

temperature of 32° Fahr. rises to the surface and becomes in its turn

re-warmed, and so on. This peculiar current often bores the holes in

the ice to a depth of many feet, and is only checked by a preponderance

of cold. It is the larger stones, therefore, which rise upon the ice,

and the smaller ones which sink.

‘SURFACE’ AND ‘TERMINAL’ MORAINES

We walk on down the ice stream, and soon the moraines on either hand

close in upon us and we find ourselves on a mere wedge of ice, at the

point of which we step on to the ‘surface’ moraine. Here the swearing

begins, and it lasts right on to the terminal face four or five miles

below, for it is one continual repetition of walking on loose and

tumbling rocks, up one hillock, along a ridge, jumping from

Rock to rock with many a shock,

down another hillock, now and then starting a whole avalanche of

many-sided and sharp-edged stones down a treacherous slope of ice,

which we take for a surface deeply covered and sound of footing.

Skate on the surface of a glacier?

‘Not much!’ (as the Colonials say).

AVALANCHES

Very strange notions also exist amongst the uninitiated as to the

nature of avalanches. The popular idea of an avalanche is derived from

heartrending accounts of great sweepings away and annihilation of whole

villages, and few of the general run of people seem to realise that in

Alpine work almost any little descending mass of rock, snow, or ice is

dignified by the name of avalanche. Snow avalanches are most frequent

after fresh falls of snow followed immediately by warm weather, and

after a little experience amongst the mountains one soon learns to

detect their customary tracks. Ice avalanches are mainly caused

through the overhanging portion of ice at the terminals of secondary

glaciers—that is, glaciers which break off before descending to the

valley or to the parent glacier below. The tracks of ice avalanches

are almost invariably unmistakable and are swept night and day without

cessation, and very frequently at regular intervals.

Rock avalanches are more treacherous, and one never knows when to

expect them from above; generally in the early morning the frost

holds the stones above in an icy grip, but as the sun melts the ice

in the chinks the hold is released and a stone will descend into the

_couloirs_ or ditches which scarp the mountain side. If one happens

to be below then it is a case of _sauve qui peut_ and a rush for the

nearest protection, for there is no saying how many tons, or indeed how

many hundreds of tons, of loose rocks or stone may start in a wild and

dusty rattle down the hillside.

But some snow avalanches almost crawl down the _couloirs_, and make a

strange and ever-continued hissing as they move. These are composed of

heavy and sodden snow, and begin after the sun has been up for some

hours, continuing until nightfall. These are not so dangerous on a

gentle slope, and one can often waddle or half glissade down in the

midst of one with perfect safety, though they make one uncomfortably

wet.

CORNICES

Cornices are a frequent source of danger to the mountaineer. They are

formed by the snow drifting over one edge of a ridge and forming a

hanging mass. It is needless to say that one soon learns to walk some

feet away from the outer edge of a cornice, for after poking one’s

axe-handle through three feet of snow, and peeping through a blue hole

down a precipice of perhaps 1,000 feet or so, it is not difficult to

fancy what the result would be should the cornice break.

With Axe and Rope in the New Zealand Alps · 第 10 / 11 章