CHAPTER IX.

THE CAUSE OF THE GLACIAL PERIOD.

In searching for the cause of the Glacial period, it is evident that we

must endeavor to find conditions which will secure over the centre of the

glaciated area either a great increase of snow-fall or a great decrease

in the mean annual temperature, or both of these conditions combined in

greater or less degree. As can be seen, both from the nature of the case

and from the unglaciated condition of Siberia and northern Alaska, a low

degree of temperature is not sufficient to produce permanent ice-fields.

If the snow-fall is excessively meagre, even the small amount of heat in

an arctic summer will be sufficient to melt it all away.

From the condition of Greenland, however, it appears that a moderate

amount of precipitation where it is chiefly in the form of snow may

produce enormous glaciers if at the same time the average temperature

is low. In southeastern Alaska, on the other hand, the glaciers are of

enormous size, though the mean annual temperature is by no means low,

for there the great amount of snow-fall amply compensates for the higher

temperature.

Snow stores the cold and keeps it in a definite place. If the air becomes

chilled, circulation at once sets in, and the cold air is transferred to

warmer regions; but if there is moisture in the air, so that snow forms,

the cold becomes locked up, as it were, and falls to the earth.

The amount of cold thus locked up in snow is enormous. To melt one

cubic foot of ice requires as much heat as would raise the temperature

of a cubic foot of water 176° Fahrenheit. To melt a "layer of ice only

one inch and a half thick would require as much heat as would raise a

stratum of air eight hundred feet thick from the freezing-point to the

tropical heat of 88° Fahrenheit." It is the slowness with which ice melts

which enables it to accumulate as it does, both in winter and upon high

mountains and in arctic regions. Captain Scoresby relates that when near

the north pole the sun would sometimes be so hot as to melt the pitch on

the south side of his vessel, while water was freezing on the north side,

in the shade, owing to the cooling effect of the masses of ice with which

he was surrounded.

Thus it will appear that a change in the direction of the moist winds

blowing from the equator towards the poles might produce a Glacial

epoch. If snow falls upon the ocean it cools the water, but through the

currents, everywhere visible in the sea, the temperature in the water in

the different parts soon becomes equalized. If, however, the snow falls

upon the land, it must be melted by the direct action of the sun and

wind upon the spot where it is. If the heat furnished by these agencies

is not sufficient to do it year by year, there will soon be such an

accumulation that glaciers will begin to form. It is clear, therefore,

that the conditions producing a Glacial period are likely to prove very

complicated, and we need not be surprised if the conclusions to which we

come are incapable of demonstration.

Theories respecting the cause of the Glacial period may be roughly

classified as astronomical and geological. Among the astronomical

theories, one which has sometimes been adduced is that the solar system

in its movement through space is subjected to different degrees of heat

at different times. According to this theory, the temperate climate

which characterised the polar regions during the Tertiary period, and

continued up to the beginning of the Glacial epoch, was produced by the

influence of the warmer stretches of space through which the whole solar

system was moving at that time; while the Glacial period resulted from

the influence upon the earth of the colder spaces through which the

system subsequently moved.

While it is impossible absolutely to disprove this hypothesis, it labors

under the difficulty of having little positive evidence in its favor,

and thus contravenes a fundamental law of scientific reasoning, that we

must have a real cause upon which to rest our theories. In endeavouring

to explain the unknown, we should have something known to start with.

But in this case we are not sure that there are any such variations in

the temperature of the space through which the solar system moves. This

theory, therefore, cannot come in for serious consideration until all

others have been absolutely disproved. As we shall also more fully see,

in the subsequent discussion, the distribution of the ice during the

Glacial period was not such as to indicate a gradual extension of it from

the north pole, but rather the accumulation upon centres many degrees to

the south.

Closely allied with the preceding theory is the supposition broached

by some astronomers that the sun is a variable star, dependent to some

extent for its heat upon the impact of meteorites, or to the varying

rapidity with which the contraction of its volume is proceeding.

It is well known that when two solid bodies clash together, heat is

produced proportionate to the momentum of the two bodies. In other

words, the motion which is arrested is transformed into heat. Mr. Croll,

in his last publication[DR] upon the subject, ingeniously attempted to

account for the gaseous condition of the nebulæ and the heat of the sun

and other fixed stars by supposing it to be simply transformed motion.

According to this theory, the original form of force imparted to the

universe was that exerted in setting in motion innumerable dark bodies,

which from time to time have collided with each other. The effects of

such collisions would be to transform a large amount of motion into

heat and its accompanying forms of molecular force. The violence of the

compact of two worlds would be so great as to break them up into the

original atoms of which they are composed, and the heat set free would

be sufficient to keep the masses in a gaseous condition and cause them

to swell out into enormous proportions. From that time on, as the heat

radiated into space, there would be the gradual contraction which we

suppose is going on in all the central suns, accompanied, of course, with

a gradual decline of the heat-energy in the system.

[Footnote DR: Stellar Evolution and its Relation to Geological Time.]

Now, it is well known that the earth and the solar system in their

onward progress pass through trains of meteorites. The tails of some of

the comets are indeed pretty clearly proved to be streams of ponderable

matter, through which, from time to time, the minor members of the solar

system plunge, and receive some accession to their bulk and weight. The

shooting-stars, which occasionally attract our attention in the sky,

mark the course of such meteorites as they pass through the earth's

atmosphere, and are heated to a glow by the friction with it. It has been

suggested, therefore, that the sun itself may at times have its amount

of heat sensibly affected by such showers of meteorites or asteroids.

Upon this theory the warm period of the Tertiary epoch, for instance,

may have been due to the heat temporarily added to the sun by impact

with minor astronomical bodies. When, afterwards, it gradually cooled

down, receiving through a long period no more accessions of heat from

that source, the way was prepared for the colder epoch of the Glacial

period, which, in turn, was dispelled by fresh showers of meteorites

upon the sun, sufficient to produce the amelioration of climate which we

experience at the present time.

As intimated, this theory is closely allied to the preceding, the

principal difference being that it limits the effects of the supposed

cause to the solar system, and looks to our sun as the varying source of

heat-supply. It has the advantage over that, however, of possessing a

more tangible _vera causa_. Meteorites, asteroids, and comets are known

to be within this system, and have occasional collisions with other

members of it. But the principal objection urged against the preceding

theory applies here, also, with equal force. The accumulations of ice

during the Glacial period were not determined by latitude. In North

America the centre of accumulation was south of the Arctic Circle--a fact

which points clearly enough to some other cause than that of a general

lowering of the temperature exterior to the earth.

The same objections would bear against the theory ably set forth by Mr.

Sereno E. Bishop, of Honolulu, which, in substance, is that there may

be considerable variability in the sun's emission of heat, owing to

fluctuations in the rate of the shrinkage of its diameter, brought about

by the unequal struggle between the diminishing amount of heat in the

interior and the increasing force of the gravitation of its particles,

and by the changes in the enveloping atmosphere of the sun, which, like

an enswathing blanket, arrests a large portion of the radiant heat from

the nucleus, and is itself evidently subject to violent movements, some

of which seem to carry it down to the sun's interior. Unknown electrical

forces, he thinks, may also combine to add an element of variability.

These supposed changes may be compared to those which take place upon

the surface of the earth when, at irregular intervals, immense sheets of

lava, like those upon the Pacific coast of North America, are exuded in a

comparatively brief time, to be succeeded by a long period of rest. The

heat thus brought to the surface of the earth would add perceptibly to

that radiated from it into space in ordinary times. Something similar to

this upon the sun, it is thought, might produce effects perceptible upon

the earth, and account for alternate periods of heat and cold.

A fourth astronomical theory is that there has been a shifting of the

earth's axis; that at the time of the Glacial period the north pole,

instead of being where it now is, was somewhere in the region of central

Greenland. This attractive theory has been thought worthy of attention

by President T. C. Chamberlin and by Professor G. C. Comstock,[DS] but

it likewise labours under a twofold difficulty: First, the shifting of

the poles observed (450 feet per year) is too slight to have produced the

changes within any reasonable time, and it is not likely to have been

continuous for a long period. But still more fatal to the theory is the

fact that the warm climate preceding the Glacial period seems to have

extended towards the present north pole upon every side; a temperate

flora having been found in the fossil plants of the Tertiary beds in

Greenland and northern British America, as well as upon Nova Zembla and

Spitzbergen.

[Footnote DS: See papers by these gentlemen read at the meeting of the

American Association for the Advancement of Science, in Washington, in

August, 1891. Professor Comstock's paper appeared in the American Journal

of Science for January, 1893.]

A fifth astronomical theory, and one which has of late years been

received with great favour, is that so ably advocated by the late Dr.

James Croll and by Professor James Geikie. Following the suggestions

of the astronomer Adhémar, these writers have attempted to show that

not only one Glacial epoch, but a succession of such epochs, has been

produced in the world by the effect of the changes which are known to

have taken place in the eccentricity of the earth's orbit when combined

with the precession of the equinoxes--another calculable astronomical

cause.

[Illustration: Fig. 99.--Diagram showing effect of precession: _A._

condition of things now; _B._ as it will be 10,500 years hence. The

eccentricity is of course greatly exaggerated.]

It is well known that the earth's orbit is elliptical; that is, it is

longer in one direction than in the other, so that the sun is one side

of the centre. During the winter of the northern hemisphere the earth

is now about three million miles nearer the sun than in the summer; but

the summer makes up for this distance by being about seven days longer

than the winter. Through the precession of the equinoxes this state of

things will be reversed in ten thousand five hundred years; at which time

we shall be nearer the sun during our northern summer, and farther away

in winter, our winter then being also longer than our summer. Besides,

through the unequal attraction of the planets the eccentricity of the

earth's orbit periodically increases and diminishes, so that there have

been periods when the earth was ten million five hundred thousand miles

farther from the sun in winter than in summer; at which times, also,

the winter was nearly twenty-eight days longer than the summer. Such an

extreme elongation of the earth's orbit occurred about two hundred and

fifty thousand years ago.

It is easy to assume that such a change in astronomical conditions would

produce great effects upon the earth's climate; and equally easy to

connect with those effects the vast extension of ice during the Glacial

period. Since, also, this period of extreme eccentricity terminated

only eighty thousand years ago, the close of the Glacial period would,

perhaps, upon Mr. Croll's theory, be comparatively a recent event; for

if the secular summer of the earth's eccentricity lags relatively as

far behind the secular movements as the annual summer does behind the

vernal equinox, we should, as Professor Charles H. Hitchcock suggests,

have to place the complete breaking up of the Ice period as late as forty

thousand years ago.[DT]

[Footnote DT: Geology of New Hampshire, vol. iii, p.327.]

We have no space to indicate, as it deserves, the comparative merits

and demerits of this ingenious theory. It would, however, be a great

calamity to have geologists accept it without scrutiny. It is, indeed,

a part of the business of geologists to doubt such theories until they

are verified by a thorough examination of all accessible _terrestrial_

evidence bearing upon the subject. There is no reason to question the

reality of the variations in the relative positions of the earth and the

sun assumed by Mr. Croll; though there may be serious doubt whether the

effects of those changes upon climate would be all that is surmised,

since equal amounts of heat would fall upon the earth during summer,

whether made longer or shorter by the cause referred to. During the short

summers the earth is so much nearer the sun that it receives each season

absolutely as much heat as it does during the longer summers, when it

is so much farther away from the sun. Thus the theory rests at last upon

the question what would become of the heat reaching the earth in these

differing conditions. It is plausibly urged by Mr. Croll that when a

hemisphere of the earth is passing through a period of long winters the

radiation of heat will be so excessive that the temperature would fall

much below what it would during the shorter winters; and so ice and snow

would accumulate far beyond the usual amount. It is also supposed that

the effect of the summer's sun in melting the ice during the short summer

would be diminished through natural increase of the amount of foggy and

cloudy weather.

Adhémar's theory is supposed by Sir Robert Ball, Royal Astronomer of

Ireland, to be considerably re-enforced by a discovery which he has made

concerning the distribution of heat upon the earth during the seasons

culminating in the summer and winter solstices. Croll had assumed,

on the authority of Herschel, that a hemisphere of the earth during

the longer winter in aphelion would receive the same actual amount of

heat which would fall upon it during the shorter summer in perihelion;

whereas, according to Dr. Ball's discovery, "of the total amount of heat

received from the sun on a hemisphere of the earth in the course of a

year, sixty-three per cent is received during the summer and thirty-seven

per cent during the winter."[DU] When, therefore, the summers occur in

perihelion the heat is more intense than Croll had supposed, and, at

the same time, the winters occurring in aphelion are more deficient in

heat than he had assumed. This discovery of Dr. Ball will not, however,

materially affect the discussion of Croll's theory upon its inherent

merits, since it is simply an intensification of the causes invoked by

him. We will therefore let it stand or fall in the light of the general

considerations hereafter to be adduced.

[Footnote DU: Cause of an Ice Age, p. 90.]

The aid of theoretical consequent changes in the volume of the Gulf

Stream, and in the area of the trade-winds, has also to be invoked by

Mr. Croll. The theory likewise receives supposed confirmation from facts

alleged concerning the present climate of the southern hemisphere which

is passing through the astronomical conditions thought to be favourable

to its glaciation. The antarctic continent is completely enveloped in

ice, even down to the sixty-seventh degree of latitude. A few degrees

nearer the pole Sir J. C. Boss describes the ice as rising from the water

in a precipitous wall one hundred and eighty feet high. In front of such

a wall, and nearly twenty degrees from the south pole, this navigator

sailed four hundred and fifty miles! Voyagers, in general, are said to

agree that the summers of the antarctic zone are much more foggy and cold

than they are in corresponding latitudes in the northern hemisphere; and

this, even though the sun is 3,000,000 miles nearer the earth during the

southern summer than it is during the northern.

Another direction from which evidence is invoked in confirmation of Mr.

Croll's theory is the geological indications of successive Glacial epochs

in times past. If there be a recurring astronomical cause sufficient of

itself to produce Glacial periods, such periods should recur as often as

the cause exists; but glaciation upon the scale of that which immediately

preceded the historic era could hardly have occurred in early geological

time without leaving marks which geologists would have discovered. Were

the "till" now covering the glaciated region to be converted into rock,

its character would be unmistakable, and the deposit is so extensive that

it could not escape notice.

In his inaugural address before the British Association in 1880,

Professor Ramsey, Director-General of the Geological Survey of Great

Britain, presented a formidable list of glacial observations in

connection with rocks of a remote age.[DV] Beginning at the earliest

date, he cites Professor Archibald Geikie, one of the most competent

judges, as confident that the rounded knobs and knolls of Laurentian

rocks exposed over a large region in northwestern Scotland, together

with vast beds of coarse, angular, unstratified conglomerates, are

unquestionable evidences of glacial action at that early period. Masses

of similar conglomerates, resembling consolidated glacial boulder-beds,

occur also in the Lower Silurian formation at Corswall, England. In

Dunbar, Scotland, Professor Forbes also found, in formations of but

little later age than the Coal period, "brecciated conglomerates,

consisting of pebbles and large blocks of stone, generally angular,

embedded in a marly paste, in which some of the pebbles are as well

scratched as those found in medial moraines." In formations of

corresponding antiquity the geologists of India have found similar

boulder-beds, in which some of the blocks are polished and striated.

[Footnote DV: Nature (August 26, 1880), vol. xxii, pp. 388, 389.]

Still, this evidence is less abundant than we should expect, if there had

been the repeated Glacial epochs supposed by Mr. Croll's astronomical

theory; and it is by no means impossible that the conglomerates of

scratched stones described by Professor Ramsey in Great Britain, and

by Messrs. Blandford and Medlicott in India, may have resulted from

local glaciers coming down from mountain-chains which have been since

removed by erosion or subsidence. We are not aware that any incontestable

evidence has been presented in America of any glaciation previous to that

of _the_ Glacial period.

Upon close consideration, also, it appears that Mr. Croll's theory has

not properly taken into account the anomalous distribution of heat which

we actually find to take place on the surface of the earth. He has done

good service in showing what an enormous transfer of heat there is

from the southern to the northern Atlantic by means of the Gulf Stream,

estimating that the heat conveyed by the Gulf Stream into the Atlantic

Ocean is equal to one fifth of all possessed by the waters of the North

Atlantic; or to the heat received from the sun upon a million and a half

square miles at the equator, or two million square miles in the temperate

zone. "The stoppage of the Gulf Stream would deprive the Atlantic of

77,479,650,000,000,000,000 foot-pounds of energy in the form of heat per

day."

Among the objections which bear against this ingenious theory is one

which will appear with great force when we come to discuss the date of

the Glacial period, when we shall show that even Professor Hitchcock's

supposition that the lingering effects of the last great eccentricity of

the earth's orbit, continued down to forty thousand years ago, is not

sufficient to account for the recentness of the close of the period as

shown by abundant geological evidence. It is certainly not more than ten

or fifteen thousand years ago that the ice finally melted off from the

Laurentian highlands; while on the Pacific coast the period of glaciation

was still more recent.

From inspection of the accompanying map the main point of Mr. Croll's

reasoning may be understood. It will be seen that the direction of the

currents in the central Atlantic is largely determined by the contour of

the northeastern coast of South America. From some cause the southeast

trade-winds are stronger than the northeast, and their force is felt in

pushing the superficial currents of warm water farther north than Cape

St. Roque, the eastern extremity of Brazil. As the direction of the South

American coast trends rapidly westward from this point to the Isthmus of

Panama, the resultant of the forces is a strong current northwestward

into the _cul-de-sac_ of the Gulf of Mexico, from which there is only the

one outlet between Cuba and the peninsula of Florida. Through this the

warm water is forced into the region where westerly winds prevail, and

spreads its genial influence far to the northward, modifying the climate

of the British Isles, and even of far-off Norway.

[Illustration: Fig. 100.--Map showing course of currents in the Atlantic

Ocean: _b_ and _b'_ are currents set in motion by opposite trade-winds;

meeting, they produce the equatorial current, which divides into _c_ and

_c'_, continuing on as _a_ and _a'_ and _e_.]

But why are the southeast trade-winds of the Atlantic stronger than

the northeast? The ultimate reason, of course, is to be found in the

fact that the northern hemisphere is warmer than the southern. The

atmosphere over the northern-central portion of the Atlantic region is

more thoroughly rarefied by the sun's heat than is that over the region

south of the equator. The strong southeast trades are simply the rush of

atmosphere from the South Atlantic to fill the vacuum caused by the heat

of the sun north of the equator.

But, again, why is this? Because, says Mr. Croll, we are now in that

stage of astronomical development favourable to the increased warmth

of the northern hemisphere. In the northern hemisphere the summers are

longer than the winters. Perihelion occurs in winter and aphelion in

summer. This is the reason why the North Atlantic is warmer than the

South Atlantic, and why the trade-winds of the south are drawn to the

north of the equator. Ten thousand five hundred years ago, however, the

conditions were reversed, and the greater rarefaction of the atmosphere

would have taken place south of the equator, thus drawing the trade-winds

in that direction.

By again inspecting the map, one will see how far-reaching the effect on

the climate of northern countries this change in the prevalences of the

trades would have been. Then, instead of having the northwest current

leading along the northeast coast of South America into the Gulf of

Mexico augmented by the warm currents circulating south of the equator,

the warm currents of the north would have been pushed down so far that

they would augment the current running to the southwest beyond Cape St.

Roque, along the southeast shore of South America; thus the northern

portion of the Atlantic, instead of robbing the southern portion of

heat, would itself be robbed of its warm currents to contribute to the

superfluous heat of the South Atlantic.

This theory is certainly very ingenious. There is a weak point in

it, however. Mr. Croll assumes that when the winters of the northern

hemisphere occur in aphelion, they must necessarily be colder than now.

But, evidently, this assertion implies a fuller knowledge than we possess

of the laws by which the heat received from the sun is distributed over

the earth.

For it appears from observation that the equator is by no means so

hot now as, theoretically, it ought to be, and that the arctic regions

are not so cold as, according to theory, they should be, and this in

places which could not be affected by oceanic currents. For example,

at Iquitos, on the Amazon, only three hundred feet above tide, three

degrees and a half south of the equator, and more than a thousand miles

from the Atlantic (so that ocean-currents cannot abstract the heat from

its vicinity), the mean yearly temperature is but 78° Fahr.; while at

Verkhojansk, in northeast Siberia, which is 67° north of the equator, and

is situated where it is out of the reach of ocean-currents, and where

the conditions for the radiation of heat are most favourable, and where,

indeed, the winter is the coldest on the globe (January averaging--56°

Fahr.), the mean yearly temperature is two degrees and a half above zero;

so that the difference between the temperature upon the equator and that

at the coldest point on the sixty-seventh parallel is only about 75°

Fahr.; whereas, if temperature were in proportion to heat received from

the sun, the difference ought to be 172°. Again, the difference between

the actual January temperature on the fiftieth parallel and that upon the

sixtieth is but 20° Fahr., whereas, the quantity of solar heat received

on the fiftieth parallel during the month of January is three times that

received upon the sixtieth, and the difference in temperature ought to be

about 170° Fahr. upon any known law in the case.

Woeikoff, a Russian meteorologist, and one of the ablest critics of Mr.

Croll's theory, and to whom we are indebted for these facts, ascribes

the greater present warmth of the northern Atlantic basin, not to the

astronomical cause invoked by Mr. Croll, but to the relatively small

extent of sea in the middle latitudes of the northern hemisphere. The

extent and depth of the oceans of the southern hemisphere would of

themselves give greater steadiness and force to its trade-winds, and

lead to a general lowering of the temperature; so that it is doubtful

if the astronomical causes introduced by Mr. Croll, even with Dr.

Ball's re-enforcement, would produce any appreciable effect while the

distribution of land and water remains substantially what it is at the

present time.

Still another variation in the astronomical theory has been set forth

and defended by Major-General A. W. Drayson, F. R. A. S., instructor

in the Royal Military School at Woolwich, England. He contends that

what has been called the precession of the equinoxes, and supposed to

be "a conical movement of the earth's axis in a circle around a point

as a centre, from which it continually decreases its distance,"[DW] is

really a second rotation of the earth about its centre. As a consequence

of this second rotation, he endeavours to show that the inclination of

the earth's axis varies as much as 12°; so that, whereas the Arctic and

Antarctic Circles and the tropics extend to only about 23° from the poles

and the equator, respectively, about thirteen thousand five hundred years

ago they extended more than 35°; thus bringing the frigid zones in both

cases 12° nearer the equator than now. This, he contends, would have

produced the Glacial period at the time now more generally assigned to it

by direct geological evidence.

[Footnote DW: Untrodden Ground in Astronomy and Geology, p. 26.]

The difficulty with this theory, even if the mathematical calculations

upon which it is based are correct, would be substantially the same as

those already urged against that of Mr. Croll. It is specially difficult

to see how General Drayson would account for the prolonged temperate

climate in high northern latitudes during the larger part of the Tertiary

epoch.

It will be best to turn again to the map to observe the possible effect

upon the Gulf Stream of a geological event of which we have some definite

evidence, and which is adduced by Mr. Upham and others as one of the

important probable causes of the Glacial period, namely, the subsidence

of the Isthmus of Panama and the adjacent narrow neck of land connecting

North with South America. It will be seen at a glance that a subsidence

sufficient to allow the northwest current of warm water, pushed by the

trade-winds along the northeast shore of South America, to pass into

the Pacific Ocean, instead of into the Gulf of Mexico, would be a cause

sufficient to produce the most far-reaching results; it would rob the

North Atlantic of the immense amount of heat and moisture now distributed

over it by the Gulf Stream, and would add an equal amount to the northern

Pacific Ocean, and modify to an unknown extent the distribution of heat

and moisture over the lands of the northern hemisphere.

The supposition that a subsidence of the Isthmus of Panama was among

the contributing causes of the Glacial period has been often made, but

without any positive proof of such subsidence. From evidence which

has recently come to light, however, it is certain that there has

actually been considerable subsidence there in late Tertiary if not in

post-Tertiary times. This evidence is furnished by Dr. G. A. Maack and

Mr. William M. Gabb in their report to the United States Government in

1874 upon the explorations for a ship-canal across the isthmus, and

consists of numerous fossils belonging to existing species which are

found at an elevation of 150 feet above tide. As the dividing ridge is

more than 700 feet above tide, this does not positively prove the point,

but so much demonstrated subsidence makes it easy to believe, in the

absence of contradictory evidence, that there was more, and that the

isthmus was sufficiently submerged to permit a considerable portion of

the warm equatorial current which now passes northward from the Caribbean

Sea and the Gulf of Mexico to pass into the Pacific Ocean.

[Illustration: Fig. 101.--Map showing how the land clusters about the

north pole.]

An obvious objection to the theory of a late Tertiary or post-Tertiary

subsidence of the Isthmus of Panama presents itself in the fact that

there is at present a complete diversity of species between the fish

inhabiting the waters upon the different sides of the isthmus. If

there had been such a subsidence, it seems natural to suppose that

Atlantic species would have migrated to the Pacific side and obtained

a permanent lodgment there, and that Pacific species would have found

a congenial home on the Atlantic side. It must be confessed that this

is a serious theoretical difficulty, but perhaps not insuperable. For

it is by no means certain that colonists from the heated waters of the

Caribbean Sea would become so permanently established upon the Pacific

side that they could maintain themselves there upon the re-establishment

of former conditions. On the contrary, it seems reasonable to suppose

that upon the re-elevation of the isthmus the northern currents, which

would then resume their course, would bring back with them conditions

unfavourable to the Atlantic species, and favourable to the competing

species which had only temporarily withdrawn from the field, and which

might now be better fitted than ever to renew the struggle with their

Atlantic competitors. It is by no means certain, therefore, that with

the re-establishment of the former conditions there would not also be a

re-establishment of the former equation of life upon the two sides of the

isthmus.

Mr. Upham's theory involves also extensive elevations of land in the

northern part of America; in this respect agreeing with the opinions

early expressed by Professors J. D. Dana and J. S. Newberry. Of the

positive indications of such northward elevations of land we have already

spoken when treating in a previous chapter of the fiords and submerged

channels which characterise northern Europe and both the eastern and

the western coasts of North America. But in working out the problem the

solution is only half reached when we have got the Gulf Stream into

the Pacific Ocean, and the land in the northern part of the continents

elevated to some distance above its present level. There is still the

difficulty of getting the moisture-laden currents from the Pacific Ocean

to carry their burdens over the crest of the Sierra Nevada and Rocky

Mountains and to deposit them in snow upon the Laurentian highlands.

An ingenious supplement to the theory, therefore, has been brought

forward by Professor Carpenter, who suggests that the immense Tertiary

and post-Tertiary lava-flows which cover so much of the area west of

the Rocky Mountains were the cause of the accumulations of snow which

formed the Laurentide Glacier. This statement, which at first seems so

paradoxical as to be absurd, appears less so upon close examination.

The extent of the outflows of lava west of the Rocky Mountains is almost

beyond comprehension. Literally, hundreds of thousands of square miles

have been covered by them to a depth in many places of thousands of feet.

These volcanic eruptions are mostly of late date, beginning in the middle

of the Tertiary and culminating probably about the time of the maximum

extent of the Laurentide Glacier. Indeed, so nearly contemporaneous was

the growth of the Laurentide Glacier with these outflows that Professor

Alexander Winchell had, with a good deal of plausibility, suggested that

the outflows of the eruptions of lava were caused by the accumulation

of ice over eastern British America. His theory was that the three

million cubic miles of ice which is proved to have been abstracted from

the ocean and piled up over that area was so serious a disturbance of

the equilibrium of the earth's crust that it caused great fissures to

be opened along the lines of weakness west of the Rocky Mountains, and

pressed the liquid lava out, as the juice is pressed out of an orange in

one place by pressing upon the rind in another.

Professor Carpenter's view is the exact reverse of Professor Winchell's.

Going back to those orographic changes which produced the lava-flows

and the elevation of the northern part of British America, he thinks

the problem of getting the moisture transferred from the Pacific Ocean

to the Canadian highlands is solved by the lava-flows west of the Rocky

Mountains. This immense exudation of molten matter was accompanied by an

enormous liberation of heat, which must have produced significant changes

in the meteorological conditions.

The moisture of the atmosphere is precipitated by means of the

condensation connected with a lowering of its temperature. Ordinarily,

therefore, when moist winds from an oceanic area pass directly over a

lofty mountain-chain, the precipitation takes place immediately, and

the water finds its way back by a short course to the sea. This is what

now actually occurs on the Pacific coast. The Sierra Nevada condense

nearly all the moisture; so that very little falls on the vast area

extending from their summits eastward to the Rocky Mountains. All that

region is now practically a desert land, where the evaporation exceeds

the precipitation. In Professor Carpenter's view the heat radiated from

the freshly exuded lava is supposed to have prevented the precipitation

near the coast-line, and to have helped the winds in carrying it farther

onward to the northeast, where it would be condensed upon the elevated

highlands, upon which the snows of the great Laurentide Glacier were

collected.

It is not necessary for us to attempt to measure the amount of truth in

this subsidiary hypothesis of Professor Carpenter, but it illustrates

how complicated are the conditions which have to be considered before we

rest securely upon any particular hypothesis. The unknown elements of the

problem are so numerous, and so far-reaching in their possible scope,

that a cautious attitude of agnosticism, with respect to the cause of

the Glacial period, is most scientific and becoming. Still, we are ready

to go so far as to say that Mr. Upham's theory comes nearest to giving

a satisfactory account of all the phenomena, and it is to this that

Professor Joseph Le Conte gives his cautious approval.

Summarily stated, this theory is, that the passage from the Tertiary

to the Quaternary or Glacial period was characterised by remarkable

oscillations of land-level, and by corresponding changes of climate, and

of ice-accumulation in northern regions; that the northern elevation

was connected with subsidence in the equatorial regions; that these

changes of land-level were both initiated and, in the main, continued

by the interior geological forces of the globe; but that the very

continental elevation which mainly brought on the Glacial period added

at length, in the weight of the ice which accumulated over the elevated

region, a new force to hasten and increase the subsidence, which would

have taken place in due time in the natural progress of the orographic

oscillations already begun. Professor Le Conte illustrates the subject by

the following diagram, which, for simplicity's sake, treats the Glacial

epoch as one; the horizontal line, A B, represents time from the later

Pliocene until now; but it also represents the present condition of

things both as to land-level and as to ice-accumulation. The full line, c

d e, represents the oscillations of land (and presumably of temperature)

above and below the present condition. The broken line represents the

rise, culmination, and decline of ice-accumulation. The dotted line

represents the crust-movement as it would have been if there had been no

ice-accumulation.

[Illustration: Fig. 102.]

_Succession of Epochs, Glacial and Fluvial Deposits, and_

Eastern Provinces and Middle and Southern

Epochs. New England. Atlantic States.

Recent or Rise of the land to its Continued subsidence of

Terrace. present height, or coast at New York and

(Mostly within somewhat higher, soon southward, and rise of

the period of after the departure of the mountainous belt, by

traditional the ice. Rivers eroding displacement along the

and written their glacial fall line of the rivers.

history.) flood-plains, leaving Much erosion of the

remnants as terraces. Columbia formation since

Warmer climate than now, culmination of second

probably due to greater Glacial epoch;

Gulf Stream, formerly sedimentation in bays,

permitted southern sounds, and estuaries.

mollusks to extend to

Gulf of St. Lawrence, now

represented by isolated

colonies.

Glacial Period of Ice Age. Pleistocene Period.

Champlain. Land depressed under Less subsidence in

ice-weight; glacial latitude of New York and

(Close of the recession; continued southward than at north;

second Glacial deposition of upper till lower Hudson Valley, and

epoch.) and deep flood-plains of part of its present

gravel, sand and clay submarine continuation,

(modified drift). above sea-level. Gravel

Terminal moraines marking and sand deposits from

pauses or readvance englacial drift in

during general retreat of Delaware and Susquehanna

ice. Marine submergence. Valleys, inclosing

150 to 230 feet on coast abundant human implements

of Maine, to 520 feet in at Trenton, N.J.

Gulf and valley of St.

Lawrence.

Second Glacial. Second great uplift of Renewal of great

the land, 3.000 to 4,000 continental elevation

feet higher than now; (3.000 feet in latitude

snow-fall again all the of New York and

year; ice probably two Philadelphia), of

miles thick on Laurentide excessive snow-fall and

highlands, and extending rains, and of wide-spread

somewhat farther south fluvial deposits, the

here than in first Columbia formation, on

glaciation. Lower till the coastal plain, during

(ground moraine), and early part of this epoch.

upper till (englacial Implements of man at

drift). Terminal Claymont, Del.

moraines, kames, osars,

valley drift.

Inter-glacial. Ice-sheet melted here; Depression, but generally

probably not more ice in not to the present level.

(Longest epoch arctic regions than now. Deep channels cut in the

of this era.) bed-rocks by the

Fluvial and lacustrine Delaware, Susquehanna,

deposits of this time, Potomac, and other

with those of the first rivers. The Appomattox

Glacial epoch, were deposits much eroded.

eroded by the second

glaciation. Relative length of this

epoch made known by McGee

from study of this

region.

First Glacial. Begun by high continental Continental elevation;

uplift, cool climate and erosion of Delaware and

snow-fall throughout the Chesapeake Bays, and of

year, producing Albemarle and Pamlico

ice-sheet. Much glacial Sounds. Plentiful

erosion and snow-fall on the southern

transportation; till and Appalachian Mountains;

stratified deposits. snows melted in summer,

Ended by depression of and heavy rains,

land; return of warm producing broad

climate, with rain; final river-floods, with

melting of the ice. deposition of the

Isthmus of Panama Appomattox formation.

probably submerged (Gulf

Stream smaller), and

again in second Glacial

epoch.

_Changes in Altitude and Climate, during the Quaternary Era._

Mississippi Basin and Cordilleran Region. Europe and Asia.

northward.

Terracing of river Including a stage of Erosion and terracing

valleys. Northward rise considerable uplift, of stratified drift in

of area of Lake Agassiz with return of humid river valleys. Land

nearly complete before conditions, Alpine passage of European

the ice was melted on glaciation (third flora to Greenland;

the country crossed by Glacial epoch), and succeeded by subsidence

Nelson River; but rise the second great rise there, admitting warm

about Hudson Bay is still of Lakes Bonneville currents to Arctic Sea.

going on; 7,000 to 8,000 and Lahontan. Very Minor climatic changes,

years since ice-melting recent subsidence including a warmer

uncovered Niagara and and change to present stage than now. Upper

falls of St. Anthony. aridity. and outer portions of

Indo-Gangetic alluvial

plain; extensive

deposits of Hwang Ho,

and destructive changes

of its course.

Abundant deposition of Depression probably Final departure of the

englacial drift. Stone almost to the present ice-sheets; glacial

implements in river level. Restoration of rivers forming eskers

gravels of Ohio, Ind., arid climate; nearly or and kames. Loess

and Minn. Laurentian quite complete deposited while the

lakes held at higher evaporation of Lakes region of the Alps was

levels, and Lake Bonneville and Lahontan.depressed lower than

Agassiz formed in Red Formation of the "adobe"now. Upper (englacial)

River basin, by continuing through the till, and asar, of

barrier of retreating second Glacial, Sweden. Marine

ice, with outlets over Champlain, and Recent submergence 500 to 600

lowest points of their epochs. feet in Scotland,

present southern Scandinavia, and

water-shed. Marine Spitzbergen.

submergence 300 to 500

feet on southwest

side of Hudson Bay.

Ice-sheet here less Probable uplift 3,0 Second elevation and

extensive than in the feet, shown by general glaciation of

first Glacial epoch, and submerged valleys near northwestern Europe;

not generally bordered Cape Mendocino. Second the ice-sheets of Great

as then by lakes in ice-sheet on British Britain probably more

valleys which now drain Columbia and Vancouver extensive than in first

southward. Island; local Glacial epoch.

glaciation of Rocky Oscillations of

Terminal moraines at Mountains, Cascade and ice-front; British

extreme limit of the Sierra range, Nevada, Lower and Upper

ice-advance, and at ten south to latitude 37°. the Chalky, Purple, and

or more stages of halt or First great rise of bowlder-clays, Hessle

readvance in its retreat. Lakes Bonneville bowlder-clays. Terminal

and Lahontan. moraines in Germany.

Depression nearly to Continental depression. Recession, or probably

present level southward; Arid climate. Long- complete departure, of

more northward, but continued denudation of the ice-sheets.

followed there, by the mountains:

differential uplift of resulting very thick Land connection between

800 or 1,000 feet. subaërial deposits of Europe and Africa,

Great erosion of loess the "adobe." permitting southern

and other modified animals to extend far

drift, and of "Orange Intermittent volcanic northward.

Sand." Valleys of this action in various parts

epoch, partly filled of this region, Erosion of the Somme

with later till, are throughout the Valley below its oldest

marked by chains of Quaternary era to very implement-bearing

lakes in southern recent times, and gravels.

Minnesota. liable to break forth

again.

Pliocene elevation of Latest rise (3.000 Uplift and glaciation

continent brought to feet) of the Colorado of northwestern Europe:

culmination at Cañon district. Sierra maximum elevation.

beginning of Nevada and other Great 2,500 feet or more

Quaternary era; this Basin mountain-ranges (depth of the Skager

whole basin probably formed by immense Rack); France and

then uplifted 3.000 uplifts, with faulting. Britain united with the

feet; excessive California river- Färöe Islands, Iceland,

snow-fall and rain; courses changed; human and Greenland. Uplifts

deposition of the bones and implements in of the Himalayas and

"Orange Sand." Ice- the old river gravels, other mountain-ranges

sheet south to lava-covered. Ice-sheet attendant on both

Cincinnati and St. on British Columbia; Glacial epochs.

Louis, at length local glaciers

depressing the earth's southward.

crust beneath it;

slackened river floods

and shallow lakes,

forming the loess.

It is seen from the diagram that the ice-accumulation culminated at a

time when the land, under the pressure of the ice-load, had already

commenced to subside; and that the subsidence was greatest at a time when

the pressure had already begun to diminish. But the fact that the land,

after the removal of the ice-load, did not return again to its former

height in the Pliocene, is proof positive that there were other and

more fundamental causes of crust-movement at work besides weighting and

lightening. The land did not again return to its former level because the

cycle of elevation, whatever its cause, which commenced in the Pliocene

and culminated in the early Quaternary, had exhausted itself. If it had

not been for the ice-load interfering with and modifying the natural

course of the crust-movement determined previously and primarily by other

and probably internal causes, the latter would probably have taken the

course represented by the dotted line. It would have risen higher and

culminated later, and its curve would have been of simpler form.

We append a carefully prepared table by Mr. Warren Upham, showing the

probable changes in altitude and climate during the Quaternary era.[DX]

[Footnote DX: On page 106 and sequel I have summarised the reasons which

lead me to discard the Inter-Glacial epoch, and to look upon the whole

Glacial period as constituting a grand unity with minor episodes. It

does not yet seem to me that the duality of the period is proved. On the

contrary, Mr. Kendall's chapter on the Glacial phenomena of Great Britain

strongly confirms my view.]

On the part of many the theory here provisionally adopted will be

regarded with disfavour by reason of a disinclination to supposing

any great recent changes of level in the continental areas. So firmly

established do the continents appear to be, that it seems like invoking

an inordinate display of power to have them exalted for the sake of

producing a Glacial period. Due reflection, however, will make it

evident that within certain limits the continents are exceedingly

unstable, and that they have displayed this instability to as great an

extent in recent geological times as they have done in any previous

geological periods. When one reflects, also, upon the size of the earth,

a continental elevation of 3,000 or 4,000 feet upon a globe whose

diameter is more than 40,000,000 feet is an insignificant trifle. On a

globe one foot in diameter it would be represented by a protuberance of

barely one thousandth of an inch. A corresponding wrinkle upon a large

apple would require a magnifying-glass for its detection. Moreover, the

activity of existing volcanoes, the immense outflows of lava which have

taken place in the later geological periods, together with the uniform

increase of heat as we penetrate to deeper strata in the crust of the

earth--all point to a condition of the earth's interior that would

make the elevations of land which we have invoked for the production

of the Glacial period easily credible. Physicists do not, indeed, now

hold to the entire fluidity of the earth's interior, but rather to a

solid centre, where gravity overcomes the expansive power of heat, and

maintains solidity even when the heat is intense. But between the cooling

crust of the earth's exterior and a central solid core there is now

believed to be a film where the influences of heat and of the pressure

of gravity are approximately balanced, and the space is occupied by a

half-melted or viscous magma, capable of yielding to a slow pressure, and

of moving in response to it from one portion of the enclosed space to

another where the pressure is for any cause relieved.

As a result of prolonged enquiries respecting the nature of the forces

at work both in the interior and upon the exterior of the earth, and

of a careful study of the successive changes marking the geological

period, we are led to believe that the continental elevations necessary

to produce the phenomena of the Glacial period are not only entirely

possible but easily credible, and in analogy with the natural progress

of geological history. In the first place, it is easy to see that

two causes are in operation to produce a contraction of the earth's

volume and a shortening of its diameter. Heat is constantly being

abstracted from the earth by conduction and radiation, but perhaps to

a greater extent through ceaseless volcanic eruptions which at times

are of enormous extent. It requires but a moment's thought to see that

contraction of the volume of the earth's interior means that the hardened

exterior crust must adjust itself by wrinkles and folds. For a long

period this adjustment might show itself principally in gentle swells,

lifting portions of the continents to a higher level, accompanied by

corresponding subsidence in other places. This gradually accumulating

strain would at length be relieved along some line of special weakness in

the crust by that folding process which has pushed up the great mountain

systems of the world.

Careful study of the principal mountain systems shows that all the

highest of them are of late geological origin. Indeed, the latter part

of the Tertiary period has been the great mountain-building epoch in the

earth's history. The principal part of the elevation of the Andes and

the Rocky Mountains has taken place since the middle of the Tertiary

period. In Europe there is indubitable evidence that the Pyrenees have

been elevated eleven thousand feet during the same period, and that the

western Alps have been elevated thirteen thousand feet in the same time.

The Carpathians, the western Caucasus, and the Himalayas likewise bear

explicit evidence to the fact that a very considerable portion of their

elevation, amounting to many thousand feet, has been effected since the

middle of the Tertiary period, while a considerable portion of this

elevation of the chiefest mountain systems of the world has occurred in

what would be called post-Tertiary time--that is, has been coincident

with a portion of the Glacial period.

The Glacial period, however, we suppose to have been brought about, not

by the specific plications in the earth's crust which have produced the

mountain-chains, but by the gentler swells of larger continental areas

whose strain was at last relieved by the folding and mashing together

of the strata along the lines of weakness now occupied by the mountain

systems. The formation of the mountains seems to have relieved the

accumulating strain connected with the continental elevations, and to

have brought about a subsequent subsidence.

Doubtless, also, correlated subsidences and elevations of the earth's

crust have been aided by the transfer of the sediment from continental

to oceanic areas, and, as already suggested, during the Glacial period

by the transfer of water evaporated from the surface of the ocean to

the ice-fields of the glaciated area. For example, present erosive

agencies are lowering the level of the whole Mississippi basin from

the Alleghanies to the Rocky Mountains at the rate of a foot in five

thousand years. All this sediment removed is being transferred to the

ocean-bed. Present agencies, therefore, if not counteracted, would

remove the whole continent of America (whose average elevation above the

sea is only 748 feet) in less than four million years; while the great

rivers which descend in all directions from the central plateau of Asia

are transferring sediment to the ocean from two to four times as fast

as the Mississippi is, and the Po is transferring it from the Alps to

the Adriatic fully seven times as fast as the Mississippi is from its

basin to the Gulf of Mexico. This rapid transfer of sediment from the

continents to the ocean is producing effects in disturbing the present

equilibrium of the earth's crust, which are too complicated for us fully

to calculate; but it is by no means improbable that when accumulating for

a considerable length of time, the ultimate results may be very marked

and perhaps sudden in their appearance.

The same may also be said of the accumulation of ice during the Glacial

period. The glaciated areas of North America and Europe combined

comprise about six million square miles. At a moderate estimate,

the ice was three-quarters of a mile deep. Here, therefore, there

would be between four and five million cubic miles of water, which

had first relieved the ocean-beds of the pressure of its weight, and

then concentrated its force over the elevated areas of the northern

hemisphere. This disturbance of the equilibrium, by the known transfer

of force from one part of the earth's crust to another, certainly gives

much plausibility to the theory of Jamieson, Winchell, Le Conte, and

Upham, that the Glacial period partly contained in itself its own cure,

and by the weight of its accumulated weight of ice helped to produce

that depression over the glaciated area which at length rendered the

accumulation of ice there impossible.

This general view of the known causes in operation during the Glacial

period will go far towards answering an objection that has probably

before this presented itself to the reader's mind. It seems clear

that the Glacial period in the southern hemisphere has been nearly

contemporaneous with that of the northern. The Glacial period proper of

the southern hemisphere is long since passed. The existing glaciers of

New Zealand, of the southern portion of the Andes Mountains, and of the

Himalaya Mountains are but remnants of those of former days. In the light

of the considerations just presented, it would not seem improbable that

the same causes should produce these similar effects in the northern and

the southern hemisphere contemporaneously. At any rate, it would not

seem altogether unlikely that the pressure of ice during the climax of

the Glacial period upon the northern hemisphere (which, as we have seen,

there is reason to believe aided in the depression of the continent to

below its present level in the latter part of the Glacial period) should

have contributed towards the elevation of mountains in other parts of the

world, and so to the temporary enlargement of the glaciers about their

summits.

Nor are we wholly without evidence that these readjustments of land-level

which have been carried on so Vigorously since the middle of the Tertiary

period are still going on with considerable though doubtless with

diminished rapidity. There has been a re-elevation of the land in North

America since the Glacial period amounting to 230 feet upon the coast of

Maine, 500 feet in the vicinity of Montreal, from 1,000 to 1,600 feet in

the extreme northern part of the continent, and in Scandinavia to the

extent of 600 feet. In portions of Scandinavia the land is now rising

at the rate of three feet in a century. Other indications of even the

present instability of the earth's surface occur in numbers too numerous

to mention.[DY]

[Footnote DY: For a convincing presentation of the views here outlined,

together with abundant references to literature, see Mr. Warren Upham's

Appendix to the author's Ice Age in North America.]

But, while we are increasingly confident that the main causes of the

Glacial period have been changes in the relative relation of land-levels

connected with diversion of oceanic currents, it is by no means

impossible, as Wallace[DZ] and others have suggested, that these were

combined with the astronomical causes urged by Drs. Croll and Geikie.

By some this combination is thought to be the more probable, because

of the extreme recentness of the close of the Glacial period, as shown

by the evidence which will be presented in the following chapter. The

continuance of glaciers in the highlands of Canada, down to within a few

thousand years of the present time, coincides in a remarkable manner with

the last occurrence of the conditions favourable to glaciation upon Mr.

Croll's theory, which took place about eleven thousand years ago.

[Footnote DZ: See Island Life, chapters viii and ix.]

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