Are we now justified in supposing that the percentage of carbon dioxide

in the air has varied to an extent sufficient to account for the

temperature changes? This question has been answered in the affirmative

by Högbom, and, in later times, by Stevenson. The actual percentage of

carbonic acid in the air is so insignificant that the annual combustion

of coal, which has now (1904) risen to about 900 million tons and is

rapidly increasing,[3] carries about one-seven-hundredth part of its

percentage of carbon dioxide to the atmosphere. Although the sea, by

absorbing carbonic acid, acts as a regulator of huge capacity, which

takes up about five-sixths of the produced carbonic acid, we yet

recognize that the slight percentage of carbonic acid in the atmosphere

may by the advances of industry be changed to a noticeable degree in

the course of a few centuries. That would imply that there is no real

stability in the percentage of carbon dioxide in the air, which is

probably subject to considerable fluctuations in the course of time.

[Footnote 3: It amounted in 1890 to 510 million tons; in 1894,

to 550; in 1899, to 690; and in 1904, to 890 million tons.]

Volcanism is the natural process by which the greatest amount of

carbonic acid is supplied to the air. Large quantities of gases

originating in the interior of the earth are ejected through the

craters of the volcanoes. These gases consist mostly of steam and of

carbon dioxide, which have been liberated during the slow cooling of

the silicates in the interior of the earth. The volcanic phenomena

have been of very unequal intensity in the different phases of the

history of the earth, and we have reason to surmise that the percentage

of carbon dioxide in the air was considerably greater during periods

of strong volcanic activity than it is now, and smaller in quieter

periods. Professor Frech, of Breslau, has attempted to demonstrate

that this would be in accordance with geological experience, because

strongly volcanic periods are distinguished by warm climates, and

periods of feeble volcanic intensity by cold climates. The ice age

in particular was characterized by a nearly complete cessation of

volcanism, and the two periods at the commencement and at the middle of

the Tertiary age (Eocene and Miocene) which showed high temperatures

were also marked by an extraordinarily developed volcanic activity.

This parallelism can be traced back into more remote epochs.

It may possibly be a matter of surprise that the percentage of

carbon dioxide in the atmosphere should not constantly be increased,

since volcanism is always pouring out more carbon dioxide into our

atmosphere. There is, however, one factor which always tends to reduce

the carbon dioxide of the air, and that is the weathering of minerals.

The rocks which were first formed by the congelation of the volcanic

masses (the so-called magma) consist of compounds of silicic acid

with alumina, lime, magnesia, some iron and sodium. These rocks were

gradually decomposed by the carbonic acid contained in the air and

in the water, and it was especially the lime, the magnesia, and the

alkalies, and, in some measure also the iron, which formed soluble

carbonates. These carbonates were carried by the rivers down into the

seas. There lime and magnesia were secreted by the animals and by the

algæ, and their carbonic acid became stored up in the sedimentary

strata. Högbom estimates that the limestones and dolomites contain at

least 25,000 times more carbonic acid than our atmosphere. Chamberlin

has arrived at nearly the same figure—from 20,000 to 30,000; he

does not allow for the precambrian limestones. These estimates are

most likely far too low. All the carbonic acid that is stored up in

sedimentary strata must have passed through the atmosphere. Another

process which withdraws carbonic acid from the air is the assimilation

of plants. Plants absorb carbonic acid under secretion of carbon

compounds and under exhalation of oxygen. Like the weathering, the

assimilation increases with the percentage of carbonic acid. The

Polish botanist E. Godlewski showed as early as 1872 that various

plants (he studied _Typha latifolia_ and _Glyceria spectabilus_ with

particular care) absorb from the air an amount of carbonic acid which

increases proportionally with the percentage of carbonic acid in the

atmosphere up to 1 per cent., and that the assimilation then attains,

in the former plant, a maximum at 6 per cent., and in the latter

plant at 9 per cent. The assimilation afterwards diminishes if the

carbonic acid percentage is further augmented. If, therefore, the

percentage of carbon dioxide be doubled, the absorption by the plants

would also be doubled. If, at the same time, the temperature rises by

4°, the vitality will increase in the ratio of 1: 1.5, so that the

doubling of the carbon dioxide percentage will lead to an increase

in the absorption of carbonic acid by the plant approximately in the

ratio of 1: 3. The same may be assumed to hold for the dependence

of the weathering upon the atmospheric percentage of carbonic acid.

An increase of the carbon dioxide percentage to double its amount

may hence be able to raise the intensity of vegetable life and the

intensity of the inorganic chemical reactions threefold.

According to the estimate of the famous chemist Liebig, the quantity of

organic matter (freed of water) which is produced by one hectare (2.5

acres) of soil, meadowland, or forest is nearly the same, approximately

2.5 tons per year in central Europe. In many parts of the tropics the

growth is much more rapid; in other places, in the deserts and arctic

regions, much more feeble. We may be justified in accepting Liebig’s

figure as an average for the firm land on our earth. Of the organic

substances to which we have referred, and which mainly consist of

cellulose, carbon makes up 40 per cent. Thus the actual annual carbon

production by plants would amount to 13,000 million tons—_i.e._,

not quite fifteen times more than the consumption of coal, and about

one-fiftieth of the quantity of the carbon dioxide in the air. If,

therefore, all plants were to deposit their carbon in peat-bogs, the

air would soon be depleted of its carbon dioxide. But it is only a

fraction of one per cent. of the coal which is produced by plants that

is stored up for the future in this way. The rest is sent back into the

atmosphere by combustion or by decay.

Chamberlin relates that, together with five other American geologists,

he attempted to estimate how long a time would be required before

the carbon dioxide of the air would be consumed by the weathering of

rocks. Their various estimates yielded figures ranging from 5000 to

18,000 years, with a probable average of 10,000 years. The loss of

carbonic acid by the formation of peat may be estimated at the same

figure. The production of carbonic acid by the combustion of coal would

therefore suffice to cover the loss of carbonic acid by weathering and

by peat formation seven times over. Those are the two chief factors

deciding the consumption of carbonic acid, and we thus recognize that

the percentage of carbonic acid in the air must be increasing at a

constant rate as long as the consumption of coal, petroleum, etc., is

maintained at its present figure, and at a still more rapid rate if

this consumption should continue to increase as it does now.

This consideration enables us to picture to ourselves the possibility

of the enormous plant-growth which must have characterized certain

geological periods of our earth—for instance, the carboniferous period.

This period is known to us from the extraordinarily large number of

plants which we find embedded in the clay of the swamps of those days.

Those plants were slowly carbonized afterwards, and their carbon is in

our age returned to its original place in the household of nature in

the shape of carbonic acid. A great portion of the carbonic acid has

disappeared from the atmosphere of the earth, and has been stored up as

coal, lignite, peat, petroleum, or asphalt in the sedimentary strata.

Oxygen was liberated at the same time, and passed into our atmospheric

sea. It has been calculated that the amount of oxygen in the air—1216

billion tons—approximately corresponds to the mass of fossil coal

which is stored up in the sedimentary strata. The supposition appears

natural, therefore, that all the oxygen of the air may have been

formed at the expense of the carbonic acid in the air. This view was

first advanced by Kœhne, of Brussels, in 1856, and later discussions

have strengthened its probability. Part of the oxygen is certainly

consumed by weathering processes, and absorbed—_e.g._, by sulphides

and by ferro-salts; without this oxidation the actual quantity of

oxygen in the air would be greater. On the other hand, there are in

the sedimentary strata many oxidizable compounds—_e. g._, especially

iron sulphides—which have probably been reduced by the interaction

of carbon (by organic compounds). A large number of the substances

which consume oxygen during their decomposition and decay have also

been produced by the intermediation of the coal which had previously

been deposited under liberation of oxygen, so that these substances

are, by their oxidation, restored to their original state. We may

hence take it as established that the masses of free oxygen in the air

and of free carbon in the sedimentary strata approximately correspond

to each other, and that probably all the oxygen of the atmosphere

owes its existence to plant life. This appears plausible also for

another reason. We know for certain that there is some free oxygen in

the atmosphere of the sun, and that hydrogen abounds in the sun. The

earth’s atmosphere may originally have been in the same condition.

When the earth cooled gradually, hydrogen and oxygen combined to

water, but an excess of hydrogen must have remained. The primeval

atmosphere of the earth may also have contained hydrocarbons, as they

play an important part in the gases of comets. To these gases there

were added carbonic acid and water vapor, coming from the interior of

the earth. Thanks to its chemical inertia, the nitrogen of the air may

not have undergone much change in the course of the ages. An English

chemist, Phipson, claims to have shown that both higher plants (the

corn-bind) and lower organisms (various bacteria) can live and develop

in an atmosphere devoid of oxygen when it contains carbonic acid and

hydrogen. It is also possible that simple forms of vegetable life

existed before the air contained any oxygen, and that these plants

liberated the oxygen from the carbonic acid exhaled by the craters.

This oxygen gradually (possibly under the influence of electric

discharges) converted the hydrogen and the hydrocarbons of the air into

water and carbonic acid until those elements were consumed. The oxygen

remained in the air, whose composition gradually approached more the

actual state.[4]

[Footnote 4: According to the opinion of a colleague of mine,

a botanist, the results of the experiments of Phipson must be

regarded as very doubtful, and some oxygen would appear to be

indispensable for the growth of plants. We have to imagine the

development somewhat as follows: As the earth separated from

the solar nebula, its temperature was very high at first in its

outer portions. At this temperature it was not able to retain

the lighter gases, like hydrogen and helium, for a long period;

the heavy gases, like nitrogen and oxygen, remained. The

original excess of hydrogen and helium disappeared, therefore,

before the crust of the earth had been formed, and the

atmosphere of the earth immediately after the formation of the

crust contained some oxygen, besides much nitrogen, carbonic

acid, and water vapor. The main bulk of the actual atmospheric

oxygen would therefore have been reduced from carbon dioxide by

the intermediation of plants. The view that celestial bodies

may lose part of their atmosphere is due to Johnstone Stoney.

The atmospheric gases escape the more rapidly the lighter their

molecules and the smaller the mass of the celestial bodies. On

these lines we explain that the smaller celestial bodies like

the moon and Mercury, have lost almost all their atmosphere,

while the earth has only lost hydrogen and helium, which again

have been retained by the sun.]

This oxygen is an essential element for the production of animal life.

As animal life stands above vegetable life, so animal life could only

originate at a later stage than plant life. Plants require, in addition

to suitable temperature, only carbonic acid and water, and these

gases will probably be found in the atmospheres of all the planets

as exhalations of their inner incandescent masses which are slowly

cooling. The presence of water vapor has directly been established, by

means of the spectroscope, in the atmospheres of other planets—Venus,

Jupiter, and Saturn—and indirectly by the observation of a snow-cap on

Mars. The spectroscope further gives us indication of the presence of

other gases. There is an intense band in the red part of the spectra of

Jupiter and Saturn, of wave-length 0.000618 mm. Other new constituents

of unknown nature have been discerned in the spectra of Uranus and

Neptune. On the other hand, there is hardly any, or at any rate only

a quite insignificant, atmosphere on the moon and on Mercury. This

is easily understood. The temperature on that side of Mercury which

is turned away from the sun is near absolute zero. All the gases of

the planetary atmosphere would collect and condense there. If, then,

Mercury had originally an atmosphere, it must have lost it as it lost

its own rotation, compelling it to turn always the same face towards

the sun. Similar reasons may account for the absence of a lunar

atmosphere. If Venus should likewise always turn the same side towards

the sun, as many astronomers assert, Venus should not have any notable

atmosphere, nor clouds either. We know, however, that this planet is

surrounded by a very marked developed atmosphere.[5]

[Footnote 5: That results from the very strong refraction which

light undergoes in the atmosphere of Venus when this planet

is seen in front of the sun’s edge during the so-called Venus

transits.]

And that is the strongest objection to the assumption that Venus

follows the example of Mercury as regards the rotation about its own

axis.

Since, now, warm ages have alternated with glacial periods, even after

man appeared on the earth, we have to ask ourselves: Is it probable

that we shall in the coming geological ages be visited by a new ice

period that will drive us from our temperate countries into the hotter

climates of Africa? There does not appear to be much ground for such

an apprehension. The enormous combustion of coal by our industrial

establishments suffices to increase the percentage of carbon dioxide

in the air to a perceptible degree. Volcanism, whose devastations—

on Krakatoa (1883) and Martinique (1902)—have been terrible in late

years, appears to be growing more intense. It is probable, therefore,

that the percentage of carbonic acid increases at a rapid rate. Another

circumstance points in the same direction; that is, that the sea

seems to withdraw carbonic acid from the air. For the carbonic acid

percentage above the sea and on islands is on an average 10 per cent.

less than the above continents.

[Illustration: Fig. 17.—Photograph of the surface of the moon,

in the vicinity of the crater of Copernicus. Taken at the

Yerkes Observatory, Chicago, U. S. A. Scale: Diameter of moon,

0.55 m. = 21.7 in. Owing to the absence of an atmosphere and of

atmospheric precipitations, the precipitous walls of the crater

and other elevations do not indicate any signs of decay.]

If the carbonic acid percentage of the air had kept constant for

ages, the percentage of the water would have found time to get into

equilibrium with it; but the sea actually absorbs carbonic acid

from the air. Thus the sea-water must have been in equilibrium with

an atmosphere which contained less carbonic acid than the present

atmosphere. Hence the carbonic acid percentage has been increasing of

late.

We often hear lamentations that the coal stored up in the earth is

wasted by the present generation without any thought of the future, and

we are terrified by the awful destruction of life and property which

has followed the volcanic eruptions of our days. We may find a kind of

consolation in the consideration that here, as in every other case,

there is good mixed with the evil. By the influence of the increasing

percentage of carbonic acid in the atmosphere, we may hope to enjoy

ages with more equable and better climates, especially as regards the

colder regions of the earth, ages when the earth will bring forth

much more abundant crops than at present, for the benefit of rapidly

propagating mankind.

III

RADIATION AND CONSTITUTION OF THE SUN

The question has often been discussed in past ages, and again in

the last century, in how far the position of our earth within the

solar system may be regarded as secure. One might apprehend two

things. Either the distance of the earth from the sun might increase

or decrease, or the rotation of the earth about its axis might be

arrested; and either of these possibilities would threaten the

continuance of life on the earth. The problem of the stability of

the solar system has been investigated by the astronomers, and their

patrons have offered high prizes for a solution of the problem. If the

solar system consisted merely of the sun and the earth, the earth’s

existence would be secure for ages; but the other planets exercise a

certain, though small, influence upon the movements of the earth. That

this influence can only be of slight importance is due to the fact

that the total mass of all the planets does not aggregate more than

one-seven-hundred-and-fiftieth of the mass of the sun, and, further,

to the fact that the planets all move in nearly circular orbits around

the centre, the sun, so that they never approach one another closely.

The calculations of the astronomers demonstrate that the disturbances

of the earth’s orbit are merely periodical, representing long cycles

of from 50,000 to 2,000,000 years. Thus the whole effect is limited to

a slight vacillation of the orbits of the planets about their mean

positions.

So far everything is well and good. But our solar system is traversed

by other celestial bodies, mostly of unknown, but certainly not of

circular orbits—namely, the comets. The fear of a collision with a

comet still alarmed the thinkers of the past century. Experience has,

however, taught us that collisions between the earth and comets do not

lead to any serious consequence. The earth has several times passed

through the tails of comets—for instance, in 1819 and 1861—and it

was only the calculating astronomer who became aware of the fact. Once

on such an occasion we have thought that we observed a glow like that

of an aurora in the sky. When the earth was drawing near the denser

parts of the comet, particles fell on the earth in the shape of showers

of shooting-stars, without doing any appreciable damage. The mass of

comets is too small perceptibly to disturb the paths of the planets.

The rotation of the earth about its axis should slowly be diminished by

the effects of the tides, since they act like a brake applied to the

surface of the earth. This retardation is, however, so unimportant that

the astronomers have not been able to establish it in historical times.

The slow shrinkage of the earth somewhat counteracts this effect.

Laplace believed that we were able to deduce, from an analysis of the

observations of solar eclipses in ancient centuries, that the length of

the day had not altered by more than 0.01 second since the year 729 B.C.

We know that the sun, unaccompanied by its planets, is moving in space

towards the constellation of Hercules with a velocity of 20 km. (13

miles) per second, which is amazing to our terrestrial conceptions.

Possibly the constituents of our solar system might collide with some

other unknown celestial body on this journey. But as the celestial

bodies are sparsely distributed, we may hope that many billions of

years will elapse before such a catastrophe will take place.

In mechanical respects the stability of our system appeared to be well

established. Since the modern theory of heat has made its triumphant

entry into natural science, however, the aspect of matters has changed.

We are convinced that all life and all motion on the earth can be

traced back to solar radiation. The tidal motions alone make a rather

unimportant exception. We have to ask ourselves: Will not the store of

energy in the sun, which goes out, not only to the planets, but to a

far greater extent into unknown domains of cold space, come to an end,

and will not that be the end of all the joys and sorrows of earthly

existence? The position appears desperate when we consider that only

one part in 2300 millions of the solar radiation benefits the earth,

and perhaps ten times as much the whole system, with all its moons.

The solar radiation is so powerful that every gramme of the mass of

the sun loses two calories in the course of a year. If, therefore, the

specific heat of the sun were the same as that of water, which in this

respect surpasses most other substances, the solar temperature would

fall by 2° Cent. (3.6° F.) every year. As, now, the temperature of the

sun in its outer portion has been estimated at from 6000° to 7000°, the

sun should have cooled completely within historical times. And though

the interior of the sun most probably has a vastly higher temperature

than the outer portions which we can observe, we should, all the

same, have to expect that the solar temperature and radiation would

noticeably have diminished in historical times. But all the documents

from ancient Babylon and Egypt seem to point out that the climate at

the dawn of historical times was in those countries nearly the same as

at present, and that, therefore, the sun shone over the most ancient

representatives of culture in the same way as it shines on their

descendants now.

The thesis has frequently been advanced, therefore, that the sun has

in its heat balance not only an expenditure side, but also an almost

equally substantial income side. The German physician R. Mayer,

who has the immortal merit of first having given expression to the

conception of a relation between heat and mechanical work, directed his

attention also to the household of the sun. He suggested that swarms

of meteorites, rushing into the sun with an amazing velocity (of over

600 km. per second), would, when stopped in their motion, generate

heat at the rate of 45 million calories per gramme of meteorites. In

future ages it would be the turn of the planets to sustain for some

time longer the spark of life in the sun, by the sacrifice of their

own existences. The sun would therefore, like the god Saturn, have to

devour its own children in order to continue its existence. Of how

little avail that would be we learn from the consideration that the

fall of the earth into the sun would not be able to prolong the heat

expenditure of the sun by as many as a hundred years. By their rush

into the sun, almost uniformly from all sides, the meteorites would,

moreover, long since have put a stop to the rotation of the sun about

its axis. Further, by virtue of the increasing mass and the hence

augmenting attraction of the sun, the length of our year would have

had to diminish by about 2.8 seconds per year, which is in absolute

contradiction to the observations of the astronomers. According to

Mayer’s thesis, a corresponding number of meteorites would, finally,

also have to tumble upon the surface of the earth, and (according to

data which will be furnished in Chapter IV.) they should raise the

surface temperature to about 800°. The thesis is therefore misleading.

Worlds in the making: The evolution of the universe · 第 4 / 15 段