VOLCANIC PHENOMENA AND EARTHQUAKES, concluded …
The map sketch (Fig. 15) by Suess represents the earthquake lines of Sicily and Calabria.
These districts have, as mentioned before, been devastated by severe earthquakes, of which the most terrible occurred in the year 1783, and again in 1905 and 1907.
They have also been the scene of many smaller concussions.
The bottom of the Tyrrhenian Sea between Italy, Sicily, and Sardinia has been lowered in rather recent ages and is still sinking.
We notice on the map five dotted lines, corresponding to cracks in the crust of the earth.
These lines would intersect in the volcanic district of the Lipari Islands.
We further see a dotted circular arc corresponding to a fissure which is regarded as the source of the Calabrian earthquakes of 1783, 1905, and 1907.
The earth-crust behaved somewhat after the manner of a windowpane which was burst by a heavy impact from a point corresponding to the Island of Lipari.
From this point radiate lines of fracture, and fragments have been broken off from the earth-crust by arc-shaped cracks, The volcano Etna is situated on the intersection of the radial and circular fissures.
In recognition of the high practical importance of earthquake observations, seismological stations have in recent days been erected in many localities.
At these observatories the earthquakes are recorded by pendulums whose styles draw lines on tapes of paper moved by clock-work.
As long as the earth is quiet the drawn line is straight.
When earthquakes set in, the line passes into a wavy curve.
As long as the movement of the paper is slow, the curve merely looks like a widened straight line.
The subjoined illustration (Fig. 16) represents a seismogram taken at the station of Shide, on the Isle of Wight, on August 31, 1898.
The earthquake recorded originated in the Centre G, in the Indian Ocean.
The origin has been deduced from the moments of arrival of the different waves at different stations.
We notice on the seismogram a faint widening of the straight line at 20 hrs. 5 min. 2 sec. (8 hrs. 5 min. 2 sec. P.M.).
The amplitude of the oscillations then began to widen, and the heaviest concussions were noticed at 20 hrs. 36 min. 25 sec., and 20 hrs. 42 min. 49 sec., after which the amplitudes slowly decreased with smaller shocks.
The first shock of 20 hrs. 5 min. 2 sec. is called the preliminary tremor.
This tremor passes through the interior of the earth at a velocity of propagation of 9.2 km. (5 1 miles) per second.
It would require twenty-three minutes to pass through the earth along a diameter.
The tremor is very feeble, which is ascribed to the extraordinarily great friction characteristic of the strongly heated gases which are confined in the interior of the earth.
The principal violent shock at 20 hrs. 36 min. 25 sec. was caused by a wave travelling through the solid crust of the earth.
The intensity of this shock is much less impaired than that of the just-mentioned tremor, and it travels with the smaller velocity of about 3.4 km. (2.1 miles) along the earth's surface.
The velocity of propagation of concussion pulses has been calculated for a mountain of quartz, in which it would be 3.6 km. (2.2 miles) per second, very nearly the same as the last-mentioned figure.
We should expect this, since the firm crust of the earth consists essentially of solid silicates i.e., compounds of quartz endowed with similar properties.
Measured at small distances from the origin, the velocity of propagation of the wave appears smaller, and the first preliminary tremor is frequently not observed.
The velocity may be diminished to 2 km. (1J miles) per second.
The reason is that the pulse partly describes a curve in the more solid portions of the crust, and partly passes through looser strata, through which the wave travels at a much slower rate than in firm ground; for instance, at 1.2 km. through loose sandstones, at 1.4 km. through the water of the ocean, and at 0.3 km. through loose sand.
We recognize that it should be possible to calculate the distance between the point of observation and the origin of the earthquake from the data relating to the arrivals of the first preliminary tremor and of the principal shock of maximum amplitude.
The violent shock is sometimes repeated after a certain time, though with decreased intensity.
It has often been observed that this secondary, less violent, shock seems to have travelled all round the earth via the longest road between the origin and the point of observation, just like one portion of the aerial waves in the eruption of Krakatoa (compare page 27).
The velocity of propagation of this secondary shock is the same as that of the principal shock.
Milne has deduced from his observations that, when the line joining the origin of the earthquake and the point of observation does not at its lowest level descend deeper than 50 km. below the surface of the earth, the pulse will travel undivided through the solid crust of the earth.
For this reason we estimate the thickness of the solid crust at 50 km.
The value is in almost perfect agreement with the one which we had (on page 16) derived from the increase of temperature with greater depths.
It should further be mentioned, perhaps, that the density of the earth in the vicinity has been determined from pendulum observation, and that this density seems to be rather variable down to the depths of 50 or 60 km., but to become more uniform at greater depths.
These 50 or 60 km. (31 or 37 miles) would belong to the solid crust of the earth.
The movement of earthquake shocks through the earth thus teaches us that the solid earth-crust cannot be very thick, and that the core of the earth is probably gaseous.
The similar conclusions, to which these various considerations had led us, may therefore come very near the truth.
A careful study of seismograms may, we hope, help us to learn more about the central portions of the earth, which at first sight appear to be absolutely inaccessible to scientific research.
TO BE CONTINUED ...
ARRHENIUS, WORLDS IN THE MAKING
Re: ARRHENIUS, WORLDS IN THE MAKING
THE CELESTIAL BODIES, IN PARTICULAR THE EARTH, AS ABODES OF ORGANISMS
THERE is no more elevating spectacle than to contemplate the sky with its thousands of stars on a clear night.
When we send our thoughts to those lights glittering in infinite distance, the question forces itself upon us, whether there are not out there planets like our own that will sustain organic life.
How little interest do we take in a barren island of the Arctic Circle, on which not a single plant will grow, compared to an island in the tropics which is teeming with life in its most wonderful variety!
The unknown worlds occupy our minds much more when we may fancy them inhabited than when we have to regard them as dead masses floating about in space.
We have to ask ourselves similar questions with regard to our own little planet, the earth.
Was it always covered with verdure, or was it once sterile and barren?
And if that be so, what are the conditions under which the earth can fulfil its actual part of harboring organic life?
That "the earth was without form" in the beginning is unquestionable.
It does not matter whether we assume that it was once all through an incandescent liquid, which may be the most probable assumption, or that it was, as Lockyer and Moulton think, formed by the accumulation of meteoric stones which became incandescent when arrested in their motion.
We have seen that the earth probably consists of a mass of gas encased within a shell which is solid on the outside and remains a viscid liquid on the inner side.
We presume with good reason that the earth was originally a mass of gas separated from the sun, which is still in the same state.
By radiation into cold space the sphere of gas which, on the whole, would behave as our sun does now, would gradually lose its high temperature, and finally a solid crust could form on its surface.
Lord Kelvin has calculated that it would not require more than one hundred years before the temperature of this crust would sink to 100.
Supposing, even, that Kelvin's calculations should not quite be confirmed, we may yet maintain that not many thousands of years would have elapsed from the time when the earth assumed its first crust at about 1000 till the age when this temperature had fallen below 100 (212 F.).
Living beings certainly could not exist so long, since the albumen of the cells would at once coagulate at the temperature of boiling water, like the white of an egg.
Yet it has been reported that some of the hot springs of New Zealand contain algae, although at a temperature of over 80.
When I went to Yellowstone Park to inquire into the correctness of this statement, I found that the algae existed only at the edge of the hot springs, where the temperature did not exceed 60 (140 F.).
The famous American physiologist Loeb states that we do not meet with algae in hot springs at temperatures above 55.
Since, now, the temperature of the earth-crust would much more quickly sink from 100 to 55 than it had fallen from 1000 to 100, we may imagine that only a few thousands of years may have intervened between the formation of the first crust of the earth and the cooling down to a temperature such as would sustain life.
Since that time the temperature has probably never been so low that the larger portion of the earth's surface would not have been able to support organisms, although there have been several glacial ages in which the arctic districts inaccessible to life must have extended much farther than at present.
The ocean will also have been free of ice over much the greatest portion of its surface at all times, and may therefore have been inhabited by organisms in all ages.
The interior of the earth cools continually, though slowly, because heat passes from the inner, warmer portions to the other, cooler portions through the crust of the earth.
The earth is able to serve as the abode of living Beings because its outer portions are cooled to a suitable temperature (below 55) by radiation, and because the cooling does not proceed so far that the open sea would continually be frozen over, and that the temperature on the Continent would always remain below freezing-point.
We owe this favorable intermediate stage to the fact that the radiation from the sun balances the loss of heat by radiation into space, and that it is capable of maintaining the greater portion of the surface of the earth at a temperature above the freezing-point of water.
The temperature conditioning life on a planet is therefore maintained only because, on the one side, light and heat are received by radiation from the sun in sufficient quantities, while on the other side an equivalent radiation of heat takes place into space.
If the heat gain and the heat loss were not to balance each other, the term of suitable conditions would not last long.
The temperature of the earth-crust could sink in a few hundreds or thousands of years from 1000 to 100, because when the earth was at this high temperature its radiation into space predominated over the radiation received from the sun.
On the other hand, about a hundred million years have passed, according to Joly, since the age when the ocean originated.
The temperature of the earth, therefore, required this long space of time in order to cool down from 365 (at which temperature water vapor can first be condensed to liquid water) to its present temperature.
The cooling afterwards proceeded at a slower rate, because the difference between the radiations inward and outward was lessened with the diminishing temperature of the earth.
Various methods have been applied in estimating these periods.
Joly based his estimate on the percentage of salt in the sea and in the rivers.
If we calculate how much salt there is in the sea, and how much salt the rivers can supply to it in the course of a year, we arrive at the result that the quantity of salt now stored in the ocean might have been supplied in about a hundred million years.
TO BE CONTINUED ...
THERE is no more elevating spectacle than to contemplate the sky with its thousands of stars on a clear night.
When we send our thoughts to those lights glittering in infinite distance, the question forces itself upon us, whether there are not out there planets like our own that will sustain organic life.
How little interest do we take in a barren island of the Arctic Circle, on which not a single plant will grow, compared to an island in the tropics which is teeming with life in its most wonderful variety!
The unknown worlds occupy our minds much more when we may fancy them inhabited than when we have to regard them as dead masses floating about in space.
We have to ask ourselves similar questions with regard to our own little planet, the earth.
Was it always covered with verdure, or was it once sterile and barren?
And if that be so, what are the conditions under which the earth can fulfil its actual part of harboring organic life?
That "the earth was without form" in the beginning is unquestionable.
It does not matter whether we assume that it was once all through an incandescent liquid, which may be the most probable assumption, or that it was, as Lockyer and Moulton think, formed by the accumulation of meteoric stones which became incandescent when arrested in their motion.
We have seen that the earth probably consists of a mass of gas encased within a shell which is solid on the outside and remains a viscid liquid on the inner side.
We presume with good reason that the earth was originally a mass of gas separated from the sun, which is still in the same state.
By radiation into cold space the sphere of gas which, on the whole, would behave as our sun does now, would gradually lose its high temperature, and finally a solid crust could form on its surface.
Lord Kelvin has calculated that it would not require more than one hundred years before the temperature of this crust would sink to 100.
Supposing, even, that Kelvin's calculations should not quite be confirmed, we may yet maintain that not many thousands of years would have elapsed from the time when the earth assumed its first crust at about 1000 till the age when this temperature had fallen below 100 (212 F.).
Living beings certainly could not exist so long, since the albumen of the cells would at once coagulate at the temperature of boiling water, like the white of an egg.
Yet it has been reported that some of the hot springs of New Zealand contain algae, although at a temperature of over 80.
When I went to Yellowstone Park to inquire into the correctness of this statement, I found that the algae existed only at the edge of the hot springs, where the temperature did not exceed 60 (140 F.).
The famous American physiologist Loeb states that we do not meet with algae in hot springs at temperatures above 55.
Since, now, the temperature of the earth-crust would much more quickly sink from 100 to 55 than it had fallen from 1000 to 100, we may imagine that only a few thousands of years may have intervened between the formation of the first crust of the earth and the cooling down to a temperature such as would sustain life.
Since that time the temperature has probably never been so low that the larger portion of the earth's surface would not have been able to support organisms, although there have been several glacial ages in which the arctic districts inaccessible to life must have extended much farther than at present.
The ocean will also have been free of ice over much the greatest portion of its surface at all times, and may therefore have been inhabited by organisms in all ages.
The interior of the earth cools continually, though slowly, because heat passes from the inner, warmer portions to the other, cooler portions through the crust of the earth.
The earth is able to serve as the abode of living Beings because its outer portions are cooled to a suitable temperature (below 55) by radiation, and because the cooling does not proceed so far that the open sea would continually be frozen over, and that the temperature on the Continent would always remain below freezing-point.
We owe this favorable intermediate stage to the fact that the radiation from the sun balances the loss of heat by radiation into space, and that it is capable of maintaining the greater portion of the surface of the earth at a temperature above the freezing-point of water.
The temperature conditioning life on a planet is therefore maintained only because, on the one side, light and heat are received by radiation from the sun in sufficient quantities, while on the other side an equivalent radiation of heat takes place into space.
If the heat gain and the heat loss were not to balance each other, the term of suitable conditions would not last long.
The temperature of the earth-crust could sink in a few hundreds or thousands of years from 1000 to 100, because when the earth was at this high temperature its radiation into space predominated over the radiation received from the sun.
On the other hand, about a hundred million years have passed, according to Joly, since the age when the ocean originated.
The temperature of the earth, therefore, required this long space of time in order to cool down from 365 (at which temperature water vapor can first be condensed to liquid water) to its present temperature.
The cooling afterwards proceeded at a slower rate, because the difference between the radiations inward and outward was lessened with the diminishing temperature of the earth.
Various methods have been applied in estimating these periods.
Joly based his estimate on the percentage of salt in the sea and in the rivers.
If we calculate how much salt there is in the sea, and how much salt the rivers can supply to it in the course of a year, we arrive at the result that the quantity of salt now stored in the ocean might have been supplied in about a hundred million years.
TO BE CONTINUED ...
Re: ARRHENIUS, WORLDS IN THE MAKING
THE CELESTIAL BODIES, IN PARTICULAR THE EARTH, AS ABODES OF ORGANISMS, continued ...
We arrive at still higher numbers when we calculate the time which must have elapsed during the deposition of all the stratified and sedimentary layers.
Sir Archibald Geikie estimates the total thickness of those strata, supposing them to have been undisturbed, at 30,000 m. (nearly 20 miles).
He concludes, further, from the examination of more recent strata, that every stratum one metre in thickness must have required from 3000 to 20,000 years for its formation.
We should, therefore, have to allow a space of from ninety to six hundred million years for the deposition of all the sedimentary strata.
The Finnish geologist Sederholm even fixes the time at a thousand million years.
Another method again starts from the consideration that, while the temperature of the surface of the earth remains fairly steady owing to the heat exchange between solar radiation and terrestrial radiation into space, the interior of the earth must have shrunk with the cooling.
How far this shrinkage extends we may estimate from the formation of the mountain chains which, according to Rudzki, cover 1.6 per cent, of the earth's surface.
The earth's radius should consequently have contracted by about 0.8 per cent., corresponding to a cooling through about 300, which would require two thousand million years.
Quite recently the renowned physical chemist Rutherford has expounded a most original method of estimating the age of minerals.
Uranium and thorium are supposed to produce helium by their slow dissociation, and we know how much helium is produced from a certain quantity of uranium or thorium in a year.
Now Ramsay has determined the percentage of helium in the uranium mineral fergusonite and in thorianite.
Rutherford then calculates the time which would have passed since the formation of these minerals.
He demands at least four hundred million years, "for very probably some helium has escaped from the minerals during that time."
Although this estimate is very uncertain, it is interesting to find that it leads to an age for the solid earth-crust of the same order of magnitude as the other methods.
During this whole epoch of almost inconceivable length of between one hundred million and two thousand million years, organisms have existed on the surface of the earth and in the sea which do not differ so very much from those now alive.
The temperature of the surface may have been higher than it is at present; but the difference cannot be very great, and will amount to 20 Cent. (36 F.) at the highest.
The actual mean temperature of the surface of the earth is 16 Cent. (61 F.).
It varies from about 20 Cent. (-4F.) at the North Pole, and -10 Cent. ( + 14 F.) at the South Pole to 26 Cent. (79 F.) in the tropical zone.
The main difference between the temperatures of the earth's surface in the most remote period from which fossils are extant and the actual state rather seems to be that the different zones of the earth are now characterized by unequal temperatures, while in the remote epochs the heat was almost uniformly distributed over the whole earth.
TO BE CONTINUED ...
We arrive at still higher numbers when we calculate the time which must have elapsed during the deposition of all the stratified and sedimentary layers.
Sir Archibald Geikie estimates the total thickness of those strata, supposing them to have been undisturbed, at 30,000 m. (nearly 20 miles).
He concludes, further, from the examination of more recent strata, that every stratum one metre in thickness must have required from 3000 to 20,000 years for its formation.
We should, therefore, have to allow a space of from ninety to six hundred million years for the deposition of all the sedimentary strata.
The Finnish geologist Sederholm even fixes the time at a thousand million years.
Another method again starts from the consideration that, while the temperature of the surface of the earth remains fairly steady owing to the heat exchange between solar radiation and terrestrial radiation into space, the interior of the earth must have shrunk with the cooling.
How far this shrinkage extends we may estimate from the formation of the mountain chains which, according to Rudzki, cover 1.6 per cent, of the earth's surface.
The earth's radius should consequently have contracted by about 0.8 per cent., corresponding to a cooling through about 300, which would require two thousand million years.
Quite recently the renowned physical chemist Rutherford has expounded a most original method of estimating the age of minerals.
Uranium and thorium are supposed to produce helium by their slow dissociation, and we know how much helium is produced from a certain quantity of uranium or thorium in a year.
Now Ramsay has determined the percentage of helium in the uranium mineral fergusonite and in thorianite.
Rutherford then calculates the time which would have passed since the formation of these minerals.
He demands at least four hundred million years, "for very probably some helium has escaped from the minerals during that time."
Although this estimate is very uncertain, it is interesting to find that it leads to an age for the solid earth-crust of the same order of magnitude as the other methods.
During this whole epoch of almost inconceivable length of between one hundred million and two thousand million years, organisms have existed on the surface of the earth and in the sea which do not differ so very much from those now alive.
The temperature of the surface may have been higher than it is at present; but the difference cannot be very great, and will amount to 20 Cent. (36 F.) at the highest.
The actual mean temperature of the surface of the earth is 16 Cent. (61 F.).
It varies from about 20 Cent. (-4F.) at the North Pole, and -10 Cent. ( + 14 F.) at the South Pole to 26 Cent. (79 F.) in the tropical zone.
The main difference between the temperatures of the earth's surface in the most remote period from which fossils are extant and the actual state rather seems to be that the different zones of the earth are now characterized by unequal temperatures, while in the remote epochs the heat was almost uniformly distributed over the whole earth.
TO BE CONTINUED ...
Re: ARRHENIUS, WORLDS IN THE MAKING
THE CELESTIAL BODIES, IN PARTICULAR THE EARTH, AS ABODES OF ORGANISMS, continued ...
The condition for this prolonged, almost stationary state was that the gain of heat of the earth's surface by radiation from the sun and the loss of heat by radiation into space nearly balanced each other.
That the replenishing supply by radiation from an intensely hot body in our case the sun is indispensable for the existence of life will be evident to everybody.
Not everybody may, however, have considered that the loss of heat into cold space or into colder surroundings is just as indispensable.
To some people, indeed, the assumption that the earth as well as the sun should waste the largest portions of their vital heat as radiation into cold space appears so unsatisfactory that they prefer to believe radiation to be confined to radiation between celestial bodies; there is no radiation into space, in their opinion.
All the solar heat would thus benefit the planets and the moons in the solar system, and only a vanishing portion of it would fall upon the fixed stars, because their visual angles are so small.
If that were really correct, the temperature of the planets would rise at a rapid rate until it became almost equal to that of the sun, and all life would become impossible.
We are therefore constrained to admit that "things are best as they are," although the great waste of solar heat certainly weakens the solar energy.
The opinion that all the solar heat radiated into infinite space is wasted, starts moreover from a hypothesis which is not proved, and which is highly improbable namely, that only an extremely small portion of the sky is covered with celestial bodies.
TO BE CONTINUED ...
The condition for this prolonged, almost stationary state was that the gain of heat of the earth's surface by radiation from the sun and the loss of heat by radiation into space nearly balanced each other.
That the replenishing supply by radiation from an intensely hot body in our case the sun is indispensable for the existence of life will be evident to everybody.
Not everybody may, however, have considered that the loss of heat into cold space or into colder surroundings is just as indispensable.
To some people, indeed, the assumption that the earth as well as the sun should waste the largest portions of their vital heat as radiation into cold space appears so unsatisfactory that they prefer to believe radiation to be confined to radiation between celestial bodies; there is no radiation into space, in their opinion.
All the solar heat would thus benefit the planets and the moons in the solar system, and only a vanishing portion of it would fall upon the fixed stars, because their visual angles are so small.
If that were really correct, the temperature of the planets would rise at a rapid rate until it became almost equal to that of the sun, and all life would become impossible.
We are therefore constrained to admit that "things are best as they are," although the great waste of solar heat certainly weakens the solar energy.
The opinion that all the solar heat radiated into infinite space is wasted, starts moreover from a hypothesis which is not proved, and which is highly improbable namely, that only an extremely small portion of the sky is covered with celestial bodies.
TO BE CONTINUED ...
Re: ARRHENIUS, WORLDS IN THE MAKING
THE CELESTIAL BODIES, IN PARTICULAR THE EARTH, AS ABODES OF ORGANISMS, continued …
That might certainly be correct if we assumed, as has formerly been done, that the majority of the celestial bodies must be luminous.
We do not possess, however, any reliable knowledge of the number and size of the dark celestial bodies.
In order to account for the observed movements of different stars, it has been thought that there must be in the neighborhood of some of them dark stars of enormous size whose masses would surpass the mass of our sun, or, at least, be equal to it.
But the largest number of the dark celestial bodies which hide the rays from the stars behind them probably consist of smaller particles, such as we observe in meteors and in comets, and to a large extent of so-called cosmical dust.
The observations of later years, by the aid of most powerful instruments, have shown that so-called nebulse and nebulous stars abound throughout the heavens.
In their interior we should probably find accumulations of dark masses.
The light intensity of most of the nebulae is, moreover, far too weak to permit of their being perceived.
We have, therefore, to imagine that there are bodies all through infinite space, and about as numerous as they are in the immediate neighborhood of our solar system.
Thus every ray from the sun, of whatever direction, would finally hit upon some celestial body, and nothing would be lost of the solar radiation, nor of the stellar radiation.
As regards the radiation-heat exchange, the earth might be likened to a steam-engine.
In order that the steam-engine shall perform useful work, it is necessary not only that the engine be supplied with heat of high temperature from a furnace and a boiler, but also that the engine be able to give its heat up again to a heat reservoir of lower temperature a condenser or cooler.
It is only by transferring heat from a body of higher temperature to another body of lower temperature that the engine can do work.
In a similar way no work can be done on the earth, and no life can exist, unless heat be conferred by the intermediation of the earth from a hot body, the sun, to the colder surroundings of universal space i. e., to the cold celestial bodies in it.
TO BE CONTINUED ...
That might certainly be correct if we assumed, as has formerly been done, that the majority of the celestial bodies must be luminous.
We do not possess, however, any reliable knowledge of the number and size of the dark celestial bodies.
In order to account for the observed movements of different stars, it has been thought that there must be in the neighborhood of some of them dark stars of enormous size whose masses would surpass the mass of our sun, or, at least, be equal to it.
But the largest number of the dark celestial bodies which hide the rays from the stars behind them probably consist of smaller particles, such as we observe in meteors and in comets, and to a large extent of so-called cosmical dust.
The observations of later years, by the aid of most powerful instruments, have shown that so-called nebulse and nebulous stars abound throughout the heavens.
In their interior we should probably find accumulations of dark masses.
The light intensity of most of the nebulae is, moreover, far too weak to permit of their being perceived.
We have, therefore, to imagine that there are bodies all through infinite space, and about as numerous as they are in the immediate neighborhood of our solar system.
Thus every ray from the sun, of whatever direction, would finally hit upon some celestial body, and nothing would be lost of the solar radiation, nor of the stellar radiation.
As regards the radiation-heat exchange, the earth might be likened to a steam-engine.
In order that the steam-engine shall perform useful work, it is necessary not only that the engine be supplied with heat of high temperature from a furnace and a boiler, but also that the engine be able to give its heat up again to a heat reservoir of lower temperature a condenser or cooler.
It is only by transferring heat from a body of higher temperature to another body of lower temperature that the engine can do work.
In a similar way no work can be done on the earth, and no life can exist, unless heat be conferred by the intermediation of the earth from a hot body, the sun, to the colder surroundings of universal space i. e., to the cold celestial bodies in it.
TO BE CONTINUED ...
Re: ARRHENIUS, WORLDS IN THE MAKING
THE CELESTIAL BODIES, IN PARTICULAR THE EARTH, AS ABODES OF ORGANISMS, continued …
To a certain extent the temperature of the earth's surface, as we shall presently see, is conditioned by the properties of the atmosphere surrounding it, and particularly by the permeability of the latter for the rays of heat.
If the earth did not possess an atmosphere, or if this atmosphere were perfectly diathermal i.e., pervious to heat radiations we should be able to calculate the mean temperature of the earth's surface, given the intensity of the solar radiation, from Stefan's law of the dependence of heat radiation on its temperature.
Starting from the not improbable assumption that, at a mean distance of the earth from the sun, the solar rays would send 2.5 gramme-calories per minute to a body of cross section of 1 sq. centimetre at right angles to the rays of the sun, Christiansen has calculated the mean temperatures of the surfaces of the various planets.
In the case of Mercury, I have added another figure, 332.
Mercury always turns the same side to the sun, and the hottest point of this side would reach a temperature of 397; its mean temperature, according to my calculation, is 332, while the other side, turned away from the sun, cannot be at a temperature much above absolute zero, 273.
I have made a similar calculation for the moon, which turns so slowly about its axis (once in twenty-seven days) that the temperature on the side illuminated by the sun remains almost as high (106) as if the moon were always turning the same face to the sun.
The hottest point of this surface would attain a temperature of 150, while the poles of the moon and that part of the other side which remains longest without illumination can, again, not be much above absolute zero temperature.
This estimate is in fair agreement with the measurements made of the lunar radiation and the temperature estimate based upon it.
The first measurement of this kind was made by the Earl of Rosse.
He ascertained that the moon disk as illuminated by the sun that is to say, the full moon would radiate as much heat as a black body of the temperature 110 Cent. (230 F.).
A later measurement by the American Very seems to indicate that the hottest point of the moon is at about 180, which would be 30 higher than my estimate.
In the cases of the moon and of Mercury, which do not possess any atmosphere to speak of, this calculation may very fairly agree with the actual state of affairs.
The temperature of the planet Venus would be about 65 Cent. (149 F.) if its atmosphere were perfectly transparent.
We know, however, that dense clouds, probably of water drops, are floating in the atmosphere of this planet, preventing us from seeing its land and water surfaces.
According to the determinations made by Zollner and others, Venus would reflect not less than 76 per cent, of the incident light of the sun, and the planet would thus be as white as a snow-ball.
The rays of heat are not reflected to the same extent.
We may estimate that the portion of heat absorbed by the planet is about half the incident heat.
The temperature of Venus will therefore be reduced considerably, but it is partly augmented again by the protective action of this atmosphere.
The mean temperature of Venus may, hence, not differ much from the calculated temperature, and may amount to about 40 (104 F.).
Under these circumstances the assumption would appear plausible that a very considerable portion of the surface of Venus, and particularly the districts about the poles, would be favorable to organic life.
TO BE CONTINUED ...
To a certain extent the temperature of the earth's surface, as we shall presently see, is conditioned by the properties of the atmosphere surrounding it, and particularly by the permeability of the latter for the rays of heat.
If the earth did not possess an atmosphere, or if this atmosphere were perfectly diathermal i.e., pervious to heat radiations we should be able to calculate the mean temperature of the earth's surface, given the intensity of the solar radiation, from Stefan's law of the dependence of heat radiation on its temperature.
Starting from the not improbable assumption that, at a mean distance of the earth from the sun, the solar rays would send 2.5 gramme-calories per minute to a body of cross section of 1 sq. centimetre at right angles to the rays of the sun, Christiansen has calculated the mean temperatures of the surfaces of the various planets.
In the case of Mercury, I have added another figure, 332.
Mercury always turns the same side to the sun, and the hottest point of this side would reach a temperature of 397; its mean temperature, according to my calculation, is 332, while the other side, turned away from the sun, cannot be at a temperature much above absolute zero, 273.
I have made a similar calculation for the moon, which turns so slowly about its axis (once in twenty-seven days) that the temperature on the side illuminated by the sun remains almost as high (106) as if the moon were always turning the same face to the sun.
The hottest point of this surface would attain a temperature of 150, while the poles of the moon and that part of the other side which remains longest without illumination can, again, not be much above absolute zero temperature.
This estimate is in fair agreement with the measurements made of the lunar radiation and the temperature estimate based upon it.
The first measurement of this kind was made by the Earl of Rosse.
He ascertained that the moon disk as illuminated by the sun that is to say, the full moon would radiate as much heat as a black body of the temperature 110 Cent. (230 F.).
A later measurement by the American Very seems to indicate that the hottest point of the moon is at about 180, which would be 30 higher than my estimate.
In the cases of the moon and of Mercury, which do not possess any atmosphere to speak of, this calculation may very fairly agree with the actual state of affairs.
The temperature of the planet Venus would be about 65 Cent. (149 F.) if its atmosphere were perfectly transparent.
We know, however, that dense clouds, probably of water drops, are floating in the atmosphere of this planet, preventing us from seeing its land and water surfaces.
According to the determinations made by Zollner and others, Venus would reflect not less than 76 per cent, of the incident light of the sun, and the planet would thus be as white as a snow-ball.
The rays of heat are not reflected to the same extent.
We may estimate that the portion of heat absorbed by the planet is about half the incident heat.
The temperature of Venus will therefore be reduced considerably, but it is partly augmented again by the protective action of this atmosphere.
The mean temperature of Venus may, hence, not differ much from the calculated temperature, and may amount to about 40 (104 F.).
Under these circumstances the assumption would appear plausible that a very considerable portion of the surface of Venus, and particularly the districts about the poles, would be favorable to organic life.
TO BE CONTINUED ...
Re: ARRHENIUS, WORLDS IN THE MAKING
THE CELESTIAL BODIES, IN PARTICULAR THE EARTH, AS ABODES OF ORGANISMS, continued …
Passing to the earth, we find that the temperature-reducing influence of the clouds must be strong.
They protect about half of the earth's surface (52 per cent.) from solar radiation.
But even with a perfectly clear sky, not all the light from the sun really reaches the earth's surface; for finely distributed dust is floating even in the purest air.
I have estimated that this dust would probably absorb 17 per cent, of the solar heat.
Clouds and dust would therefore together deprive the earth of 34 per cent, of the heat sent to it, which would lead to a reduction of the temperature by about 28.
Dust and the water-bubbles in the clouds also prevent the radiation of heat from the earth, so that the total loss of heat to be charged to clouds and dust will amount to about 20 (36 F.).
It has now been ascertained that the mean temperature of the earth is 16 (61 F.), instead of the calculated 6.5 (43.7 F.).
Deducting the 20 due to the influence of dust and clouds, we obtain 14 (7 F.), and the observed temperature would therefore be higher than the calculated by no less than 30 (54 F.).
The discrepancy is explained by the heat-protecting action of the gases contained in the atmosphere, to which we shall presently refer (page 51).
There are but few clouds on Mars.
This planet is endowed with an atmosphere of extreme transparency, and should therefore have a high temperature.
Instead of the temperature of -37 (35 F.), calculated, the mean temperature seems to be +10 ( + 50 F.).
During the winter large white masses, evidently snow, collect on the poles of Mars, which rapidly melt away in spring and change into water that appears dark to us.
Sometimes the snow-caps on the poles of Mars disappear entirely during the Mars summer; this never happens on our terrestrial poles.
The mean temperature of Mars must therefore be above zero, probably about +10.
Organic life may very probably thrive, therefore, on Mars.
It is, however, rather sanguine to jump at the conclusion that the so-called canals of Mars prove its being inhabited by intelligent beings.
Many people regard the "canals" as optical illusions; Lowell's photographs, however, do not justify this opinion.
As regards the other large planets, the temperatures which we have calculated for them are very low.
This calculation is, however, rather illusory, because these planets probably do not possess any solid or liquid surface, but consist altogether of gases.
Their densities, at least, point in this direction.
In the case of the inner planets, Mars and our moon included, the density is rather less than that of the earth.
Mercury stands last among them, with its specific gravity of 0.564.
There follows a great drop in the specific gravities of the outer large planets.
Saturn, with a density of 0.116, is last in this order; the densities of the two outermost planets lie somewhat higher by 0.3 or 0.4 about but these last data are very uncertain.
Yet these figures are of the same order of magnitude as that assumed for the sun 0.25 and we believe that the sun, apart from the small clouds, is wholly a gaseous body.
It is therefore probable that the outer planets, including Jupiter, will also be gaseous and be surrounded by dense veils of clouds which prevent our looking down into their interior.
That view would contend against the idea that these planets can harbor any living beings.
We could rather imagine their moons to be inhabited.
If these moons received no heat from their planets, they would assume the above-stated temperatures of their central bodies.
Looked at from our moon, the earth appears under a visual angle, 3.7 times as large as that of the sun.
As the temperature of the sun has, from its radiation, been estimated at 6200 Cent., or 6500 absolute, the moon would receive as much heat from the earth as from the sun, if the earth had a temperature of about 3100 Cent., or 3380 absolute.
When the first clouds of water vapor were being formed in the terrestrial atmosphere, the earth's temperature was about 360, and the radiation from the earth to the moon only about 1.25- thousandth of that of the sun.
The present radiation from the earth does not even attain one- twentieth of this value.
It is thus manifest that the radiation from the earth does not play any part in the thermal household of the moon.
TO BE CONTINUED ...
Passing to the earth, we find that the temperature-reducing influence of the clouds must be strong.
They protect about half of the earth's surface (52 per cent.) from solar radiation.
But even with a perfectly clear sky, not all the light from the sun really reaches the earth's surface; for finely distributed dust is floating even in the purest air.
I have estimated that this dust would probably absorb 17 per cent, of the solar heat.
Clouds and dust would therefore together deprive the earth of 34 per cent, of the heat sent to it, which would lead to a reduction of the temperature by about 28.
Dust and the water-bubbles in the clouds also prevent the radiation of heat from the earth, so that the total loss of heat to be charged to clouds and dust will amount to about 20 (36 F.).
It has now been ascertained that the mean temperature of the earth is 16 (61 F.), instead of the calculated 6.5 (43.7 F.).
Deducting the 20 due to the influence of dust and clouds, we obtain 14 (7 F.), and the observed temperature would therefore be higher than the calculated by no less than 30 (54 F.).
The discrepancy is explained by the heat-protecting action of the gases contained in the atmosphere, to which we shall presently refer (page 51).
There are but few clouds on Mars.
This planet is endowed with an atmosphere of extreme transparency, and should therefore have a high temperature.
Instead of the temperature of -37 (35 F.), calculated, the mean temperature seems to be +10 ( + 50 F.).
During the winter large white masses, evidently snow, collect on the poles of Mars, which rapidly melt away in spring and change into water that appears dark to us.
Sometimes the snow-caps on the poles of Mars disappear entirely during the Mars summer; this never happens on our terrestrial poles.
The mean temperature of Mars must therefore be above zero, probably about +10.
Organic life may very probably thrive, therefore, on Mars.
It is, however, rather sanguine to jump at the conclusion that the so-called canals of Mars prove its being inhabited by intelligent beings.
Many people regard the "canals" as optical illusions; Lowell's photographs, however, do not justify this opinion.
As regards the other large planets, the temperatures which we have calculated for them are very low.
This calculation is, however, rather illusory, because these planets probably do not possess any solid or liquid surface, but consist altogether of gases.
Their densities, at least, point in this direction.
In the case of the inner planets, Mars and our moon included, the density is rather less than that of the earth.
Mercury stands last among them, with its specific gravity of 0.564.
There follows a great drop in the specific gravities of the outer large planets.
Saturn, with a density of 0.116, is last in this order; the densities of the two outermost planets lie somewhat higher by 0.3 or 0.4 about but these last data are very uncertain.
Yet these figures are of the same order of magnitude as that assumed for the sun 0.25 and we believe that the sun, apart from the small clouds, is wholly a gaseous body.
It is therefore probable that the outer planets, including Jupiter, will also be gaseous and be surrounded by dense veils of clouds which prevent our looking down into their interior.
That view would contend against the idea that these planets can harbor any living beings.
We could rather imagine their moons to be inhabited.
If these moons received no heat from their planets, they would assume the above-stated temperatures of their central bodies.
Looked at from our moon, the earth appears under a visual angle, 3.7 times as large as that of the sun.
As the temperature of the sun has, from its radiation, been estimated at 6200 Cent., or 6500 absolute, the moon would receive as much heat from the earth as from the sun, if the earth had a temperature of about 3100 Cent., or 3380 absolute.
When the first clouds of water vapor were being formed in the terrestrial atmosphere, the earth's temperature was about 360, and the radiation from the earth to the moon only about 1.25- thousandth of that of the sun.
The present radiation from the earth does not even attain one- twentieth of this value.
It is thus manifest that the radiation from the earth does not play any part in the thermal household of the moon.
TO BE CONTINUED ...
Re: ARRHENIUS, WORLDS IN THE MAKING
THE CELESTIAL BODIES, IN PARTICULAR THE EARTH, AS ABODES OF ORGANISMS, continued …
The relations would be quite different if the earth had the 11.6 times greater diameter of Jupiter, or the diameter of Saturn, which is 9.3 times greater than its own.
The radiation from the earth to the moon would then make up about a sixth or a ninth of the actual solar radiation, taking the temperature of the earth's surface at 360.
We can easily calculate, further, that Jupiter and Saturn would radiate as much heat against a moon at a distance of 240,000 or 191,000 km. respectively (since the distance of the moon from the earth amounts to 384,000 km.) as the sun sends to Mars taking the temperature of those planets at 360 Cent.
Now we find, near Jupiter as well as near Saturn, moons at the distances of 126,000 and 186,000 km. respectively, which are smaller than those mentioned, and it is not inconceivable that these moons receive from their central bodies sufficient heat to render life possible, provided that they be enveloped by a heat-absorbing atmosphere.
The conditions appear to be less favorable for the innermost satellites of Jupiter and Saturn.
When their planets are shining at the maximum brilliancy, their light intensity is only a sixth or a ninth of the solar light intensity, which upon these satellites is itself only one-twenty-seventh or one-ninetieth of the intensity on the earth.
During the incandescence epoch of these planets their moons will certainly for some time have been suitable for the development of life.
That the atmospheric envelopes limit the heat losses from the planets had been suggested about 1800 by the great French physicist Fourier.
His ideas were further developed afterwards by Pouillet and Tyndall.
Their theory has been styled the hot-house theory, because they thought that the atmosphere acted after the manner of the glass panes of hot-houses.
Glass possesses the property of being transparent to heat rays of small wave lengths belonging to the visible spectrum; but it is not transparent to dark heat rays, such, for instance, as are sent out by a heated furnace or by a hot lump of earth.
The heat rays of the sun now are to a large extent of the visible, bright kind.
They penetrate through the glass of the hot-house and heat the earth under the glass.
The radiation from the earth, on the other hand, is dark and cannot pass back through the glass, which thus stops any losses of heat, just as an overcoat protects the body against too strong a loss of heat by radiation.
Langley made an experiment with a box, which he packed with cotton-wool to reduce loss by radiation, and which he provided, on the side turned towards the sun, with a double glass pane.
He observed that the temperature rose to 113 (235 F.), while the thermometer only marked 14 or 15 (57 or 59 F.) in the shade.
This experiment was conducted on Pike's Peak, in Colorado, at an altitude of 4200 m. (13,800 ft.), on September 9, 1881, at 1 hr. 4 min. p.m., and therefore at a particularly intense solar radiation.
TO BE CONTINUED ...
The relations would be quite different if the earth had the 11.6 times greater diameter of Jupiter, or the diameter of Saturn, which is 9.3 times greater than its own.
The radiation from the earth to the moon would then make up about a sixth or a ninth of the actual solar radiation, taking the temperature of the earth's surface at 360.
We can easily calculate, further, that Jupiter and Saturn would radiate as much heat against a moon at a distance of 240,000 or 191,000 km. respectively (since the distance of the moon from the earth amounts to 384,000 km.) as the sun sends to Mars taking the temperature of those planets at 360 Cent.
Now we find, near Jupiter as well as near Saturn, moons at the distances of 126,000 and 186,000 km. respectively, which are smaller than those mentioned, and it is not inconceivable that these moons receive from their central bodies sufficient heat to render life possible, provided that they be enveloped by a heat-absorbing atmosphere.
The conditions appear to be less favorable for the innermost satellites of Jupiter and Saturn.
When their planets are shining at the maximum brilliancy, their light intensity is only a sixth or a ninth of the solar light intensity, which upon these satellites is itself only one-twenty-seventh or one-ninetieth of the intensity on the earth.
During the incandescence epoch of these planets their moons will certainly for some time have been suitable for the development of life.
That the atmospheric envelopes limit the heat losses from the planets had been suggested about 1800 by the great French physicist Fourier.
His ideas were further developed afterwards by Pouillet and Tyndall.
Their theory has been styled the hot-house theory, because they thought that the atmosphere acted after the manner of the glass panes of hot-houses.
Glass possesses the property of being transparent to heat rays of small wave lengths belonging to the visible spectrum; but it is not transparent to dark heat rays, such, for instance, as are sent out by a heated furnace or by a hot lump of earth.
The heat rays of the sun now are to a large extent of the visible, bright kind.
They penetrate through the glass of the hot-house and heat the earth under the glass.
The radiation from the earth, on the other hand, is dark and cannot pass back through the glass, which thus stops any losses of heat, just as an overcoat protects the body against too strong a loss of heat by radiation.
Langley made an experiment with a box, which he packed with cotton-wool to reduce loss by radiation, and which he provided, on the side turned towards the sun, with a double glass pane.
He observed that the temperature rose to 113 (235 F.), while the thermometer only marked 14 or 15 (57 or 59 F.) in the shade.
This experiment was conducted on Pike's Peak, in Colorado, at an altitude of 4200 m. (13,800 ft.), on September 9, 1881, at 1 hr. 4 min. p.m., and therefore at a particularly intense solar radiation.
TO BE CONTINUED ...
Re: ARRHENIUS, WORLDS IN THE MAKING
THE CELESTIAL BODIES, IN PARTICULAR THE EARTH, AS ABODES OF ORGANISMS, continued …
Fourier and Pouillet now thought that the atmosphere of our earth should be endowed with properties resembling those of glass, as regards permeability of heat.
Tyndall later proved this assumption to be correct.
The chief invisible constitutents of the air which participate in this effect are water vapor, which is always found in a certain quantity in the air, and carbonic acid, also ozone and hydrocarbons.
These latter occur in such small quantities that no allowance has been made for them so far in the calculations.
Of late, however, we have been supplied with very careful observations on the permeability to heat of carbonic acid and of water vapor.
With the help of these data I have calculated that if the atmosphere were deprived of all its carbonic acid of which it contains only 0.03 per cent, by volume the temperature of the earth's surface would fall by about 21.
This lowering of the temperature would diminish the amount of water vapor in the atmosphere, and would cause a further almost equally strong fall of temperature.
The examples, so far as they go, demonstrate that comparatively unimportant variations in the composition of the air have a very great influence.
If the quantity of carbonic acid in the air should sink to one-half its present percentage, (296 ppm) the temperature would fall by about 4; a diminution to one-quarter would reduce the temperature by 8.
On the other hand, any doubling of the percentage of carbon dioxide in the air would raise the temperature of the earth's surface by 4; and if the carbon dioxide were increased fourfold, the temperature would rise by 8.
Further, a diminution of the carbonic acid percentage would accentuate the temperature differences between the different portions of the earth, while an increase in this percentage would tend to equalize the temperature.
The question, however, is whether any such temperature fluctuations have really been observed on the surface of the earth.
The geologists would answer: yes.
Our historical era was preceded by a period in which the mean temperature was by 2 (3.6 F.) higher than at present.
We recognize this from the former distribution of the ordinary hazel-nut and of the water-nut (Trapanalans).
Fossil nuts of these two species have been found in localities where the plants could not thrive in the present climate.
This age, again, was preceded by an age which, we are pretty certain, drove the inhabitants of northern Europe from their old abodes.
The glacial age must have been divided into several periods, alternating with intervals of milder climates, the so-called inter-glacial periods.
The space of time which is characterized by these glacial periods, when the temperature according to measurements based upon the study of the spreading of glaciers in the Alps must have been about 5 (8 F.) lower than now, has been estimated by geologists at not less than 100,000 years.
This epoch was preceded by a warmer age, in which the temperature, to judge from fossilized plants of those days, must at times have been by 8 or 9 (14 or 16 F.) higher than at present, and, moreover, much more uniformly distributed over the whole earth (Eocene).
Pronounced fluctuations of this kind in the climate have also occurred in former geological periods.
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 Hogbom, 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, 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.
TO BE CONTINUED...
Fourier and Pouillet now thought that the atmosphere of our earth should be endowed with properties resembling those of glass, as regards permeability of heat.
Tyndall later proved this assumption to be correct.
The chief invisible constitutents of the air which participate in this effect are water vapor, which is always found in a certain quantity in the air, and carbonic acid, also ozone and hydrocarbons.
These latter occur in such small quantities that no allowance has been made for them so far in the calculations.
Of late, however, we have been supplied with very careful observations on the permeability to heat of carbonic acid and of water vapor.
With the help of these data I have calculated that if the atmosphere were deprived of all its carbonic acid of which it contains only 0.03 per cent, by volume the temperature of the earth's surface would fall by about 21.
This lowering of the temperature would diminish the amount of water vapor in the atmosphere, and would cause a further almost equally strong fall of temperature.
The examples, so far as they go, demonstrate that comparatively unimportant variations in the composition of the air have a very great influence.
If the quantity of carbonic acid in the air should sink to one-half its present percentage, (296 ppm) the temperature would fall by about 4; a diminution to one-quarter would reduce the temperature by 8.
On the other hand, any doubling of the percentage of carbon dioxide in the air would raise the temperature of the earth's surface by 4; and if the carbon dioxide were increased fourfold, the temperature would rise by 8.
Further, a diminution of the carbonic acid percentage would accentuate the temperature differences between the different portions of the earth, while an increase in this percentage would tend to equalize the temperature.
The question, however, is whether any such temperature fluctuations have really been observed on the surface of the earth.
The geologists would answer: yes.
Our historical era was preceded by a period in which the mean temperature was by 2 (3.6 F.) higher than at present.
We recognize this from the former distribution of the ordinary hazel-nut and of the water-nut (Trapanalans).
Fossil nuts of these two species have been found in localities where the plants could not thrive in the present climate.
This age, again, was preceded by an age which, we are pretty certain, drove the inhabitants of northern Europe from their old abodes.
The glacial age must have been divided into several periods, alternating with intervals of milder climates, the so-called inter-glacial periods.
The space of time which is characterized by these glacial periods, when the temperature according to measurements based upon the study of the spreading of glaciers in the Alps must have been about 5 (8 F.) lower than now, has been estimated by geologists at not less than 100,000 years.
This epoch was preceded by a warmer age, in which the temperature, to judge from fossilized plants of those days, must at times have been by 8 or 9 (14 or 16 F.) higher than at present, and, moreover, much more uniformly distributed over the whole earth (Eocene).
Pronounced fluctuations of this kind in the climate have also occurred in former geological periods.
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 Hogbom, 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, 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.
TO BE CONTINUED...
Re: ARRHENIUS, WORLDS IN THE MAKING
THE CELESTIAL BODIES, IN PARTICULAR THE EARTH, AS ABODES OF ORGANISMS, continued …
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 Freeh, 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, arid, 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 algse, and their carbonic acid became stored up in the sedimentary strata.
Hogbom 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.
TO BE CONTINUED ...
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 Freeh, 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, arid, 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 algse, and their carbonic acid became stored up in the sedimentary strata.
Hogbom 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.
TO BE CONTINUED ...