Cooling by mixture is the sufficient cause in the majority of cases;

and this may be effected from above, by descent of the air from the

upper regions; from below, by ascent, with the assistance of rising

currents created by solar radiations; or, finally, in any and every

direction under the influence of the winds and the general movements of

the atmosphere. Furthermore, the cooling need not be very great in order

to provoke rain under certain conditions of temperature and humidity of

frequent occurrence.

Rain clouds very frequently descend a little below the altitude of the

Puy-de-Dôme. It is, therefore, not difficult, in order to determine the

degree of cooling necessary for the formation of rain, to take advantage

of observations that have been made there. The hygrometer sometimes

remains near saturation without there being precipitation of vapor;

and, supposing that the temperature is near 3° or 4° C., which is about

the mean temperature of the year, it will require a cooling of only one

or two degrees centigrade at most for the air to be unable to hold all

its vapor and for the excess of it to be transformed into rain. This is

confirmed by experiment and observation.

I will mention a remarkable example illustrating this point. Not rarely,

when the west wind is blowing violently on the top of the Puy-de-Dôme,

an east wind, blowing opposite to it, prevails at Clermont. Then an eddy

is formed behind the plateau and the chain of puys that runs from north

to south, a little west of Clermont. This eddy gradually becomes a vast

whirlwind with a horizontal axis, several leagues long, a few kilometres

wide, and seven hundred or eight hundred metres high. It commonly gives

rise to an abundant and continuous formation of black clouds, which

appear in an instant along its length, following its intersection

with the upper current. The phenomenon is frequent, and is sometimes

produced under very interesting conditions, as on a certain day when

the temperature at Clermont was five degrees above zero, centigrade,

while the hygrometer indicated that the air contained seven tenths of

the quantity of vapor required for saturation. Under such conditions

the temperature on the Puy-de-Dôme would have only had to be a very

little above the freezing point for the vapor of the horizontal eddy to

be transformed into rain on meeting the upper current coming from the

west. Now, on the top of the mountain the thermometer marked 4°C. below

the freezing point. Hence, every time the lower east wind increased a

little, this having the effect of carrying the vapor and the air of the

lower regions a little higher, the black clouds could be seen developing

with a recrudescence of intensity. A few instants afterward a torrential

rain fell at Clermont.

In some cases--and such frequently occur in summer--the mingling of

strata of air of different temperatures is effected by ascending

currents. The sky is clear; the moist air in contact with the soil is

warmed under the action of the sun, rises, and more or less quickly

reaches a much colder stratum. Light mists are formed; they may

frequently be seen rising and spreading out over the warmer or moister

spots. On the flanks of the Puy-de-Dôme one may often find himself among

ascending currents of this sort which succeed one another intermittingly

when the air is calm, after a rain; they rise with a velocity of four or

five metres at least per second.

These fogs finally become stationary in a region of the same density

with themselves. There they accumulate and form a cloud or a group of

clouds that go on developing. When penetrated by the rays of the sun,

which they almost wholly absorb, these clouds are warmed up again in

the interior, and budding protuberances are seen, which are especially

developed on the upper parts of the cloud. These protuberances are

formed and grow so rapidly as to almost suggest the presence of a

steam generator within every cloud. The external parts of the cloud,

however, cool very soon by radiation, evaporation, or dissolution,

but especially by their contact with the cold air, into which they

continue going. Hence, when the vapors emitted by the cloud reach its

periphery, they are cooled at once as if in a condenser; they then

take on a rapid movement of descent, which is easily distinguished,

and suffer condensation in their lower parts. As the surface of the

cloud in contact with the cold air around it is considerable in

proportion to that which receives the influence of the solar rays, the

warm ascending currents slacken speed and are extinguished, because

the cloudy mass, drawn on by the higher currents, removes from the

place where it is formed, or because it stops the rays of the sun and

prevents their reaching the ground. There results a more and more

complete condensation, and the watery vapor is at last transformed into

drops of rain. The condensation into rain is accelerated and augmented

when the mass of cloud rises with great rapidity, especially when it

enters abruptly into very cold atmospheric strata. A sudden mixture

of the cloud with the air around it takes place then, and sudden and

abundant rains result like those which are produced at the instant of

thunderstorms.

The formation and mixture of masses of air of different temperatures

are effected by ascending currents in zones of restricted extent, but

sometimes very numerous. Local showers and thunderstorms are produced

in this way. The phenomenon becomes much more important and at the same

time extends over vast regions, when it is brought about by the aid of

the wind and the larger movements of the atmosphere, and general rains

result.

Babinet, in his Studies on the Sciences of Observation, explains the

formation of rain by supposing that when the wind meets an obstacle,

it ascends; the moving air cools in rarefying, and deposits its excess

of vapor over saturation. This fact, when it occurs, should indeed

contribute to the condensation of the vapor contained in the air; but it

does not afford an adequate explanation of all rains; for, first, how

can it rain on the vast oceans which present no obstacles to cause the

air to ascend? It is necessary to suppose that internal movements of the

atmosphere intervene in the production of rain.

Monk, Mason, de Saussure, and many others fix the prime condition for

the formation of rain in the superposition of two beds of cloud. This

assertion, although it is still repeated in a number of treatises

on physics, is inexact. A single stratum of cloud--yes, a solitary

cloud--has been seen, on the Puy-de-Dôme, to produce rain and lightning,

with thunder.

Frequently, under the influence of the centers of perturbation which

often exist south of the Alps, a vast sea of clouds, the upper face of

which does not exceed an altitude varying from seven hundred to twelve

hundred metres, covers all central France, and probably other countries.

Only the high table-lands and mountains rise above this stratum of

clouds over which the sun shines in a perfectly clear sky. Yet rain is

found in such strata of clouds, however homogeneous they may be, and

it rains in the regions they cover. I have long been able to affirm

this fact, important because it destroys old errors elaborated in the

isolation of the study, and to support it with authentic proof.

We may witness the formation of rain when we rise into the usual region

of the clouds, either in balloon ascents or by climbing mountains.

The phenomenon may be observed under five aspects: First, we may

find ourselves in a fog of greater or less thickness, the hygrometer

indicating that the air is nearly saturated with vapor, without one

being able to detect the fall of the smallest liquid particle, and

without exterior objects being moistened. Second, while we can not

observe the fall of a single liquid drop, however small, everything

enveloped in the cloud will be rapidly moistened. We are in the

atmospheric stratum where the rain is beginning to form. Inhabitants

of mountainous regions say at such times that there is a wet fog. At

the top of the Puy-de-Dôme, when this condition lasts for a day, we can

collect three, four, or five millimetres of water. Third, we may remark,

in the fog, the fall of exceedingly fine droplets, which we can hardly

distinguish--it is drizzling. Fourth, the rain is falling, while we are

still in the fog; and, fifth, the rain is falling and we are below the

fog--that is, below the clouds.

These five aspects may be present in the same cloud, when we will find

them in the order given in successive strata, one beneath another; so

that, entering such a cloud from the upper part, we may traverse, in

regular order, "dry" fog, wet fog, fog with drizzle, fog with rain, and,

as we leave the cloud at the bottom, rain without fog. Mr. Glaisher,

the English scientific aëronaut, thus records his experience in an

ascension he made July 1, 1863: "We let ourselves drop at eight hundred

metres, and went into a fog which was dry for the first thirty metres,

but shortly afterward became moist. As we descended, the fog seemed to

become more charged with water, and seemed very dark beneath us; at five

hundred or six hundred metres we heard the sound of the rain striking

the trees, so violent was the fall."

Rain drops, in fact, grow as they fall, whether by continuance of

condensation, or by union with other drops. They should, therefore, be

larger when they issue from the cloud in proportion as the region where

drizzle is formed is higher above the base of the cloud. There is,

however, a limit to the size they can attain, for the velocity of their

fall increases with their mass, and they are divided by the resistance

of the air.

The five aspects under which we have regarded the formation of rain are

evidently five phases distinguished by our senses in the progressive

transformation which the vapor of water undergoes in passing to the

liquid state. It also sometimes happens that the condensation of the

vapor in a cloud can only reach the first or second stage of the

transformation without extending to the other stages. At other times it

stops at the third phase, that of drizzling, which may then, as rain

does, cross atmospheric regions below the cloud, and reach the ground,

provided the base of the cloud is not too high and the air passed

through is not too dry. In short, we may conclude that the formation of

rain is due simply to variations in the temperature and moisture of the

air. There is, however, another element, the intervention of which is

indispensable, if not to reduce the vapor to water, at least to cause

that water to fall in rain, or under the form of drops. This element is

the atmospheric dust.

We designate generally as atmospheric dust all the corpuscles which the

atmospheric envelope of the earth holds in suspension; but distinctions

should be made. Some dust occurs in the air fortuitously and for the

moment, such as troubles us in dry weather when the wind is blowing.

This is coarse, and so evident that we say "It is dusty," and soon falls

by its weight to the ground. There is other dust which remains in the

air almost permanently. It becomes visible to the eye when illuminated

against a dark background, as when a sunbeam comes into a dark room.

Other dust may be studied under a microscope of low power; and still

other, and the largest proportion of that in the atmosphere, is so

fine that it can not be distinguished, even with the most powerful

instruments.

This extremely fine and light dust is disseminated to heights that may

exceed fifteen or twenty or more miles. Cyclones, volcanic eruptions,

and immense prairie fires are the principal causes of its production

and expansion in the atmosphere. Mr. Aitken, a Scotch meteorologist,

has made some remarkable experiments to demonstrate the existence of

this dust. For that purpose he employed a very ingenious method, which

permitted him to count all the particles, even those which could not be

seen with a microscope. The principle of his method is as follows: If

we fill a receiver with air that has been deprived of all its dust by

passing it through a liquid, and saturate it with vapor, and then by

cooling cause the vapor to condense, the resultant water is deposited

directly. If the receiver is filled with air not cleared of its dust,

the cooling of the mixture of air and vapor provokes first the formation

of a fog that marks the presence of dust, because each particle of dust

becomes a nucleus, a center of condensation, for the vapor. Finally,

if the cooling is carried far enough, the water formed falls in very

fine droplets, each one of which incloses a dust particle. Mr. Aitken

has succeeded in counting these droplets, by introducing only a very

small volume of dusty air into the receiver and finally filling it with

absolutely pure air. He has thus found that the external air contains

on the average 32,000 particles of dust per cubic centimetre after a

rain of considerable duration, and 130,000 particles in fine weather.

There are 1,860,000 particles in the same volume of air in the middle

of a room, and 5,420,000 particles near the ceiling. The figures look

fanciful, but they are exact, for they have been corroborated by

numerous consistent experiments and agree with the determinations that

have been made by other methods.

As to the formation of rain, it should be observed that absolutely pure

air can not give either fog or drops of water when it is supersaturated

with vapor. If there were no dust in the atmosphere we should have no

clouds or rain. The sky would always be clear, and the sun would shine

uninterruptedly as long as it was above the horizon. There would be no

dawn or twilight, and day and night would succeed one another instantly,

without transition. Atmospheric water would be deposited only when in

contact with things, as in Aitken's experiments, very much as dew is

deposited.

The causes of the formation of rain are evidently the same everywhere.

The secondary conditions change only according to climates; but they

vary so much that rains are distributed very unequally over the earth.

According to Desanis, the quantity of vapor contained in a column of

air as high as the atmosphere would give, in France, a layer of water

about four centimetres thick. Few rain storms would furnish so much;

but there are storms sometimes that give much more. On August 17, 1888,

seven centimetres of water fell at Clermont in five hours; and September

12, 1875, the pluviometer measured ten centimetres for the whole day.

Still more copious rains fall in some tropical countries; at Purneah, in

India, eighty-nine centimetres have fallen in twenty-four hours.

Mr. John Murray has calculated, from the charts of Elias Loomis, that

the quantity of rain falling every year over the whole earth would form

a bed of water averaging nine hundred and seventy millimetres in depth.

When we consider the annual quantities of rain in particular regions or

localities, we find the numbers exceedingly variable, and some of them

surprising. Clermont receives 630 millimetres, and the mean of the fall

in Europe is about the same. About one metre falls on the western coast

of Iceland, two metres in Norway, 2.80 metres in Scotland, 4.60 metres

at Vera Cruz, 5.20 metres at Buitenzorg, in the Dutch East Indies, 7.10

metres at Maranhão, Brazil, and 12.50 metres at Cherrapunji, in British

India. On the other hand, it rarely rains in some regions of the globe

north and south of the equator; as in the center of the Sahara and of

Arabia, the plateau of eastern Persia and Beluchistan, the desert of

Kalahari, and the desert of Atacama. The plains or pampas of the eastern

slopes of the Andes, in about 23° south latitude, are likewise subject

to extreme droughts, in one of which, lasting three years, three million

head of cattle perished.--_Translated for the Popular Science Monthly

from Ciel et Terre._

FOOTNOTE:

[12] An address before the Society of Horticulture and Viticulture at

Clermont-Ferrand.

DREAM AND REALITY.

BY M. CAMILLE MELINAND.

There is a very striking resemblance between dreams and waking

perceptions. We see in dreams objects, persons, and events identical

with those of the waking state. The belief in their reality is as

complete as in that of what we see when awake; the emotions are as deep

and vivid. Pleasures have a delicious savor, and pains are even more

intense than those of the reality--as, for instance, those of nightmare,

and the distresses to which we give ourselves up in full. In all cases

these dream troubles seem as real as those of life, and are taken by us

quite as seriously; and the existence of everything we see and feel is

as evident as in life.

Still we oppose the dream to the reality. The waking world is our true,

our only world; the world of the dream seems to us purely interior and

chimerical. The incoherence and absurdity of our dreams surprise and

amuse us, and we are amazed to find that we have been able to believe,

while asleep, in such foolish things. In short, dreaming is synonymous

to us with illusion, phantasmagoria, and falsehood. The clearest of

the prevailing theories about dreams rest upon the postulate that

waking perceptions are the true ones, and the visions of the dream are

false. They have answers to the three questions we are used to ask

concerning dreams--Where do they come from? why are they incoherent?

and why do we take their visions for realities? They explain dreams

as former sensations reviving within us under different combinations,

and as therefore simply confused reflexes of the reality. Dreams may,

however, sometimes be produced by a present impression suffered by one

of our senses, half awakened--a contact, the way we are lying, and the

condition of the organic functions being thus the causes or occasions

of dreams. The incoherence of dreams seems no more mysterious in these

theories, and is explained as the result of two causes--the slumber of

the "reflecting" faculties, judgment, reason, the will, the exercise of

choice and control; and, secondly, the unrestricted reign of imagination

and the association of ideas. Our faith in the reality of the things

dreamed is accounted for by the mechanical play of the images, the law

being set up that every image that is not opposed by stronger images

appears to us a real object. The problem, therefore, resolves itself:

the senses being asleep, the images that arise within us are not

contradicted by normal sensations, and that is why we take them for

realities. Further, our reflective faculties, being likewise dormant,

can not contradict the images, in the absence of sensations, reasonings,

or recollections. Hence a credence, as absolute as unreasonable. We

purpose to show that there is something artificial and prejudiced in the

classical theory of opposition between dreams and waking, which assigns

illusion, confusion, and incoherence to the former, and solid and

permanent reality to the latter, and that the difference between them is

not so clean cut.

Most persons in talking of this subject say that they are sure of the

reality of things when awake because their different senses concur in

attesting it. They see a tree, and satisfy themselves that it is a tree

by going up and touching it. They smell a rose, and go find the rose,

look at it and handle it; while in dreams we are not able to apply

these supplementary tests. The distinction is imaginary, for our senses

likewise seem to support one another in dreams. We dream not only that

we see an object, but also that we feel and hear it. When I dream of

meeting a friend, I believe that I see him and shake hands with him and

hear him speak. There is, therefore, a complete identity of the two

conditions as to this point, and the thing that appears to me in a dream

is a "bundle of sensations," visual, tactile, auditive, muscular, and

often olfactory, just as it appears to me when awake.

We are told of another difference. When awake, we find others agreeing

with us in recognizing the reality of things. I see a tree, and so

do those with me; I show it to them, and they look at it; I feel of

it, and they touch it; I hear the rustling of the leaves, and so do

they. Our perceptions in practical life are thus tested by comparison

with those of others, whereas in our dreams we have our solitary and

fanciful visions all within ourselves, with none to participate in our

perceptions of them.

This supposed contrast is no more real than the former one. What is

true is that when we are once awake we change our point of view, and our

vision of the night then seems to have been wholly interior, solitary,

and subjective. But, notwithstanding the common illusion, _while we are

dreaming_ affairs pass, to us, exactly as when we are awake. It is true

that in the waking state we find ourselves mingled with other men, who

perceive the same objects that we do. Do we not sometimes dream that we

are one of an audience looking at a play? that we are talking with a

friend, and exchange views with him? and that we understand one another

perfectly? There is, therefore, in this aspect, not a difference but

identity between the dream and the waking. The interior condition, the

sensation, the credence, are identical. The dreaming man believes, sees,

and feels himself in intercourse with his fellows, just as the man awake

believes, sees, and feels it. When we wake, we discover our mistake, but

what of that? It does not prevent us from believing completely in it

while we are asleep. And this is the point; for, after all, am I sure

that I shall not awake some day from what I now call my waking life? And

who knows whether I shall not then judge that I have been dreaming a

solitary dream? It may be added that the agreement of witnesses is not a

decisive sign by which to distinguish the reality from the dream. There

are collective hallucinations.

We come now to a more important difference, which includes the principle

and has a characteristic apparently essentially distinguishing the

dream--its looseness, disorder, inconstancy, and incoherence. In the

dream visions succeed one another without connection; no law determines

their order; an unrestricted fancy reigns among them, and the normal is

broken up in them at every point. We are transported instantaneously

from one country to another. We pass without transition from childhood

to age, and causes have the strangest effects. The most essential laws

of thought are constantly violated. There are facts without any causes,

metamorphoses, magical disappearances. Even the absurd is realized,

and the "principle of contradiction" does not seem to be any more

respected than the others. We are at the same time in two places; we

pronounce words, we hold conversations of which we can not when we

wake recover the thread, so strange is their logic, so fugitive the

sense, and so fanciful the combination. A practiced psychologist, M.

Delbœuf, succeeded in taking down in the morning the last phrase of a

book which he had been reading in a dream, and which had seemed then

remarkably lucid. Here it is: "The man raised by the woman and separated

by aberrations pushes facts disengaged by the analysis of the tertiary

nature into the way of progress."

Appletons' Popular Science Monthly, November 1898 Volume 54, November 1898 · 第 9 / 16 段