Fogs which have a peculiar smell at some seasons of the year, remind us of

these accidental admixtures in the lower strata of the atmosphere. Winds

and currents of air caused by the heating of the ground even carry up to a

considerable elevation solid substances reduced to a fine powder. The dust

which darkens the air for an extended area, and falls on the Cape Verd

Islands, to which Darwin has drawn attention, contains, according to

Ehrenberg's discovery, a host of silicious-shelled infusoria.

As principal features of a general descriptive picture of the atmosphere, we

may enumerate:

1. 'Variations of atmospheric pressure': to which belong the horary

oscillations, occurring with such regularity in the tropics, where they

produce a kind of ebb and flow in the atmosphere, which can not be ascribed

to the attraction of the moon,* and which differs so considerably according

to geographical latitude, the seasons of the year, and the elevation above

the level of the sea.

[footnote] *Bouvard, by the application of the formulae, in 1827, which

Laplace had deposited with the Board of Longitude shortly before his death,

found that the portion of the horary oscillations of the pressure of the

atmosphere, which depends on the attraction of the moon, can not raise the

mercury in the barometer at Paris more than the 0.018 of a millimeter, while

eleven years' observations at the same place show the mean barometric

oscillation, from 9 A.M. to 3 P.M., to be 0.756 millim., and from 3 P.M. to

9 P.M., 0.373 millim. See 'Memoires de l'Acad. des Sciences', t. vii.,

1827, p. 267.

2. 'Climatic distribution of heat', which depends on the relative position

of the transparent and opaque masses (the fluid and solid parts of the

surface of the earth), and on the hypsometrical configuration of continents;

relations which determine the geographical position and curvature of the

isothermal lines (or curves of equal mean annual temperature) both in a

horizontal and vertical direction, or on a uniform plane, or in different

superposed strata of air.

3. 'The distribution of the humidity of the atmosphere'. The quantitative

relations of the humitidy depend on the differences in the solid and oceanic

surfaces; on the distance from the equator and the level of the sea; on the

form in which the

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aqueous vapor is precipitated, and on the connection existing between these

deposits and the changes of temperature, and the direction and succession of

winds.

4. 'The electric condition of the atmosphere'. the primary cause of this

condition, when the heavens are serene, is still much contested. Under this

head we must consider the relation of ascending vapors to the electric

charge and the form of the clouds, according to the different periods of the

day and year; the difference between the cold and warm zones of the earth,

or low and high lands; the frequency or rarity of thunder storms, their

periodicity and formation in summer and winter; the causal connection of

electricity, with the infrequent occurrence of hail in the night, and with

the phenomena of water and sand spouts, so ably investigated by Peltier.

The horary oscillations of the barometer, which in the tropics present two

maxima (viz., at 9 or 9 1/4 P.M., and 4 A.M., occurring, therefore, in

almost the hottest and coldest hours), have long been the object of my most

careful diurnal and nocturnal observations.*

[footnote] *'Observations faites pour constater la Marche des Variations

Horaires du Barometre sous les Tropiques', in my 'Relation Historique du

Voyage aux Regions Equinoxiales', t. iii., p. 270-313.

Their regularity is so great, that, in the daytime especially, the hour may

be ascertained from the height of the mercurial column without an error, on

the average, of more than fifteen or seventeen minutes. In the torrid zones

of the New Continent, on the coasts as well as at elevations of nearly

13,000 feet above the level of the sea, where the mean temperature falls to

44.6 degrees, I have found the regularity of the ebb and flow of the aerial

ocean undisturbed by storms, hurricanes, rain, and earthquakes. The amount

of the daily oscillations diminishes from 1.32 to 0.18 French lines from the

equator to 70 degrees north latitude, where Bravais made very accurate

observations at Bosekop.*

[footnote] *Bravais, in Daemtz and Martins, 'Meteorologie', p. 263. At

Halle (51 degrees 29' N. lat.), the oscillation still amounts to 0.28 lines.

It would seem that a great many observations will be required in order to

obtain results that can be trusted in regard to the hours of the maximum and

minimum on mountains in the temperate zone. See the observations of horary

variations, collected on the Faulhorn in 1832, 1841, and 1842 (Martins,

'Meteorologie', p. 254.)

The supposition that, much nearer the pole, the height of the barometer is

really less at 10 A.M. than at 4 P.M., and consequently, that the maximum

and minimum influences of these hours

p 315

are inverted, is not confirmed by Parry's observations at Port Bowen (73

degrees 14').

The mean height of the barometer is somewhat less under the equator and in

the tropics, owing to the effect of the rising current,* than in the

temperate zones, and it appears to attain its maximum in Western Europe

between the parallels of 40 degrees and 45 degrees.

[footnote] *Humboldt, 'Essai sur la Geographie des Plantes', 1807, p. 90;

and in 'Rel. Hist.', t. iii., p. 313; and on the diminuation of atmospheric

pressure in the tropical portions of the Atlantic, in Poggend., 'Annalen der

Physik', bd. xxxvii., s. 245-258, and s. 463-486.

If with Kämtz we connect together by 'isobarometric' lines those places

which present the same mean difference between the monthly extremes of the

barometer, we shall have curves whose geographical position and inflections

yield important conclusions regarding the influence exercised by the form of

the land and the distribution of seas on the oscillations of the atmosphere.

Hindostan with its high mountain chains and triangular peninsulas, and the

eastern coasts of the New Continent, where the warm Gulf Stream turns to the

east at the Newfoundland Banks, exhibit greater isobarometric oscillations

than do the group of the Antilles and Western Europe. The prevailing winds

exercise a principal influence on the diminution of the pressure of the

atmosphere, and this, as we have already mentioned, is accompanied,

according to Daussey, by an elevation of the mean level of the sea.•

[footnote] *Dausay, in the 'Comptes Rendus', t. iii., p. 136.

As the most important fluctuations of the pressure of the atmosphere,

whether occurring with horary or annual regularity, or accidentally, and

then often attended by violence and danger,* are like all the other

phenomena of the weather, mainly owing to the heating force of the sun's

rays, it has long been suggested (partly according to the idea of Lambert)

that the direction of the wind should be compared with the height of the

barometer, alternations of temperature, and the increase and decrease of

humidity.

[footnote] *Dove, 'Ueber die Sturme', in Poggend., 'Annalen', bd. lii., s.

1.

Tables of atmospheric pressure during different winds, termed 'barometric

windroses', afford a deeper insight into the connection of meteorological

phenomena.*

[footnote] *Leopold von Buch, 'Barometrische Windrose', in 'Abhandl. der

Akad. der Wiss. zu Berlin aus den Jahren', 1818-1819, s. 187.

Dove has, with admirable sagacity, recognized, in the "law of rotation" in

both hemispheres, which he himself established, the cause of many important

processes in the aerial ocean.*

[footnote] *See Dove, 'Meteorologishe Untersuchungen', 1837, s. 99-313; and

the excellent observations of Kämtz on the descent of the west wind of the

upper current in high latitudes, and the general phenomena of the direction

of the wind, in his 'Vorlesungen uber µeterologie', 1840, s. 58-66,

196-200, 327-336, 353-364; and in Schumacher's 'Jahrbuch fur' 1838, s.

291-302. A very satisfactory and vivid representation of meteorological

phenomena is given by Dove, in his small work entitled

'Witterungsverhältnisse von Berlin', 1842. On the knowledge of the earlier

navigators of the rotation of the wind, see Churruca, 'Viage at Magellanes',

1793, p. 15; and on a remarkable expression of Columbus, which his son Don

Fernando Colon has presented to us in his 'Vida del Almirante', cap. 55, see

Humboldt, 'Examen Critique de l'Hist. de Geographie', t. iv., p. 253.

The difference of temperature between the

p 315

equatorial and polar regions engenders two opposite currents in the upper

strata of the atmosphere and on the Earth's surface. Owing to the

difference between the rotatory velocity at the poles and at the equator,

the polar current is deflected eastward, and the equatorial current

westward. The great phenomena of atmospheric pressure, the warming and

cooling of the strata of air, the aqueous deposits, and even, as Dove has

correctly represented, the formation and appearance of clouds, alike depend

on the opposition of these two currents, on the place where the upper one

descends, and on the displacement of the one by the other. Thus the figures

of the clouds, which form an animated part of the charms of a landscape,

announce the processes at work in the upper regions of the atmosphere, and,

when the air is calm, the clouds will often present, on a bright summer sky,

the "projected image" of the radiating soil below.

Where this influence of radiation is modified by the relative position of

large continental and oceanic surfaces, as between the eastern shore of

Africa and the western part of the Indian peninsula, its effects are

manifested in the Indian monsoons, which change with the periodic variations

in the sun's declination,* and which were known to the Greek navigators

under the name of 'Hippalos'.

[footnote] *'Monsun' (Malayan 'musim', the 'hippalos' of the Greeks) is

derived from the Arabic word 'mausim', a set time or season of the year, the

time of the assemblage of pilgrims at Mecca. The word has been applied to

the seasons at which certain winds prevail, which are, besides, named from

places lying in the direction from whence they come; thus, for instance,

there is the 'mausim' of Aden, of Guzerat, Malabar, etc. (Lassen, 'Indische

Alterthumskunde', bd. i., 1843, s. 211). On the contrasts between the solid

or fluid substrata of the atmosphere, see Dove, in 'Der Abhandl. der Akad.

der Wiss. zu Berlin aus dem Jahr' 1842, s. 239.

In the knowledge of the monsoons, which undoubtedly dates back thousands of

years among the inhabitants of Hindostan and China, of the eastern parts of

the Arabian Gulf and of the western shores of the Malayan

p 317

Sea, and in the still more ancient and more general acquaintance with land

and sea winds, lies concealed, as it were, the germ of that meteorological

sciences which is now making such rapid progress. The long chain of

'magnetic stations' extending from Moscow to Pekin, across the whole of

Northern Asia, will prove of immense importance in determining the 'law of

the winds', since these stations have also for their object the

investigation of general meteorological relations. The comparison of

observations made at places lying so many hundred miles apart, will decide,

for instance, whether the same east wind blows from the elevated desert of

Gobi to the interior of Russia, or whether the direction of the Aerial

current first began in the middle of the series of the stations, by the

descent of the air from the higher regions. By means of such observations,

we may learn, in the strictest sense, 'whence' the wind cometh. If we only

take the results on which we may depend from those places in which the

observations on the direction of the winds have been continued more than

twenty years, we shall find (from the most recent and careful calculations

of Wilhelm Mahlmann) that in the middle latitudes of the temperate zone, in

both continents, the prevailing aerial current has a west-southwest

direction.

Our insight into the 'distribution of heat' in the atmosphere has been

rendered more clear since the attempt has been made to connect together by

lines those places where the mean annual summer and winter temperatures have

been ascertain by correct observations. The system of 'isothermal,

osotheral' and 'isochimenal' lines, which I first brought into use in 1817,

may, perhaps, if it be gradually perfected by the united efforts of

investigators, serve as one of the main foundations of 'comparative

climatology'. Terrestrial magnetism did not acquire a right to be regarded

as a science until partial results were graphically connected in a system of

lines of 'equal declination, equal inclinatiion', and 'equal intensity'.

The term 'climate', taken in its most general sense, indicated all the

changes in the atmosphere which sensibly affect our organs, as temperature,

humidity, variations in the barometrical pressure, the calm state of the air

or the action of opposite winds, the amount of electric tension, the purity

of the atmosphere or its admixture with more or less noxious gaseous

exhalations, and, finally, the degree of ordinary transparency and clearness

of the sky, which is not only important with respect to the increased

radiation from the Earth, the organic development of plants, and the

ripening of fruits, but

p 318

also with reference to its influence on the feelings and mental condition of

men.

If the surface of the Earth consisted of one and the same homogeneous fluid

mass, or of strata of rock having the same color, density, smoothness, and

power of absorbing heat from the solar rays, and of radiating it in a

similar manner through the atmosphere, the isothermal, isotheral, and

isochimenal lines would all be parallel to the equator. In this

hypothetical condition of the Earth's surface, the power of absorbing and

emitting light and heat would every where be the same under the same

latitudes. The mathematical consideration of climate, which does not

exclude the supposition of the existence of currents of heat in the

interior, or in the external crust of the earth, nor of the propagation of

heat by atmospheric currents, proceeds from this mean, and, as it were,

primitive condition. Whatever alters the capacity for absorption and

radiation, at places lying under the same parallel of latitude, gives rise

to inflections in the isothermal lines. The nature of these inflections,

the angles at which the isothermal, isotheral, or isochimenal lines

intersect the parallels of latitude, their convexity or concavity with

respect to the pole of the same hemisphere, are dependent on causes which

more or less modify the temperature under different degrees of longitude.

The progress of 'Climatology' has been remarkably favored by the extension

of European civilization to two opposite coasts, by its transmission from

our western shores to a continent which is bounded on the east by the

Atlantic Ocean. When, after the ephemeral colonization from Iceland and

Greenland, the British laid the foundation of the first permanent

settlements on the shores of the United States of America, the emigrants

(whose numbers were rapidly increased in consequence either of religious

persecution, fanaticism, or love of freedom, and who soon spread over the

vast extent of territory lying between the Carolinas, Virginia, and the St.

Lawrence) were astonished to find themselves exposed to an intensity of

winter cold far exceeding that which prevailed in Italy, France, and

Scotland, situated in corresponding parallels of latitude. But, however

much a consideration of these climatic relations may have awakened

attention, it was not attended by any practical results until it could be

based on the numerical data of 'mean annual temperature'. If, between 58

degrees and 30 degrees north latitude, we compair Nain, on the coast of

Labrador, with Gottenburg; Halifax with Bordeaus; New

p 319

York with Naples; St. Augustine, in Florida, with Cairo, we find that, under

the same degrees of latitude, the differences of the mean annual temperature

between Eastern America and Western Europe, proceeding from north to south,

are successively 20.7 degrees, 13.9 degrees, 6.8 degrees, and almost 0

degrees. The gradual decrease of the differences in this series extending

over 28 degrees of latitude is very striking. Further to the south, under

the tropics, the isothermal lines are every where parallel to the equator in

both hemispheres. We see, from the above examples, that the questions often

asked in society, how many degrees America (without distinguishing between

the eastern and western shores) is colder than Europe? and how much the mean

annual temperature of Canada and the United States is lower than that of

corresponding latitudes in Europe? are, when thus 'generally expressed',

devoid of meaning. There is a separate difference for each parallel of

latitude, and without a special comparison of the winter and summer

temperatures of the opposite coasts, it will be impossible to arrive at a

correct idea of climatic relations, in their influence on agriculture and

other industrial pursuits, or on the individual comfort or discomfort of

manking in general.

In enumerating the causes which produce disturbances in the form of the

isothermal lines, I would distinguish between those which 'raise' and those

which 'lower' the temperature. To the first class belong the proximity of a

western coast in the temperate zone; the divided configuration of a

continent into peninsulas, with deeply-indented bays and inland seas; the

aspect of the position of a portion of the land with reference either to a

sea of ice spreading far into the polar circle, or to a mass of continental

land of considerable extent, lying in the same meridian, either under the

equator, or, at least, within a portion of the tropical zone; the prevalence

of southerly or westerly winds on the western shore of a continent in the

temperate northern zone; chains of mountains acting as protecting salls

against the winds coming from colder regions; the infrequency of swamps,

which, in the spring and beginning of summer, long remain covered with ice,

and the absence of woods in a dry, sandy soil; finally the constant serenity

of the sky in the summer months, and the vicinity of an oceanic current,

bringing water which is of a higher temperature than that of the surrounding

sea.

Among the causes which tend to 'lower' the mean annual temperature I include

the following: elevation above the level of the sea, when not forming part

of an extended plain; the

p 320

vicinity of an eastern coast in high and middle latitudes; the compact

configuration of a continent having no littoral curvatures or bays; the

extension of land toward the poles into the region of perpetual ice, without

the intervention of a sea remaining open in the winter; a geographical

position, in which the equatorial and tropical regions are occupied by the

sea, and consequently, the absence, under the same meridian, of a

continental tropical land having a strong capacity for the absorption and

radiation of heat; mountain chains, whose mural form and direction impede

the access of warm winds, the vicinity of isolated peaks, occasioning the

descent of cold currents of air down their declivities; extensive woods,

which hinder the isolation of the soil by the vital activity of their

foliage, which produces great evaporation, owing to the extension of these

organs, and increases the surface that is cooled by radiation, acting

consequently in a three-fold manner, by shade, evaporation, and radiation;

the frequency of swamps or marshes, which in the north form a kind of

subterranean glacier in the plains, lasting till the middle of the summer; a

cloudy summer sky, which weakens the action of the solar rays; and, finally,

a very clear winter sky, favoring the radiation of heat.*

[footnote] *Humboldt, 'Recherches sur les Causes des Inflexions des Lignes

Isothermes', in 'Asie Centr.', t. iii., p. 103-114, 118, 122, 188.

The simultaneous action of these disturbing causes, whether productive of an

increase or decrease of heat, determines, as the total effect, the

inflection of the isothermal lines, especially with relation to the

expansion and configuration of solid continental masses, as compared with

the liquid oceanic. These perturbations give rise to convex and concave

summits of the isothermal curves. There are, however, different orders of

disturbing causes, and each one must, therefore, be considered separately,

in order that their total effect may afterward be investigated with

reference to the motion (direction, local curvature) of the isothermal

lines, and the actions by which they are connected together, modified,

destroyed, or increased in intensity, as manifested in the contact and

intersection of small oscillatory movements. Such is the method by which, I

hope, it may some day be possible to connect together, by empirical and

numerically expressed laws, vast series of apparently isolated facts, and to

exhibit the mutual dependence which must necessarily exist among them.

The trade winds -- easterly winds blowing within the tropics -- give rise,

in both temperate zones, to the west, or west-southwest

p 321

sinds which prevail in those regions, and which are land winds to eastern

coasts, and sea winds to western coasts, estending over a space which, from

the great mass and the sinking of its cooled particles, is not capable of

any considerable degree of cooling, and hence it follows that the east winds

of the Continent must be cooler than the west winds, where their temperature

is not affected by the occurrence of oceanic currents near the shore.

Cook's young companion on his second voyage of circumnavigation, the

intelligent George Forster, to whom I am indebted for the lively interest

which prompted me to undertake distant travels, was the first who drew

attention, in a definite manner, to the climatic differences of temperature

existing in the eastern and western coasts of both continents, and to the

similarity of temperature of the western coast of North America in the

middle latitudes, with that of Western Europe.*

[footnote] *George Forster, 'Klein Schriften', th. iii., 1794, s. 87; Dove,

in Schumacher's 'Jahrbuch fur', s. 289; Kämtz, 'Meteorologie', bd. ii., s.

41, 43, 67, and 96; Arago, in the 'Comptes Rendus', t. i., p. 268.

Even in northern latitudes exact observations show a striking difference

between the 'mean annual temperature' of the east and west coasts of

America. The mean annual temperature of Nain, in (lat. 57 degrees 10'),

is fully 6.8 degrees 'below' the freezing point, while on the northwest

coast, at New Archangel, in Russian America (lat. 57 degrees 3'), it is 12.4

degrees 'above' this point. At the first-named place, the mean summer

temperature hardly amounts to 43 degrees, while at the latter place it is 57

degrees. Pekin (39 degrees 54'), on the eastern coast of Asia, has a mean

annual tempeerature of 52.8 degrees, which is 9 degrees below that of

Naples, situated somewhat further to the north. The mean winter temperature

of Pekin is at least 5.4 degrees below the freezing point, while in Western

Europe, even at Paris (48 degrees 50'), it is nearly 6 degrees above the

freezing point. Pekin has also a mean winter cold which is 4.5 degrees

lower than that of Copenhagen, lying 17 degrees further to the north.

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