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METEOROLOGY (Gr. JerEwpa, and hb'yos,...

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Originally appearing in Volume V18, Page 271 of the 1911 Encyclopedia Britannica.
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METEOROLOGY (Gr. JerEwpa, and hb'yos, i.e. the See also:science of things in the See also:air)  , the See also:modern study of all the phenomena of the See also:atmosphere of gases, vapours and dust that surrounds the See also:earth and extends to that unknown See also:outer See also:surface which marks the beginning of the so-called interstellar space . These phenomena may be studied either individually or collectively . The collective study has to do with See also:statistics and See also:general See also:average conditions, sometimes called normal values, and is generally known as Climatology (see See also:CLIMATE, where the whole subject of regional climatology is dealt with) . The study of the individual items may be either descriptive, explanatory, See also:physical or theoretical . Physical See also:meteorology is again sub-divided according as we consider either the changes that depend upon the motions of masses of See also:air or those that depend upon the motions of the gaseous molecules; the former belong to See also:hydrodynamics, and the latter are mostly comprised under See also:thermodynamics, See also:optics and See also:electricity . See also:History.—The See also:historical development of meteorology from the most See also:ancient times is well presented by the quotations from classic authors compiled by See also:Julius See also:Ludwig See also:Ideler (Meteorologia veterum graecorum et romanorum, See also:Berlin, 1832) . We owe to the Arabian philosophers some slight advance on the know-ledge of the Greeks and See also:Romans; especially as to the See also:optical phenomena of the atmosphere . The Meteorologia of See also:Aristotle (see See also:Zeller, Phil. der Griechen) accords entirely with the Philosophica of See also:Thomas See also:Aquinas, the poetic songs of the troubadours, and the writings of See also:Dante (see See also:Kuhn's Treatment of Nature in Dante's Divina Commedia; See also:London, 1897) . Dante's See also:work completed the passage from the ancient mythological treatment of nature to the more rational recognition of one creator and lawgiver that pervades modern See also:science . The progress of meteorology has been coincident with the progress of physics and See also:chemistry in general, as is shown by considering the See also:works of See also:Alhazen (1050) on See also:twilight, Vitellio (1250) on the See also:rainbow, Galileo (16o7) on the thermometer and on the See also:laws of inertia, on attractions and on the See also:weight of the air, Toricelli (1642) on the See also:barometer, See also:Boyle (1659) on the elastic pressure of the air in all directions, See also:Newton (1673) on optics; See also:Cavendish (176o), elastic pressure of aqueous vapour; See also:Black (1752), separation of carbonic See also:acid See also:gas from See also:ordinary air; See also:Rutherford (1772). separation of See also:nitrogen; See also:Priestley and See also:Scheele (1775) and Cavendish (1777), separation of See also:oxygen; See also:Lavoisier (1783), general See also:establishment of the See also:character of the atmosphere as a See also:simple mixture of gases and vapour; De See also:Saussure's measurement of relative humidity by the accurate See also:hair See also:hygrometer (178o), See also:Dalton's measurement of vapour tension at various temperatures (1800), See also:Regnault's and See also:Magnus's revision of Dalton's tension of See also:water vapour (184o), Marvin's and Juhlins's measurements of tension of See also:ice vapour (1891), and the See also:isolation of See also:argon by See also:Rayleigh and See also:Ramsay (1894) . Theoretical meteorology has been, and always must be, wholly dependent on our knowledge of thermodynamics and on mathematical methods of dealing with the forces that produce the motions within the atmosphere . Progress has been due too. the most eminent mathematicians at the following approximate See also:dates: See also:Sir See also:Isaac Newton (167o), Leonhard-See also:Euler (1736), See also:Pierre See also:Simon See also:Laplace (178o), See also:Jean See also:Baptiste See also:Joseph See also:Fourier (1785), Simon See also:Denis See also:Poisson (1815), Sir See also:George See also:Gabriel See also:Stokes (1851), See also:Hermann von See also:Helmholtz (18.57), See also:Lord See also:Kelvin (186o), C .

A . Bjerknes (1868), V . Bjerknes (1906), and to their many distinguished followers . The earliest systematic daily See also:

record of See also:local See also:weather phenomena that has survived is that kept by See also:William Merle, See also:Cohen, Meteoritenkunde (See also:Stuttgart, 1894-1905) ; L . See also:Fletcher, An See also:rector of Driby, during seven years 1331-1338: the See also:manuscript Introduction to the Study of Meteorites, loth ed . (London, 1908); I is preserved in the See also:Digby MS., Merton See also:College, See also:Oxford, and was published in facsimile by George G . See also:Symons in 1891 . Doubt-less many similar monastic diaries have been lost to us . In 1653 See also:Ferdinand I_I. of See also:Tuscany organized a local See also:system of stations and daily records which extended over and beyond See also:northern See also:Italy . This was the first fairly See also:complete meteorological system in See also:Europe . The records kept during the years 1655—1670 at the See also:Cloister See also:Angelus near See also:Florence were reduced by Libri, See also:professor of See also:mathematics at See also:Pisa, and published in 183o . The history of meteorology is marked by the See also:production of comprehensive See also:treatises embodying the current See also:state of our knowledge .

Such were See also:

Louis Cotte's Traite de meteorologic (See also:Paris, 1974) and his Memoires sur la meteorologie, supplement au traite (1788); Ludwig Karatz's Lehrbuch der Meteorologie (See also:Halle, 1831—1836) and his Vorlesungen (184o; See also:French 1842, See also:English 1845); Sir See also:John See also:Herschel's Meteorology (London, 1840); the splendid See also:series of See also:memoirs by H . W . See also:Brandes in Gehler's Physikalisches Worterbuch (See also:Leipzig, 1820—1840); E . E . F . W . Schmid's Grundriss 'der Meteorologie (Leipzig, 1862); Ferrel's See also:Recent Advances in Meteorology (See also:Washington, 1885); the See also:great works of Julius Hann, as summarized in his Handbuch der Klimatologie (1883; 2nd ed., Stuttgart, 1897; vol. i .. English 1903) and his Lehrbuch der Meteorologie (Leipzig, 1901,,2nd ed . 1906); the extensive studies of J . E . Woeikoff (Voeikof), as presented in his Klima der Erde (See also:Russian 1883, See also:German 1885) and his Meteorologte (Russian 1904) . The development of this science has been greatly stimulated by the See also:regular publication of See also:special See also:periodicals such as the Zeitschrifl of the See also:Austrian Meteorological Society, 1866—1885, vol .

21 appearing with vol . 3 of the Meteorologische Zeitschrifl of the German Meteorological Society in 1886, and since that date this See also:

journal has been jointly maintained by the two See also:societies . The analogous See also:journals of the Royal Meteorological Society, London, 1850 to date, the Scottish Meteorological Society, 186o to date, the Meteorological Society of See also:France, 1838 to date, the See also:Italian Meteorological Society, and the See also:American Meteorological Journal, 1885—1895, have all played important parts in the history of meteorology . On the other See also:hand, the See also:Annals of the Central Meteorological See also:Office at Paris, the Archie of the Deutsche Seewarte at See also:Hamburg, the Annals and the Repertorium of the Central Physical See also:Observatory at St See also:Peters-See also:burg, the Annales of the Central Meteorological Office at See also:Rome, Bulletin of See also:International Simultaneous Met . Obs. and the Monthly Weather See also:Review of the Weather See also:Bureau at Washington, the Abhandlungen of the Royal Prussian Meteorological See also:Institute at Berlin, the Meteorological Papers of the Meteorological Office, London, and the transactions of numerous scientific societies, have represented the important See also:official contributions of the respective See also:national governments to technical meteorology . The recent international See also:union for aerial exploration by kites and balloons has given rise to two important publications, i.e. the Veroffentlichungen of the International . See also:Commission for Scientific Aerostatics (See also:Strassburg, 1905, et seq.), devoted to records of observations, and the Beitrdge zur Physik der freien Atmosphdre (Strassburg, 1904, et seq.), devoted to See also:research . The See also:necessity of studying the atmosphere as a unit and of securing See also:uniform accuracy in the observations has led to the formation of a permanent International Meteorological See also:Committee (of which in 1909 the secretary was Professor Dr G . Hellmann of Berlin, and the See also:president Dr W . N . See also:Shaw of London) . Under its directions conferences and general congresses have been held, beginning with that of 1872 at Leipzig .

Its Inter-national Tables, See also:

Atlas of Clouds, Codex of Instructions, and Forms for Climatological Publications illustrate the activity and usefulness of this committee . Modern meteorology has been See also:developed along two lines of study, based respectively on maps of monthly and See also:annual averages and on daily weather maps . The latter study seems to have been begun by H . W . Brandes in Leipzig, who first, about 1820, compiled maps for 1783 from the data collected in the Ephemerides mannheimensis, and subsequently published maps of the See also:European storms of 182o and 1821 . Simultaneously with Brandes we find William C . Redfield in New Yorkcompiling a See also:chart of the See also:hurricane of 1821, which was published in 1831, and was the first of many memoirs by him on hurricanes that completely established their rotary and progressive See also:motion . Soon after this Piddington and Sir William See also:Reid began their great works on the storms of the Orient . About 1825 See also:James See also:Pollard Espy, in See also:Philadelphia, began the publication of his views as to the See also:motive See also:power of thunderstorms and tornadoes, and in 1842 was appointed " meteorologist to the U.S. See also:government " and assigned to work in the office of the surgeon-general of the See also:army, where he prepared daily weather maps that were published in his four successive " Reports." In 1848 the three American leaders See also:united in letters to Professor Joseph See also:Henry, secretary of the Smithsonian Institution, urging that the See also:telegraph be used for See also:collecting data for daily maps and weather predictions . Favourable See also:action was taken in 1849, the Smithsonian maps began to be compiled about 1851 and were displayed in public from 1853 onwards . Meanwhile in See also:England James See also:Glaisher, with the help of the daily See also:press, carried out similar work, See also:publishing his first See also:map in 1851 as soon as daily weather maps of sufficient extent could be promptly prepared by the help of the telegraph . The destructive See also:storm of the 14th of See also:November 1854, in the See also:Crimea gave U .

J . J . Le Vervier, at Paris, an opportunity to propose the proper action, and his proposals were immediately adopted by the secretary of See also:

war, See also:Marshal Valliant . On the 17th of See also:February 1855 the See also:emperor ordered the director-general of government telegraph lines to co-operate completely with Le Verrier in the organization of a bureau of telegraphic meteorology . The international daily bulletin of the Paris Observatory began to be printed in regular See also:form on the 1st of See also:January 1858, and the daily map of isobars was added to the See also:text in the autumn of 1863 . The further development of this bulletin, the inclusion of See also:British and ocean reports in 186r, the addition of special storm warnings it1 1863, the publication of the Atlas See also:des mauvements generaux covering the See also:Atlantic in 1865, the study of local thunderstorms by Hippolyte See also:Marie-See also:Davy, Sonrel, Fron, Peslin, in France, and the work of See also:Fitzroy, See also:Buys-See also:Ballot, See also:Buchan, Glaisher and See also:Thomson in Great See also:Britain, parallel the analogous works of the American students of meteorology and form the beginnings of our modern dynamic meteorology . The details of the historical development of this subject are well given by See also:Hugo See also:Hildebrand-Hildebrandsson and See also:Leon Teisserenc de See also:Bort in their See also:joint work, See also:Les Bases de la meteorologie dynamique (Paris, 1898-1907) . The technical material has been collected by Hann in his Lehrbuch . Many of the See also:original memoirs have been reproduced by Brillouin in his Memoires originaux (Paris, 1900), and in See also:Cleveland See also:Abbe's See also:Mechanics of the Earth's Atmosphere (vol. i., 1891; vol. ii., 1909) . The publication of daily weather charts and forecasts is now carried on by all civilized nations . The See also:list of government bureaux and their publications is given in See also:Bartholomew's Atlas (vol. iii., London, 1899) . Special establishments for the exploration of the upper atmospheric conditions are maintained at Paris, Berlin, See also:Copenhagen, St See also:Petersburg, Washington and Strassburg .

The general problems of climatology (1900) are best presented in the Handbook of Dr Julius Hann (2nd ed., Stuttgart, 1897) . The general See also:

distribution of temperature, winds and pressure over the whole globe was first given by Buchan in charts published by the Royal Society of See also:Edinburgh in 1868, and again greatly revised and improved in the See also:volume of the Challenger reports devoted to meteoro+ logy . The most complete atlas of meteorology is Buchan and Herbertson's vol. iii. of Bartholomew's Atlas (London, 1899) . Extensive works of a more special character have been published by the London Meteorological Office, and the Deutsche Seewarte for the Atlantic, Pacific and See also:Indian Oceans . Daily charts of atmospheric conditions of the whole northern hemisphere were published by the U.S . Weather Bureau from 1875 to 1883 inclusive, with monthly charts; the latter were continued through .1889 . The physical problems of meteorology were discussed in Ferrel's Recent Advances in Meteorology (Washington, 1885) . Mathematical papers on this subject will be found in the author's collection known as The Mechanics of the Earth's Atmosphere; the memoirs by Helmholtz and Von Bezold contained in this. collection have been made, the basis of a most important work by Brillouin (Paris, 1898), entitled Vents contigus et nuages . A general ,See also:summary of our knowledge of the mechanics and physics of the atmosphere is contained in the See also:Report on the International See also:Cloud Work, by F . H . See also:Bigelow (Washing-ton, 1900) . The extensive Lehrbuch (Leipzig, 1901; 2nd ed., 1906) by Dr Julius Hann is an authoritative work .

The optical phenomena of the atmosphere are well treated by E . Mascart in his Traite d'optique (Paris, 1891-1898), and by J . M . Penter, Meteorologische Optik (1904-1907) . Of See also:

minor treatises especially adapted to collegiate courses of study we may mention those by Sprung (Berlin, 1885) ; W . Ferrel (New See also:York, 1890) ; Angot (Paris, 1898) ; W . M.See also:Davis, (See also:Boston, 1893) ; See also:Waldo (New York, 1898) ; See also:Van Bebber (Stuttgart, 189o) ; See also:Moore (London, 1893) ; T . See also:Russell (New York), 1895 . The brilliant volume by Svante See also:Arrhenius, Kosmische Physik (Leipzig, 1900) contains a See also:section by Sandstrom on meteorology, in which the new hydrodynamic methods of Bjerknes are developed . I.—FUNDAMENTAL PHYSICAL DATA There can be no proper study of meteorology without a See also:consideration of the various physical properties of the atmospheric gases and vapours, each of which plays an See also:independent See also:part, and yet also reacts upon its neighbours . Atmospheric air is a mixture of nitrogen, oxygen, aqueous vapour, carbonic acid gas (See also:carbon dioxide), See also:ammonia, argon, neon, See also:helium, with slight traces of See also:free See also:hydrogen and hydro-carbons . The proportions in which these gases are See also:present are quite See also:constant, except that the percentage of aqueous vapour is subject to large See also:variations .

In an atmosphere that is saturated at the temperature of 90° F., as may occur in such a climate as that of See also:

Calcutta, the water may be 240A of the whole weight of any given volume of air . When this aqueous vapour is entirely abstracted, the remaining dry gas is found to have a very uniform constitution in all regions and at all altitudes where examination has been carried out . In this so-called dry atmosphere the relative weights are about as follows: Oxygen, 23.16; nitrogen and argon, 76.77; carbonic acid, o•o4; ammonia and all other gases, less than o•oi in the See also:lower See also:half of the atmosphere but probably in larger percentages at great altitudes . Of still greater rarity are the highly volatile gases, argon (q.v.), neon, krypton and helium (q.v.) . Outer Limit.—These exceedingly volatile components of the atmosphere cannot apparently be held down to the earth by the attraction of See also:gravitation, but are continually diffusing through the atmosphere outwards into interstellar space, and possibly also from that region back into the atmosphere . There are doubtless other volatile gases filling interstellar space and occasionally entering into the atmosphere of the various See also:planets as well as of the See also:sun itself ; possibly the hydrogen and hydro-carbons that See also:escape from the earth into the lower atmosphere ascend to regions inaccessible to See also:man and slowly diffuse into the outer space . The laws of See also:diffusion show that for each gas there is an See also:altitude at which as many molecules diffuse inwards as outwards in a unit of See also:time . This See also:condition defines the outer limit of each particular gaseous atmosphere, so that we must not imagine the atmosphere of the earth to have any general boundary . The only intimation we have as to the presence of gases far above the surface of the globe come from the phenomena of the See also:Aurora, the See also:refraction of See also:light, the See also:morning and evening twilight, and especially from the See also:shooting stars which suddenly become luminous when they pass into what we See also:call our atmosphere . (See C . C . See also:Trowbridge, ' On Luminous See also:Meteor Trains " and " On Movements of the Atmosphere at Very Great Heights," Monthly Weather Review, See also:Sept .

1907.) Such observations are supposed to show that there is an appreciable quantity of gas at the height of, See also:

loo m., where it may have a See also:density of a millionth part of that which prevails at the earth's surface . Such See also:matter is not a gas in the ordinary use of that See also:term, but is a collection of particles moving independently of each other under those influences that emanate from sun and earth, which we call radiant See also:energy . According to Stormer this radiant energy is that of electrons from the sun, and their movements in the magnetic See also:field surrounding the earth give rise to our auroral phenomena . According to Professor E . W . See also:Morley, of Cleveland, See also:Ohio, the relative proportions of oxygen and nitrogen vary slightly at the surface of the earth according as the areas of high pressure and See also:low pressure alternately pass over the point of observation; his remarkably exact work seems to show a possible variation of a small fraction of i %, and he suggests that the air descending within the areas of high pressure is probably slightly poorer in oxygen . The proportion of carbonic acid gas varies appreciably with the exposure of the region to the See also:wind, increasing in proportion to the amount of the shelter; it is greater over the See also:land than over the See also:sea, and it also slightly increases by See also:night-time as compared with See also:day, and in the summer and See also:winter as compared with the See also:spring and autumn months . During the See also:year 1896 Professor S . Arrhenius in the Phil . Mag., and in 1899 Professor T . C . Chamberlin in the Amer .

Geol . Jour., published memoirs in which they argued that a variation of several per cent. in the proportion of carbonic acid gas is quite consistent with the existence of See also:

animal and See also:vegetable See also:life and may explain the variations of climate during See also:geological periods . But the specific absorption of this gas for See also:solar radiations is too small (C . G . See also:Abbot, 1903) tosupport this See also:argument . The question whether free See also:ozone exists in the atmosphere is still debated, but there seems to be no satisfactory See also:evidence of its presence, except possibly for a few minutes in the neighbourhood of, and immediately after, a See also:discharge of See also:lightning . The general proportions of the See also:principal gases up to considerable altitudes can be calculated with See also:close approximation by assuming a quiescent atmosphere and the ordinary laws of diffusion and elastic pressure; on the other hand, actual observations show that the rapid convection going on in the atmosphere changes these proportions and brings about a fairly uniform percentage of oxygen, nitrogen and carbonic acid gas up to a height of io m . Aqueous Vapours.—The distribution of aqueous vapour is controlled by temperature quite as much as by convection and has very little to do with diffusion; the See also:law of its distribution in altitude has been well expressed by Hann by the simple See also: