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See also:ARGON (from the Gr. 6.-, privative, and Epyov, See also:work; hence meaning " inert ")
, a gaseous constituent of atmospheric See also:air
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For more than a See also:hundred years before 1894 it had been supposed that the See also:composition of the See also:atmosphere was thoroughly known
.
Beyond variable quantities of moisture and traces of carbonic See also:acid, See also:hydrogen, See also:ammonia, &c., the only constituents recognized were See also:nitrogen and See also:oxygen
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The See also:analysis of air was conducted by determining the amount of oxygen See also:present and assuming the See also:remainder to be nitrogen
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Since the See also:time of See also: 143 . o I 2 3 4 5 6 Holes uncovered . convenient method devised by See also:Vernon See also:Harcourt, in which air charged with ammonia is passed over red-hot See also:copper . Under the See also:influence of the See also:heat the atmospheric oxygen; unites with the hydrogen of the ammonia, and when the excess of the latter is removed with sulphuric acid, the See also:gas properly desiccated should be pure nitrogen, derived in See also:part from the ammonia, but principally from the air . A few concordant determinations of See also:density having been effected, the question was at first regarded as disposed of, until the thought occurred that it might be desirable to try also the more usual method of preparation in which the oxygen is removed by actual oxidation of copper without the aid of ammonia . Determinations made thus were equally concordant among themselves, but the resulting density was about -ro 0 6 part greater than that found by Harcourt's method (See also:Rayleigh, Nature, vol. xlvi. p . 512, 1892) . Subsequently when oxygen was substituted for air in the first method, so that all (instead of about one-seventh part) of the nitrogen was derived from ammonia, the difference See also:rose to 1% . Further experiment only brought out more clearly the diversity of the gases hitherto assumed to be identical . Whatever were the means employed to rid air of accompanying oxygen, a See also:uniform value of the density was arrived at, and this value was z % greater than that appertaining to nitrogen extracted from compounds such as nitrous See also:oxide, ammonia and ammonium nitrite . No impurity, consisting of any known substance, could be discovered capable of explaining an excessive See also:weight in the one case, or a deficiency in the other . Storage for eight months did not disturb the density of the chemically extracted gas, nor had the silent electric See also:discharge any influence upon either quality .
(" On an See also:Anomaly encountered in determining the Density of Nitrogen Gas," Proc
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See also:Roy
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See also:Soc., See also:April 1894.)
At this See also:stage it became clear that the complication depended upon some hitherto unknown See also:body, and See also:probability inclined to the existence of a gas in the atmosphere heavier than nitrogen, and remaining unacted upon during the removal of the oxygen —a conclusion afterwards fully established by See also:Lord Rayleigh and See also:Sir See also: Some doubted the See also:discovery of a new gas altogether, while others denied that it was present in the atmosphere . Yet there was nothing inconsistent with any previously ascertained fact in the asserted presence of x % of a non-,oxidizable gas about See also:half as heavy again as nitrogen . The nearest approach to a difficulty See also:lay in the behaviour of liquid air, from which it was supposed, as the event proved erroneously, that such a constituent would See also:separate itself in the solid See also:form . The evidence of the existence of a new gas (named Argon on See also:account of its chemical inertness), and a statement of many of its properties, were communicated to the Royal Society (see Phil . Trans, clxxxvi. p . 187) by the discoverers in See also:January 1895 . The See also:isolation of the new substance by removal of nitrogen from air was effected by two distinct methods . Of these the first is merely a development of that of Cavendish . The gases were contained in a test-tube A (fig . 1) See also:standing over a large .quantity of weak alkali B, and the current was conveyed in wires insulated by U-shaped See also:glass tubes CC passing through the liquid and See also:round the mouth of the test-tube . The inner See also:platinum ends DD of the See also:wire may be sealed into the glass insulating tubes, but reliance should not be placed upon these sealings . In order to secure tightness in spite of cracks, See also:mercury was placed in the bends .
With a See also:battery of five See also: The spectrum may now be further examined with a more powerful See also:instrument . The most conspicuous See also:group in the argon spectrum at atmospheric pressure is that first recorded by A . Schuster (fig. a) . Water vapour and excess of oxygen in moderation do not interfere seriously with its visibility, It is of interest to See also:note that the argon spectrum may be fully See also:developed by operating upon a miniature See also:scale, starting with only 5 C.C. of air (Phil . Mag. vol. i. p . 103, 1901) . The development of Cavendish's method upon a large scale involves arrangements different from what would at first be expected . The transformer working from a public See also:supply should give about 6000 volts on open circuit, although when the electric See also:flame is established the voltage on the platinums is only from 1600 to 2000 . No sufficient See also:advantage is attained by raising the pressure of the gases above atmosphere, but a capacious See also:vessel is necessary . This may consist of a glass See also:sphere of 5o litres' capacity, into the See also:neck of which, presented downwards, the necessary tubes are fitted . The whole of the interior See also:surface is washed with a See also:fountain of alkali, kept in circulation by means of a small centrifugal See also:pump . In this apparatus, and with about one See also:horse-See also:power utilized 4t the transformer, the absorption of gas is 21 litres per hour (" The Oxidation of Nitrogen Gas," Trans . Chem . Soc., 1897) . In one experiment, specially undertaken for the See also:sake of measurement, the See also:total air employed was 9250 c.c., and the oxygen consumed, manipulated with the aid of partially de-aerated water, amounted to Io,82o c.c . The oxygen contained in the air would be 1942 c.c.; so that the quantities of atmospheric nitrogen and of total oxygen which enter into combination would be 7308 c.c. and 12,762 C.C. respectively . This corresponds to N+ I.75 0, the oxygen being decidedly in excess of the See also:pro-portion required to form nitrous acid . The argon ultimately found was 75.0 c.c., or a little more than r % of the atmospheric nitrogen used . A subsequent determination over mercury by A . M . Kellas (Proc . Roy . Soc. lix. p . 66, 1895) gave 1.186 c.c. as the amount of argon present in See also:loo c.c. of mixed atmospheric nitrogen and argon . In the earlier stages of the inquiry, when it was important to meet the doubts which had been expressed as to the presence of the new gas in the atmosphere, See also:blank experiments were executed in which air was replaced by nitrogen from ammonium nitrite . The residual argon, derived doubtless from the water used to manipulate the gases, was but a small 43 44 45 16 47 48 49 saw — . Red I I 1I Hy F FIG . 2 . fraction of what would have been obtained from a corresponding quantity of air . The other method by which nitrogen may be absorbed on a considerable scale is by the aid of See also:magnesium . The See also:metal in the form of thin turnings is charged into hard glass or See also:iron tubes heated to a full red in a See also:combustion See also:furnace . Into this air, previously deprived of oxygen by red-hot copper and thoroughly dried, is led in a continuous stream . At this temperature the nitrogen combines with the magnesium, and thus the argon is concentrated . A still more potent absorption is afforded by See also:calcium prepared in situ by See also:heating a mixture of magnesium dust with thoroughly dehydrated See also:quick-lime . The density of argon, prepared and purified by magnesium, was found by Sir William Ramsay to be 19.941 on the 0=16 scale . The See also:volume actually weighed was 163 c.c .
Subsequently large-scale operations with the same apparatus as had been used for the principal gases gave an almost identical result (19'940) for argon prepared with oxygen
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Argon is soluble in water at 12° C. to about 4.0%, that is, it is about 22 times more soluble than nitrogen
.
We should thus expect to find it in increased proportion in the dissolved gases of See also:rain-water
.
Experiment has confirmed this anticipation
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The weight of a mixture of argon and nitrogen prepared from the dissolved gases showed an excess of 24 mg. over the weight of true nitrogen, the corresponding excess for the atmospheric mixture being only 11 mg
.
Argon is contained in the gases liberated by many thermal springs, but not in See also:special quantity
.
The gas collected from the See also: The same value had previously been found for mercury vapour by Kundt and Warburg, and had been regarded as confirmatory of the monatomic character attributed on chemical grounds to the mercury See also:molecule . It may be added that See also:helium has the same character as argon in respect of specific heats (Ramsay, Proc . Roy . Soc . 1. p . 86, 1895) . The refractivity of argon is •q61 of that of air . This See also:low refractivity is noteworthy as strongly antagonistic to the view. at one time favoured by eminent chemists that argon was a condensed form of nitrogen represented by N3 . The viscosity of argon is 1.21, referred to air, somewhat higher than for oxygen, which stands at the See also:head of the See also:list of the principal gases (" On some Physical Properties of Argon and Helium," Proc . Roy . Soc. vol. lix. p . 198, 1896) .
The spectrum shows remarkable peculiarities
.
According to circumstances, the See also:colour of the See also:light obtained from a See also:Plucker. vacuum tube changes " from red to a See also:rich See also:steel See also:blue," to use the words of See also:Crookes, who first described the phenomenon
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A third spectrum is distinguished by J
.
M
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Eder and See also:Edward Valenta
.
The red spectrum is obtained at moderately low pressures (5 mm.) by the use of a Ruhmkorff coil without a jar or air-See also:gap
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The red lines at 7056 and 6965 (Crookes) are characteristic
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The blue spectrum is best seen at a somewhat See also:lower pressure (r mm. to 2.5 mm.), and usually requires a Leyden jar to be connected to the secondary terminals
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In some conditions very small causes effect a transition from the one spectrum to the other
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The course of electrical events attending the operation of a Ruhmkorff coil being extremely complicated, special interest attaches to some experiments conducted by See also: At a pressure of I mm. the red glow of argon was readily obtained with a voltage of 2000, but not with much less . After the discharge was once started, the difference of potentials at the terminals of the tube varied from 63o volts upwards . The introduction of a capacity between the terminals of the See also:Geissler tube, for example two plates of metal 1600 sq. cm. in See also:area separated by a glass See also:plate cm. thick, made no difference in the red glow so See also:long as the connexions were good and the See also:condenser was quiet . As soon as a spark-gap was introduced, or the condenser began to emit the humming sound See also:peculiar to it, the beautiful blue glow so characteristic of argon immediately appeared . (Phil . Mag. xhii• p . 77, 1897.) The behaviour of argon at low temperatures was investigated by K . S . Olszewski (Phil . Trans., 1895, p . 253) . The following results are extracted from the table given by him: Name . See also:Critical Critical Boiling Freezing See also:Tempera- Pressure, Point, Point, See also:ture, Cent . Atmos . Cent . Cent . Nitrogen . -146.0 35'0 -194'4 -214.0 Argon —I2I.0 50.6 -187.0 -189.6 Oxygen -118.8 5o•8 -182.7 The smallness of the See also:interval between the boiling and freezing points is noteworthy . From the manner of its preparation it was clear at an See also:early stage that argon would not combine with magnesium or calcium at a red heat, nor under the influence of the electric discharge with oxygen, hydrogen or nitrogen . Numerous other, attempts to induce combination also failed . Nor does it appear that any well-defined See also:compound of argon has yet been prepared . It was Argon See also:zinc Hydrogen 478 found, however, by M . P . E . See also:Berthelot that under the influence of the silent electric discharge, a mixture of See also:benzene vapour and argon underwent contraction, with formation of a gummy product from which the argon could be recovered . The facts detailed in the original memoir led to the conclusion that argon was an See also:element or a mixture of elements, but the question between these alternatives was See also:left open . The behaviour on liquefaction, however, seemed to prove that in the latter case either the proportion of the subordinate constituents was small, or else that the various constituents were but little contrasted . An See also:attempt, somewhat later, by Ramsay and J . See also:Norman Collie to separate argon by See also:diffusion into two parts, which should have different densities or refractivities, led to no distinct effect . More recently Ramsay and M . W . Travers have obtained evidence of the existence in the atmosphere of three new gases, besides helium, to which have been assigned the names of neon, krypton and xenon . These gases agree with argon in respect of the ratio of the specific heats and in being non-oxidizable under the electric spark . As originally defined, argon included small proportions of these gases, but it is now preferable to limit the name to the principal constituent and to regard the newer gases as " companions of argon." The physical constants associated with the name will scarcely be changed, since the proportion of the " companions " is so small . Sir William Ramsay considers that probably the volume of all of them taken together does not exceed Thth part of that of the argon . The physical properties of these gases are given in the following table (Prot . Roy . Soc. lxvii. p . 331, 1900) : Helium . Neon . Argon . Krypton . Xenon . Refractivities .1238 .2345 •968 1.449 2.364 (air = 1) 1.98 9'97 19.96 40.88 64 Densities (0=16) Boiling points c . 6° 1 ? 86.9° 121.33° 163.9° at 76o mm. abs . abs. abs. abs . Critical See also:tern- ? below 155.6° 210.5° 287.7° peratures 68° abs. abs. abs. abs . Critical pres- ? ? 40.2 41'24 43'5 slues metres. metres. metres . Weight of 'c.c . ? ? I.2I2 2.155 3.52 of liquid gm. gm. gm . The glow obtained in vacuum tubes is highly characteristic, whether as seen directly or as analysed by the spectroscope . Now that liquid air is available in many laboratories, it forms an advantageous starting-point in the preparation of argon . Being less volatile than nitrogen, argon accumulates relatively as liquid air evaporates . That the proportion of oxygen in-creases at the same time is little or no See also:drawback . The following analyses (Rayleigh, Phil.Mag., See also:June 1903) of the vapour arising from liquid air at various stages of the evaporation will give an See also:idea of the course of events: Percentage of Percentage of Argon as a Percentage Oxygen . Argon. of the Nitrogen and ce on Argon . |
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