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CHEMICAL NEWS,

July 6, 1917

Reducing Gas, Volumes to Standard Temperature and Pressure.

moves the carrier, cd, to which CD is fixed. The arm, AB, will be called the "pressure" arm, and the arm CD the "temperature" arm.

To use the apparatus the temperature arm, CD, is set with its centre or "zero" line over the reading 760 mm. on the pressure scale, and the slide, a b, is moved to the position indicated by the index, i, on A B. The cursor is then set to the temperature o° C., or 273° on scale TM т. The volume factor is 1'o, as shown in Fig. 1.

P mm.

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The cursor reading on the scale, v v, now gives the required volume factor. Suppose we require to find the volume-factor for a change from o° C. to 15° C., and from pressure 760 mm. to pressure 750 mm. The cursor is set to the reading 15° C. (or 288), and the volume-factor reading is 1056 (factor for temperature change only at pressure 760 mm.). The arm, CD, is now set to the new pressure 750 mm., and the volume factor becomes 1'070. (d) The reduction of the volume of a gas measured at temperature to C., and under pressure of P mm. to its volume at o° C., and pressure of 760 mm., is effected as FIG. M

(a) If the cursor is moved to above o° C. or 273° absolute, the pressure being unchanged, the cursor will

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ive the "volume-factor" for temperature to C., and pres
ure 760 mm.
(b) It the temperature is kept at o° C. or 273° absolute,
and the arm, CD, is moved by the screw e to a pressure P
mm., the cursor reading on the scale, v v, gives the volume-
factor at o° C. to change to pressure P mm. from
760 mm.

(c) If the volume-factor for a change from o° C. to t° C., and from pressure 760 mm. to pressure P mm. is required, the cursor is moved to above o° C. (or 273°), and the arm CD is then set with its centre line at the new pressure

follows:-The scales are first set as shown in Fig. 1 and
explained above. The cursor is moved to the temperature
(273°+), and the arm, Er, clamped in position. The
arm CD is now moved along A B until the volume-factor
ro is under the cursor, and slide ab is clamped.
cursor is moved to the reading to, on the scale op,
зhown to the right of TT. This scale, op, is called the
"reduction temperature" scale, and is necessary because
the changes of volume are being made on the volume at

The

and not on the volume at o° C. A similar scale, om, is shown on the left for changes made at temperatures

below o° C. These "reduction temperature" scales are marked respectively and . In the figure the graduations are only shown for every 10° and are not numbered. When the cursor has been set to t° on the "reduction temperature" scale the reading on vv is the volume factor to reduce volume to o° C. at pressure P mm. The pressure is now changed to 760 mm. by moving C D along the pressure scale, and the volume-factor required is read off. An example will make this clear. A volume of V cc. of gas, measured at 30° C. and under a pressure of 720 mm., is to be reduced to volume at o° C. and 760 mm. The apparatus being set as shown in Fig. 1, the cursor is set to temperature reading 273° +30° = 303°, and the arm CD moved inwards until the volume-factor is 1o, and then the arm EF is moved down to 30° on the + "reduction temperature" scale, op. The volume-factor is now o 900 (for volume at o° C. and pressure of 720 mm.). The arm CD is now set at pressure 760 mm., and the volume-factor is now o 853. Therefore V cc. x 0·853 will give the volume at o° C. and 760 mm.

In Figs. 2 and 3 modified forms of the apparatus are shown. Fig. 2 shows the apparatus arranged on the slide rule pattern. The corresponding parts are denoted by the same lettering in all the figures. The temperature scale, TT, and the factor scale, v v, are arranged side by side, but one of them is movable, parallel to the other, preferably the scale v v. The cursor carrier, E F, moves along the scales, as in a slide rule. The cursor, cd, c'd', is shown separately for clearness; fg is the 760 mm. pressure line, and the other pressure lines are slightly diver- | gent, and are crossed by the zero temperature line, 00; other temperature lines are drawn parallel to line oo, and correspond to temperature intervals of 20° between +100° C. and 100° C. The scale cd, c'd' moves horizontally in the carrier E F, and thus any required temperature line can be set over the factor scale, v v. The "reduction temperature" scales, marked + and, are placed on opposite sides of the apparatus.

THE REALITY OF ATOMS.

By A. FINDLAY, M.A., D.Sc.

Ar a time when the purely utilitarian applications of physical science occupy, not unreasonably, a chief place in men's minds, it is well to turn aside occasionally to the contemplation of other aspects of science and to consider some of the triumphs which have been won in the domain of pure knowledge. The man of science is no mere dealer in "cold facts," no mere gatherer of stones by the wayside of life; but he seeks also, by the divine gift of an intuitive intelligence, " to explain the complications of the visible in terms of invisible simplicity." It was to such intuitive intelligence that we owe the Atomic Theory, put forward by the Manchester schoolmaster, John Dalton, in the early years of last century-a theory which recently formed the theme of the presidential address to the Chemical Society. Although the march of knowledge has carried us far from the point where Dalton stood, the theory which he propounded still remains the essential basis of modern physical science.

By means of an additional arm between CD and E, and parallel to CD, graduated from o to 100, the apparatus can be used to calculate percentage compositions and results From the earliest dawn of thought men's minds have of combustion experiments. This arm is not shown in been busied with the question of the constitution of Fig. 1. The extra arm, in conjunction with an additional matter; and throughout all time one has had to decide scale along the arın AB, can be used to find "weight-between the two alternatives of continuity and disconfactors," by which the weights of volumes of gases, tinuity. With the speculations of the ancient Greek measured at t° C. and pressure of P mm., can be found philosophers (grand and comprehensive as they often by multiplying the measured volumes by the "weight- were), with the Aristotelian doctrine of the four elements factors." (based on the Empedoclean conception of a continuous primordial matter), or with the Atomic Theory of Leucippus and Democritus-we need not longer delay. They helped but little, if at all, towards the explanation and co-ordina tion of the facts of science. However much the idea of continuity appealed to the older thinkers, in modern times it has come to be recognised that "the notion of continuity is the result of an arbitrary limitation of our attention to a part only of the data of experience." The further we extend our investigations, the more refined and powerful the instruments we employ, the more does the coarse grainedness of matter become evident. Apart from the conception of discontinuity the atomic theory of Dalton had nothing in common with the ancient philosophy so admirably expounded by Lucretius. In the older theory the atoms were all regarded as consisting of the same primordial material, although differing in size and shape; but to Dalton the atoms differed in their nature. In the case of any particular element, the atoms were assumed to be all exactly alike in their properties, including their mass, but they differed from the atoms of any other element. At first no distinction was made between the smallest particle of an element and the smallest particle of a compound, and a certain amount of difficulty and confusion was thereby caused, for it is clear that, although we may regard the atom of an element as indivisible, the atom of a compound must be capable of being broken up into the atoms of its component elements. A new name was therefore introduced by the Italian chemist Avogadro, who called the smallest particle of a compound a molecule, and for the advance of chemical science this new concep tion has been of inestimable value.

Fig. 3 shows a circular form of the apparatus. The factor scale, v v, is shown inside the temperature scale, TT, but the reverse arrangement may be adopted; one of these scales is movable, preferably the outer one, which is usually TT. The 66 temperature reduction" scales are marked on the same scale as that on which the temperatures are marked, and move with scale TT if this is movable. The cursor-carrier, E F, revolves round the centre E, and the cursor scale, which is similar to that of Fig. 2, moves horizontally in a slide in the carrier, EF, which can be clamped in position by the screw, E. The circular cursor, shown below Fig. 3, may replace the sliding cursor described above. The pressure scale, cd, from 720 to 800 mm. is marked in separate segments for intervals of temperature of 20° C. between o° C. and +100° C., and 0° C. and 60° C.

The method of using these forms is similar to that described above for the original form; when a change of pressure is to be made at a temperature to the cursor is set with the temperature line along the edge of the scale, v v, before the pressure change is made.

In the apparatus as described the temperature range extends from o° absolute temperature to 373° absolute, but for most purposes a more limited range would be sufficient. The range of the apparatus, both as regards temperature and pressure, may be easily extended much beyond the above limits without enlarging the apparatus. The Whitgift School, Croydon, May 9, 1917.

The theory of Dalton, we have seen, postulated definite properties for the atoms of the elements, and consequently the atom of an element must have a definite mass or weight; and the determination, not of the absolute mass but of the relative masses or weights of the atoms, became one of the main preoccupations of chemists in the first half of the nineteenth century, and still forms the subject of exact investigation. It was, in fact, just because Dalton's theory was capable of quantitative expression in terms of the relative weights of the atoms of the different elements that it was possible for the hypothesis of the atomic constitution of matter to become for science the invisible simplicity behind the complications of the visible. But is it anything more than an hypothesis, useful but not necessarily representing actual fact? Recent discoveries

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in science allow us now to answer this question with confidence. They have, from several different directions, con. tributed towards establishing the atomic hypothesis in a position of unassailable strength, and have furnished a proof of the real and actual existence of atoms or discrete particles as constituting the fundamental basis of matter. Only a few of these proofs can be indicated here, but a clear account of the evidence accumulated in support of the real existence of discrete particles has recently been published by one whose work has greatly advanced our knowledge of this subject ("Atoms," by Jean Perrin).

The phenomena of diffusion, more especially in gases, led to the conclusion that the particles or molecules of which matter was assumed to be constituted are not in a state of rest. In the case of a gas, these molecules are regarded as being in a state of constant and tumultuous commotion, which is not entirely subdued even when the gas is condensed to the liquid, or frozen to the solid state. That, at least, is the picture of matter which presented itself to the inner vision of a genius like Clerk Maxwell, and which forms the basis of what is known as the kinetic theory, a theory which was developed by applying to these still hypothetical molecules the general laws of mechanics. In this way it became possible, on the basis of experimental data, to calculate not only the absolute mass of the molecule-the hydrogen molecule weighs about three quadrillionths (million million million millionths) of a gramme-but also its dimensions (approximately one hundred millionth of an inch in diameter), and the speed of its movement (several hundred yards per second); and the agreement between the values derived from the different kinds of measurement cannot but excite our admiration. And yet the theory cannot carry complete conviction, by reason of the number of hypotheses which it involves; and s there have not been wanting some who refused to accept the objective reality of molecules. And yet, even in 1827, these molecules had, all unknown to their observers, made their presence manifest by the effects which they produced. In that year the botanist, Brown, observed that when suspensions of pollen grains were examined under the microscope the particles were seen to be in rapid motion, vibrating, rotating, moving along a zigzag path, sinking, rising-perpetually in motion. In this so-called Brownian movement-observed long ago by Buffon and Spallanzani, who saw in it a manifestation of lite-we see, not, it is true, the molecules themselves, but the effects of the incessant bombardment of the coarser particles of the suspension by the molecules of the liquid. When one applies to the suspension the law of the equi partition of energy, it follows that, in a condition of equilibrium, the kinetic energy of the relatively coarse particles will be the same as that of the molecules of the liquid. We have, then, in the Brownian movement merely a magnified picture, as it were, nf molecular movement; and if this is so, then the magnitudes calculated from these comparatively coarse suspensions should be the same as those calculated according to the molecular kinetic hypothesis. This conclusion has been tested in various ways, more especially by the French physicist, Jean Perrin, and has been found to be correct.

As a result of the combined action of gravity and of the kinetic energy of the molecules, the molecules in a column of gas are more crowded together at the bottom of the column than at the top, in accordance with the law that when the distances from the bottom increase in arithmetical progression the concentration of the particles diminishes in geometrical progression. By counting the number of particles at different levels of a column of a fine suspension of gamboge in water, Perrin found that the distribution of the particles accurately obeyed the same law. These particles in Brownian movement, therefore, behave exactly as the molecules of a gas would behave according to the kinetic theory; and in a number of other ways also the suspensions of particles which can be seen behave in exact concordance with the laws which have been deduced for invisible particles. Our belief in the actual

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existence of these particles is thereby greatly strengthened. The extension of our limits of vision, also, which the invention of the ultramicroscope has made possible, has disclosed the existence of particles in what hitherto bad appeared, even under the most powerful magnification, to be homogeneous matter; and by this means particles not greatly exceeding in dimensions those of the molecules have been detected. The smaller the particles the more lively is their motion, so that we can scarcely hesitate to believe that in the rapid, darting motions of the ultramicroscopic particles we have made manifest to us something of the extraordinary stir and commotion which is going on in that world of molecules which is beyond the power of our direct observation.

But the grained or discontinuous structure of matter has been still more clearly demonstrated in the recent striking work on radio-activity. The phosphorescent light emitted by certain materials, when bombarded by the a rays emitted by radio-active substances was found by Sir William Crookes to be resolved, when examined by a magnifying glass, into separate scintillations or points of light, each of the star-like points of light marking the impact of a projectile; and in the spinthariscope, invented by Sir William Crookes, one is enabled to see the individual effect of a single atom. But these a-rays, as Sir Ernest Rutherford most definitely has shown, are positively charged atoms of helium, which he has even succeeded in counting, and the atomic structure of this gas is thereby demonstrated.

Whether we calculate the fundamental molecular magnitudes from the viscos ty of gases; from the Brownian movement of fine, but visible particles; from the phenomena of radio-activity; or from the blue colour of the sky, by which also the discontinuous structure of matter is made manifest, the same results are obtained, and the real existence of molecules is thereby established with a probability amounting to a certainty. But while we can regard the atomic constitution of matter as established beyond any reasonat le doubt, yet, in the words of Prof. Perrin: "Atoms are no longer eternal indivisible entities, setting a limit to the possible by their irreducible simplicity; inconceivably minute though they be, we are beginning to see in them a vast host of new worlds. . . Nature reveals the same wide grandeur in the atom and the nebula, and each new aid to knowledge shows her vaster and more diverse, more fruitful and more unexpected, and, above all, unfathomably immense." - The New Statesman, June 16, 1917.

NITROGEN FROM THE AIR. MANCHESTER'S NEW ENTERPRISE.

WE are able to supplement from a well-informed source the interesting announcement in the Manchester Guardian of June 23 that plant is about to be erected in Manchester for the manutacture of nitrogenous products from the nitrogen in the air. For reasons that will be obvious, fuller details must be reserved until the conclusion of the

war.

Ever since the British blockade was enforced, Germany has found it impossible to import Chilian nitrates for the manufacture of explosives and fertilisers. It reverted, therefore, to the expedient of "fixing" the nitrogen from the air, and has adopted it to a huge extent since almost the beginning of the war. It has been stated in German technical journals that the output of nitrogenous products by the Bädische-Anilin Fabrik, with the aid chie fly of the Haber-catalytic process, amounts now to about 500,000 tons a year. By these means the Germans get all the nitrogenous ingredients for their high explosives.

Attempts have been made to work the Haber process in this country, but all have failed, and the general consensus of opinion now is that this is not a commercial process, as

the expense and risk appear to be enormous. Germans, however, it is a case of needs must.

With the that the whole of the ovens and appliances necessary were destroyed before it could be attained. Another obstacle was placed in the way by the shipping trade, who feared the loss, if the experiments then made proved a success, of the nitrate shipping trade. Means were subsequently found of overcoming the difficulty created by the intense heat required, and further efforts were made in France which proved to be successful. There is a works in that country now which has for a number of years been producing nitrates from the air."

The only other way by which nitrogen can be fixed from the air is by the electric processes, of which up to now the principal have been the Baekeland and Evde, the Schönhurr, and the Pauling. All of these are single-phase and electrical processes, and are considered workable commercially only in places like Norway, where electricity can be generated cheaply by water power. None of them has been worked in England, because of the high cost of electricity here, which makes them uneconomic under ordinary conditions.

The consequence is that the fixation of atmospheric nitrogen has not been adopted in this country, which relies for its supplies of this valuable ingredient of high explosives and an indispensable part of all the principal fertilisers on the utilisation of Chilian nitrates, the price of which has increased enormously since the beginning of the

war.

A New Process: English Discovery.

A new factor in the situation has now arisen in the new method of nitrogen fixation from the air which is about to be started in Manchester. National considerations preclude details being given at present, but it is believed that with this process nitrogen can be "fixed" anywhere in England at a very low cost, even where electricity is fairly expensive, because it apparently achieves the highest efficiency of nitrogen fixation per kilowatt hour of energy used that has ever been achieved or even dreamt of by any of the other processes mentioned. Its inventor is a British subject.

The Manchester Corporation succeeded in being the first to get the industry started, because it went out of its way to help the promoters, the International Nitrogen and Power Company, 8, Waterloo Place, London, who hold the exclusive rights to work the process in Great Britain. The new industry is believed to have great possibilities, not only for war purposes but after the war. Possibly when the method comes to be worked throughout the United Kingdom it will make this country independent of oversea supplies of fixed organic nitrogen, and provide a new security against the danger of interruption of oversea supplies of essential ingredients of explosives in time of war. If it can be done the whole of our nitric acid supplies could be obtained in this way, and also picric acid, an essential ingredient in synthetic dyes.

Above all, it would bring to realisation Sir William Crookes's prediction to the British Association at Bristol over thirty years ago that the future of the white race would largely depend on the economic fixation of atmospheric nitrogen, by which the world might be made to yield larger quantities of wheat and other foodstuffs.

Through the good offices of the Manchester Corpora tion an excellent site for the works has been provided. Construction has already begun, and the establishment should be working within six months from now.

There is no special virtue in the air of Manchester that has led to the selection of the city for this important pioneer enterprise. The choice was determined by other circumstances. Nor need the public have the least apprehension of the effects of the process on atmospheric conditions. The volume of air used up is an infinitesimal fraction of the aerial ocean.

Inquiries made recently by a representative of the Man chester Guardian showed that a movement for carrying into effect a project for obtaining nitrates from the atmos phere was started in Manchester ten or twelve years ago, the motive being, of course, mainly a commercial one. The promoters were, for the most part, engaged in the bleaching industry, who desired to avoid, if it was possible, the expense of bringing nitrates so largely used in their business from South America. It was found, however, that an obstacle to the development of that scheme was the intense heat required to make the process successful. "We needed heat," one of the promoters of that time said recently, "of an intensity of 2000°, and the result was

A chemist at a large house in the dyeing trade expressed the view recently that but for the fact that the Germans had for years obtained nitrates from the air the war would have been over long ago, considering the present diffi culties in the way of their obtaining them from Chili or other South American sources.

MAKING ANIMALS TRANSPARENT. WHAT THE ROYAL COLLEGE OF SURGEONS HAS TO SAY TO THE SPALTEHOLZ MEthod.

(From a Correspondent).

IN the CHEMICAL NEWS of June 13 appeared an account of the Spalteholz method of making animals transparent, as exemplified in successful specimens exhibited to a CHEMICAL NEWS representative by Dr. S. F. Harmer, F.R.S., at the Natural History Museum, South Kensington. When Dr. Harmer applied to the Patents Court for licence to employ this method, which is covered by a German patent, the Controller of Patents, Mr. Temple Franks, threw doubt on the validity of the patent because, apparently, it seeks to patent a principle of optics by basing the method on the refraction of light. The dead animal, after chemical treatment, is placed in a solution having tho same index of refraction as its own tissues. Skeleton, muscles, and arteries are then revealed through the fabric of the outer tissues.

At the Royal College of Surgeons, however, doubt is cast on the subject matter of the patent from another point of view-that fruitful source of contention known, in the term of the lawyers, as prior user! In a word, there is nothing new in the method at all! They have used it at the Royal College of Surgeons for years!

Prof. Keith (who sat with the imposing skeleton of the Irish giant O'Bryne behind him-an eighteenth century worthy who looked out on the world from the unusual altitude of 8ft. 4in.) assured the CHEMICAL NEWS interviewer that the idea of clarifying tissues was as old as the hills. Instead of applying the process to a small piece of tissue Spalteholz had used it for large bodies-" a thing none of us have wanted to do particularly," said Dr. Keith, "because we don't see much use in it. It has long been used in microcopy. Indeed, the principle of the employment of clarifying oils is tolerably obvious. You go into a wooden building, in the daylight, and you see the sun shining through a resinous knot-and there you are, the whole thing is complete! The rat, by this process, is transparent, instead of the knot, because of an essential oil.

"But Spalteholz cannot claim to have invented transparencies, even of animals. Thoy were first made in the fifties by Prof. Beale, of King's College, in the Strand. Beale used as alkali-potassium hydrate will servethongh Beale never patented his method. He was too busy with other things. Beale's method was afterwards re-discovered on the Continent, where it came to be known as Schultze's method. We have employed Beale's method in the College for the last fifty or sixty years, and have several specimens in the museum.

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