946 THE COLLIERY GUARDIAN. May is, 1917. CURRENT SCIENCE Economy of Coke Gasification. Mr. J. E. Enright (Gas Journal) reports that the carburetted hydrogen plant installed at Tralee, for the gasification of coke, has now been in operation for a period of 10 months, with the following results:—Car- buretted hydrogen gas made, 15,225,100 cu. ft.; coke used, including boiler fuel and stand-by fuel, 363 tons 9 cwt.; tar used in plan^, 10,197 gals. ; wages, £128 12s. 6d. ; working out at an average cost of 9d. per 1,000 cu. ft. into the holder. During the same period the quantity of coal gas made was 14,885,900 cu. ft., and the coal carbonised was 1,357 tons. The working of the plant throughout has been most satis- factory ; and, quite apart from the financial point of view, the worry and anxiety that it has saved would alone have been worth the capital outlay. There are other important economies effected, such as in the renewal, repair, and maintenance of retorts, the abnormal wear and tear on the whole carbonising plant in keeping up excessive heats, the number of stokers required, and the many other expenses incidental to the retort house. The operation of the plant is so simple that one man can work it, and, when the holders are full, he closes it down, and is then finished until the next morning. Often he completes his work as early as two o’clock in the afternoon. With regard to the distribution and consumption of the mixed gas, it has been found that the burner adjustment for a 50 per cent, gas will suit for any mixture up to all carburetted hydrogen gas. On two different occasions last winter, carburetted hydrogen gas was sent out exclusively, and the town was solely depending on the carburetted hydrogen plant for its supply of gas. During this period, an extra quantity of tar was employed, together with some coal in the generator. This was used with a view to increasing the hydrogen and methane in the gas, and reducing the carbonic oxide (this can be kept well below 18 per cent.). By these means, they were able to make a gas averaging upwards of 400 British thermal units. The mixed gas varies between 475 and 500 British thermal units; but a variation of anything between 400 and 500 British thermal units causes no trouble or com- plaint whatever once the burners or stoves are adjusted for the mixed gas; and Mr. Enright would have no hesitation in sending out straight carburetted hydrogen gas of 400 British thermal units, made from coal and tar or a mixture of coal, coke, and tar, with a carbonic oxide content of not more than 20 per cent. With gas engine trials, it has been found that the b.h.p. was not affected by the variation of the British thermal units; but the consumption of gas worked out practically in accordance with the British thermal units—that is to say, the consumption of gas of 400 British thermal units would be 20 per cent, more than with 500 British thermal units. Coal Gas for Internal Combustion Engines. The high price of petrol, and the increasing restric- tions placed upon its use, have induced motor users to turn again to the question of utilising ordinary coal gas as a fuel for internal combustion engines. The Commercial Motor, in a recent issue, describes and illustrates a valve for the necessary reduction of pres- sure when charging the engine. This valve is in use in connection with the service cars on the Neath tram- ways, where coal gas has been used on the system for some years. The principle involved in the construc- tion of the valve is that of a leather diaphragm, which is inflated on pressure above the desired amount, and deflated when that pressure is not reached; the action of the diaphragm closes or opens respectively a valve on the gas supply pipe. The gas first passes through a filter on its way to a small conical valve, which opens or closes the inlet to a chamber which, besides con- taining the mechanism of the special device, serves as a reservoir containing about J cu. ft. of gas. The exit is by means of a branch pipe, coupled up to the engine induction. The reservoir is covered by a leather diaphragm stiffened in the centre by perforated brass washers. The centre of the diaphragm is coupled by means of links and a lever to the small valve already mentioned. A light spring rests on the top of the leather diaphragm, which is adjustable for strength by a screw. The object of any regulation of the pres- sure exerted by the spring is to make it possible to maintain gas at varying pressures, and to obviate diffi- culties which might arise owing to frictional resist- ance of the mechanism. A flat spring held lightly at one end by a bracket in the base of the chamber tends always to close the valve. The excess of pres- sure above that desired lifts the leather diaphragm, closing the valve. So soon, however, as the pressure in the chamber drops below that which it is desired to maintain, the spring above the diaphragm will depress the leather and open the valve. Estimating the Heat Value of Similar Fuels. In a paper recently delivered before the Society of Chemical Analysts (Cheap Steam), Mr. Proctor Smith lays great stress on the need for ascertaining the calorific values of fuels so as to obtain figures which at a glance enable the buyer or user to have a ready means of classifying them, and to obtain a comparative if not scientifically accurate knowledge of the amount of heat which can be obtained from each fuel for a fixed sum of money. He suggests as a basis for com- parison the number of British thermal units which can be obtained for Id. from each different class of fuel. Mr. Smith is careful to state that in this comparison the different grades of fuel must be compared sepa- rately, that is to say, a nut coal cannot be compared with a slack, as the price is necessarily higher on the former owing to the amount of work in screening, etc. Taking, however, the coals in their different grades, i.e., nuts, through-and-through, slack, smudge, etc., very valuable information may be obtained which will constitute a trustworthy method of assembling the fuels in the order of their relative values. AND TECHNOLOGY. Mr. Smith emphasises the usefulness of knowing the mechanical condition of a fuel, and suggests that the coal should be put through different sizes of sieves, and by this means a faithful record of the condition of the fuel can be kept. For instance, in an ordinary steel works gas producer, the coal remaining on a 1| in. sieve would well serve the purpose, and that which passes through a J in. sieve (fine slack) could be weighed, and the percentage on and through the sieve thus ascertained. Mr. Smith includes in his paper an example on the lines suggested by himself, of a report of a coal analysis for the purpose of keeping a record : —Calcu- lated calorific value, 12,380 British thermal units per lb.; colour of ash, reddish-brown; coking test, good strong coke; a good clean fuel, free from shale, yields a long clear flame, particularly suitable for boiler use; clinker well burnt, free from much unconsumed carbon and showing very little signs of fusion; mechanical condition very good. Estimating Washable Products in Gaseous Mixtures. Mr. N. P. Broadbridge (Gas World) proposes a sim- plified method of determining the percentage of wash- able products in gases, based on the principle that when a hydroxylic solvent, such as ethyl-alcoho], con- tains in solution hydrocarbons immiscible with water, these latter are thrown out, when water is added, with which the alcohol is miscible in all proportions. A test constructed on this principle would be carried out in the following manner : —Three absorption bottles are arranged in series, the first two immersed in a freez- ing mixture. The size of the bottles is such that 50 c.c. of alcohol will produce a seal of, approximately, 1 in. This amount is accordingly introduced into the first tw’O, while a similar quantity of water is placed in the last, to retain the small amount of solvent which vaporises with the gas, the freezing mixture serving to reduce this vaporisation to a minimum. A convenient quantity of gas, determined by its con- tent of washable products, is passed through the bottles . at a rate of from 1 to 2 cu. ft. per hour. After this, all three are drained out into a tall stoppered cylinder of 400 c.c. capacity, and further rinsed with a few c.c. of distilled water, which is added to the contents of the cylinder. The volume is then made up to 400 c.c. with water, and the contents of the cylinder allowed to stand for half an hour or so, in order that the hydro- carbons, insoluble in dilute alcohol, may rise to the surface, where their volume is determined. Other liquids may be used for the determination, providing they embody the requisite requirements—viz., low viscosity, moderate volatility, miscibility with water, and solvent power for benzol. Rectified pyridine is one such liquid, and the quality should be of the 90 per cent, at 140 degs. Cent, variety. It should be previously tested by the usual method for oily matter by dehydration, distillation, and the dilution of the first few c.c. of distillate. It should be noted that the extent of dilution of the alcohol—viz., 1 to 4—should not be departed from, as otherwise, if the mixture is too concentrated, benzene, etc., would be held in solution ; or, if water is added in excess of this ratio, the total mixture becomes incon- veniently large, and presents occasion for minute globules of hydrocarbons to become entangled, and therefore remain in suspension. These precautions apply more especially to the estimation of very small quantities, as, for instance, in a washed or partly- washed gas. OiGlectrics io Electrostatic Fields. The problem whether dielectrics will change their dimensions when exposed to strong electrostatic fields has received little experimental investigation. One would expect some change, although not more than a small change probably. Righi and Quincke made some experiments 30 years ago, and Cantone and Pozzani followed the matter up in 1900; but the results were not concordant. Resuming these investigations recently, L. Bouchet (Comptes Itendus de V Academic des Sciences—abstracted by Engineering) first studied the expansion in a direction normal to the electric field. He placed cylinders of glass, paraffin, or ebonite between two concentric cylinders of brass, filling the annular space left with water; the system formed a tubular condenser. On the top of the cylinder of the dielectric material he placed a glass plate, and on this a leiis; when the electric field was excited by an influence machine (Voss) the cylinder expanded in the direction normal to the electric field, and pressed the glass plate against the lens, causing displacement of the interference rings. The length of the cylinders was about 40 cm., the diameter 1-5 cm., the thickness up to 2 mm. The expected dilatations were observed, but they amounted to 1 part in 1010 or less. The expansion was proportional to 1/E, how- ever, E being the Young modulus of elasticity, an interesting relation. On the other hand, the numerical results were not what they should have been for perfect dielectrics, and glass and ebonite (half-hard), which disagreed most, are, indeed, far from being considered perfect dielectrics. There seemed to be no direct- external electrostatic pressure effect on the length of the insulator. In the second series of experiments, Bouchet studied the effect of the electric field in the direction of the electric lines of force. The electro- static pressure effect would probably be more marked in this case, and there might be superposed either a contraction or a dilatation of the dielectric owing to the internal stress. The materials chosen for these experiments were pure Para rubber, vulcanised or unvulcanised, and, further, glass. Discs were formed, 15 cm. in diameter, up to 0-65 cm. in thickness, and .soldered (with paraffin) to discs of brass; on the top of each disc was placed a piece of aluminium or tin- foil, the brass and foil thus forming the condenser elec- trodes. Changes in the thickness of the disc were again measured by the method of interference. In the case of the vulcanised rubber, the observed contraction (amounting to 22 x 10-6 cm. maximum) was somewhat larger (although less than 100 per cent, larger, certainly) than the calculated contraction, and increased with the square of the field intensity; the unvulcanised rubber seemed to conduct the current, and behaved less satisfactorily. In order to ascertain whether the direct electrostatic pressure (attraction between the top and bottom of the condenser) was an important factor, Bouchet piled five of the vulcanised rubber condensers upon the top of one another, to form a multiple condenser; in that case the direct attraction effect should be the same as in a simple con- denser, because the attractions upwards and down- ward would balance one another in the intermediate condensers (of the multiple arrangement). The observed contractions were double those of the experi- ments with the simple condenser. Thus the contraction due to the internal electric stress would appear to be much stronger than the direct pressure effect. SUBSIDENCE RESULTING FROM MINING* By L. A. Young and H. H. Stoek. (Continued from page 910.) Underlying Rocks. The physical character of the rocks immediately underlying the mineral deposit is of great importance. Frequently coal beds are underlaid with beds of clay of such consistency that it will not support the pillars when the weight upon them is increased by the open- ing of rooms. The pillars are slowly pushed into the clay, while the • clay is forced into the rooms which have been mined. Similarly, when water reaches clay beds underlying the coal, the clay may be softened and forced into the rooms by the weight of the pillars, and a subsidence results. The term “ creep ” is very com- monly applied to such a movement. Very few tests have been made upon the bearing power of the clays occurring in mines, but numerous tests have been made upon clays and soils upon the surface. Owing to the importance of not placing upon the clay floor of a mine a burden which shall exceed the bearing power of clay, which is usually much less than the compressive strength of coal, the following values (Baker) are of interest: — Safe bearing power in tons per sq. ft. Kind of material. Minimum. Maximum. Rock—the hardest—in thick layers in native bed ............ 200-0 Rock equal to best ashlar masonry... 25-0 Rock equal to best brick masonry... 15-0 Rock equal to poor brick masonry... 5-0 Clay in thick beds, always dry .... 6-0 Clay in thick beds, moderately dry... 4-0 Clay in soft beds ................. 1-0 Gravel and coarse sand, well cemented .................... 8-0 Sand, dry, compact, and well cemented .................... 4-0 Sand, clean, dry .................. 2-0 Quicksand, alluvial soils, etc.... 0-5 30-0 20-0 10-0 8-0 6-0 2-0 10-0 6-0 4-0 1-0 The data on clay given in the table are not for fire- clay, and no data have been obtainable which are the results of observations upon the supporting power of such; clay of the character and occurring under con- ditions similar to those found in coal mines. Overlying Rocks. The study of subsidence due to mining operations involves particularly a consideration of the rocks over- lying the mineral deposit. Lack of uniformity in the overlying measures is the rule, not the exception, and this fact must be recognised in all attempts to formu- late theories and rules. The effect of different condi- tions of the overlying beds is well illustrated by two examples in England. At Sunderland, where the measures contain 50 per cent, of hard rock beds, seams at a depth of from 1,400 to 1,800 ft. have been worked for 70 years without reference to the surface. On the other hand, in the Midland and South Yorkshire coal fields, where the cover is composed largely of soft shales, the effect of workings at as much as 2,000 ft. is appreciable on the surface. Investigations of the thickness and physical char- acter of each overlying bed are fundamentally neces- sary to the accurate study of subsidence in any dis- trict. Much of the data as to the behaviour of various strata that can be secured will be at best only rela- tive. However, the more data that can be secured the fewer will be the variables with which the investigator must deal. Practically every theory of subsidence which has been advanced, when analysed, involves some funda- mental principle of mechanics. The beds may be sub- ject to tension, compression, bending, or shear. Samples of the various rocks may be tested in the laboratory in order to secure data to be used in the study of each problem. The great difficulty of obtain- ing specimens which will be representative of the section undet investigation is largely responsible for the scarcity of data along certain lines, n'otably those concerning the strength of rock in tension and in bending. Data on the strength of the rocks that are of import- ance in the study of subsidence have been collected and published by Bunting, who stated that numerous tests of various stones have proved that sandstones take permanent sets for the smallest loads, whereas granite and limestones are nearly perfectly elastic. It has also been proved by tests on various stones that the modulus of elasticity in compression is practically the same as in cross bending, but no fixed relation has been determined of the compressive, tensile, or shear- ing strength of the various kinds of stone. The shear- ing strength of sandstones and slates per sq. in. is * From University of Illinois Engineering Experiment Station Bulletin No. 91.