1186 THE COLLIERY GUARDIAN June 23, 1916, M. Weitz based his calculations on the following T> JO formula :—E = (2), but stated that this similarity is only approximate. M. Sachlier used the formula :— T) p E = — - . With this formula, the thickness would N -P only become infinite when N = P. After referring in minute detail to the foirmulee adopted by several Continental engineers, the author went on to say that in an examination of the ice wall a great many assumptions have to be made in calcu- lating the power of the freezing plant, but several coefficients have been approximately determined by experience. Thickness of Ice Wall. It is also possible to determine the necessary thickness of the ice wall, though the formulee are not entirely satis- factory. What, however, is more difficult to determine beforehand is the proportion of rock and water. It is necessary to assume that the conductivity for cold is the same for the full depth of the shaft, an assumption which is not absolutely exact, for it has been pointed out that clay and overlying lignites are not such good conductors as sand; and, finally, the entire theory assumes that the freezing columns are equidistant throughout their length —which is never correct, owing to the deviations of the boreholes. On the other hand, only vague data exist as to the real thickness of the ice walls. Holes drilled in the wall to prove the thickness may cause a dangerous influx of water. It is, therefore, very important to determine the thickness of the ice walls, if possible, previous to the commencement of sinking, so as to be able to concentrate the energy of the freezing plant on the weak places. The following experiences may be noted. From tests made in mines it has been averred that dry docks will allow Hertzian waves to pass through, but that wet strata offer a resistance, which increases with the percentage of water. Frozen ground acts like dry rock. It is, therefore, possible to examine the thickness of an ice wall by two different methods. (1) Taking two freezing tubes as antennae, or feelers, the electric wave will easily pass from the transmitter to the receiver if the wall is thick; but if there is any break in the wall the wave will be almost stopped. (2) It is possible to communi- cate electric vibrations to the freezing columns. The amplitude of the wave will be a large one, if the tube is not surrounded by a thick coating of ice, but will be reduced if water is in the vicinity, and becomes almost nil if the column is surrounded by water. As a large number of freezing tubes are employed, the test has to be repeated, and the weak spots of the ice wall can be exactly located. These experiencest are, however, only in their infancy, but the results already obtained are encouraging enough to justify the hopes that they will be pursued further. However, many co- efficients will have to be deter- mined by experience, as the various kinds of intersected rocks have a different permeability for Hertzian waves. Details of the Poetsch Method. When this method was intro- duced it was not viewed with favour, as one of the essential conditions for its success was the absolute verticality of the boreholes; and as there were no means of verifying this verti- cality, the general idea was that the new process was of no value beyond a depth of 40 or 45 yds. The first application of the process was in 1883 at the Archibald lignite mine, near Schneid- lingen, Saxony. The work was quite successful, but took an extremely long time on account of an artificial current which was connected with the lignite below by a centre tube. In 1884 the process was tried at two shafts 125 ft. deep at the Emilie lignite mine, near Finster- walde, Germany, but both there and at the Centrum mine, Koenigswusterhausen (Brandenburg) water broke in, through the boreholes not being deep enough, and the shafts had to be abandoned. The first really successful sinking by this process was carried out at the Lens Collieries in 1890, the credit being largely due to M. Reumeaux, the general manager of the mines. Subsequently, the Poetsch process was largely used in northern France for shafts from 100 ft. to 350 ft. in depth. Among them special mention may be made of two shafts 335 ft. deep sunk in 1884 at Vicq, for the Anzin Mines Company. In 1897 a shaft 460 ft. deep was sunk at Auboue, in East France. For the first time a successful test was made to verify the verticality of the boreholes. The result of this experience was that the freezing process was quickly adopted in other countries. An early contract was made in Germany at Ronneberg by a French company, and the number of applications in that country exceeds 60. Great Britain, United States, Austria, Russia, Holland, and Belgium followed. In the latter country sinkings o>f 1,200 to 2,000ft. were made in the new coal fields of the Campine. Such operations natu- rally require apparatus which will correctly measure the deviations of the boreholes, but even this question is not entirely solved. Bore Shaft and Freezing Cellar. At a general rule, excavation is started with a larger diameter for a short depth, in order to receive the inside guide tubes. This chamber will also receive the brine mains. The depth of this cellar depends to a large extent on the method of boring employed. If several sets of boring apparatus are employed, more especially in deep shafts, this excavation is the first operation, and is surrounded by a brick wall which will also support the headgear. If, however, the boring apparatus can do the work quickly, for shallow depths it is not always essential to make this cellar, though there must be a derrick which will travel round the outside of the shaft. In that case the cellar will only be needed for the circular mains, and will not be required until the bore- holes are completed. This system was employed at one of the Bruay collieries, where the ground was frozen to about 450 ft. For very deep shafts the same method has also been used. For example, at the Levant-du- Flenu Colliery, Belgium, two derricks were employed for a shaft which had to be frozen to 760 ft. On the Continent the advantage of this system is that very large and high headgear is not required, but in Great Britain the Mining Regulations demand a detach- ing hook, which necessitates the pulleys being always fixed at a considerable height. Where there is a water level in close proximity to the surface, the bore shaft should only be very shallow, but, as a general,rule, it is from 10 to 13 ft. in depth. There are, however, cases in which it is sunk to greater depths, the No. 9 shaft of the La Louviere and Sars Longchamp collieries, Belgium, being 140 ft. in depth. As the freezing cellars are for the reception of the brine mains, they are insulated from the shaft by means of a wooden skirting, which makes it an enclosed chamber, or sometimes by means of a circular brick wall, which will eventually surround the headgear. But as the whole weight of the headgear is carried by this inner wall, and the boring excavations will considerably weaken the foundation of the wall, the latter may be incapable of giving the necessary support to the head- gear. Of the Flines-les-Raches Colliery in North France, where the natural water level was at about 6 ft. above the ground, the brine mains were placed in the brick chamber above the ground, in order to re-establish the equilibrium of the water which filled it and made a kind of tank. Boring Methods. Several systems of boring have been employed—rods (with or without free-fall), water-flush, and rope boring. .jm JW ■ 'f w •,•11 ■'j Fig. 2.—Bkine Mains and Connecting Pipes. Quick boring apparatus should be adopted for deep shafts, but it has been found that the vibrations set up in the hole floor by excessive boring speed is unfavour- able to the verticality of the boreholes. An attempt has been made to overcome that defect by erecting the boring engines on solid concrete foundations outside the freezing cellars altogether, but though this method facili- tates the removal of the apparatus for each hole, it does not obviate altogether the excessive vibration caused by high speed. The Liegeois Colliery in North Belgium probably holds the record for speed in boring, but the holes were a great deal out of vertical, necessitating a number of supplementary boreholes. Distribution of the Boreholes. The freezing tubes are spaced round the shaft at a distance of not more than 3 ft. from the side of the shaft, and about 3 ft. 4 in. apart. For deep shafts the former distance has to be increased to allow a very large ice wall to be made and for th© deviations from the vertical not exceeding -1 per cent. Beyond this limit, it is generally necessary to bore supplementary holes, which, however, is not always easy, it being very difficult to make a straight hole in ground which has been softened by borings in the vicinity. In the early application of the freezing process in France, the freezing tubes were also inserted in the inside of the shaft, to he sure of finding the hard ground at their base, but where it was, however, found that too many masses of ice were created, which exercised great pressure on each other and fractured the freezing tubes. At No. 3 shaft of the Dourges Colliery, only one freezing tube was inserted in the centre, and at Vicq the shafts of the Anzin Colliery Company in 1894, the central tubes were completely suppressed, since which time they have only been used in very exceptional oases. At the shaft No. 6 of the Maries Colliery the base of frozen ground was not very firm, and had to be solidified in the centre of the shaft. In this case the greater part of the centre tube was also- insulated. As a rule, central holes are bored if the ground con- tains a certain amount of clay, to allow an outlet for the water which is found between the circular ice wall and the two horizontal planes of watertight clay. The holes round the shaft must penetrate into the solid or water- tight strata below. Freezing Columns : Ascending Tubes. In the early stages it was thought that copper tubes would give better results than iron or steel, because of their conductivity. Comparative tests have proved that this effect is only transient, and disappears after five days. In the early application of the freezing process, the casing tubes of the boreholes were used for the circu- lation of cold brine, but these tubes could not be made watertight, and have since been superseded by tubes with closed welded bottoms. The outside diameter is generally about 5 in. The freezing tubes must be quite free from any cracks or fissures. They must be strong enough to resist the pressure of the ice (which may exceed that of the ground), and therefore it is nece-ssary to test each tube, before insertion, at a pressure of at least double that of the water which is contained in the ground. The nipples must be longer than would be necessary for air tubes, because of the enormous strain put on them during freezing, and as the different strata are not all solidified in the same time, two parts of the freezing columns may be strongly secured by the ice wall, while the middle portion continues to contract. To meet this contingency, Gebhardt placed several stuffing boxes in the column, but it is impossible to see whether they are watertight, and in many cases leak- age of brine has occurred which made dangerous holes in the ice wall. The writer thinks it would be better not to extend the freezing tubes to the bottom of the boreholes but to suspend them, thus allowing for their contraction when the freezing has commenced. Inner Tubes : Descending Tubes. These are about 2 in. in diameter, and are inserted in the larger tubes, to direct the cold brine to the bottom. In the early application of the freezing process, the bottom end of the tube was closed by a wooden plug, and the brine had an outlet through several small holes in the walls of the tube, but these are liable to choke with impurities or rust, and the result may be a com- plete interruption of the brine current. It is therefore advisable to have the lower end about 2 ft. from the bottom of the outer tube. Brine Mains. When all boreholes are provided with outer and inner tubes,, cappings are fitted to the outer tubes, to connect both sets of tubes, through pipes of lead or steel, to two cast iron or steel mains, one acting as a distributor, and the other as a collector (fig. 2). These are, as a rule, arranged in circles, but for a square shaft would be laid in a rectangle. Each main has a number of flanges corresponding to the freezing tubes, and each flange has a valve to regulate the brine circu- lation. It is essential to know whether the brine is running through each tube, and also if the circulation of the brine is regular. Should one of the tubes be obstructed, this will be indicated by the head or capping being free from rime, since when the circulation is in order these cappings quickly get covered with ice. It is advisable to provide the cap with a small cock, which can be opened from time to time to measure the temper- ature of the outflowing brine, and also to release any air imprisoned in the brine circulator. Choice of Circulating Medium. The selection of the refrigerating liquid depends upon the temperature to which the ground has to be frozen. As a general -rule, a solution of calcium or magnesium chloride is adopted. With the former it is possible to get down to — 25 degs. Cent. ( —13 degs. Fahr.), but with a saturated -solution a temperature of — 40 degs. Cent. (— 40 degs. Fahr.) can be obtained. This process is not free from drawbacks, -as the salt settles easily by crystallisation. With a solution of magnesium chloride, temperatures between —40 and — 45 degs. Cent. ( -40 and — 49degs. Fahr.) can easily be attained; but it has been suggested -that this class of brine will affect the metal of the freezing tube. For very low tempera- tures denatured alcohol is used, by which a temperature of — 75 degs. Cent. (— 103 degs. Fahr.) can be obtained before the freezing point is -reached. As these three liquids dissolve ice it is absolutely necessary that the joints of the freezing columns should be perfectly water- tight, to prevent the risk of holes being formed in the ice wall. Non-freezing oil could be adopted to avoid this risk, but until recently the high price of this product prevented its adoption. Rofrig .rating Machinery and Medium. The systems used for the production of cold are absorption and compression machines, and -the media are ether, ammonia, or carbonic acid g-as. The writer thinks that an ether compressor was employed in 1864 in Wales, but since that time the freezing industry has made con- siderable progress and ether i-s no longer used. In the early days of the Poetsch method, absorption machines of the Carre system were used, but compressors of the Fixa-ry, Linde, and Oseinbruck systems or other similar types are now preferred. For very low temperatures carbonic acid machines are convenient, but for the purpose of shaft freezing they are more difficult to supervise than ammonia compressors. The cooling tanks, or evaporators, are insulated as much as possible. At Llay Main Collieries they are placed in an insulating chamber (fig. 3) an arrangement which has the advantage of easily maintaining the brine at a low temperature, should the plant be stopped for any reason. For the brine and water circulation, centrifugal or plunger pumps are used, the latter being generally preferred for the brine, as they allow for -the removal of any obstruction .in the columns, and can retard the speed of the whole plant, when less cold is required after the complete formation of the ice wall. The freezing plant is connected with the brine mains by a double pipe line. The Freezing Process. If the brine pipes and mains are carefully insulated the running of the compressors must be regulated so that