November 19, 1915. THE COLLIERY GUARDIAN. 1029 d = sag in feet under the worst conditions as calcu- lated from the usual formula d = 8 » Where I = span length in feet. i; tv - resultant of weight and wind pres- sure in in. (per foot). S = tension in conductor in lb. if, - corresponding sag at same temperature when wind and icfe arts removed; w, = weight per ft. of.wire Only. M = modulus of elasticity . (say; 1R ,000,000). A = cross section of wire in sq. in; Then, to find d,, use the formula u-, ____________w____64 (d, 2 — d2) M A d — 31* From d, it is possible to find the sag d2 at any Other temperature from the formula :—• f — f = 8 (fZ-’2 ~ d\ *1 + £ , /]— (3 1‘ 4-8d, 2)c MAc \ d2/ Where t, = temperature in degs. Fahr., with sag, t2 = any other temperature in degs. Fahr. d2 = sag at temperature. c = coefficient of expansion per deg. Fahr. Modulus of Elasticity. An examination of the stress strain curve of any hard-drawn copper wire will show that the modulus must be constant for the particular size, since the curve is a straight line up to the elastic limit, but the modulus is not necessarily the same for different sizes of wire. In making measurements for true modulus values, it is necessary to work on long lengths of wire, which approximate to the span length employed on a tramway or other overhead line, since this method would tend to eliminate sources of error. The Engineering Standards Committee’s Report No. 55 stated that the values of the “ apparent moduli obtained on the first application of the load would be of interest and use, since it is these which must be taken into account in the erection of long lengths of wire.” This statement, however, is objected to, because in all well constructed overhead lines the wires should, first be strained to a tension higher than that at which they will be permanently bound in, in order to get rid of kinks, and to allow the wires, especially stranded conductors, to ‘‘settle down.” This preeedure makes it permissible to take advantage of the real modulus value, which may, on the average, be considered as 18,000,000, instead of the , I. —-"V ---’ Large Locomotive for the Natal Coal Traffic. usual text book figure of 16,000,000. It will, however, hardly be practicable to embody a minimum modulus value in ordinary specifications of hard-drawn copper, in view of the difficulties and delays which would occur in most works in carrying out the sensitive tests required. In special cases, however, it might be advisable to specify a minimum value, and to make arrangements with the National Physical Laboratory, or other testing institutions to provide the necessary apparatus, and carry out the tests on specimens provided for the purpose. Tensile Strength. An interesting point arises out of the widely held belief that the strength of hard-drawn wire lies in its skin being hardened during the drawing process. An examination of the matter does not disclose any con- clusive evidence in support of this theory. Effect of Temperature on the Strength of Hard-Drawn Copper. The question of the maximum permissible tempera- ture of hard-drawn copper is of importance on overhead power lines, because of the effect of heat in reducing its tensile strength. The National Physical Laboratory found that, on wires up to 0-194 in. diameter, the reduction in breaking load due to temperature appears to be approximately one-tenth of one per cent, of the breaking load at normal temperature per degree Cent, rise of temperature. The results of the speaker’s own experiments seem to confirm that the determination will hold good for all sizes of circular copper wire. A number of experiments have been carried out by Dr. F. J. Brislee to determine the permanent effects of prolonged heating on the strength of wire, from which it appears that with 1/0 S.W.G. trolley wire, the permanent decrease in strength after two hours heating at 150 degs. Cent. (302 degs. Fahr.) is only 0-5 per cent., while a 4/0 S.W.G. wire was not affected after four hours. Among tramway engineers, it is generally understood that the temperature of trolley wires never exceeds 220 degs. Fahr, (say, 105 degs. Cent.), and it is a fair deduction from the above tests that the limiting temperature is not reached. In view, however, of the fact that the temperature rise occurs on wires while under strain, it would not appear to be advisable to exceed a temperature of 250 degs. Fahr, in practice. At this temperature the tensile strength of the wire would be about 10 per cent, less than at normal tempera- ture, but the strain would be relieved by the expansion due to heating. The Engineering Standards Com- mittee’s Report No. 55 gives the coefficient of expansion of copper per 1 deg. Cent, as varying between 0-0000163 and 0-0000167. The average of these is equal to 0-0000093 per 1 deg. Fahr. The voltage drop due to resistance would appear to ■ be the limiting feature in overhead wires rather than the question of temperature. In case it should be necessary to know the resistance of copper resulting from change of temperature this formula may be used R, = R (1 + 0‘0042£). Where R “ the resistance at odegs. Cent. If' — „ t degs. Cent. LARGE LOCOMOTIVES FOR THE SOUTH African coal traffic. A new series of exceptionally large and powerful locomotives,- of the Mallet articulated compound type, has been designed by Mr. £). A. Hendrie, the chief mechanical engineer of the South African Railways, and built by the North British Locomotive Company Limited, of Glasgow.- These locomotives are primarily intended for the haulage of the {fatal coal traffic over the heaviest sections of line, and also the general freight traffic to and from the Rand district. The locomotives are of the 2-6-B-2 wheel arrangement,- the front group of wheels being driven by the low-pressure' cylinders, 31/in. diameter and 26 in. stroke, whilst the rear group is driven by the high-pressure cylinders, 20 in. diameter by 26 in. stroke. Steam is distributed to all of the four cylinders by Walschae-rt’s valve gear, actuating piston valves working above the cylinders. The front bogie wheels are 2 ft. 4|in. diameter, the coupled wheels 4 ft. diameter, and the hind wheels 2 ft. 9/ in. The rigid wheelbase is 8 ft. 8 in. and the total engine wheelbase is 43 ft. 7 in. The boiler is of very large proportions, and, with the superheater, contains 3,827 sq. ft. of heating surface. The firegrate area is 53 sq. ft. At 50 per cent, of the working pressure (2001b. per square' inch) the tractive force is no less than 43,3301b. A system of spring equalisation is provided which embraces the springs of the bogie wheels at front and rear. These wheels have their springs connected with those of the foremost and hindmost coupled wheels. The engines are fitted with a change valve, which enables them to be worked either simple or compound, at the will of the driver. There is also a steam brake, and the tender is fitted with the automatic vacuum brake. Although these engines are built for the 3 ft. 6 in. gauge (the South African standard), they have each an adhesion weight of no less than 106 tons, and the weight in working order is 128 tons 5 cwt. The tender is carried upon two four-wheeled bogies, the wheels of which are 2 ft. 9/ in. diameter. The bogie wheelbase is 16 ft. 9 in. The tank has a carrying capacity of 4,250 gals, of water, and 450 eu. ft. space for coal. In working order, the tender weighs 51 tons 8 cwt. Engine and tender combined have a weight, in working order, of no less than 179 tons 13 cwt. 1 qr., a wheel- base of 70 ft. 10|in., and a total length of 81ft. 2 in. over buffers. The photograph is of additional interest, inasmuch that it shows one of these Mallet type loco- motives, the largest and heaviest railway engines ever built in Great Britain, alongside one of the Pechot articulated engines recently built at Glasgow for the French military railways. These engines have each a weight of 13/ tons, a heating surface of 288sq. ft., and a tractive force (at 75 per cent, of the boiler pressure) of 4,4501b. The awarding of the Nobel Prize for physics for 1915, by the Swedish Royal Academy of Science, to Prof. W. H. Bragg, M.A., D.Sc., F.R.S., of University College (jointly with his son), for an examination of the formation of crystals by X-rays, renders of special interest the announce- ment that Prof. Bragg is to deliver the 1916 May lecture before the Institute of Metals on the subject of the structure of metal crystals as revealed by X-rays. The Acting British Consul at Honolulu (Mr. G. H. Phipps) reports that a Honolulu company, which practically holds a monopoly of the coaling business done at that port, has recently made a contract with a New York firm for the construction of a new coal handling plant on the western side of the harbour, adjoining the course of the proposed Kalihi Channel. The storage capacity of this new plant is to be some 60,000 tons at the outset, and it is contemplated to increase it ultimately to 200,000 tons. The present plant, which has a capacity of only 30,000 tons, has become wholly inadequate to cope with the large increase of steamers calling for bunkers, consequent on the opening of the Panama Canal. The coal supplied comes exclusively from Australia and Japan. The new plant is to be up to date in every respect, and the entire system is to be electrically operated. Work has already been begun, and it is hoped to have the plant in operation by the beginning of July 1916. PROBLEMS OF THE SOUTH LANCA- SHIRE COAL FIELD. MANCHESTER GEOLOGICAL AND MINING SOCIETY. (Continued from page 977./ DISCUSSION. On the motion of the Chairman, seconded by Mr. Wordsworth, a vote of thanks was accorded Dr. Hiekling for his address. Mr. Stanley Atherton said he was particularly struck by the reference to the Wigan smash, and he would like to know whether the author had taken the ordnance without any outside observations for one end—-he assumed that it was the Carriage rock there—and taken the Upholland rock at the other end by quite a different process. Some years ago he (Mr. Atherton) came to the same conclusion as Dr. Hiekling, but he worked on a, different basis. The two certainly seemed to bear a very great resemblance to each other. Accepting that the Carriage rock was similar to the Upholland rock, and using that as a basis, he should like to ask the author to tell them whether, in the Manchester smash, he had come across anything -that really compared. There seemed to be quite a resemblance between the two ends. The Radcliffe field was very much broken up with smaller faults, and he did not agree with Dr. Hickling’s description of the part immediately north of Heaton Park. There was a resemblance between the North Radcliffe series and the Upper Irwell and lower portion of the Manchester smash, and if, from field work, the doctor had definitely decided any points, he should be most happy to compare notes with him. Mr. J. Gerrard said that, from what the lecturer had told them, it was practically hopeless to seek for further coal measures until they got some miles to the south of New Astley. There were no borings in that particular area that he was acquainted with. A test boring was put down about | mile to the south of New Astley: it went down about 400yds., and, as nothing was found, it was given up. He gathered now that, if the boring had been continued 200 or 300 yds. further, it might have struck the coal measures. That was extremely interesting, because it indicated the area within which an examination should be made. Dr. Hickling said there was no doubt whatever there were coal measures which did not appear on the original Geological Survey at all. There was, in fact, a coal measure which was reached, very near the surface, in a borehole on the site of the High-street baths of the Manchester Corporation, about a mile from that University, and it was again exposed in the railway cutting near Fallowfield Station, a few miles out of the city. That coal field was actually exposed to the surface, and it followed that -there must be coal very near the surface in that area. There might be, at the maximum, a thousand feet of red rocks just above the coal measures, but nowadays that would not stop the sinking of an important colliery. Mr. Gerrard remarked that the thickness of the red rocks was not the only point to be considered; the important question was the proximity of workable seams to the base of the red rocks. A colliery owner would not care to sink through 3,000 ft. of comparatively worthless upper coal measures in order to get in touch with workable seams. The author’s prognostication, as he understood it, was that there were workable seams within a reasonable distance of the base of the red rocks. Dr. Hickling replied that it was quite clear that, in that area at any rate, there was no great thickness of upper coal measures; and it was extremely improbable that a greater thickness of upper coal measures would be met with than existed above the Bradford Four-foot at Bradford. Mr. J. Lomax suggested that the statement that the denudation of the upper coal measures occurred before the deposition of the red sandstone was based on an assumption formed from the knowledge they already possessed of the unconcealed portion of the coalfield. Dr. Hickling replied that it was more than an assumption; it was based on actual facts. Mr. Lomax asked whether that meant there were no upper coal measures, so far as thickness was concerned, like there were in Staffordshire. Dr. Hickling said he had gone as far on that matter as he could go at the present time. Mr. Wordsworth said that, assuming the basin theory was correct, would not one expect, in getting from the north towards the centre of the basin, a flattening in the inclination of the seams? Dr. Hickling : In general, certainly. Mr. Wordsworth contended that, as a matter of fact, it was not so; it was rather steeper than flatter. That could be seen if they went two or three miles along the Irwell Valley fault. At Pendleton they went down, roughly, 3,000 yds. from north to south, and that would take them nearly into the centre of the basin. It was steeper on the dip than it was to the rise. Dr. Hickling said it was a very interesting point, and just the kind of information he was anxious to have. He