1078 THE COLLIERY GUARDIAN. June 8, 1917. as the load for all practical purposes is equally distri- buted, the curve will be a parabola with a longer or shorter focal distance depending on the nature of the strata. Let fig. 14 represent the section of a coal seam from which the coal has been removed between A and B, the roof having fallen to the irregular line ACB. The dotted line A' C' B' will indicate the line of stress. This, it will be seen, impinges on the coal close to the edge at A. The stress at this point represents half the weight of the strata overlying the span A B which is assumed to be sufficient to crush the coal about the point A. The integrity of the arch being destroyed, the line of stress must seek a new position such as DEB. Naturally this movement will be no greater than is absolutely necessary to gain a solid footing for the arch, which will again be so near the edge of the coal already crushed that it will fail again in a short while, necessitating a further adjustment of the position of the arch. With this continuing failure and re- adjustment we have the well-known phenomena of a crush or squeeze advancing slowly over the workings, destroying coal as it goes. E w \\ X... Fig. 14.—Arch Stresses in Mine Roof. If now a considerable body of ;the seam, as A H G F, is quickly removed a “fall” may result which will reach high above the seam, say to the line F J B, which will cause the line of stress to move quickly and reach the coal well back from the point F, where it is suffi- ciently solid to give the needed support, and the working will be said to have “ gotten ahead of the crush,” when in fact the crushing force has gone ahead of the working. This explains the common experience of the relief at the working end of the pillar caused by an extended break in the roof over the exhausted area. Under other conditions, especially when the arching line of stress has a wide span, thus carrying a large amount of weight, the crushing force may prove too much for even the solid coal well back from the end of the pillar and cause the phenomena of crushed coal, broken timbers, creeping floor, etc., well down the room or stall, while the ends of the pillars will be free from any trouble, as they carry only the small amount of material which is below the line of stress. This con- dition will sometimes be cured automatically by the material falling from the top of the cavity over the exhausted area in such a manner that the space between the material already down and the undisturbed measures will be filled and the opposite limb of the arch (the right hand in the figure) will find support on this already fallen material and thus shorten the span of the arch and lessen the total weight. When the break has reached the surface, this filling takes place more rapidly owing to the fracture of the overhanging beds along the edge of the break, and since the arch has a new point of support for its inner or right hand limb, the conditions are ripe for further working undisturbed under the smaller arch. While the general shape of the line of stress in the cases under consideration is the parabola, for all practical purposes the ratio between the span and the rise or height of the arch will vary much as the material varies in which it exists. After the fall of the first mass the cavity grows through the crushing and falling of the material along the top of the arch, due to the pressure along the line of stress, and by the splitting oft along the joint planes of the material on the sides due to the same cause. Since the pressure along the upper portion of the line of stress is manifestly less in a high sharp arch than in a low flat one, the shape of the arch in this respect may be expected to vary with the capacity of the material to withstand this stress. Hence, there will be a high arch in a soft material with numerous joints and a flat arch in tough material with fewer joints, This may be verified practically by the examination of old drifts or tunnels where the over- lying material has had an opportunity to fall and take the shape due to such conditions without regard to other influences. If, then, the cavity in its upward progress encounters a bed of tough resistant shale or sandstone, it may fall so slowly that a large area may be opened by con- tinuous mining during the delay, resulting in a heavy weight along the line of stress due to the wide span and crushing the coal either at the working end of the pillar or at such point along the course of the room as the line of stress may meet the coal. Such a crush is not likely to find relief until the overlying measures are sufficiently broken down to .fill the space S S, and allow the development of a new smaller arch of stress A B C, which, having less span and consequently less load, will transmit less load to the point A. According to Dr. F. W. McNair the readjustments that take place when a pillar fails sometimes put an enormous longitudinal thrust on the foot wall, and in places its surface portion has buckled under such stress. Experience seems to show that at the great depths recently reached it is useless to expect to hold up the hanging rock mass for a long time by any scheme of pillars unless far too much of the lode is left in place, and that the only feasible method is to cut away the entire lode and permit the hanging to cave as rapidly as it will to the point where the broken rock fills again the whole space and redistributes the weight over the foot wall. C. T. Rice considers that in supporting the roof of a stope, only that portion of the roof that is below the line of the dome of equilibrium requires support; the rock above this dome sustains itself. If, therefore, the shape of this dome of equilibrium in each kind of rock were known, it would be easy to calculate the weight of rock hanging below the dome, and so timber the stope as to hold up this weight. The shape of this dome is fairly constant in each kind of rock; especially in the same rock in the same district. Of course, slips and joints, sudden changes in chemical composition, the dip of the strata in sediments, and many other facts, would affect the shape of the dome, but as long as these were small their effect would also be small. If investigation of the shape of this dome should suggest any formula to determine the strength of timber necessary to support the ground below the dome, the effect of these joints, etc., could easily be included by the factor of safety used. ENGINEERING DATA AND OBSERVATIONS. In America very few data have been collected on sub- sidence due to mining operations, at least the data, if collected, have not been made available for scientific purposes. In order that observations may be of value the following correlated data are desirable: (1) The elevations of a number of points on the surface for a period of years both prior to, during, and following the mining directly beneath. (2) The position of these points with regard to permanent stations located outside of the mining field or upon ground which has not been or will not be subject to the influence of the mining operations. (3) The position of the working face in the mine on the various dates of survey. (4) An accurate location and description of the character of the portions of the mineral deposit left unmined. (5) An accurate location and a description of the supporting materials placed in the excavated area. (6) The thickness and dip of the material mined. (7) The thickness and character of the bed immedi- ately underlying. (8) The thickness, dip and character of the overlying rocks and all available information in regard to structure. (9) The thickness and character, of the surficial material. (10) The quantity of water removed from the mine. (11) The location, extent and data of underground movements of rocks overlying the mineral deposit. In Europe records have been kept for many years in various districts in order to determine the vertical amount, lateral extent, rate and duration of subsidence. Among the first surveys made to determine the movement of the surface were those of Fayol. At PlaiiafLevbl AB ; firet