September 17, 1915. THE COLLIERY GUARDIAN. 569 Coal entangled with sandstone, and coal associated with clod, behave mechanically as if the coal were two different materials; and the writer suspects that under shearing stress its mechanical properties are intermediate between the two classes of rock—much more yielding than sandstone, but harder and more brittle than clod or fireclay. Associated with sandstone coal is the usual material which fills the cracks and fissures already described, and among massive sandstones, as displayed in section, ribbons of coal tailing out in ragged streamers can be followed for many yards, usually along, occa- sionally across, the bedding, ending in the most hair- like of narrow cracks. By increase of the relative pro- portion of coal to sandstone, blocks of rock appear as if enveloped in a matrix of coal. In this case also tapering films of coaly substance penetrate, to the thin- ness of thin paper, any fissures that there may be in the rock. With further increase in the proportion of coal to sandstone, any appearances which might suggest a solid sandstone invaded by plastic or liquid coal are lost, and one-time plates of rock, subjected to end pressure, but supported at the sides by solid though yielding coal, have decreased in length and have become puckered in the process. Among weak rocks, which in most cases are dark in colour, the outlines of coal inclusions are less easy to observe. Generally, any large mass that has preserved its individuality is a com- pound fragment, in which clod or holing dirt has failed to separate from the coal, and such pieces as a rule have bi-convex outlines and tail off as a spindle at each end. Smaller fragments occur as angular splinters with concave faces ending in cusps, and often, where on one side these adjoin pieces of stronger material, tapering wedges or films of coal persist bounded on that side by the stronger material and link up with other sharp- angled fragments which are associated by the side of similar surfaces. Thin plates of coal not infrequently occur strung out along the surfaces where the lenticles of bind adjoin, but the writer has not discovered any signs of slip along the boundaries of the coal. On the contrary, wherever plates of coal show signs of end pressure, they have become puckered and buckled after the manner of the sandstone plates previously described. 14. As already mentioned, the majority of the rock chunks as they lie in the rock fault jumble can be recognised as pieces which have been detached from an already consolidated parent rock. As- fragments, most of them show traces of the original planes of deposition, which in the sandstones (as often as not) are of cross- or current-bedded type. The usual altera- tions of coarser and finer sediment also show up plainly, and as an extreme case of this, bands of sandstone with true pebbles, almost always of rounded ironstone, are not infrequent. Fossils within the pieces are not unusual, and are interesting as affording a true index to the bedding planes, and a trustworthy indication of the amount of mechanical distortion which has been suffered by the pieces of rock in which they occur. From a careful study of the lie of the bedding planes in some thousands of rock chunks as they show in the rock-fault exploration headings at South Kirkby, Normanton, and elsewhere, the writer has arrived at the conclusion that in these rock-fault aggregates the rock fragments are hardly ever upside down. Often, especially with large pieces, the bedding planes are reared up as if a wedge had been pushed under the rock mass, or as if the rock mass itself had been driven forward against or over a withstanding obstacle. In these cases, however, the bedding planes seldom or never reach vertically, and the only examples of real inversion known to the writer are in binds of medium strength which underlie the upper member of a dupli- cated coal seam in the marginal thickened strip of a rock fault at Altofts Colliery, and have evidently been bent back on themselves as that upper seam was driven forward. (This case is illustrated in fig. 2, section B-C.) 15. In normal coal measure ground, quite one of the most striking characteristics is the regularity of the jointing of the rocks, and the persistence with which the joints maintain a direction over considerable tracts of country. In rock-fault fillings (with the very important exception noted below) regularity either in frequency or in direction of jointing is unknown, and from the absence of joint-block outlines to the rock chunks of the jumble, it may be argued that at the time of the filling of the rock fault the system of jointing now general over the district had not yet affected the rocks. This con- clusion is rendered the more acceptable by a considera- tion of the condition of the coal inside and outside the rock-fault areas. As mentioned above, no rock collected from a “ jumble ” has been proved to be in any way chemically different from the rock of similar texture in the measures outside. This constancy the writer inter- prets as meaning that all the displacement of rock pieces (coal as well as stone) had been completed before the “ sline ” was imposed, and that “ sline,” therefore, like the jointing of the rocks, w’as due to earth movements at a period subsequent to the formation of the “ rock faults.” Alternative Hypotheses. Having assembled the available data, the writer will now consider how the various items of evidence are fitted by the alternative hypotheses, which he may re-state as follow :— I. —Rock faults may be due to contemporaneous erosion of coal seams by flowing streams during coal measure time. II. —Rock faults may be due to lateral adjustments between beds by earth movements, at an early period subsequent to the consolidation of the rocks. That rock faults affect individual coal seams [1]* at particular places [2], and that they cut off the seams obliquely [4], is only to be expected on either hypo- thesis. That they are only frequent in seams in which a normally weak roof is closely overlain by a strong * The numbers in brackets refer to the numbered para- graphs. sandstone or conglomeratic rock [3] is the chief buttress on which upholders of hypothesis (I.) rely. These advocates of contemporaneous erosion will point out that the change from the quiet conditions required for deposition of fine sediment to conditions which would allow of the laying down of coarse sand and gravel over the same area is indicative of important alterations in the local topography, and that during the adjustment of these conditions continuity of the process of deposi- tion must have been interrupted, at least for a time. It was during that interruption that the local erosion, which they allege, must have taken place. Advocates of the earth movement explanation point out that, by reason of the change in the character of the sediment, there has resulted a corresponding variation in the mechanical properties of the rocks into which the sedi- ments have consolidated, and that at bedding planes where there were abrupt changes in the character of the sediment there are now the most marked contrasts of rigidity between the materials on either side of the bounding surface. As mentioned already, the contrast in behaviour of hard sandstone and soft clod under the mechanical con- ditions which prevailed during the production of a rock fault is very striking; and the writer sees no reason to believe that where thick masses of strong sandstone, interstratified between weaker beds of bind, etc., and extending over square miles of country, would, when the region is subjected to side and end pressure, do otherwise than allow the weak rocks to slide upon them. Such slipping is a process quite analogous to the con- traction, under vertical pressure, of muddy sediments past the hard concretions of ironstone, etc., in the pro- Figs. 7 to 9. Diagrams showing the fingering-out of a coal seam or fragment along “ stream-lines ” which are determined by the arrangement of the other and harder rocks of the rock- fault jumble. Often also in the termination of the seam the beds and partings are wedged open by bind or stony material, and the coal comes to an end in a sheaf of divergent wedges, the transverse sections of which recall fluttering pennons or the fin-scales of a swimming fish. duction of pot holes, as already described. This admitted, the origin of rock faults follows easily. For with the driving forward of hard rigid masses of sand- stone separated by weak bind from coal, which, if not strong as compared with the sandstone, was certainly more rigid than the separating bind, the shearing would be localised in the bind, which in shearing became some- what schistose, and was converted into clod. It is unlikely that mud resting upon a coal seam and covered by sand would remain uniformly thick, and the base of the sandstone might be correspondingly wavy. Hence, in the shearing, portions of the bind might be gripped beneath the sandstone and be carried forward with it. A continuation of the movement, especially if the pressure increased until the rock began to bend, would “ roll up ” the weaker rock into flattened cylinders, each with a lenticular-like section and tapering ends. These piling one upon another at certain places form the patches of “ bad roof ” that are frequent in many pits, which, though themselves free from rock faults, are working in seams which are liable to rock faults else- where. Between the patches of “ bad roof ” appear the “ rock rolls,” under which for a space the clod is completely pinched out, and the rock comes to rest directly upon the coal. It was (in 1913) from observations made on the structure of the “ jumbled ” bind in the roof, between rock rolls in the Park Gate seam workings at Tinsley Park Colliery, that the writer’s attention was drawn to the whole subject, and he noted then, as he affirms now, that the “jumbled” structure of the bad roof between rock rolls differs in no way from that of a fault breccia. From rock rolls to rock faults is but a further stage of the same process, for, granted that a rock roll is in contact with the coal, and a further for- ward movement takes place, the rock roll must “ seize ” with the upper layers of the coal, which, by reason of their greater rigidity, will offer special local resistance. This being overcome by the accumulation of the shear- ing stress, a tearing both of coal and rock results, and the rock fault is formed and filled in one and the same process. The plan of the rock fault area [5] and [6] is also critical evidence. Stream courses or hollows exca- vated by tidal scour have shapes which, although governed by complex laws, are quite determinate. It is unnecessary to discuss here the details either of the shapes or of the laws which govern them, but the writer may mention that the tributaries of streams enter the main stream at intervals which are commensurate with the volume of water carried, and that in present-day geography it is difficult to match the occurrence of several streams, each 50 or more yards wide, flowing in sub-parallel courses and eroding channels across the same half-mile of country. Streams also, though they may meander, can hardly have excavated hollows arranged en echelon, and the matter may be dismissed with the remark that in comparing detailed plans of rock fault areas with river causes they cannot be made to fit. Masses of rock undergoing distortion under earth pressure are subject to the harmonic folding which gives rise to the wave forms of anticlines and synclines. More rigid beds between others of less rigidity, when they fold, push the weaker rocks aside, and, as has already been shown, the troughs of the sandstone waves come down and touch the coal. Rock rolls are the waves, rock faults the breakers, and the plan of the only York- shire rock fault area which has yet been even moderately completely explored in mining (the workings of the Haigh Moor seam between Normanton and Kippax) recalls nothing so much as the irregular oval splashes of light thrown upon a ceiling by the reflection of a sun- beam from the surface of ripples on agitated water. The prevalence of slickensides at the under boundary, and the frequency with which glossy surfaces appear, both in the partings among the unmoved coal and between the lenticular units of the rock-fault filling, are not explained by the erosion hypothesis. By the advo- cates of that view slickensides are looked upon as adventitious, and as produced by earth movement at a period subsequent to the formation of the rock fault itself. The burnish or slickensides is due to surface powdering between masses which are shearing past each other under considerable stress, and the parallel grooved furrows and fine striae on the glossy surfaces give a trustworthy indication of the direction along which the shear took place. Slickensided surfaces on coal or bind decrepitate rapidly on exposure to the air, and when found preserved in abundance, as in rock fault material, it may be assumed with certainty that from the time of their formation until their present exposure the pressure which has held them tightly has never been completely released. The thickening of the coal [8], whether by bulk com- pression or by overthrusting, is the best evidence of a large scale shearing by lateral pressure that could have been preserved. The arrangement of the thrust planes is not dissimilar to the arrangement of the rock fault patches. The lines of the faults are generally parallel with the curving boundaries of the rock fault. Each overthrust bends round somewhat at each end as the throw of the fault dies away, and in bending round it often happens that two or more of them run together. In plan their relative arrangement may be likened to the arrangement of the wrinkles in crinkly paper, and, if the coal seam be regarded as having been crinkled by the overdrag of the roof, which had seized and, con- tinuing to move, was tearing away the coal below, the simile will bear a close analysis. Upholders of the stream erosion theory seem to have ignored the evidence of overthrust coal seams, and explain “ proud ” coal as due to a sort of sweeping out of the peaty material from the stream course and a piling up of the debris among the marsh growth on the banks. This process is not unknown near the mouths of sluggish rivers, like the Lower Mississippi, which by deposition of alluvium in times of flood has built up its banks some scores of feet above the level of the sides of its own valley. Such explanation, however, seems far-fetched, and becomes the more inadequate when the associated occurrence of “ foreign bodies ” [9] and the wedges of rock [10] which break into the proud (and the lean) coal both from above and from below, are taken into consideration. By those who accept the contemporaneous-erosion hypothesis the “ blocks of isolated sandstone ” and other foreign bodies are explained as “ doubtless being the result of cavities formed in the coal about the time of denudation and afterwards filled with sand, etc.” * On close examination, however, each foreign body proves ■to be a fragment or complex of fragments, bent, broken, rolled over, twisted, or sheared, but always preserving some traces of the bedding planes which were developed during the original deposition as part of a continuous sheet of sediment. Tongues of rock can also be seen following surfaces of overthrusting, and it is suggested that both they and the “ foreign bodies ” have really been dragged into their present position along displace- ments which are a minor manifestation of the same shearing as that which has produced the larger thrust planes and rock faults (fig. 3). Surpassing all other difficulties in the way of the acceptance of the origin of rock faults by erosion, is the character of the rock fault “filling.” Sand or gravel drifting into a submerged stream course must undergo a sorting of the grains by size, and in their deposition the fragments could not develop any arrange- ment less orderly than current bedding. Materials brought for deposition might come from anywhere within •the watershed of the stream which brought them, or, if a tidal drift were the carrier, might be derived from anywhere along the coast. The size of the fragment would, however, be a measure of the strength of the * Hendy, loc. cit., p. 435.