*170 THE COLLIERY GUARDIAN. October 9, 1914. ____________________________________________________________________________________ Honeycomb and Clinker Formation.* By 5. W. PARR.f As a general proposition the first step in any attempt to solve a difficulty should doubtless be taken along the line of a search for the underlying cause. If we approach the matter of honeycomb formation on flue sheets from this standpoint, we are confronted at once with the fact that the cause must of necessity be more or less obscure owing to the difficulty of obtaining experimental evidence in the vital or formative phase of the matter. We may be justified therefore in resorting to the process of theorising or setting up of a hypothetical explanation in the hope that by this means some suggestions may be developed which will remove or mitigate the evil. If this should be the result of our hypothetical speculation, I think you will agree that it does not make any differ- ence whether our hypothesis is right or wrong, so long as the desired end is attained. I may say, also, in passing, that perhaps this theoretical viewpoint of method in the present instance will be regarded as an apology why I attempt to discuss a subject concerning which I have so little experience. The first suggestion which offers itself to the minds of everyone who approaches this topic is the question of the fusibility of the ash. A great deal of activity is just now being carried on in connection with the study of ash ■ fusibilities, and it is entirely possible that the clinkering which occurs in ordinary steam heating appliances, in which the fusibility of the ash doubtless plays a large part, may have some relation to the clinkering on flue sheets, but I am disposed to think otherwise. For instance, in a recent number of the Journal of the Society of Chemical Industry! results are given on an elaborate series of ash determinations, in which both the fusibility of the various ashes and the component parts of the ash are set forth, with the con- clusion that the constituents as determined by chemical analysis seem to offer no explanation for clinkering on the grates. The statement is further emphasised that high sulphur and high iron seem to be wfliolly inadequate as offering an explanation. I certainly agree that we get little light in studying either the chemical compo- sition of the final ash product as it ordinarily comes from the grates or the composition of the final clinkering product which runs on the grate bars or fastens itself to the flue sheets. Take this illustration. I have from Mr. J. G. Crawford, fuel engineer for the Chicago, Burlington and Quincy Railroad, under date of December 12^ 1911, the following results of analyses covering a sample of honeycomb and the ash of the coal used at the time. Analysis of honeycomb and coal ash from engine 2133, Chicago, Burlington and Quincy Railway, November 1911 :— Honey- Ash in comb. coal. Per cent. Per cent. Volatile on ignition .......... 0*65 ... 0*00 Silica (SiO2).................. 51*82 ... 50*78 Iron oxide (Fe2O3) ............ 12*19 ... 9*53 Aluminium oxide (ALO3) .... 21*34 ... 28*20 Calcium oxide (CaO).......... 8*97 ... 7’84 Magnesium oxide (MgO) ...... 1*72 ... 2*78 Sulphuric anhydride (SO3) .... 0*44 ... 0*26 Alkali oxides (K2O and Na20) by difference ...................__ 2*87 ... 0*61 Total............... 10000 ... 100*00 Numerous analyses of honeycomb from other sources show a substantial agreement with the analyses of the ash of the coals, which were being used on the engines. Now, as a rule, these ashes of themselves, or as analysed, are not of a type to clinker easily. Notwithstanding that fact, the honeycomb prevails. Some coaling stations, it is true, will furnish a coat with more fusible ash than others, but it does not appear from any data which we have been able to secure that these were the coals which were giving the trouble. In studying the conditions of fusibility of the mineral constituents of coal, the composition of the ultimate ash product will throw but little light on the subject, if, indeed, it may not be actually misleading. We must keep in mind the fact that there are two stages in the various transformations that are going on. Each stage has its own fusion temperature, and the components must be separated; and any study of the final stage will have value only as it may furnish information as to the possible conditions existing in the intermediate stage of the combustion process. I refer here in the main to the iron pyrites in the coal. The average of this constituent for most of the coals of the Mississippi valley will be in excess of 3 per cent, of sulphur, which means substanti- ally that 6 per cent, of the weight of the coal is in the form of pyritic iron; and it is not unusual for this con- tent to reach 10 and even 12 per cent, of the gross weight of the coal. If this material is allowed to burn at a leisurely rate until all of this sulphur has burned out, the resulting product is ferric oxide, Fe2O3, and a study of the ash residue in which the iron has reached its final state will not disclose any increased tendency on the part of the ash to clinker. So far as this sort of investigation would be concerned, therefore, we would say that this high content of sulphur and iron in the coal does not produce a final ash which is any more fusible than a coal where this constituent is low. Studying the iron pyrites in the intermediate stage, we find that it very readily parts with one-half of its sulphur content, and drops down from an indicated com- position of FeS2 to the composition of FeS. This action does not require any oxygen to remove the one atom of * A paper read before the International Railway Fuel Association, Chicago, Illinois. t Professor of Applied Chemistry, University of Illinois. I Vol. 33, p. 1144. sulphur, which is purely the result of heat, and takes place at a temperature between 750 and 900 degs. Fahr., 400 and 500 degs. Cent. Now the further removal of the final atom of sulphur does not take place at any ordinary temperature, and, indeed, requires about 1650 degs. Fahr., 900 degs. Cent., for its rapid elimi- nation; or, provided air in sufficient quality is avail- able, it will burn out to a resulting product of oxide of iron, Fe2O3, which is not only highly infusible, but does not add anything to the fusibility of its associated mineral matter in the coal. So I repeat again, a final ash, with all of the iron burnt to the Fe2O3 stage, may be a very infusible mixture, and the more ferric oxide present the more fusible it may be; but in this stage its fusibility not only bears no relation to the inter- mediate stage, but it may, and usually does, have a directly opposite tendency. It is this intermediate stage in the transformation, therefore, namely, the iron sulphide in the FeS form, which, it seems to me, is of vital concern in studying this problem, because it is an easily fusible constituent, and, being present in an amount so large, as we have already indicated, it fur- nishes, when in this stage, magma sufficient in amount to dominate the mass and give it a pasty character. Now it must be evident that if conditions are favourable for the formation of this intermediate product, and these conditions are maintained for any considerable length of time, at the high temperatures of the fire box, this material will run into clinker. We do not need to go far for evidence that these clinkers are some sort of a compound of sulphur, for doubtless everyone is familiar with the pronounced sulphur smell that arises from these live clinkers when pulled out of the fire. They still retain the power of combustion for the reason that all the sulphur retained in this sulphide of iron form burns readily and continues to burn for some time after being exposed to the air. The tendency to form clinker, or, to put it on the basis fusibility, the fusibility of the ash at this stage, bears little relation to the ultimate product that comes in the form of loose ash. We should rather consider the fusibility of the mass in which this iron sulphide has reached the half-way stage. Here is a condition of fusibility which not only bears no relation whatever to the final product, but it is also a condition in which it is exceedingly difficult to catch the material in place, or in a condition to measure its degree of fusibility. Hence the futility of the average ash analysis as show- ing anything like the fusion temperature that really exists in the process of combustion. It will be seen from the above that we have been discussing the tendency towards the formation of clinker on the grate bars. What explanation may that afford for the formation of clinker on the flue sheets? To this we would reply that two conditions must exist in order to furnish any explanation along the lines sug- gested. First, a chemical condition in which the pyritic iron is'transformed only to the ferrous sulphide, or FeS stage. We have already said that this transformation may be brought about by heat alone; but it is also true chat to remain in the ferrous sulphide stage it must have an insufficient supply of air, otherwise it would continue the process of decomposition until it reached the oxidised form. Chemically speaking, therefore, we need only a moderately high heat and either a shortage in the oxygen supply or such a limitation in the time element that the oxygen action is incomplete. We should follow the possibilities a step further at this point. If the ash in this half-way condition should be in contact with the higher temperatures of the fire box, or be moved into such a zone by stirring or by die movement of the grate, it is entirely possible that large masses thus exclude the further action of oxygen. We will by this means prevent the passage of the material from the easily fusible ferrous iron stage. It will be trapped, so to speak, in this form. Second, there are physical conditions which provide an explanation for the solid material transferring itself from the fuel bed to the flue sheets. I cannot conceive it possible that the burning mass on the grate bars can possibly arrive at a condition of fusion in such a liquid state that the air draught could lift the molten material into the combustion current, and thus throw it against the flue sheets. On the other hand, it is entirely reasonable to suppose that a condition of this sort in the burning mass on the grates will cut down the oxygen supply to such an extent that the combustion chamber itself is somewhat deficient in oxygen. We are driven, therefore, to the hypothesis that the coal itself, as it is thrown into the fire box, has those physical conditions present which are conducive to the furnishing of particles which are fine enough to be drawn up into the draught currents. Such finely divided material is especially pronounced in the run-of-mine which so largely predominates in the fuel supply for railroads, especially of those States where the custom prevails of putting out coal on the run-of-mine basis. Suppose, for example, that the coal, as fired, has an undue amount of fines. This in itself not only has a tendency to cut down the amount of air which may pass through the grate bars, but it also makes it possible for a large amount of fine material to be drawn up by the draught and into a combustion zone deficient in oxygen and of sufficiently high temperature to change the pyritic iron to the FeS stage. In this condition it is thrown against the front end of the fire box, and will lodge there, especi- ally if there is a slight leak about the flue opening. Now, if we examine these incrustations, our first conclusion would be that on this hypothesis our mass of clinker would be largely impregnated with the sulphide of iron, FeS, but a test for such sulphur in these clinker forma- tions does not reveal any appreciable amount of that constituent. Our hypothesis is not endangered thereby, for the reason that, as already mentioned, with a heat sufficiently high, say about 1600 degs., the sulphur is dissociated and driven off. This liberation of the sulphur causes small gas pockets or bubbles throughout the mass, and this is very characteristic of these clinker formations. Precisely the same thing is met with in the burning of shales for brick manufacture, which are highly impregnated with iron pyrites. At one stage in the burning, where the ferrous sulphide condition is reached and one-half of the sulphur has been driven out, that stage which we have been describing is reached. If now the heat is raised to the point where the sulphur dissociates the bricks puff up into a spongy mass and are worthless. If, on the other hand, a slow heat is con- tinued over a longer time while the bricks are still in the porous stage, the oxygen will perform its functions by having access to the sulphur and burn it all out, thus yielding dense masses even from shale of this description. Exactly the same conditions prevail in the fire box of a locomotive, excepting that usually no slow moving processes are in evidence. The term “ honeycombing ” itself is somewhat of an explanation of the chemical processes which are going on. Particles of coal which are fine enough to be caught up by the draught have, in the short distance they may travel, about the right conditions as to temperature, oxygen supply, and the time element to bring them to this inter- mediate or easily fusible stage. They are thrown, there- fore, against the flue sheet in a semi-pasty condition. The outer surface glazes over, and no more oxygen may reach the interior. They are, however, subjected to the most extreme heat of the fire box, sufficient to dissociate the remaining sulphur, which thus passes off as a gas, producing the spongy or honeycomb effect. The iron remains behind, it is true, but as ferrous iron, and in this form it readily unites with the silica present to form an easily fusible slag. The same ratio of iron to silica, if it were burned to the ferric stage, would represent a combination with altogether different characteristics, and a very much higher fusion point. Some confirmation of this rather hypothetical line of reasoning is furnished by the study of the ordinary flue incrustations, and by an examination of the constituents of the clinker with reference to the form in which the iron occurs, ferrous iron being prominently in evidence. A brief discussion of mining methods and mine output will be suggestive at this point. In the first place the fine material produced in the ordinary process of mining is much higher in ash than the lump coal. The amount of pyritic iron is in a higher ratio also. In a series of analyses conducted on coals from 75 mines of the State, each mine being represented by a sample of screened lump and one of screenings, the results show an almost uniform ash percentage in the screenings, which is at least double that of the ash in the lump. Now, in run-of-mine coal the product is somewhat deceiving, for the reason* that it has the appearance in the mass of being very largely lump material. Indeed, it is for occasional car lots of run-of-mine to be fully equal to the best screened lump from that mine, but there is a very considerable amount of fine material which must come along somewhere in the output. It should be recalled that after the blast and the breaking down of the coal at the working face the miners enter and clean up the rooms by sending out first the coarse or lump material. At the clean-up w’hich is made before new drill holes are started that part of the underlying floor which has been more or less pulverised and loosened in the various processes which have been going on is shovelled up and sent out along with the coal. In this way it is easily seen that the fine material is much higher in ash, and is. composed of mineral constituents which are usually in themselves higher in sulphur. We have, therefore, in the run-of-mine material exactly those physical conditions of fineness of division and high content of iron pyrites which, in the processes already described, are conducive to the furnishing of pasty particles which can be made to grow by small accretions, forming, as we have seen, the honeycomb structure on the flue sheets. From an examination of numerous specimens in which a chemical test for iron in the ferrous form has been made, there is indicated the presence of this material, and to that extent affording a confirmation of our hypo- thetical line of reasoning. It will be seen also that the various physical conditions described are in evidence. One other phase of ash fusibility ought to be men- tioned in this connection. With the work of the Illinois Geological Survey the fact has been developed that there is rather an unusually large distribution of coals having a high percentage of calcium carbonate pre- sent. This material, when it reaches a certain amount, forms a fluxing agent with the silica present; but these cases are hardly common enough to explain the every- day occurrences of honeycomb. However, it is given here as undoubted evidence, where such quantities of this material are met with, of a reason for the easy clinkering property of the ash. Four coals were taken in which the silica of the ash was approximately the same in amount. In this series the calcium oxide show’ed a marked effect on the fusibility of the ash, while the iron oxide was substantially without influence. The table below shows four such coals arranged in the order of fusibility, No. 1 being easily fusible and No. 4 being the least fusible :— 1. Carterville, Ill., Madison No. 8, No. 2255........ 2. Cambria, Ill., C. M. B. C. Co., No. 2254.......... 3. Cambria, Ill., M. C. Co., No. 2256............... 4. Herrin, Ill., C. H. C. Co., No. 2257............... SiO.. JfQ3' CaO. MgO. Perc. Perc. Perc. Perc. 48*1 ... 27’2 ... 23*8 ... 0*8 47’5 ... 46*7 ... 5*0 ... 0*8 56*5 ... 37’6 ... 5*0 ... 0*9 53*3 ... 41*0 ... 4*9 ... 0*8