A METHOD FOR DECOMPOSITION OF HYDROCARBONS

Abstract: In a method for decomposition of hydrocarbons for the production of hydrogen and carbon black, the feed stock is passed through a plasma torch, which causes a pyrolytic decomposition of the feed stock. The feed stock is transported through the plasma torch (A) in a cooled lead-in tube (1) and undergoes a first heating in an area in the immediate vicinity of the plasma flame. In the area immediately below the plasma flame a mixing of the hydrocarbon material and the plasma gas occurs, the temperature being increased to decomposition temperature for the raw material. In this area free hydrogen and dehydrogenated carbon material are produced in the form of drops of liquid. The material thereby produced is passed on to one or more subsequent stages where the final and complete decomposition of the hydrocarbons to carbon black and hydrogen occurs. In this area further raw material may be added which causes quenching and reacts with the already produced carbon black. An increase is thereby caused in particle size, density and amount produced without further energy supply, whereafter the products produced are expelled and separated and hot gas may be transported in a return pipe to the torch, in order to further increase the energy yield.

Description: A method for decomposition of hydrocarbons The invention concerns a method for decomposition of hydrocarbons for the production of hydrogen and carbon black, the method employing a pyrolytic process with a torch in a reaction chamber. The traditional production methods for carbon black consist in a combustion of hydrocarbons by the supply of air. The quality achieved will be dependent on the supply of air or oxygen and the use of different amounts of oxygen in a surplus or a deficit. In the known methods substantial parts of the hydro¬ carbons are consumed in supplying sufficient energy for the decomposition, thus realizing a relatively low yield of carbon black. In addition to a low yield the combustion process will cause environmental pollution, since both carbon dioxides and nitrogen oxides will be produced. The waste gases from the processes will be able to be used only as fuel gas. For the decomposition of hydrocarbons other pyrolytic methods have also been used in which plasma torches have been utilized, but it has not been possible to use these methods for continuous production due to deposits on the electrodes, which have led to stoppages in the process and expensive cleaning procedures. Carbon which is formed by pyrolysis of hydrocarbons can be divided into two different qualities, viz. carbon black and coke (pyrolytic carbon) . Carbon black is light and soft with low density and is produced in the gas phase, while coke is harder, has high density and is produced on surfaces with rela tively low temperatures, normally lower than 1100°C. The object of the present invention is to provide an improved method for the decomposition of hydrocarbons by pyrolysis without the supply of extra energy and without the use of materials or gases which pollute the decomposition products. A further object of the invention is to provide a method which can be implemented continuously without stoppages for cleaning of the apparatus, while at the same time the raw materials should be able to be converted as completely as possible into the desired product. A further object of the invention is to provide a method wherein the quality of the products obtained should be able to be extensively controlled and checked. A final object of the invention is to provide a method by means of which the method can be implemented without pollution of the environment. The invention also comprises an apparatus which can be used for the implement-ation of such a method. The above-mentioned objects are achieved by a method and ah apparatus which are characterized by the features in the patent claims presented. The invention is primarily intended for the production of hydrogen and carbon black, in that the quality and degree of density of the carbon black component should be able to be controlled as required. In the invention the raw materials are supplied, viz. the hydrocarbons to a plasma torch, in whose active zone are created at least two reaction zones and where the process is divided into several stages. Thus the method according to the invention is a reaction process divided into stages in which the parameters for the individual zones wil be capable of determining the quality of the products. In the first reaction zone of the process, the pyrolytic decomposition will be performed and particles of carbon will be primarily produced, macromolecules in the gas phase condensing into drops which hydrogenate into solid carbon. Thus the first decomposition is obtained here in the two main feed stocks which are of interest, viz. hydrogen and carbon black. The number of primary particles of carbon and the size of these can be controlled by means of temperature and pressure in this reaction zone. This is done by controlling the amount of hydrocarbon fed in in relation to the energy supply emitted by the torch or by controlling the residence time of the particles in the first reaction zone. The quality of the carbon product as well as its properties will be determined by the further progress through the reactio zones. The finest quality is obtained when the products from the first reaction zone are exposed to quenching in the next reaction zone. The admixture of additional hydrocarbons in a secondary feed flow in the second reaction zone will lead to a growth in the particles which are created in zone 1. In this way a product is obtained with larger particles, higher densit and a smaller surface. The amount of admixture of hydrocarbons in any subsequent reaction zones will determine the size of th carbon particles. For the largest particles additional energy will be required which can be added by supplying C-H-0 compounds in their reaction zones. Alternatively, the additional energy can be supplied by means of plasma torches located in these zones. Such alternatives and the supply of extra energy provide a control of the product quality. It has been found that the method according to the invention provides a yield of carbon and hydrogen of almost 100% of the hydrocarbon and none of the products in the reaction process will be polluted. Furthermore, it has been possible to control the quality of the produced carbon black both with regard to the desired size, surface, density and acidity without affecting the purity of the decomposition products, while at the same time the method uses very little energy in relation t previously used production methods. This is due to the fact that it is possible to exploit exothermic decomposition energy, e.g. for the decomposition of extra raw material. Methane has been chosen as the feed stock in the method according to the invention, but it will undoubtedly also be possible to use other forms of hydrocarbons and natural gases or components, thus enabling the method according to the invention to be used substantially for hydrocarbons. It is assumed that the reaction path for the production of carbon black consists in the fact that those hydrocarbons produced by pyrolysis are first converted to acetylene (ethyne) and subsequent aromatic cores polymerise and form macro¬ molecules, i.e. large molecules with a high molecular weight. These macromolecules become supersaturated, thereby condensing into drops of liquid which further pyrolyze the solid carbon molecule. Once drops of liquid have been formed it will no longer be possible to achieve supersaturation. This is due to the fact that the macromolecules which are formed will be adsorbed on those drops or pellets which are already formed. This adsorption will occur more rapidly than the formation of the macromolecules. In consequence the number of elementary particles which are formed is given and is only dependent on pressure, temperature and reactant. This forms the basis for controlling the quality of the created product. If, e.g., hydrocarbons are introduced into the area where drops of liquid have been formed, no new particles will be formed but the existing ones will grow. Hydrocarbons which are added here will form macromolecules which attach themselves to the particles which have already been formed. The physical properties of the carbon produced will vary with the temperature. At higher temperatures the carbon black produced will be more airy. The pressure relations will also be significant in this connection. The quality is closely related to which molecules the macromolecules are composed of and how they are connected. The apparatus for use in the method according to the invention comprises in principle a main plasma torch whose active area is located in a reaction chamber which may be equipped with pressure and temperature control devices and possibly additional torches. The chamber is equipped with an outlet for gas and carbon from which outlet a branch pipe leads to a heat exchanger with a return pipe to the plasma torch for recirculatiion of heat energy. In the following section the method according to the invention will be illustrated in more detail by means of an embodiment and a drawing which illustrates purely schematically the principle for the construction of an apparatus according to th invention. In this connection it should be emphasized that the apparatus in the drawing is intended only as an illustration o the principle construction and is meant to elucidate the individual stages of the method according to the invention. Fo a person skilled in the art, this illustration will nevertheless also provide guidance in the construction of an apparatus according to the invention. In the illustrated embodiment the raw material selected for us is the hydrocarbon which at present appears to be the most suitable for the process, namely methane. The apparatus according to the invention therefore comprises i principle two main components, viz. a plasma torch which is indicated by A and the reaction chamber B. It should be obvious that this reaction chamber B can also be divided into several sections if this is considered expedient. Furthermore, at the end of the reaction chamber B which is remote from the plasma torch A there will be outlet means for the reaction products, which are indicated by the general reference designation C. A plasma torch as schematically illustrated by A is described in more detail in the applicant's simultaneous Norwegian patent application No. 91 4907 and its construction is therefore not described in more detail here. It will also be possible to use torches with a different construction. Methane is introduced into the reactor chamber B through a lead-in tube 1. The lead-in tube 1 is preferably liquid-cooled and coated with an outer heat-insulating layer and is located coaxially in the internal electrode 2 in the tubular plasma torch A. The lead-in tube 1 can be moved in the axial directio for positioning of the nozzle in relation to the plasma zone. It is vital that the methane which is introduced through the lead-in tube 1 has a low temperature when it leaves the nozzle If the temperature of the methane exceeds a value of approximately 650-700°C, the decomposition will start too early. This is undesirable because decomposition products can be formed inside the lead-in tube 1 before the methane reaches the plasma flame, thus causing precipitation of such products in the form of coke on the walls of the feed tube and on the plasma torch's electrodes. Thus it is essential for the produc fed into the lead-in tube to receive a proper cooling in order to avoid this type of fouling. The plasma torch A consists of tubular electrodes 2, 3, 4 wherein the innermost electrode 2 is supplied with electrical direct voltage with a polarity and wherein the two external electrodes are connected to opposite polarity. Each of the electrodes can be positioned independently of one another in the axial direction. All the electrodes are made of graphite and can be replaced during consumption so that the process remains continuous. It is an advantage for the electrodes to be made of graphite which is carbon. The electrodes will not pollute the process, but on the contrary will become an integral part of the process and the part which erodes will be converted in the process in the same way as the reactants. The electrodes can also be produced from carbon which is formed in the process and which is particularly free of polluting materials, thus making it self-supporting. In the lining of the reactor in the area where the arc from the plasma torch is burning, a magnetic coil 5 has been inserted connected to a separate power supply which makes it possible to adjust the magnetic field in the area where the arc is burning. In this way the arc's rotation rate can be controlled, while at the same time the arc can be extended in the longitudinal direction, i.e. from burning between the two innermost electrodes to burning between the innermost and the outermost electrodes. The plasma gas used is hydrogen, which can be produced in the process. The plasma torch A with the lead-in tube 1 for hydrocarbons, methane in the example illustrated, is located at the entrance to the reaction chamber B where the inner walls are composed o graphite. Since the plasma torch A and the lead-in tube 1 can be moved in the axial direction, the volume and thereby the residence time and temperature can be controlled. The active area for this process is indicated by zone 1. In this first reaction zone the number of drops of liquid is determined. The temperature can also be controlled by the ratio of power to th plasma torch and the amount of methane. In zone 1, i.e. the first reaction zone, three of the stages take place in the method according to the invention, divided into three differen areas. This can be described as follows: (the areas described below are indicated by Roman numerals in the figure) . Area I In this area unmixed methane is introduced at such a low temperature that in reality no reaction takes place here. The temperature is lower than 1000°C. At high feed rates some of the methane could pass without conversion to the next reaction zone, which is designated as zone 2 in the reactor chamber B. The methane begins to react at approximately 700°C, but at temperatures below 1000°C the reaction rate is so low that the bulk of the material in the area I will not react. In the border area between area I and Roman numeral II the temperature is between 1000 and 1200°C. Area II Around area I lies the area for burning off the plasma gas, a process which takes place at an extremely high temperature. There are no reactions in this area. Area III Outside this plasma gas area is an area where mixing of methan and plasma gas takes place. As already mentioned the temperature of the plasma gas is extremely high but the temperature in the mixture is kept down due to the strong endothermic production of acetylene (ethyne) . The temperature here will be between 1200 and 2000°C. The lowest temperatures will be found in the central area of the reactor furthest away from the torch. Between the reactor wall and the area III it will be possible for drops of liquid which are formed to be precipitated on the wall before they are completely dehydrogen ted. These drops can cause a hard coating to form on the reactor which is difficult to remove. The product stream or feed stream from zone 1, which covers the areas I-III, determines the number of carbon particles based on temperature and pressure in this section and the air stream of carbon particles is passed on directly into the next zone, zone 2 in the reactor housing where the further reaction takes place. In the drawing the reaction areas are indicated as area IV. Area IV In this area the last remains of acetylene (ethyne) react to form carbon black and hydrogen. The temperature here is between 1200 and 1600°C. In this area it is possible to add extra amounts of raw material, i.e. methane, in order to cool the product mixture by quenching with methane. This methane will cool down the product by itself reacting with carbon black and hydrogen. Based on the theory that the number of carbon black particles is given, the carbon material produced in this part of the reactor will be deposited on already existing particles. These will thus grow larger, resulting in a product which is more compact. By adding more energy to the product by means of an oxygen-containing medium or extra plasma torches in zone 2 , the process described for area IV can be repeated until the desired size and density of the product are achieved. This area can therefore be repeated with further subsequent areas, possibly in new sections of the reaction chamber B. The lead-in tube for additional amounts of methane and an oxygen-containing medium is indicated by 8 and is passed into zone 2. In addition the zone has the possibility for the connection of extra plasma torches (not illustrated in more detail) . That part of the reactor volume which lies outside these areas will normally be "dead volume". The "dead volume" will reduce the deposit of solid material on the reactor wall and is therefore desirable. Between areas III and IV there will be low axial velocity which can lead to a build-up of carbon material in this area. In this area a floor is almost formed in the reactor. The material will have a low mechanical strength and can easily be removed by mechanical means. High velocity through the reactor will also counteract such tendencies. A special design of the reactor helps to limit this type of fouling by causing liquid particles which are formed to be dehydrogenated before they hit the wall and form a hard coating. In order to prevent undesirable fouling from causing re-fouling and stoppage of the reactor, it is equipped with an internal mechanical scraping device which regularly scrapes down the walls of the reactor. The mechanical scraper can also be equipped with channels with internal washing down of the reactor walls with a suitable oxidation medium. In order to further increase the energy yield realized by the method, the methane can be heated by means of a heat exchange process obtaining heat from the product stream from the reactor chamber and thereby have a temperature of almost 700°C when the methane is fed into the lead-in tube 1 or into zone 2 through the lead- in tubes 8. In the above only one example of the method according to the invention and the principle sides of an apparatus according to the invention are described. As already mentioned there will be many possibilities for variations and for determination of quality and type of feed stock within the scope of the inven¬ tion. This will also be dependent on the feed stock which is fed in. This is generally described as hydrocarbon and the preferred hydrocarbon to-day is methane. Alternatives could also be, e.g., chip material or shavings from the woodworking and cellulose industry, other oil products and natural gas in general. In connection with the invention it is also important for the method to be implemented without being affec ed by factors such as fouling of apparatus, etc. In this connection it can be expedient to incorporate the method which is described in the applicant's Norwegian patent application no. 91 4908.

Claims: PATENT CLAIMS 1. A method for decomposition of hydrocarbons for the production of hydrogen and carbon black, wherein the feed stock is passed through a plasma torch, which causes a pyrolytic decomposition of the feed stock and wherein the reaction takes place in a reaction area, characterized in that the feed stock, preferably methane, is transported through the plasma torch in a temperature- controlled lead-in tube so that it has a temperature lower than 1000°C, preferably between 400°C and 600°C when it leaves the lead-in tube, that the feed stock undergoes a first approximately uniform heating in an area in the immediate vicinity of the plasma flame, the feed stock being fed in centrally in relation to the plasma torch's flame, that in an area immediately behind the plasma flame, there occurs a mixing of the hydrocarbon material and the plasma gas which is preferably hydrogen and which preferably is recycled, the temperature being increased to over 1600°C which is the decomposition temperature for the raw material, and that free hydrogen and dehydrogenated carbon material in the form of drops of liquid are formed in this area, that the material formed thereby is passed on to one or more subsequent stages where the temperature is kept between 1200°C and 1600°C and where the final and complete decomposition of the hydrocarbons to carbon black and hydrogen is performed, that further raw materials may be added in this area which cause quenching and react with the already produced carbon black, thereby causing an increase in the particle size, density and amount produced without further energy supply, whereafter the products created are discharged and separated and that hot gas may be trans¬ ported in a return pipe to the torch in order to further increase the energy yield, and that the temperatures in the reaction area are controlled by adjusting the feed rates for reactant and plasma gas and/or by regulating the energy supply to the plasma torch and/or by adjusting the pressure in the reaction area, thus enabling the quality of the carbon black created to be controlled to achieve the desired quality. 2. A method according to claim 1, characterized in that in the final stage of the method extra plasma torches are used in order to control the temperature. 3. An apparatus for use in the implementation of the method according to claim 1 for decomposition of hydrocarbons, comprising a plasma torch and a reaction chamber, characterized in that the plasma torch is equipped with a central, temperature-controlled lead-in tube for the feed stock, that it includes at least three electrodes and is located at the end of a reaction chamber, that the inside of the reaction chamber is lined with carbon, has lead-in openings in its side wall areas for additional feed stock, possibly for installing additional plasma torches, and that the end of the reaction chamber opposite the plasma torch is provided with an outlet for the end products and possibly also a recirculation pipe for produced gas, normally hydrogen, which leads to the plasma torch. 4. A method according to claim 1, characterized in that no other materials, particularly polluting materials, are included in the decomposition products than those which exist in the feed stocks.

Inventors: HAUGSTEN KJELL, HOX KETIL, HUGDAHL JAN, LYNUM STEINAR, MYKLEBUST NILS, HAUGSTEN, KJELL, HOX, KETIL, HUGDAHL, JAN, LYNUM, STEINAR, MYKLEBUST, NILS
Applicants: KVAERNER ENG, KVAERNER ENGINEERING A.S
Application year: 1992
Main classification: C01B3
IPC codes: C01B3, C01B31, C09C1