Title of Invention	"METHOD FOR MONITORING A THERMODYNAMIC PROCESS"
Abstract	A method for monitoring a thermodynamic process in a system, according to which image material (5) is generated of the process and said image material (5) is evaluated, an eigenvalue problem approach being used at least in large part as a starting point for the automatic image evaluation.

Full Text

The invention relates to a method for monitoring a thermodynamic process in an installation. In a known method of this type, first specific features for image evaluation are defined which appear to be promising to the operator of the installation for modeling the process. For example, one defines specific moments and then reproduces the image material on this - necessarily reduced - functions system. The selected features - and only these - are then examined and used for creating a process model. Optionally, only parts of the information contained in the image material are extracted and used. The present invention is based on the object of improving a method of the type mentioned above. Since the image evaluation is based on an eigen value problem for an approach, at least for the largest part of the high-dimensional image space, the information contained in the images can be transformed into a lower- dimensional space for evaluation, without any significant loss of information. The images are then represented by means of characteristic image features (,,eigen flames") resulting from the eigen value problem. Image evaluation is done automatically, the evaluation approach being intrinsic to the system and not depending on features selected by the operator of the installation. Preferably, singular events which may significantly impair the process, are taken into account for solving the eigen value problem, so that they can be identified more quickly in subsequent image evaluations. A typical thermodynamic process serves to transform material, the necessary temperature being generated and maintained by a combustion process having at least one flame. Simultaneous capture of the flame and the material in the image material, i.e. of the radiation emitted by the flame and the material, has the advantage of providing information on the interaction between the flame and the material in a unique manner. It is then possible to subject the description of one entire scene to image evaluation. The environment of the flame is preferably complemented by also capturing the walls of the combustion chamber, i.e. their emissions. The invention is explained in greater detail below by means of three exemplary embodiments illustrated in the drawing, in which: Fig. 1 is a basic draft, partially in sectional view, of an installation for producing cement according to a first exemplary embodiment, Fig. 2 is a simplified camera image of the installation in Fig. 1, Fig. 3 is a schematic representation of a garbage incinerator installation according to a second exemplary embodiment, Fig. 4 is a schematic representation of a power plant furnace installation according to a third exemplary embodiment as longitudinal section, Fig. 5 is a corresponding horizontal transverse section, and Fig. 6 is a schematic representation of the image material in the third exemplary embodiment. In all three exemplary embodiments, a thermodynamic process runs in an installation, in which, at least partially, combustible material G is subjected to oxidation by the adduction of air L, there being at least one flame F. The thermodynamic process is to be monitored and then regulated in such a way as to have, on the on the one hand, a certain stability and, on the other hand, a certain flexibility, i.e. adapting itself to different conditions, there being certain optimization goals. The condition in the installation is described by different process parameters, some of which are also control parameters. By actions, i.e. by changing control parameters, the condition of the installation is modified. For on-line monitoring and control as well as forecasts of future conditions of the installation, a neuronal network is implemented in a data processing unit 1. By means of at least one camera 3, images of the thermodynamic process are captured. The camera 3 is set in such a way that it captures both the flame F and the burning material G, preferably also the walls 7 of the combustion chamber including cakings B, if applicable, i.e. the emissions from the entire environment. The image material 5 produced by the camera 3 thus contains the description of one entire scene also including the interaction between the flame F and the material G. The image material 5 is fed into a data processing unit 1, whereby, on the one hand, a live video image is displayed and, on the other hand, some process parameters are computed from the information contained in the image material 5. In order to process the information in the image material 5 in an intelligent way without loss of information, i.e. due to its complexity in order to transform it first into a low-dimensional space, one selects, at least in large part, an eigen value problem for an approach, i.e. one attempts a kind of principal component analysis. Each image is then described by a (usually) small number of scalar eigen values (mostly fewer than 20, for example eight), i.e. of transformed coordinates in the new coordinate system, and of vectorial eigen images or eigen flames, i.e. by coordinate axes for the new coordinate system, the eigen flames with the highest values dominating according to the system. The term of eigen flames must be interpreted in a large sense, since the emissions are not only included from the flame F, but also from the material G. In a classical principal component analysis, the zero digits of the characteristic polynom of the co-variance matrix would have to be calculated. In order to maintain the system of orthonormal eigen flames, one can alternatively use a stochastic approximation method in a neuronal network, first randomly initializing the weightings of all neurons and then, using the image material, iteratively first adapting the weightings of the first neuron, the second neuron, etc. The eigen flames show up mostly as compact regions, since adjacent pixels also monitor adjacent vectors of the combustion chamber whose light emissions are strongly correlated. In addition to some average luminosity distributions, singular events are also selected from the captured images as an eigen flame approach for the eigen value problem, for example a sudden adduction of new material G. Using the process parameters to be computed by means of the - at least in large part solved - eigen value problem, a process model is created in the neuronal network, by means of which one can improve the precision of the forecasts. With this approach, any singular event can be quickly detected, so that different additional measurements can then be started in order to obtain more information on the present process status following the singular event. Since the image evaluation no longer depends on a pre-determined selection of parameters, but itself extracts suitable information from the image material 5, the image evaluation can be automatized. In addition, the risk of not factoring in relevant information contained in the image material 5 is clearly reduced. The simultaneous consideration of emissions from the material G in the image material 5 provides information which, in its interaction with the flame F, cannot be obtained in any other way. By means of the chosen approach using image material 5 captured at different intervals, the eigen value problem takes developments in time into account. The first exemplary embodiment relates to a rotary kiln 11 for the production of cement, being operated in a well-known manner. The camera 3 is focused on the inside of the rotary kiln 11, capturing the image of the flame F of a burner 13, of the material being transformed G as well as of the walls 7 including cakings B . The data processing unit 1 subjects the image material 5 from the camera 3 to the described eigen value approach. The neuronal network, in addition to the compressed data, also receives information on the mass flows of the air L adducted via different pathways, on the fuel and the material G. The optimization goal, on the one hand, is a high FCAO value of the produced clinker K, said FCAO value being determined not only from the condition inside the rotary kiln 11, but also from the conditions on the cooling path 15. On the other, the mixture of the fuel is to be set in such a way that a maximum of secondary fuel, i.e. waste, is used up. Finally, the cakings B on the walls 7 of the rotary kiln 11 are also to be kept at a minimum. The second exemplary embodiment concerns a garbage incinerator 21. Here as well, the camera 3, preferably several cameras, capture the image of the flame F and material G as one common frame. In a special embodiment for hazardous waste incineration, garbage containers 23 containing hazardous waste are dumped into the garbage incinerator 21 a certain intervals. The burst of such a waste container 23, due to the high temperature, is a singular event which is quickly detected by means of the eigen value approach according to the invention. Several additional measurements can then be initiated, such as taking a sample, in order to obtain more information on the present process status following said singular event. Preferably, as soon as the door through which the garbage container 23 is dumped is opened, a high speed camera is started, providing additional image material 5 at shorter intervals, shortly before and after the singular event. The third exemplary embodiment concerns a power plant in which, in addition to the air L, fuel 33, for example ground coal, is fed into a furnace 31 via the corners of the furnace 31, indicated by double arrows. A huge, rotary flame F forms inside the furnace 31. Several cameras 3 are arranged, for example, at three different levels on each side of the furnace 31. Each camera 3 captures the flame F as well as the adduction area for the fuel 33 in one scene, particularly the entry of the fuel 33 into the flame F providing interesting information, since, as a rule, for the fuel 33 - as opposed to the air L - only the total mass flow from the coal grinder can be measured, but not the partial flows to the individual adduction areas. The image material 5 displays the two- dimensional x-y frames of the cameras 3 combined to one x'-y' instantaneous image at different times t, i.e. a three-dimensional field. The image material 5, which is thus (as in the other exemplary embodiments as well) quasi three- dimensional, is subjected to the described eigen value approach. WE CLAIM; 1. A method for monitoring a thermodynamic process in an installation, the method comprising: providing image material obtained from the process; and subjecting the image to an automatic image evaluation that is at least substantially based upon an eigen value problem approach, wherein providing of the image material includes simultaneously capturing in one common frame at least both (a) emissions from at least one flame of the thermodynamic process and (b) emissions from material to be transformed through the thermodynamic process, so that the image material includes the frame, the frame includes information about the emissions from the at least one flame, the frame further includes information about the emissions from the material to be transformed though the thermodynamic process, and the frame includes information about interaction between the at least one flame and the material to be transformed through the thermodynamic process, and wherein the subjecting of the image material of the image material to the automatic image evaluation includes subjecting the entire frame to the automatic image evaluation. 2. The method as claimed in claim 1, wherein the providing of the image material further includes capturing emissions from walls of a combustion chamber of the installation. 3. The method as claimed in claim 1, wherein the providing of the image material further includes: creating a combined image, with the creating of the combined image including instantaneously capturing emissions in a plurality of frames and arranging the plurality of frames into the combined image; creating a plurality of combined images, with the creating of the plurality of combined images including sequentially repeating the creating of the combined image at a plurality of different times so that the plurality of combined images respectively correspond to the plurality of different times, and creating a three-dimensional field, with the creating of the three- dimensional field including arranging the plurality of combined images in a time-dependent series. 4. The method as claimed in claim 1, wherein the image material is at least substantially represented by eigen flames and transformed coordinates. 5. The method as claimed in claim 4, further comprising selecting at least one singular event as an approach for eigen flames. 6. The method as claimed in claim 1, wherein the installation in which the thermodynamic process takes place is a rotary kiln of a cement plant, a garbage incinerator, or a furnace of a power plant. 7. The method as claimed in claim 1, wherein the installation in which the thermodynamic process takes place is a garbage incinerator, the method further comprises selecting at least one singular event as an approach for eigen flames, and the singular event comprises bursting of a garbage container in the garbage incinerator. 8. The method as claimed in claim 2, wherein the providing of the image material further includes: creating a combined image, with the creating of the combined image including instantaneously capturing emissions in a plurality of frames and arranging the plurality of frames into the combined image; creating a three-dimensional filed, with the creating of the three- dimensional filed including arranging the plurality of combined images in a time-dependent series. 9. The method as claimed in claim 2, wherein the image material is at least substantially represented by eigen flames and transformed coordinates. 10. The method as claimed in claim 3, wherein the image material at least substantially represented by eigen flamesand transformed coordinates. 11. The method as claimed in claim 10, further comprising selecting at least one singular event as an approach for eigen flames. 12. The method as claimed in claim 3, wherein the installation in which the thermodynamic process takes place is a rotary kiln of a cement plant, a garbage incinerator, or in a furnace of power plant. 13. The method as claimed in claim 3, wherein the subjecting of the image material to the automatic image evaluation, and method further comprises: comparing the process parameters to optimization targets, and carrying out actions for regulating the process in response to the comparing of the process parameters to the optimization targets. 14. An apparatus for carrying out a method as claimed in any of the preceding claims for monitoring a thermodynamic process in an installation, wherein the thermodynamic process includes at least one flame and is for transforming material, the apparatus comprising: at least one camera positioned for producing image material that includes one common frame in which a plurality of emissions have been simultaneously captured, with the plurality of emissions including at least both emissions from the at least one flame and emissions from the material to be transformed, and so that the frame includes information about the emissions from the at least one flame, the frame further includes information about the emissions from the material to be transformed through the thermodynamic process; and a data processing unit for subjecting the image material to an automatic image evaluation that is at least substantially based upon eigen value problem approach, with the data processing unit being operative so that the subjecting of the image material to the automatic image evaluation includes subjection the entire frame to the automatic image evaluation. 15. The apparatus as claimed in claim 14, wherein the data processing unit includes a neural network. 16. The apparatus as claimed in claim 14, wherein at least one camera is positioned so that the plurality of emissions further includes emissions from walls of a combustion chamber of the installation. 17. The apparatus as claimed in claim 14, wherein the image material includes a three-dimensional field, and wherein the camera is one of a plurality of cameras that are cooperative for: creating a combined image by instantaneously capturing emissions in a plurality of frames and arranging the plurality of frames into the combined image; creating a plurality of combined images, with the creating of the plurality of combined images including sequentially repeating the creating of the combined image at a plurality of different times so that the plurality of combined images respectively correspond to the plurality of different times, and creating the three-dimensional field, with the creating of the three- dimensional field including arranging the plurality of combined images in a time-dependent series. 18. The apparatus as claimed in claim 14, wherein the data processing init is operative so that the image material is at least substantially represented by eigen flames and transformed coordinates. 19. The apparatus as claimed in claim 14 in combination with the installation, wherein the installation is a rotary kiln of a cement plant, a garbage incinerator, or a furnace of a power plant. 20. The apparatus as claimed in claim 19, wherein the image material includes a three-dimensional field, and wherein the camera is one of a plurality of cameras that are cooperative for: creating a combined image by instantaneously capturing emissions in a plurality of frames and arranging the plurality of frames into the combined image; creating a plurality of combined images, with the creating of the plurality of combined images including sequentially repeating the creating of the combined image at a plurality of different times so that the plurality of combined images respectively correspond to the plurality of different times, and creating the three-dimensional field, with the creating of the three- dimensional field including arranging the plurality of combined images in a time-dependent series. 21. A method as claimed in claim 1 for monitoring a thermodynamic process in an installation, the method comprising: providing image material obtained from the process; and subjecting the image material to an automatic image evaluation that is at least substantially based upon an eigen value problem approach, wherein the providing of the image material includes simultaneously capturing in one common frame at least both (a) emissions from at least one flame of the thermodynamic process and (b) emissions from material to be transformed through the thermodynamic process, whereby the image material includes the frame, wherein the subjecting of the image material to the automatic image evaluation, and wherein the installation in which the thermodynamic process takes place is a garbage incinerator, the method further comprises selecting at least one singular event as an approach for eigen flames, and the singular event comprises bursting of a garbage container in the garbage incinerator. 22. The method as claimed in claim 1, wherein: the subjecting of the image material to the automatic image evaluation comprises representing the image material by eigen flames and transformed coordinates; the subjecting of the entire frame to the automatic image evaluation comprises calculating the eigen flames; and both the information about the emissions from the at least one flame and the information about the emissions from the material to be transformed through the thermodynamic process are included in the calculating of the eigen flames. 23. The method as claimed in claim 1, wherein: the capturing of the emissions from the at least one flame comprises capturing an image of the at least one flame, so that the frame includes the image of the at least one flame, and the capturing of the emissions from the material to be transformed through the thermodynamic process comprises capturing an image of the material to be transformed through the thermodynamic process, so that the frame includes the image of the material to be transformed through the thermodynamic process. 24. The method as claimed in claim 23, wherein the capturing further comprises capturing an image of a wall of a combustion chamber of the installation, so that the frame includes the image of the wall of the combustion chamber. 25. The method as claimed in claim 1, wherein the material, which is to be transformed through the thermodynamic process, comprises a solid material, so that: the capturing of the emissions from the material to be transformed through the thermodynamic process comprises capturing emissions from the solid material to be transformed through the thermodynamic process; the frame includes information about the emissions from the solid material to be transformed through the thermodynamic process; the frame includes information about interaction between the at least one flame and the solid material to be transformed through the thermodynamic process. 26. The method as claimed in claim 25, wherein: the capturing of the emissions from the at least one flame comprises capturing an image of the at least one flame, so that the frame includes the image of the at least one flame, and the capturing of the emissions from the solid material to be transformed through the thermodynamic process, so that the frame includes the image of the solid material to be transformed through the thermodynamic process. 27. The method as claimed in claim 25, wherein solid material comprises coal. 28. The method as claimed m claim 25, wherein solid material comprises garbage. 29. The method as claimed in claim 3, wherein the instantaneously capturing of the emissions in the plurality of frames comprises: using a plurality of cameras, which are spaced apart from one another, to respectively capture the emissions in the plurality of frames. 30. The method as claimed in claim 8, wherein the subjecting of the image material to the automatic image evaluation comprises: subjecting the three-dimensional field to the automatic image evaluation. 31. The method as claimed in claim 8, wherein the subjecting of the three-dimensional field to the automatic image evaluation comprises: representing the three-dimensional field by eigen flames and transformed corordinates. Dated this 17th day of December 2004 A method for monitoring a thermodynamic process in a system, according to which image material (5) is generated of the process and said image material (5) is evaluated, an eigenvalue problem approach being used at least in large part as a starting point for the automatic image evaluation.

Documents:

1948-KOLNP-2004-FORM-27.pdf

1948-kolnp-2004-granted-abstract.pdf

1948-kolnp-2004-granted-claims.pdf

1948-kolnp-2004-granted-correspondence.pdf

1948-kolnp-2004-granted-description (complete).pdf

1948-kolnp-2004-granted-drawings.pdf

1948-kolnp-2004-granted-examination report.pdf

1948-kolnp-2004-granted-form 1.pdf

1948-kolnp-2004-granted-form 18.pdf

1948-kolnp-2004-granted-form 2.pdf

1948-kolnp-2004-granted-form 26.pdf

1948-kolnp-2004-granted-form 3.pdf

1948-kolnp-2004-granted-form 5.pdf

1948-kolnp-2004-granted-reply to examination report.pdf

1948-kolnp-2004-granted-specification.pdf

1948-KOLNP-2004-OTHERS PATENT DOCUMENTS.pdf