JP2010064251A - Laser machining method for high temperature firebrick - Google Patents

Abstract

<P>PROBLEM TO BE SOLVED: To provide a laser machining method enhancing accuracy and quality in machining the vicinity of a boundary line between a machined region and an unmachined region, in laser machining of a high temperature firebrick. <P>SOLUTION: The laser machining method for irradiating the firebrick of 500°C or higher with laser beams to cut the firebrick includes; temporally modulating power density at irradiation points of laser beams between power density of fusing the firebrick and power density of not fusing the firebrick and scanning the irradiation points of the laser beams to form a plurality of through holes or non-penetrating holes; and superimposing the plurality of through holes or non-penetrating holes to provide groove-shaped or penetrating cutting. <P>COPYRIGHT: (C)2010,JPO&INPIT

Description

The present invention relates to a laser processing method for high-temperature refractory bricks, and more particularly to a technique for repairing a structure made of refractory bricks in a high-temperature environment.

Although refractory bricks are used in various structures such as furnaces, there are cases where refractory bricks are required to be processed in a high temperature environment as the refractory bricks deteriorate. As an example, there is a process for hot repairing a wall surface of a coke oven for carbonizing coal.

The coke oven is divided into a combustion chamber for heating the furnace and a carbonization chamber for generating coke, and refractory bricks are used for the wall surface. Over many years of use of the furnace, refractory bricks have surface damage and cracks, and finally punctures that penetrate from the carbonization chamber to the combustion chamber. In particular, when a puncture occurs, the inserted coal spills into the combustion chamber and closes the combustion gas supply port, or coke gas flows from the carbonization chamber into the combustion chamber, causing incomplete combustion and generating black smoke It becomes.

Since the coefficient of thermal expansion of the refractory brick on the furnace wall changes abruptly at around 600 ° C, there is a risk of damage to the entire furnace wall due to thermal shock if the furnace is cooled below this temperature. For this reason, it is desirable to repair the furnace wall in a high temperature environment from 700 ° C. to 1000 ° C. which is the operation temperature.

As a method of processing bricks at a high temperature, a laser method is attracting attention. Laser machining has the advantage that it does not cause mechanical stress compared to mechanical machining such as cutting, and does not affect the strength of the normal furnace wall around the broken hole and can be safely shaped. In Patent Document 1, a furnace wall brick is crushed or melt-cut by laser irradiation from the carbonization chamber side, and the broken hole cross-sectional shape is shaped into a stepped shape or a tapered shape that narrows from the carbonization chamber toward the combustion chamber. Next, shape the brick material so that a groove portion is formed at the boundary between the refractory brick material to be inserted and the pierced hole portion in accordance with the sectional shape of the pierced hole of the shaping portion, and insert into the broken hole portion. Next, a method of spraying an irregular refractory material on the groove and fixing the inserted refractory brick to the broken hole portion is disclosed.
JP 2008-143966 A

However, little knowledge is accumulated about laser processing of high-temperature refractory bricks. For this reason, it cannot be said that the laser conditions suitable for processing a high temperature material are sufficiently understood. The following two laser irradiation methods disclosed in Patent Document 1 have room for further improvement in terms of processing accuracy as described below. The first method is a method in which a brick having a relatively low power density is scanned to break up bricks by thermal expansion due to rapid heating of the laser irradiation unit and remove them almost without melting. This method is based on local crushing due to thermal shock, but it may crush including the periphery of the laser irradiation part, so it is difficult to machine the boundary between the machining area and the unmachined area with an accuracy of less than 1 mm. There was a possibility of becoming. The second method is a method in which a beam is scanned while maintaining a relatively high power density, and melt cutting is performed while blowing oxygen gas. In this method, the melt may swell on the side of the unprocessed area near the boundary between the processed area and the unprocessed area, so that it may be difficult to obtain sufficient processing accuracy. It was.

An object of the present invention is to solve the above-mentioned problems and to provide a laser processing method with improved processing accuracy and quality in the vicinity of a boundary line between a processed region and an unprocessed region in laser processing of a high-temperature refractory brick.

The present inventors investigated in detail the melt cutting process phenomenon of a high-temperature refractory brick by a laser. As a result, it was found that the cause of deterioration in processing accuracy and quality was that the temperature of the refractory bricks was as high as 500 ° C. or more, so that heat was accumulated and excessive melting was likely to occur. And, as a result of examining the countermeasures, the present invention in which the laser beam irradiation is discontinuously performed temporally and the spatial processing order is devised, thereby avoiding melting due to excessive heat storage and improving the processing quality. It came. That is, the present invention is as follows.

The laser processing method for a refractory brick according to the present invention is a laser processing method for irradiating a refractory brick having a temperature of 500 ° C. or higher with a laser beam and cutting the refractory brick, wherein the laser at the laser beam irradiation point on the surface of the refractory brick The power density of the beam is temporally modulated between the power density that melts the refractory brick and the power density that does not melt the refractory brick, and the irradiation point of the laser beam is scanned on the refractory brick, A plurality of through holes are formed so that the positions of the through holes are continuously arranged, and the fire brick is cut by overlapping at least adjacent through holes among the plurality of through holes. .

Moreover, the laser processing method of the refractory brick according to the present invention is characterized in that in the formation of the plurality of through holes, the order in which the plurality of through holes are formed is discontinuous.

Furthermore, the laser processing method of the refractory brick according to the present invention is a laser processing method for processing the refractory brick by irradiating the refractory brick having a temperature of 500 ° C. or higher with a laser beam at a laser beam irradiation point on the surface of the refractory brick. The power density of the laser beam is temporally modulated between a power density that melts the refractory brick and a power density that does not melt the refractory brick, and the irradiation point of the laser beam is scanned on the refractory brick. A plurality of non-through holes are formed so that the positions of the non-through holes are continuously arranged, and a groove is formed in the refractory brick by overlapping at least adjacent non-through holes among the plurality of non-through holes. It is characterized by forming.

Moreover, the laser processing method of the firebrick according to claim 3 of the present invention is characterized in that in the formation of the plurality of non-through holes, the order in which the plurality of non-through holes are formed is discontinuous. .

Furthermore, the laser processing method of the refractory brick according to the present invention is characterized in that the groove depth is increased by repeating the formation of the groove a plurality of times.

Moreover, the laser processing method of the firebrick according to the present invention is characterized in that the firebrick is cut by repeating the formation of the groove a plurality of times.

Furthermore, in the laser processing method of the firebrick according to the present invention, the plurality of the through holes are formed so that the positions of the through holes are continuously arranged, or the positions of the non-through holes are continuous. In the process of forming a plurality of such through holes, the intensity of electromagnetic waves radiated from the periphery of the through holes or non-through holes is measured, and the remaining through holes or non-through holes are formed based on the intensity of the electromagnetic waves. It is characterized by determining the order to perform.

Furthermore, the laser processing method of a refractory brick according to the present invention is characterized in that the refractory brick is a refractory brick used for a furnace wall separating a carbonization chamber and a combustion chamber of a coke oven.

By the method of the present invention, laser processing with improved processing accuracy and quality is realized in laser processing of high-temperature refractory bricks. In the repair of the coke oven hole, which is an example of application, the gap between the inserted refractory brick material to be inserted and the shaping part can be made constant by increasing the processing accuracy and quality of shaping by laser. Contributes to stable spraying. Furthermore, since heat input to the unprocessed region can be suppressed during laser processing, an improvement in the breakdown pressure strength of the furnace wall is expected.

Hereinafter, the present invention will be described in detail with reference to the drawings. First, a processing head optical system used for laser irradiation will be described with reference to FIG. Although FIG. 1 describes the case where the non-through hole 1 is formed, the same apparatus is used when the through hole 3 is formed. The laser beam is output from a laser device (not shown). The type of laser to be used is not particularly limited, but when transmission through an optical fiber is necessary, a YAG laser having a wavelength of 1.1 μm or a fiber laser is suitable. Further, since transmission by mirror reflection is possible, a CO ₂ laser can also be used. Here, the former will be described as an example. The laser beam is transmitted through the optical fiber 15 and output from the collimator head 8. The collimator head 8 converts the output beam from the optical fiber 15 into a parallel beam 14. The laser beam is reflected by the reflecting mirror 6, condensed by the condenser lens 4, passes through the laser transmitting pinhole 13, and is irradiated onto the high-temperature refractory brick 2.

The laser displacement meter 7 and the CCD camera 10 function as a processing unit observation unit. The refractory bricks are at a high temperature, and in order to reduce the influence of thermal radiation, the laser processing head unit 5 and the processing unit observation unit 9 are preferably housed in an adiabatic cooling box 11 having a water cooling mechanism. The adiabatic cooling box 11 is preferably filled with the purge gas 12.

The irradiation position of the laser beam can be changed by the following two methods. First, as a large movement, the entire adiabatic cooling box 11 can be moved up and down and left and right by a manipulator. Further, a small movement on the order of mm is realized by adjusting the tilt angle of the reflecting mirror 6. The reflection mirror 6 is a galvano-type mirror, and a laser beam irradiation point can scan a certain area on the surface of the refractory brick. The present invention is a processing method in which the refractory brick 2 is melted and removed, and the power density of the laser beam is preferably 1000 W / mm ² or more in order to efficiently melt.

The gist of the present invention is that the laser beam irradiation is performed discontinuously in time to modulate the power density, and the order in which the plurality of through holes 3 or non-through holes 1 are formed is discontinuous, and the spatial processing order is changed. By devising, it is to avoid melting due to excessive heat storage and to improve processing quality. The specific method will be described below.

A first embodiment of the present invention will be described with reference to FIGS. In the present embodiment, at a certain irradiation position, the power density at the irradiation point of the laser beam is repeatedly modulated temporally between the power density that melts the refractory brick 2 and the power density that does not melt the refractory brick 2. The state where the through hole 3 is formed and the state where the through hole 3 is not formed are repeated alternately. And cutting | disconnection is obtained by performing through-hole 3 formation in multiple times, shifting an irradiation position. The cross-sectional shape of the processed hole obtained by one-time modulation is a non-through hole 1 as shown in FIG. 2 or a through hole 3 as shown in FIG. In the case of the non-through hole 1 in FIG. 2, this is repeated a plurality of times for the same irradiation position to form the through hole 3 as shown in FIG. In the present embodiment, cutting is obtained by repeating the formation of the through hole 3 while shifting the irradiation position to the side. As shown in FIG. 4, the through holes 3 are formed while overlapping adjacent holes. Numbers a1 to a8 in FIG. 4 represent the order in which the through holes 3 are formed. In this way, the formed through-holes 3 move to the adjacent positions one after another, and the order in which the through-holes 3 are formed is continuous. The time for increasing the power density by one modulation is set in a range where excessive melting does not occur outside the beam diameter. This time is determined according to the wavelength, power density, and beam diameter of the laser. The non-processing time for reducing the power density is set so that heat is diffused from the processing position so that excessive melting does not occur during subsequent processing.

The second embodiment of the present invention is a modification of the first embodiment, and the method of forming the through hole 3 as shown in FIG. 3 is the same as that of the first embodiment. The order of formation is different. That is, as shown in FIG. 5, after processing a certain through hole 3, the next through hole 3 is selected so as not to overlap therewith, and the order in which the through holes 3 are formed is discontinuous. To do. In addition, the numbers a1-a16 in FIG. 5 represent the order in which the through-hole 3 is formed like FIG. By increasing the distance from one processing position to the next processing position, the thermal effect is reduced, and the non-processing time for reducing the power density can be shortened. Therefore, as shown in FIG. 5, an order that allows a large distance between successive processing spots is effective.

In the third embodiment of the present invention, at a certain irradiation position, the power density at the irradiation point of the laser beam is temporally modulated between the power density at which the refractory brick 2 is melted and the power density at which the refractory brick 2 is not melted. The non-through hole 1 as shown in FIG. 2 is formed by repeating this process once or a plurality of times, and the groove shape is obtained by performing this non-through hole 1 a plurality of times while shifting the irradiation position. As shown in FIG. 6, the non-through hole 1 is formed while overlapping adjacent holes. The numbers a1 to a8 in FIG. 6 represent the order in which the non-through holes 1 are formed, as in FIG. The time for increasing the power density by one modulation is set in a range where excessive melting does not occur outside the beam diameter. This time is determined according to the wavelength, power density, and beam diameter of the laser. The non-processing time for reducing the power density is set so that heat is diffused from the processing position so that excessive melting does not occur during subsequent processing.

The fourth embodiment of the present invention is a modification of the third embodiment, and the method of forming the non-through hole 1 as shown in FIG. 2 is the same as that of the third embodiment. The order of forming a plurality is different. That is, as shown in FIG. 7, after processing a certain non-through hole 1, the next non-through hole 1 is selected so as not to overlap with this, and the formation of the non-through holes 1 overlapping each other is continuously performed in time. It is characterized by not performing. In addition, the numbers a1-a16 in FIG. 7 represent the order in which the non-through-hole 1 is formed like FIG. By increasing the distance from one processing position to the next processing position, the thermal effect is reduced, and the non-processing time for reducing the power density can be shortened. Therefore, as shown in FIG. 7, an order in which the distance between successive processing spots is large is effective.

The fifth embodiment of the present invention is a modification of the third or fourth embodiment. As shown in FIG. 8, the groove depth is increased by repeating the groove shape processing obtained in the third or fourth embodiment (hereinafter referred to as one-step processing) a plurality of steps, or A cutting line is obtained by making it penetrate. Compared with the first and second embodiments, which are also methods for obtaining a penetrating cutting line, this embodiment has a shallow depth of processing in one stage at a certain irradiation position, so that the thermal effect can be suppressed. Yes, it is an effective form for particularly thick refractory bricks 2. With the progress of groove processing over several stages, the distance between the condenser lens 4 and the processing surface changes. However, the entire adiabatic cooling box 11 in the apparatus diagram of FIG. By moving, it is possible to compensate for changes in power density on the machined surface.

A sixth embodiment of the present invention will be described. This embodiment measures the intensity of the electromagnetic wave radiated from the periphery of the through hole 3 or the non-through hole 1 in the formation of the machining spot of the plurality of through holes 3 or the non-through holes 1, and converts this to temperature information. Based on this information, the position or time for forming the next and subsequent machining spots is determined. That is, the order in which the plurality of non-through holes 1 are formed is determined. For the temperature measurement, for example, a radiation thermometer or the CCD camera 10 shown in FIG. 1 is used. If calibration is performed in advance using a black body furnace or the like, it is possible to measure the temperature distribution around the processing portion using the processing portion observation CCD camera 10 shown in FIG. At this time, in order to remove the stray light from the wavelength region where the CCD camera 10 element is not sensitive and improve the temperature measurement accuracy, a filter 16 for blocking radiation in the wavelength region of 1 μm or more is attached in front of the CCD camera 10. May be. FIG. 9 is a flowchart of the machining control method of the present embodiment. The temperature around the next planned processing portion is measured, and a certain threshold value is set there. If the measured value is higher than that temperature, do not perform the next processing and keep the laser power density in a low unprocessed state for a while, or move the laser beam to a place where the temperature has not risen, etc. Take control. Since the material of the refractory brick 2 has non-uniformity, excessive melting sometimes occurs. According to the present embodiment, the length of the non-processing time can be controlled in response to such variations. As a result, the processing efficiency and stability can be improved. In the above description, the example in which the intensity of electromagnetic waves is converted into temperature information through calibration using a black body furnace or the like is described, but it is also possible to directly determine from the received light intensity of the CCD camera 10.

In any of the forms described above, the through hole 3 or the non-through hole 1 is continuously superimposed, but the method of the present invention includes two-dimensional superposition. This is a method of overlapping the through holes 3 or the non-through holes 1 along a plurality of straight lines that overlap each other as shown in FIG. The third or fourth embodiment described above is expanded to such a surface processing method in the repair of coke oven broken holes to obtain a flat portion as shown by the hatched portion in FIG. Suitable for

Hereinafter, the result of the laser processing test conducted for verifying the effect of the present invention will be described. The laser processing apparatus shown in FIG. 1 was used. All the refractory bricks 2 to be processed were kept at 1000 ° C. A fiber laser installed outside the furnace was used as the laser device, and the laser beam was transmitted to the laser processing head unit 5 through the optical fiber 15. The following two methods were used in combination as the laser beam scanning method. First, as a large movement, the entire adiabatic cooling box 11 was moved up and down and left and right by a manipulator. A small movement of the order of mm was made by adjusting the tilt angle of the reflection mirror 6 which is a galvano-type mirror. As shown in FIG. 10, the processing results were evaluated based on the kerf width (w) and the height of the melt swell (h). Each index took an average value of five maximum values along the processing length of about 30 mm.

First, an example using a conventional method will be described. The thickness of the refractory brick was 50 mm. Processing was performed with a laser power of 2000 W, a power density of 20000 W / mm ² , and a beam scanning speed of 1 mm / s. As shown in FIG. 11, the laser irradiation was started at the same time as the scanning of the beam was started, and thereafter, it was maintained at a constant power density (20000 W / mm ² ). In this processing result, excessive melting was observed, and both w = 4.1 mm and h = 3.5 mm were large values. When the same processing was performed on a brick at 20 ° C., w = 1.6 mm and h = 2.2 mm, which were better than the result at a high temperature of 1000 ° C. In addition, when scanning processing was performed while changing the temperature under the same laser conditions as above, w = 1.8 mm and h = 2.3 mm at 200 ° C., and no influence of excessive melting was observed, but at 500 ° C. w = 2.8 mm, h = 2.9 mm, and an influence of excessive melting was observed. Therefore, it can be said that the method of the present application is particularly effective for the refractory brick 2 of 500 ° C. or higher.

The reason is considered as follows. The melting point of refractory bricks is around 1700 ° C, depending on the components. Since {(1700-1000) / (1700-20)} ≈0.4, in the range of rough estimation ignoring the temperature dependence of the physical property value such as specific heat, the case of 1000 ° C. is 40 in the case of 20 ° C. It can be seen that melting occurs at a laser power of%. Moreover, when the temperature of a refractory brick is high, the thermal diffusion to the processing peripheral part also becomes slow. For these reasons, excessive melting occurs in the refractory bricks at 1000 ° C, which is thought to lead to a reduction in processing accuracy and quality.

Next, a first embodiment of the present invention will be described. This is an example corresponding to the first embodiment described above, and the beam was scanned by the method shown in FIG. 4 so that the order in which the through holes are formed is continuous. The thickness of the refractory brick was 50 mm. The power density of the laser beam was modulated as shown in FIG. First, the processing time with a high power density was set such that the laser power was 2000 W, the power density was 20000 W / mm ² , and the time width was 200 ms. The non-processing time with a low power density was set at a laser power of 0 W and a time width of 800 ms. That is, it can be said that the power density is pulse-modulated with a repetition frequency of 1 Hz. In a preliminary study, a through-hole was obtained by three times of machining under this modulation condition. Based on this, in the cutting process, the processing is performed at a fixed position three times, and when the three processes at the fixed position are completed, the adjacent irradiation position is reached during the next 800 ms when the laser power is 0 W. Processing was performed while shifting the irradiation spot. This movement was performed by adjusting the tilt angle of the galvanometer mirror. The diameter of one through hole obtained by three times of processing was about 1 mm, and the interval between the centers of adjacent irradiation spots was 0.5 mm. As a result, w = 1.9 mm and h = 1.1 mm, and the effect of increasing the machining accuracy was confirmed.

Next, a second embodiment of the present invention will be described. This is an example corresponding to the second embodiment described above, and the beam was scanned by the method shown in FIG. The thickness of the refractory brick was 50 mm. The power density of the laser beam was modulated as shown in FIG. The processing time with a high power density was set to a laser power of 2000 W, a power density of 20000 W / mm ² , and a time width of 200 ms. The non-processing time with a low power density was set at a laser power of 0 W and a time width of 400 ms. Under this modulation condition, as described above, a through hole having a diameter of about 1 mm can be obtained by three times of processing. Therefore, processing is performed at a fixed position three times, and when the three processing at the fixed position is completed, processing is performed while shifting the irradiation spot to the next irradiation position within the next 400 ms when the laser power is 0 W. Went. The order of shifting the irradiation spot in the through holes is as shown in FIG. For example, the interval between a1 and a2 in FIG. 5 is 2 mm, the interval between a2 and a3 is 1 mm, etc. so that the through holes are finally formed at a pitch of 0.5 mm. In the range of 3.5 mm length from a1 to a8, the irradiation position was changed by tilting the reflection angle of the mirror. The movement from a8 to a9 took the method of moving the whole heat insulation box. The moving speed is limited compared to the mirror system, and a8 and a9 are adjacent to each other, and therefore, in order to avoid heat storage, a long non-processing time with a low power density is required. The non-machining time between machining a8 and a9 was 1000 ms. As a result of processing by the above method, w = 1.8 mm and h = 1.0 mm. Since the non-processing time can be shortened by processing in an order in which two consecutive irradiation spots are not overlapped, the second embodiment has an advantage that the processing time can be shortened compared to the first embodiment.

Next, a third embodiment of the present invention will be described. This is an example corresponding to the third embodiment described above, and the beam was scanned by the method shown in FIG. The thickness of the refractory brick was 100 mm. The power density of the laser beam was modulated as shown in FIG. The processing time with a high power density was set to a laser power of 2000 W, a power density of 20000 W / mm ² , and a time width of 200 ms. The non-processing time with a low power density was set at a laser power of 0 W and a time width of 800 ms. During this 800 ms, processing was performed while shifting the irradiation spot to the adjacent irradiation position. This movement was performed by adjusting the tilt angle of the galvanometer mirror. Under this modulation condition, the diameter of the non-through hole formed by one processing was about 0.8 mm, and the distance between the centers of adjacent irradiation spots was 0.4 mm. As a result, a groove having a depth of 20 mm was formed. w = 1.5mm and h = 1.1mm, and there was no excessive melting effect.

Next, a fourth embodiment of the present invention will be described. This is an example corresponding to the third embodiment described above, and the beam was scanned by the method shown in FIG. The refractory brick thickness is 100mm. The processing time with a high power density was set to a laser power of 2000 W, a power density of 20000 W / mm ² , and a time width of 200 ms. The non-processing time with a low power density was set at a laser power of 0 W and a time width of 400 ms. Under this modulation condition, as described above, a non-through hole having a diameter of about 0.8 mm can be obtained by one processing. The order of shifting the irradiation spots is as shown in FIG. For example, the interval between a1 and a2 in FIG. 5 is 1.6 mm, the interval between a2 and a3 is 0.8 mm, etc. so that the non-through holes are finally connected at a pitch of 0.4 mm. In the range of 2.8 mm from a1 to a8, the irradiation position was changed by tilting the reflection angle of the mirror. The movement from a8 to a9 took the method of moving the whole heat insulation box. For the same reason as described in the second embodiment above, the non-processing time between the processing of a8 and a9 was set to 1000 ms. As a result of processing by the above method, a groove having a depth of 20 mm was formed. w = 1.5mm and h = 1.0mm, and there was no excessive melting effect.

Next, a fifth embodiment of the present invention will be described. This is an example corresponding to the fifth embodiment described above. The refractory brick thickness is 100mm. The method of modulating the laser power density at each stage and the method of moving the irradiation spot were the same as in the third embodiment. Similar to the third embodiment, a groove having a depth of 20 mm was formed by one scan, and the same processing was repeated from above. As a result, a hole penetrated the 100mm thick refractory brick in the sixth step. At this time, w = 1.7 mm and h = 1.3 mm, and there was no influence of excessive melting.

Next, a sixth embodiment of the present invention will be described. This is an example corresponding to the above-described sixth embodiment. The refractory brick thickness is 100mm. The method of moving the irradiation spot and the point that the groove formed by one stage of processing is repeated in multiple stages are the same as in the fifth embodiment, but the temperature in the vicinity of the processing spot using the CCD camera 10 of FIG. Was changed to a method of modulating the laser power density based on the measurement. Machining was performed according to the control rule that the next machining was performed at the timing when the average temperature within 1mm radius near the next machining point was below 1300 ℃. A 20mm deep groove was formed in one scan, and the same process was repeated from above. As a result, the hole penetrated into the refractory brick with a thickness of 100mm in the 6th groove process. Is the same. At this time, w = 1.7 mm and h = 1.1 mm, which were almost the same quality as the fifth embodiment, but the processing time was shortened by 20%.

The reason for this is explained as follows. The non-working time required to prevent overmelting for each work hole has a certain variation due to non-uniformity of the refractory brick material. The non-machining time of 800 ms (see FIG. 12) employed in the fifth embodiment is set longer in consideration of this variation. In contrast, in the present embodiment in which the length of the non-machining time is determined by measuring the temperature, the non-machining time is set for a machining hole in which thermal diffusion from the vicinity of the next machining hole becomes fast, that is, when excessive melting is small. Can be shortened. Therefore, the average value of the non-machining time for a large number of machining holes can be made smaller than in the fifth embodiment in which a constant non-machining time is set, and therefore the machining time can be shortened.

It is explanatory drawing of the apparatus used for the laser processing of this invention. It is explanatory drawing of the laser processing on irradiation position fixed conditions. It is explanatory drawing of the laser processing on irradiation position fixed conditions. It is explanatory drawing of the laser processing method in 1st embodiment of this invention. It is explanatory drawing of the laser processing method in 2nd embodiment of this invention. It is explanatory drawing of the laser processing method in 3rd embodiment of this invention. It is explanatory drawing of the laser processing method in 4th embodiment of this invention. It is explanatory drawing of the laser processing method in 5th embodiment of this invention. It is a flowchart of a process control method. It is a figure explaining the evaluation method of the processing result in the Example of this invention. It is a figure explaining the laser irradiation method of a prior art example. It is a figure explaining the laser irradiation method of the Example of this invention. It is a figure explaining the laser irradiation method of the Example of this invention. It is explanatory drawing of the laser processing method by embodiment of this invention. It is a figure explaining the example of a repair method of the broken hole of the coke oven using this invention.

Explanation of symbols

DESCRIPTION OF SYMBOLS 1 Non-through-hole 2 Refractory brick 3 Through-hole 4 Condensing lens 5 Laser processing head part 6 Reflection mirror 7 Laser displacement meter 8 Collimator head 9 Processing part observation part 10 CCD camera 11 Adiabatic cooling box 12 Purge gas 13 Laser transmission pinhole 14 Parallel Beam 15 Optical fiber 16 Filter

Claims (8)

A laser processing method of irradiating a refractory brick having a temperature of 500 ° C. or higher with a laser beam and cutting the refractory brick,
The power density of the laser beam at the laser beam irradiation point on the surface of the refractory brick is temporally modulated between a power density that melts the refractory brick and a power density that does not melt the refractory brick, and the refractory brick. The laser beam irradiation point is scanned to form a plurality of through holes so that the positions of the through holes are continuously arranged, and at least adjacent through holes are overlapped among the plurality of through holes. A method for laser processing a refractory brick, characterized by cutting the refractory brick. The method for laser processing a refractory brick according to claim 1, wherein in forming the plurality of through holes, the order in which the plurality of through holes are formed is discontinuous. A laser processing method of irradiating a refractory brick having a temperature of 500 ° C. or higher with a laser beam to process the refractory brick,
The power density of the laser beam at the laser beam irradiation point on the surface of the refractory brick is temporally modulated between a power density that melts the refractory brick and a power density that does not melt the refractory brick, and the refractory brick. Scan the laser beam irradiation point above,
A plurality of non-through holes are formed so that the positions of the non-through holes are continuously arranged, and a groove is formed in the refractory brick by overlapping at least adjacent non-through holes among the plurality of non-through holes. A laser processing method for refractory bricks. 4. The method for laser processing a refractory brick according to claim 3, wherein in forming the plurality of non-through holes, the order in which the plurality of non-through holes are formed is discontinuous. The method for laser processing a refractory brick according to any one of claims 3 and 4, wherein the groove depth is increased by repeating the formation of the groove a plurality of times. The method for laser processing a refractory brick according to any one of claims 3 and 4, wherein the refractory brick is cut by repeating the formation of the groove a plurality of times. In the course of forming a plurality of the through holes so that the positions of the through holes are continuously arranged, or in the course of forming the plurality of the non-through holes so that the positions of the non-through holes are continuously arranged, the through holes The intensity of electromagnetic waves radiated from the periphery of the hole or non-through hole is measured, and the order of forming the remaining through holes or non-through holes is determined based on the intensity of the electromagnetic wave. The laser processing method of the refractory brick of any one of -6. The refractory brick laser processing method according to any one of claims 1 to 7, wherein the refractory brick is a refractory brick used for a furnace wall separating a carbonization chamber and a combustion chamber of a coke oven.

Images