Method and apparatus for high frequency pulse ARC welding

Abstract: A method for high frequency pulse welding and an apparatus therefor and use thereof are provided. In the method and the apparatus, a highly directive arc can be obtained by eliminating effect of inductance of the welding cable make a high frequency electromagnetic pinch force large. In a method and an apparatus for high frequency pulse arc welding which is performed by generating an arc between an inconsumable electrode or a consumable electrode arranged near a portion of a base metal to be welded and the base metal with main pulse current, when the main pulse current is shifted from ON to OFF, a reverse pulse current having a polarity opposite to a polarity of the main pulse is supplied between the electrode and the base metal to improve stiffness (directivity) of the arc by making rises and falls of the pulses steeper. A rail-car and a nuclear power plant obtained by the method are also provided.

Description: The present invention relates to a novel method for high frequency pulse arc welding, and an apparatus therefor and use thereof. It is known that, in a conventional high frequency pulse arc welding method, as a peak value of high frequency pulse current is higher, a quenching force by an electromagnetic force becomes larger and consequently stiffness of an arc and pressure of the arc are increased largely. It is also said that vibration effect if the high frequency peak pulse current can decease grain size of a welding portion and reduce blowholes. However, the welding current in actual welding work is a ripple current due to inductance L of a welding cable as shown in FIG. 12, and accordingly there is a disadvantage in that the effect of high frequency pulse current cannot be obtained sufficiently. Further, in a conventional direct current TIG arc welding method, stiffness of the arc is obtained by a gas pinching force using a mixed gas of argon and hydrogen for the shielding gas as a means for giving the arc stiffness (directivity). This stiff arc is used for weld with a very narrow edge groove of austenitic stainless steels. However, this welding method cannot be used for welding of ferritic stainless steels or steels because of hydrogen embrittlement. Further, this welding method cannot be used for welding of aluminum or aluminum base alloys because hydrogen causes blowhole. On the other hand, the conventional pulse welding cannot apply to aluminum welding either because of lack of cleaning action. Arc welding methods and apparatuses involved with high frequency pulse current are disclosed in Japanese Patent Application Laid-Open No.53-119758, Japanese Patent Application Laid-Open No.54-131548 and Japanese Patent Application Laid-Open No.59-92169. In the past, the pulse arc welding method has been small in arc stiffness, and consequently it has been difficult to perform welding with a narrow weld edge groove and welding of deep melting penetration. US 4861965 and DE 4233818 both disclose methods of arc welding which apply a pulse having the opposite polarity to the main welding pulse after the main welding pulse to make the arc more directive. The present invention seeks to provide a method for high frequency pulse welding and an apparatus for high frequency pulse welding in which the effect of inductance of the welding cable is eliminated, or at least reduced, and the high stiff arc and a cleaning action may be obtained. Thus, according to a first aspect of the present invention there is provided a method for high frequency pulse arc welding which is performed by generating an arc between any one of an inconsumable electrode and a consumable electrode arranged near a portion of a base metal to be welded and the base metal with main pulse current, characterised in that said main pulse current has a current conducting time of 5-100 µsec per one pulse; and when said main pulse current is shifted from ON to OFF, a reverse pulse current having a polarity opposite to a polarity of said main pulse current is, immediately following the main pulse, supplied between the electrode and the base metal to make the rate of passage from the peak value of the main pulse current to the peak value of the reverse pulse current not smaller than 50A per 1 µsec. According to a second aspect of the present invention, there is provided a method for high frequency pulse arc welding which is performed by generating an arc between an inconsumable electrode arranged near a portion of a base metal to be welded and the base metal with main pulse current while a filler wire is being supplied, characterised in that said main pulse current has a current conducting time of 5-100 µsec per one pulse and when said main pulse current is shifted from ON to OFF a reverse pulse current having a polarity opposite to a polarity of said main pulse is, immediately following the main pulse, supplied between the electrode and the base metal to make the rate of passage from the peak value of the main pulse current to the peak value of the reverse pulse current not smaller than 50A per 1 µsec. According to a third aspect of the present invention there is provided an apparatus for high frequency pulse arc welding by which welding is performed by generating an arc between any one of an inconsumable electrode and a consumable electrode arranged near a portion of a base metal to be welded and the base metal with main pulse current, the apparatus comprising: a welding power source for supplying said main pulse current; a high frequency converter for converting a direct current to a high frequency pulse welding current having a polarity opposite to a polarity of the direct current; characterised in that said apparatus further comprises: a control unit for applying a reverse pulse current having a polarity opposite to a polarity of said main pulse current, immediately following the main pulse, between the electrode and the base metal to make the rate of passage from the peak value of the main pulse current to the peak value of the reverse pulse current not smaller than 50A per 1 µsec when said main pulse current is shifted from ON to OFF, said main pulse having a current conducting time of 5 -100 µsec per one pulse. Preferably the converter is composed of semiconductors such as IGBT elements or the like. Preferably the welding power source and the converter are separated and connected using a welding cable or a coaxial cable between them. It is thus possible for the present invention to provide a method for high frequency pulse welding and an apparatus for high frequency pulse welding which is excellent in stiffness (directivity) and stability of the arc, and particularly capable of preventing the arc from burning on side walls of very narrow weld edge groove having a gap smaller than 6 mm, and capable of performing deep melting penetration welding and high speed welding of aluminium or aluminium base alloys. In addition to this, an object of the present invention is to provide a butt welded structure and a rail-car body structure manufactured by the method and the apparatus. The present invention may also provide a structure to be made of carbon steel or a low-alloy steel manufactured by butt welding with a narrow weld edge groove, and a nuclear power plant using the butt welded structures. In the above aspects of the present invention, the rate of passage from the peak value of the main pulse current to the peak value of the reverse pulse current is not smaller than 50A per 1 µsec. Preferably this rate is not smaller than 100A per 1 µsec, and a rate of above 200A per 1 µsec is particularly preferable. In order to do so, the welding load voltage is set to a voltage not lower than 60 V, and preferably to a voltage not lower than 80 V. The welding load voltage is preferably set to a voltage within a range of 60 to 200 V, and the welding load voltage within a range of 80 to 160 V is particularly preferable. The present invention is characterized by that in a method for TIG high frequency pulse arc welding with a very narrow weld edge groove having a weld edge gap width below 6 mm, a directive arc is produced between an inconsumable electrode and a base metal by a main pulse current to prevent a side-wall arc and stably maintain the arc in the narrow weld edge groove. A method for high frequency pulse arc welding of aluminum or an aluminum base alloy in accordance with the present invention is characterized by that a cleaning action and a directive arc are produced by properly selecting a current conducting time period ratio of the main pulse current to the reverse pulse current or a peak current ratio of the main pulse current to the reverse pulse current to make deep melting penetration welding and high speed welding possible. It is preferable that a current stopping period is provided during a period between the reverse pulse current and the main pulse current after the reverse pulse current. It is also preferable that a base current smaller than the main pulse current is conducted during a period between the reverse pulse current and the main pulse current after said reverse pulse current. It is preferable that either of peak values of the main pulse current and the base current the current conducting time periods of the main pulse current and the base current are periodically varied. It is preferable that the main pulse current is varied with a frequency in a range of several Hz to several tens Hz and the molten metal is stirred to prevent grain growth. It is preferable that the reverse pulse current, the base current and the current conducting time period, the current stopping period can be independently varied. In a method for high frequency pulse arc welding of aluminum or an aluminum base alloy in accordance with the present invention, it is preferable that a cleaning action and a directive arc are produced by varying a current conducting time period ratio of the main pulse current to the reverse pulse current or a peak current ratio of the main pulse current to the reverse pulse current to make deep melting penetration welding and high speed welding possible. It is preferable that the rise time and the fall time of said main pulse current are not longer than 50 µ sec. It is preferable that the welding power source and the high frequency converter are separated and connected using a welding cable or a coaxial cable. The present invention is characterized by a butt welded structure made of aluminum and an aluminum base alloy, wherein structural parts composing the butt welded structure are joined by forming a weld metal of the aluminum or aluminum base alloy inside an I-shaped weld groove having a gap not larger than 6 mm. The present invention is characterized by a rail-car body structure made of an aluminum alloy, wherein all of or part of structural parts composing the rail-car body structure are joined by welding with an I-shaped weld groove having a gap not larger than 6 mm. The present invention is characterized by a butt welded structure made of a carbon steel or a low-alloy steel, wherein structural parts composing the butt welded structure are joined by forming a weld metal of the carbon steel or the low-alloy steel inside an I-shaped weld groove having a gap not larger than 6 mm; and stress relief annealing treatment after welding is omitted. The present invention is characterized by a nuclear power plant comprising a nuclear reactor, a steam turbine, a condenser, a condensate demineralizer and pipes connecting between the components, the pipes being made of a carbon steel or a low-alloy steel, wherein the pipes have a butt weld structure, and are joined by forming a weld metal of the carbon steel and the low-alloy steel inside an I-shaped weld groove having a gap not larger than 6 mm; and stress relief annealing treatment after welding is omitted. FIG. 12 is a schematic diagram showing a conventional pulse weld. The reference character 1 is a welding power source, the reference character 8 is a transistor for converting the welding power to a high frequency pulse current, and the reference character 9 is a floating inductance of a welding cable. Let a welding current flowing the circuit when the transistor 8 is turned ON be I, a power source voltage of the welder be E1, an arc voltage be E2, and an ON voltage of the transistor be E3. Here, assuming that the arc voltage is a constant value determined by a welding condition and not depending on the welding current, the following equation holds when the component of resistance is neglected. E1 - E2 - E3 = L · (dI/dt) Therefore, the following equation holds. I = [(E1 - E2 - E3)/L] · t It can be understood from the equation that the welding current does not increase steeply, but increases linearly at a constant speed. When the welding power source voltage, the welding load voltage and the transistor ON voltage are assumed to be invariable, increase of the current is in inverse proportion to the inductance L. When the transistor is turned OFF, the current decreases in nearly the same gradient as the gradient at rising. That is, in the first invention of the present application, a voltage supplied to the arc load is increased in order to make the rise of a pulse current steeper, as can be understood from the equation, and a voltage (current) is applied in the reverse direction (reversing the polarity) to forcefully interrupt the main direction current in order to make the fall of a pulse current steeper, as shown in FIG. 2. Further, in regard to the fall of the reverse direction current, as the reverse direction voltage is higher or the reverse direction time t2 is longer if the reverse direction voltage is constant, the effect becomes larger. As for the reversing of the polarity, the polarity is reversed by switching an applying direction of the voltage using four IGBT elements as shown in FIG. 1. In welding work for maintenance at a site such as welding of a cooling pipe in a nuclear plant, distance between the welder and the position of welding work sometimes becomes 50 to 100 m. In such a case, since the effect of the inductance of the cable is too large in a conventional high frequency pulse weld, the high frequency pulse current becomes a ripple current waveform, as shown in FIG. 13, and the effect of the high frequency pulse current is hardly obtained. In the present invention, the problem can be solved by increasing the load voltage and reversing the polarity. However, in the present invention, in addition to this, the effect of the inductance of the cable is reduced by separating the welding power source and the high frequency pulse converting portion, placing the converting portion near the welding work place and connecting the welding power source and the converting portion using a coaxial cable. When a base metal is in the negative polarity (during the reverse direction current), the base metal is cleaned because positive ions collide onto the base metal to remove the oxide film. However, since the depth of penetration becomes shallower during that period, the conducting time t2 of the reverse direction current (the base metal is in the negative polarity) is preferably set shorter except for welding of aluminum or an aluminum alloy. Therefore, it is necessary to set the conducting time t2 to a value within a range capable of obtaining an optimum waveform by observing consumption of the electrode or the like. In a continuous pulse current of repeating main pulse current, reverse pulse current and main pulse current, reverse pulse current and so on, if the peak current is increased, the average current cannot be lowered because the average current is also increased corresponding to increase of the peak current and. Therefore, in the present invention, a current stopping period is provided between the reverse pulse current and the main pulse current after the reverse pulse current. The average current can be lowered by setting the time period long even if the peak current is increased. This method is effective in welding of a thin plate in which welding is performed with a small current and in stiffness of the arc and stability of the arc in weld with a very narrow edge groove. In FIG. 2, when the main pulse current, the reverse current and the current conducting times are fixed constant and a small current (a base current) is conducted during t3 between the reverse direction current and the next main pulse, the average current is increased. That is, the average current can be varied by changing the base current. In general, a high average current is required in welding thick plates. However, if the high average current is obtained only by increasing the peak current, cost of the apparatus becomes expensive. Therefore, it is possible to weld thick plates by adding the base current in the period of t3 to increase the average current. If the structure of a joined portion is grown to large grains, there are some cases where the boundary between the base metal and the joined portion cannot be clearly detected by ultrasonic wave inspection, which is a trouble of inspection. Therefore, in the present invention, by varying the main pulse current, the base current or any one of current conducting time of the main pulse current and the base current with a period in a range of several Hz to several tens Hz, an average arc pressure (average arc current) is varied to stir the molten metal to prevent grain growth. In arc weld with a very narrow edge groove having a gap smaller than 6 mm, weld can be performed with an amount of input heat approximately 1/2 as small as that in arc weld with a common narrow edge groove having a gap of 8 mm. However, it is necessary that the arc current of small input heat can be maintained in the very narrow weld edge groove. One method of weld with a very narrow edge groove is that an arc is stiffly concentrated by a pinch force of a mixed gas of argon and hydrogen to reduce side wall arc (in some cases, helium gas is mixed, but the effect is small because of a weak pinch force). However, the method cannot be used for steel or a ferritic alloy since hydrogen is used for the shield gas and causes hydrogen embrittlement. In the method of very narrow edge groove welding in accordance with the present invention, the average current can be lowered and the peak current can be increased by using a high frequency pulse arc welding current waveform even if inductance of the cable is large. Therefore, the arc is made stiff and the directive arc can be stably maintained even in weld with a very narrow edge groove and a small heat input (welding current). Further, the method in accordance with the present invention can be applied to welding of steel or a ferritic alloy because hydrogen embrittlement is not caused. The conventional pulse weld cannot be used for welding of aluminum because of lack of cleaning action and blowhole caused by hydrogen. On the other hand, the pulse welding in accordance with the present invention can be used for welding of aluminum or an aluminum alloy because the polarity is alternatively reversed and the oxide film can be removed by cleaning action of argon when the polarity of the welded base metal is reversed to negative. In addition to this, it is possible to perform deep melting penetration welding and high speed welding by the action of stiffness (directivity) of the high frequency pulse arc and by properly selecting the current conducting time period ratio of the positive polarity to the negative polarity or the peak current ratio of the positive polarity to the negative polarity. In the drawings FIG. 1 is a schematic block diagram showing the construction of a high frequency pulse welding apparatus in accordance with the present invention; FIG. 2 is a schematic chart showing a waveform of high frequency current pulse used in the present invention; FIG. 3 is a schematic chart showing a waveform of another high frequency current pulse used in the present invention; FIG. 4 is a schematic view showing the overall construction of another high frequency pulse arc welding apparatus in accordance with the present invention; FIG. 5 is a view showing a welding torch used in the present invention; FIG. 6 is a diagram showing the construction of a waveform control power source of a high frequency pulse arc welding apparatus in accordance with the present invention; FIG. 7 is a schematic diagram showing a nuclear power plant; FIG. 8 is a schematic chart showing a modification of a waveform of high frequency current pulse used in the present invention; FIG. 9 is a schematic chart showing another modification of a waveform of high frequency current pulse used in the present invention; FIG. 10 is a perspective view showing a welded structure of honeycomb panels; FIG. 11 is a perspective view showing a welded structure of a rail-car body; FIG. 12 is a diagram showing the construction of an example of a pulse welder of a conventional method; and FIG. 13 is a schematic chart showing a waveform of high frequency pulse current of the conventional method. [Embodiment 1] FIG. 1 is a schematic block diagram showing the construction of a high frequency pulse welding apparatus in accordance with the present invention. FIG. 2 is a schematic chart showing a waveform of high frequency current pulse in accordance with the present invention. Referring to FIG. 1, the pulse welding apparatus in accordance with the present invention comprises a power source 1 such as a high response power source of inverter type, analogue type, chopper type or the like; a DC high frequency pulse converting portion 2 for converting a direct current to a high frequency pulse current, the converting portion being composed of four IGBT switching elements; coaxial cables 4 connecting the welding power source 1 of direct current power source and the high frequency pulse converting portion 2; a control unit 3 for controlling the welding power source and the DC high frequency pulse converting portion; and a control cable 7 for applying a signal to bases of the IGBT elements. Operation of the apparatus will be described below. When a main pulse control signal voltage of FIG. 2 is input to the bases of the IGBT elements T2 and T3 from the control unit 3 and the IGBI elements are turned ON, a welding current i sequentially flows from T2 through a base metal of objects 6 to be joined (arc load) of, a welding torch 5, T3 and returns to a negative polar terminal. When a reverse pulse control signal voltage of FIG. 2 is input to the bases of the IGBT elements T1 and T4 and the IGBI elements are turned ON, a welding current i sequentially flows from T1 through the welding torch 5, the base metal of objects 6 to be joined (arc load) of base metal, T4 and returns to the negative polar terminal. Therefore, the polarity at the welding portion is reversed. By periodically performing this operation, it is possible to obtain a continuous high frequency pulse current waveform having a steep fall as the ideal current waveform shown by the schematic chart of FIG. 2. The current conducting time periods t1, t2, t3 and a peak current in the waveform are set by changing setting values of the signals of the control unit. An example of application of the apparatus to a very narrow edge groove welding will be described below. A welding test was conducted under the following conditions. The objects to be joined 6 were plates of a carbon steel having a thickness of 30 mm. The other welding conditions were as follows. Gap width of I-shaped weld edge groove: 3 mm (the beveling angle of 3 degrees), shield gas: argon, tungsten electrode: flat electrode, welding filler (carbon steel) wire: 0.9 mm diameter, welding load voltage: 120 V, peak current: 500 A, and current conducting time period t1: 20 µsec (5 to 100 µsec). The reverse pulse current was 500 A at maximum and the current conducting time period t2 of the reverse pulse current was determined to set to 4 µsec (1 to 50 µsec) so that the welding current waveform became an optimum waveform on observation. Current conducting time period t3: 25 µsec (10 to 200 µsec), welding speed: 260 cm/min, length of the coaxial cable connecting between the DC high frequency pulse converting portion and the welding power source: 50 m, and length of the cable connecting between the DC high frequency pulse converting portion and the welding torch: 2 m. The result of welding the above conditions was that the arc was stiff (directive) and stably maintained in the narrow edge groove and a good weld result was obtained. The current changing rate in the rise time and the fall time of the pulse in this embodiment was 200 to 300 A per 1 µsec. The reverse pulse current was approximately one half of the main pulse current. A welding test was also conducted by the conventional method, but the test pieces could not be welded using a shield gas of solely argon because of occurrence of side wall arc. Further, a welding test was also conducted by the conventional method changing the shield gas to a mixing gas of argon and 50 % helium, but the arc became unstable when the length of the arc was fluctuated, and a joining fault occurred because of a narrow suitable range of the length of the arc. Furthermore, a series of tests by the method of the present invention were conducted by variously changing the gap width of the I-shaped weld edge groove, and the result showed that welding of a weld edge groove of 2.5 mm (the beveling angle of 3 degrees) and a plate thickness of up to 30 mm was possible. FIG. 3 is a schematic chart showing a practical current waveform. The reference characters in the figure indicate the same corresponding current conducting time periods in FIG. 2, respectively. Each of the peak current and the reverse pulse current is composed of a plurality of waveforms while each of the currents in FIG. 2 is a rectangular waveform. FIG. 4 shows the construction of a high frequency pulse TIG welding apparatus in accordance with the present invention. A TIG torch 5 and a TIG wire supply unit 13 are mounted on a movable cart 14 moving on a periphery of an object to be welded 6 of pipe. Argon gas for shielding the arc portion is supplied to the welding torch 5. A cooling water recirculation unit 12 is a cooling unit for preventing over heating of a welding power source 1 of AC 200 V, a semiconductor unit of a DC high frequency pulse converting portion 2 and the welding torch 5. Cooling water is recirculated through a coaxial cable 4 capable of making water flow. Control of the high frequency pulse current is performed by that a control signal of the welding power source 1 controls the semiconductors of the DC high frequency pulse converting portion 2 through a control signal cable 7. FIG. 5 shows the construction of a high frequency pulse MIG welding apparatus. The construction of high frequency pulse MIG welding apparatus is the same as that of FIG. 4 except for a MIG torch 10 and a MIG wire supplying unit 15. Automatic welding can be performed by mounting the MIG torch 10. FIG. 6 is a diagram showing the construction of a waveform control power source. The reference character 17 indicates a cable of which inductance is reduced by closely attaching a positive and a negative cables having a length of approximately 50 m to each other, the reference character 18 indicates an adder for performing feedback control of the average current by changing the current conducting time period t3. The current feedback is used for the TIG welding, and the voltage feedback is used for the MIG welding. [Embodiment 2] FIG. 7 is a schematic diagram showing the system of a BWR power plant having a butt welding structure in accordance with the present invention. Referring to the figure, the reference character 30 is a nuclear reactor, the reference character 31 is a turbine, the reference character 32 is a condenser, the reference character 33 is a condensate demineralizer, the reference character 34 is a low pressure condensate water pump, the reference character 35 is a feed water recirculation line, the reference character 36 is an electric conductivity detector, the reference character 37 is a dissolved oxygen concentration meter, the reference character 38 is an injector for oxygen or an inert gas or an alkali agent, the reference character 39 is a pH meter, the reference character 40 is a feed water heater and the reference character 41 is a reactor water clean-up system. Pipes made of austenitic steel of SUS 304L or SUS 316L are used for the primary cooling system piping of the nuclear reactor 30, but pipes made of a carbon steel or a low alloy steel are used for the other piping. In this embodiment, pipes made of the carbon steel or the low alloy steel were joined with the same weld edge groove and in the same welding method as those of Embodiment 1. The result showed that stress release annealing after welding could be eliminated. That is, the remaining stress was so small that the pipes could be used after welded as they were. Further, the primary cooling system pipes were welded in the same method as Embodiment 3 to be described below. [Embodiment 3] When the structure of a joined portion is grown to large grains, there are some cases where the boundary between the base metal and the joined portion cannot be clearly detected by ultrasonic wave inspection. Prevention of grain growth will be described below, as an example of application of the present invention. A welding test was conducted under the following conditions. Welding method: TIG welding with wire supply, base metal: austenitic steels of SUS 304L and SUS 316L, plate thickness: 30 mm, V-shaped weld edge groove: bevel angle of 30 degrees, and welding load voltage: 120 V. While the welding peak current and the time period were kept at 600 A and 79 µ sec constant, respectively, the current conducting time periods were alternatively switched between t1: 50 µsec, t2: 4 µsec, t3: 25 µsec and t1: 20 µsec, t2: 4 µsec, t3: 55 µsec. The weld result was that the average current (average arc pressure) was varied in synchronism with the switching period and the molten weld metal was stirred corresponding to the variation to prevent grain growth of the weld metal. The current changing rate in the rise time and the fall time of the pulse in this embodiment was similar to that in Embodiment 1. The reverse current was one half of the peak current. Vibration of the high frequency pulse current also accelerated the prevention of grain growth. An inspection result of the test piece welded under the conditions showed that the joined portion and the base metal could be discriminated more clearly than those welded by the conventional TIG welding method. The above test was conducted by varying the current conducting time period (t1) of the main peak current in order to change the average current (average arc pressure) while the switching time period was kept constant. However, the same effect can be obtained by periodically varying the base current in the current conducting time period t3 or the peak current of the main current. [Embodiment 4] An example of welding of deep melting penetration with aluminum will be described below. Since the polarity is reversed in the high frequency pulse current waveform in the present invention, aluminum can be welded because the base metal is cleaned and the oxide film is removed by positive argon ions when the base metal to be joined is in negative polarity. The cleaning effect is higher as the time period when the base metal is in negative polarity is longer. However, the depth of penetration is shallow and a consuming rate of a tungsten electrode is large. Therefore, the depth of penetration can be increased by shortening the time period of the base metal in negative polarity and lengthening the time period of in positive polarity within a range capable of being welded. A welding test was conducted under the following conditions. Base metal to be joined: aluminum plate, plate thickness: 6 mm, joining: I-butt joining, electrode: tungsten electrode of 4 mm diameter, welding load voltage: 120 V, welding peak current: 500 A. The current conducting time periods were t1: 30 µsec, t2: 3 µsec, t3: 20 µsec, and the welding speed was 200 cm/min. The welding result showed that welding could be performed by once-through passing with good wave beads in the reverse side. The current changing rate in the rise time and the fall time of the pulse in this embodiment was similar to that described previously. A conventional alternating current welding having the cleaning action can be perform welding by decreasing the welding speed to 150 cm/min. However, there is a disadvantage in that the beads become wider in width and in heat affected portion. Further, a welding test was conducted by setting the power source condition to a constant voltage condition and changing the tungsten electrode to a tungsten wire. The result showed that high speed welding could be performed at the same speed as described above. [Embodiment 5] FIG. 10 is a perspective view showing a welded structure of honeycomb panels used for a car body of a rail car which is butt-welded through the same method as in Embodiment 4. The honeycomb panel is constructed by joining a surface plate 51 made of an aluminum alloy, a core member 52 made of an aluminum alloy and a frame member 56 of an aluminum alloy with a solder. The honeycomb panels were joined through the frame members 56 by forming welded portions 55 of a narrow edge groove in the obverse and reverse sides using a welding torch 54 under the same welding condition as described above. In this embodiment, the honeycomb panels were joined by MIG welding. The filler used had the same composition as that of the base metal, the weld edge groove was I-shaped, and the gap of the weld edge groove was 3 mm. FIG. 11 is a perspective view showing a car body of the rail-car assembled though the welding method in accordance with the present invention. The main car body is composed of ceiling boards 60, car-body side walls 61 and floor boards of the car body, and these members are welded and assembled at welded portions 63 through the welding method of the present embodiment. The total length of the car body is 25 m. According to the present invention, by the stiff (directive) arc which is obtained by the high frequency electromagnetic pinch force eliminated the effect of inductance of the welding cable, narrow edge groove welding can be stably performed without using a hydrogen containing mixed gas causing hydrogen embrittlement as the shield. Further, by the cleaning action of the polarity reversing current, deep penetration welding of aluminum and high speed welding can be performed. Since the effect of inductance of the welding cable does not exist even at a place 50 m apart from the welding power source, the present invention can be applied to maintenance welding by remote operation of a pipe in a nuclear plant. Since grain growth can be prevented by varying the average current (arc pressure) with several Hz, the base metal and the joined portion cannot be clearly detected by ultrasonic wave inspection and accordingly the ultrasonic wave inspection can be easily performed. The effect of the high frequency pulse can be obtained even if the present invention is applied to a carbon oxide gas arc weld or a shielded metal arc weld.

Claims: A method for high frequency pulse arc welding which is performed by generating an arc between any one of an inconsumable electrode (5) and a consumable electrode (5) arranged near a portion of a base metal (6) to be welded and the base metal (6) with main pulse current, characterised in that : said main pulse current has a current conducting time of 5-100 µsec per one pulse; and when said main pulse current is shifted from ON to OFF, a reverse pulse current having a polarity opposite to a polarity of said main pulse current is supplied between the electrode (5) and the base metal (6) to make the rate of passage from the peak value of the main pulse current to the peak value of the reverse pulse current not smaller than 50A per 1 µsec, the reverse pulse immediately following the main pulse. A method for high frequency pulse arc welding according to claim 1, wherein a current stopping period is provided between said reverse pulse current and said main pulse current. A method for high frequency pulse arc welding according to claim 1, wherein a base current smaller than said main pulse current is applied during a period between said reverse pulse current and said main pulse current after said reverse pulse current. A method for high frequency pulse arc welding according to claim 3, wherein any one of peak values of said main pulse current and said base current and current conducting time periods of said main pulse current and said base current are periodically varied. A method for high frequency pulse arc welding according to any one of claim 1 to claim 4, wherein said main pulse current is varied with a period in a range of several Hz to several tens Hz to stir the molten metal to prevent grain growth. A method for high frequency pulse arc welding according to claim 1 which is performed by generating an arc between an inconsumable electrode (5) arranged near a portion of a base metal (6) to be welded and the base metal (6) with main pulse current while a filler wire (13, 15) is being supplied. A method for high frequency pulse arc welding, wherein I-shaped groove butt welding having a gap not larger than a width of 6mm is carried out using the welding method for high frequency pulse arc welding, according to any one of claim 1 to claim 6. A method for high frequency pulse arc welding according to any one of claim 1 to claim 7, wherein the rise and the fall time of said main pulse current are not longer than 50 µsec. An apparatus for high frequency pulse arc welding by which welding is performed by generating an arc between any one of an inconsumable electrode (5) and a consumable electrode (5) arranged near a portion of a base metal (6) to be welded and the base metal (6) with main pulse current, the apparatus comprising: a welding power source (1) for supplying said main pulse current; a high frequency converter (2) for converting a direct current to a high frequency pulse welding current having a polarity opposite to a polarity of the direct current; characterised in that said apparatus further comprises: a control unit (3) for applying a reverse pulse current having a polarity opposite to a polarity of said main pulse current, immediately following the main pulse, between the electrode (5) and the base metal (6) to make the rate of passage from the peak value of the main pulse current to the peak value of the reverse pulse current not smaller than 50A per 1 µsec when said main pulse current is shifted from ON to OFF, said main pulse having a current conducting time of 5 -100 µsec per one pulse. An apparatus for high frequency pulse arc welding according to claim 9, wherein said welding power source and said high frequency converter are separated and connected using any one of a welding cable and a coaxial cable (4). An apparatus for high frequency pulse arc welding according to claim 9 or claim 10, wherein said control unit has a means for establishing a current stop period between said main pulse current and said reverse pulse current or for establishing a base current which is smaller than said main pulse current. An apparatus for high frequency pulse arc welding according to claim 11, wherein said main pulse current, said reverse pulse current, said base current and said current conducting time period, said current stopping period can be independently varied. A method for butt welding of a aluminium or an aluminium alloy, wherein said butt welding is carried out using the welding method according to any one of claims 1 to 8. A method of welding of a rail-car body structure (60, 61, 62, 64) made of an aluminium alloy, wherein said welding is carried out using the welding method according to any one of claims 1 to 8. A method for butt welding of a carbon steel or a low-alloy steel, wherein said butt welding is carried out using the welding method according to any one of claims 1 to 8. A method for butt welding of a carbon steel or a low-alloy steel according to claim 15, wherein a stress relief annealing treatment after said butt welding is omitted. A method for manufacturing a nuclear power plant comprising a nuclear reactor (30), a steam turbine (31), a condenser (32), a condensate demineraliser (33) and pipes (35) connecting between the components, said pipes being made of any one of a carbon steel and a low-alloy steel, wherein said pipes have a butt weld structure, and are joined using the welding method according to claim 15 or claim 16.

Inventors: FUNAMOTO TAKAO, NIHEI MASAYASU, ONUKI JIN, ONUMA AKIRA, SAKURAI IZUMI, FUNAMOTO, TAKAO, NIHEI, MASAYASU, ONUKI, JIN, ONUMA, AKIRA, SAKURAI, IZUMI
Applicants: HITACHI LTD, HITACHI, LTD.
Application year: 1998
Main classification: B23K9
IPC codes: B23K9