The present invention relates to a welding structural member and a welding method. More specifically, the present invention relates to a welding structural member having a highly ductile spot-welded portion and a method for welding the structural member.
A spot welding device is used to weld overlapped steel plates.
Furthermore, an expulsion 56 may be formed in the void 58. The expulsion 56 is escaping of molten steel from the molten and solidified part 54 to outside through the heat-affected zone 55 during spot welding. The expulsion occurs in the void 58 between overlapped steel plates 50, 50, forming a part of the molten and solidified part 54. The expulsion 56 is also called an expulsion at edge. Once the expulsion 56 occurs, a blow hole, which is a spherical cavity, may be formed within the welded part 53, or splashed expulsion 56 may attach to a part of the steel plates other than the spot-welded part 53. The occurrence of the expulsion 56 is undesirable because a defect may result in a painting process performed after spot welding. At present, however, expulsions 56 are occurring unavoidably.
By the way, with spot welding performed in vehicle production lines, high-tension steel plates have recently been used as a raw material for vehicles in order to ensure compatibility between the weight reduction and the safety of vehicles.
It has been reported that in spot welding of high-tension steel plates, the peel strength of a cross joint hardly increases with the increase in material strength, but rather stable strength can hardly be obtained. The reason why the stable tensile strength cannot be obtained in peeling of cross joints is assumed to be extremely high concentration of stress on the circumference of the nugget 54. Under such circumstances, from a viewpoint of ensuring ductility of a welded region, limitations are set in compositions and combinations with other materials at present when using high-strength steel plates for vehicles. For example, the amount of carbon is maintained at a certain level or lower to prevent welded regions from becoming too hard.
Meanwhile, when using high-tension steel plates, the weight of a vehicle body can be trimmed efficiently, but high-tension steel plates having improved strength and ductility at the same time are desired. By further improving the strength of steel plates for vehicles, more weight reduction is expected. By further improving the ductility of steel plates for vehicles, press molding performance and sufficient deformability as products in case of a crash can be ensured. Generally, with the increase in the strength of steel plates for vehicles, their ductility tends to decrease. To improve the strength and ductility of steel plates for vehicles themselves, it is efficient to increase the amount of carbon in materials. However, in spot welding of steel plates for vehicles, since spot-welded regions become harder and more brittle in proportion to the carbon content, the stable and sufficient strength has hardly been ensured.
Various efforts have been made to solve the above problem in the strength of spot-welded part by devising welding methods. For example, an attempt is being made to perform tempering by subsequent energization after welded part is molded into a predetermined size. However, in resistance spot welding used for assembling vehicles, it is required to maintain the process time per point in as short as one second. When tempering is performed by subsequent energization with current welding facilities, the effect of the tempering becomes quite limited. Or, to ensure sufficient effect of tempering, the process time far exceeding the required time is necessary. The reason is that since the part directly under electrodes is energized when the tempering is performed using a conventional welding machine, the position requiring the effect of tempering deviates from the position heated mainly.
In conventional spot welding, the ensuring the strength of welded part was the attempt to ensure the ductility of molten and solidified part. In the heat-affected zone around a nugget, a region of weak bonded state called corona bond exists. This bonded state has been considered not to affect the bonding strength of spot-welded part because the corona bond is weak. In other words, the hardness of this region has been considered to be determined by the material composition of steel plates. That is why no attempts have been made to improve the strength and ductility or the strength in the bonded state in this region.
Patent Literature 1 discloses a spot welding device having a pair of electrodes and a spot welding device equipped with a high-frequency induction heating means having a heating coil installed by being wrapped around one of the pair of electrodes. This high-frequency induction heating means includes the heating coil for heating the part of a work to be welded and a high-frequency power supply for supplying high-frequency power to the heating coil.
As steel ensuring high strength and high ductility at the same time, a dual-phase steel having fine crystal grains has been studied, and deposition of carbon has been found to be an effective means (Patent Literature 2). To deposit carbon, it is necessary to ensure high carbon content in the material. However, when the carbon content increases, the spot-welded part becomes too hard and brittle, causing junction strength to decrease significantly. That is the reason why the carbon content of steel plates generally used for vehicles has been maintained to be around 0.15% by weight or lower. Meanwhile, the shape of electrodes for spot welding and energization conditions have been studied. It was found thus far that the spot-welded region formed by energizing electrodes is cooled down rapidly, and thus the metal structure in the molten and solidified part and the heat-affected zone becomes martensite structure as a result of this cooling. However, no further studies have been made.
Patent Literature 3 discloses a method for spot-welding overlapped steel plates by feeding low-frequency power and then high-frequency power.
Meanwhile, high-frequency current concentrates on the surface and the outer peripheral region of the electrodes 52. The difference in distribution of low-frequency current and that of high-frequency current is related to so-called skin depth.
In other words, when electric power is applied simultaneously to two overlapped steel plates 50 from low-frequency and high-frequency power supplies, as shown in
In conventional spot welding, an attempt to ensure the strength of welded part was started with the technology disclosed in Patent Literature 3. However, the improvement in the strength of molten and solidified part is further required.
In view of the above problem, a first objective of the present invention is to provide a welded structural member having a spot-welded part with sufficient strength and ductility and ensuring high rupture strength proven by a rupture test such as the cross tensile test. A second objective of the present invention is to provide a method for welding such a structural member.
To achieve the first objective described above, a welded structural member of the present invention includes: steel plates bonded by overlapping their surfaces and forming a welded part by spot welding, and is characterized in that the welded part contains a molten and solidified part and a heat-affected zone surrounding the molten and solidified part, and that the hardness on the welded surface increases, becoming higher than the hardness of base material of the steel plates, along a direction from outer region of the heat-affected zone toward the heat-affected zone.
In the above structure, the metal structure of the heat-affected zone and that of the molten and solidified part are preferably in a tempered martensite structure. The steel plates in the heat-affected zone are preferably bonded by solid-phase bonding. A crack on the welded part preferably progresses along a region other than the molten and solidified part as a rupture path in a cross tensile test. This welded part preferably has a bonding strength allowing a crack as a rupture path in a cross tensile test to change within the heat-affected zone.
According to the above structure, a welded structural member whose spot-welded part has high strength, high ductility, and high rupture strength proven by a rupture test such as the cross tensile test can be obtained. It is desirable that the welded part be cooled in a cooling period to a temperature lower than the temperature allowing martensitic transformation of the steel plates to finish.
To achieve the second objective described above, the spot-welding method of the present invention includes: sandwiching steel plates whose surfaces are laid on top of each other by a pair of electrodes; and applying DC power or a power having a first frequency between the pair of electrodes, thereby spot-welding the steel plates by the welded part thus formed. The method is characterized in that a cooling period is provided after the DC power or the power having the first frequency is applied to the pair of electrodes, and then a power having a second frequency, which is higher than the first frequency, is applied to the electrodes to heat the proximity region of the outer periphery of the area where the steel plates and the pair of electrodes contact, together with the connecting end region where the steel plates in the welded part overlap.
In the above configuration, a pressurization to the electrodes may be terminated when the power having the second frequency has been applied for a predetermined period of time.
According to the above configuration, by sandwiching the overlapped steel plates by the pair of electrodes, performing resistance heating to form a molten and solidified part, and heating a peripheral region of the molten and solidified part by high-frequency power having higher frequency than DC power or low-frequency power, a welded structural member having high strength and ductility can be produced.
According to the present invention, the welded structural member including spot-welded part having high strength, high ductility, and high rupture strength proven by the cross tensile test, and the welding method can be provided.
Embodiments of the present invention will hereinafter be described in detail by referring to drawings.
(Welding Device)
The welding device 10 for metallic materials further includes: a fixed base for supporting the electrode arm 12; a driving mechanism for driving the electrode arm 12; a thrust mechanism for thrusting one of the electrodes 14 from the electrode support 13, etc. (none of them are shown). The thrust mechanism is used to pressurize steel plates 2, 2, which will become a welded structural member 1 to be described later.
The electrode arm 12 has the top arm 12A and the bottom arm 12B, which are respectively connected to the electrodes 14, 14 via each electrode support 13. The electrode arm 12 is also called a gun arm. Since the gun arm 12 shown is in a so-called C shape, it is also called C-type gun arm. In addition to the C-type gun arm 12, an X-type gun arm, etc. can be used for portable-type or robot-type welding devices. The electrode arm 12 of any type is applicable, but a case where the C-type gun arm 12 is used for welding will hereafter be described.
Each of the electrode pair 14, 14 faces each other via a gap, into which two steel plates 2, 2 are inserted. The electrodes 14 are made of copper for example, and in a shape of a circle, an ellipse, or a rod.
The welding power supply 16 is a low-frequency power supply, and includes: for example, a commercial power supply 22 whose output frequency is 50 Hz or 60 Hz; a low-frequency power supply controller 24 connected to one end of the commercial power supply 22; and a welding transformer 26 connected to the other end of the commercial power supply 22 and to the output end of the low-frequency power supply controller 24. Both ends of the secondary winding of the welding transformer 26 are respectively connected to the left end of the top arm 12A and the left end of the bottom arm 12B of the C-type gun arm. The low-frequency power supply controller 24 is made up mainly of a semiconductor device for power control such as a thyristor, and a gate drive circuit, and controls feeding of power from the commercial power supply 22 to the electrodes 14.
A bypass capacitor 21 is connected to the side of the C-type gun arm 12 of the welding transformer 26, namely to the secondary winding 26A, in parallel. The bypass capacitor 21 has a low capacitive impedance with respect to the frequency of the high-frequency power supply 18. Consequently, the high-frequency voltage from the high-frequency power supply 18 can minimize the voltage applied to the secondary winding 26A, thereby lowering the high-frequency inductive voltage to the primary side of the welding transformer 26. Also, an inductance 23 for inhibiting high-frequency current is connected to the secondary winding 26A of the welding transformer 26 in series. The inductance 23 for inhibiting high-frequency current rarely affects the low-frequency current but has a function of preventing current from the high-frequency power supply 18 from flowing into the low-frequency power supply 16.
The high-frequency power supply 18 includes an oscillator 28 and a matching transformer 30 connected to the output end of the oscillator 28. An end of the matching transformer 30 is connected to the top arm 12A of the C-type gun arm 12. The other end of the matching transformer 30 is connected to the bottom arm 12B of the C-type gun arm 12 via the capacitor 17. This capacitor 17 can also be used as a matching capacitor in a series resonance circuit, which will be described later. The capacitance value of the capacitor 17 depends on the oscillating frequency of the oscillator 28 and the floating inductance 15 of the C-type gun arm 12. The oscillator 28 includes an inverter using various transistors, and controls the power fed from the high-frequency power supply 18 to the electrodes 14.
As shown in
(Welding Method)
A method for welding the structural member of the present invention will hereinafter be described.
(Current Distribution Generated on the Steel Plates)
(Skin Depth)
The skin depth of the steel plates 2 is an approximate depth where current is fed when low-frequency or high-frequency power is applied to the steel plates 2. The skin depth of the steel plates 2 varies in proportion to the frequency minus the half power i.e. f1/2. Consequently, the lower the frequency, the thicker the skin depth, and higher the frequency, the thinner the skin depth, of the steel plates 2, provided that the material is the same. Since the power used for welding is generally 50 Hz or 60 Hz, the current is fed through the entire electrodes 14 if the diameter of the tip of the electrodes 14 is approximately 6 mm.
Meanwhile, when the surface of the steel plates 2 only is to be heated, the skin depth from the surface can be set to be a predetermined value by adjusting the frequency of the high-frequency power supply 18. Therefore, to select a heating width of the ring-shaped proximity regions in the outer periphery to be heated by the high-frequency power supply 18, it is only necessary to set the frequency of the high-frequency power supply 18. In other words, by changing the frequency of the high-frequency current 32, the heating width of the outer peripheral region can be changed, and by having the ring-shaped proximity regions 2B and the end 2C undergo heating process such as tempering, the ring-shaped proximity regions 2B and the end 2C can be softened.
In order for the welded part to be tempered by the high-frequency energization and change into highly ductile tempered martensite structure, it is necessary for the spot-welded part 3 to be cooled to a temperature lower than the martensite transformation finish (Mf) point (called Mf temperature). The temperatures lower than the Mf point vary depending on the composition of the steel plates 2. For example, the Mf temperature of the steel plates 2 containing carbon (C) by 0.26% is approximately 300° C.
When the part whose temperature has decreased to lower than the Mf point is heated again, the tempered martensite structure is created, allowing ductility to improve. The feature of the present invention is that the uniform hardness distribution without angles can be obtained. When the tempering is started in a state where the temperature of the entire welded region has not reached 300° C., which is the Mf temperature, namely where the incompletely quenched part is included, the hardness distribution on the cross section of the welded part becomes a shape of M, the high-hardness regions generated between the steel plates 2 (base material) and the heat-affected zone 5 remaining as angles, as shown in Comparative Example in
Provided that the entire region of the spot-welded part 3 of the present invention is cooled to 300° C. or lower, the hardness distribution becomes mostly uniform, as shown in Example 1 in
The basic form of hardness distribution is created by cooling time (cooling), and the increase and the decrease in the hardness within the welded part can be adjusted by the amount of high-frequency electric power (heat) applied. The structure of the part whose temperature has decreased by cooling to the Mf point (300° C.) or lower changes from the quenched martensite structure to the tempered martensite structure.
As shown in
For example, in the hardness distribution of the spot-welded part 3, assuming that the optimum hardness of angled part falls within a range from 550 to 560 (HV), the relation between the cooling time and the high-frequency power of the structure is as follows:
(a) The higher the output, the rougher the structure.
(b) The higher the output and longer the application time, the rougher the structure and darker the color because of the deposition of carbide.
(c) The longer the time, the darker the color because of the deposition of carbide.
Meanwhile, the structure created only by the conventional low-frequency energization, no clear outline is created but shading only appears, as shown in
The part whose temperature does not decrease to the Mf point or lower by cooling remains in an angular shape in the hardness distribution as a transitive part from austenite structure. Its structure is hard and brittle.
According to the present invention, the cooling time, the magnitude of high-frequency power, and the application time of high-frequency power can be determined by comparing the tensile break strength, the breaking mode, and the structure. The above is provided that the plate thickness is 1.2 mm (t=1.2 mm).
The example where steel plates 2, 2 are spot welded was described above. However, any shapes can be selected in addition to plates. Also, the case where two steel plates 2 are spot welded was described, but three or more plates may be welded.
In the interfacial rupture shown in
With the welded structural member 1 in the Examples shown below, the rupture patterns in the cross tensile test are represented by the JIS classification in
The present invention will hereinafter be described further in detail by referring to Examples.
An example where two steel plates 2 are spot-welded by the welding device 10 will be described in detail.
Two steel plates 2 were spot-welded. Conditions such as details of the steel plates 2, low-frequency power supply 16, and the high-frequency power supply 18 used were:
Steel plates 2: Thickness; 1.2 mm, size; 50 mm×150 mm
Low-frequency power supply 16: 50 Hz, Electrodes 14 were made of copper, the diameter of the tip of each electrode 14 was 6 mm, the radius of curvature (R) of the tip was 40 mm, and the power capacity was 50 kVA.
Energization time by the low-frequency power supply 16: 0.34 sec
High-frequency power supply 18: 18.25 kHz, 29 kW
Energization time by the high-frequency power supply 18: 0.7 sec.
As the composition of the steel plates 2 (percentage by mass), carbon (C) was contained by 0.26%, for example, as a component other than iron.
The application of power from the low-frequency and the high-frequency power supplies 16, 18 in Example 1 will be described by referring to
First, the welding was performed by applying power from the low-frequency power supply 16. As shown in
In Example 1, the cooling period shown in
As Comparative Example 1 with respect to Example 1, two steel plates 2 were spot-welded by energization by the low-frequency power supply 16 only. In other words, the general spot welding was performed. The same steel plates 2 and the electrodes 14 used for Example 1 were used.
Rise of a first current by a first energization: 1 cycle (0.02) sec.
First energization (represented as “Low-frequency No. 1” in the FIG.): 9 kA, 1 cycle (0.02 sec.)
Cooling: 1 cycle (0.02 sec.)
Second energization (represented as “Low-frequency No. 2” in the FIG.): 5.5 kA, 6 kA, 7.2 kA, 14 cycles (0.28 sec.)
Third energization (represented as “Low-frequency No. 3” in the FIG.): 3.6 kA, 5 cycles (0.1 sec.)
The diameter of the nugget is determined by the current value of the second energization. The diameter of the nugget was measured by observing the cross section of the part welded by the general spot welding. The diameters of the nugget were approximately 4.4 mm, 4.9 mm, 5.4 mm, and 6 mm when the current of the second energization were approximately 5.5 kA, 6 kA, 6.5 kA, and 7.2 kA respectively.
The spot welding was performed in Comparative Example 2 by inserting a cooling period of one sec. between the second and the third energization in Comparative Example 1. Heating conditions other than the insertion of the cooling period, such as the first to the third energization, were the same as those in Comparative Example 1.
Rise of the first current by the low-frequency first energization: 1 cycle (0.02 sec.)
Low-frequency first energization: 9.0 kA, 1 cycle (0.02 sec.)
Low-frequency cooling: 1 cycle (0.02 sec.)
Low-frequency second energization: 7.2 kA, 14 cycles (0.28 sec.)
Cooling period: 50 cycles (1 sec.)
Low-frequency third energization: 6.0 kA, 10 cycles (0.2 sec.)
Hold time: 1 cycle (0.02 sec.)
As Comparative Example 3 with respect to Example 1, the welding was performed by the low-frequency power supply 16 only in the energization pattern in Comparative Example 1, and the welded steel plates were made to undergo heat treatment in an electric furnace. The heat treatment was performed at 300° C. for 30 minutes.
Rise of a first current by first energization: 1 cycle (0.02 sec.)
First energization: 9 kA, 1 cycle (0.02 sec.)
Cooling: 1 cycle (0.02 sec.)
Second energization: 7.2 kA, 14 cycles (0.28 sec.)
Third energization: 3.6 kA, 5 cycles (0.1 sec.)
As shown in
As shown in
The hardness distribution of the spot-welded part 3 in Example 1 and that in Comparative Example 1 are compared as follows. Example 1 does not exhibit an angle such as the one generated in the outermost side of the heat-affected zone 5 in Comparative Example 1, showing generally low hardness. The hardness at the center of the molten and solidified part 4 fell within a range approximately from 530 to 550 HV, which is 85 HV higher than the hardness of the base material of 465 HV.
The spot-welded part 3 in Example 1 exhibited mostly the same hardness distribution as that in Comparative Example 3, where the tempering was performed in the electric furnace as heat treatment after the low-frequency power was applied, although the hardness at the center of the molten and solidified part 4 was slightly lower.
(Observation of the Structure of Cross Section at the Edge of the Nugget)
As shown in
Welded samples in Example 1 and Comparative Examples 2 and 3 were made to undergo the cross tensile test to find their breaking force F (kN).
As shown in
From the result of the above cross tensile test, the strength of the welded sample in Example 1 was found to be high.
The number of samples of welded structural member 1 in Example 1 is five.
When the diameter of the nugget was 6 mm, the breaking force of each welded structural member 1 was 8.39 kN, 8.02 kN, 7.90 kN, 7.26 kN, and 8.64 kN respectively. The average value of breaking force FAV was 8.04 kN, the range R of difference between the maximum and the minimum values of breaking force was 1.38 kN, the standard deviation (σ) was 0.47 kN, and the ratio of average value of breaking force FAV to the diameter of the nugget (FAV/ND) was 1.34 kN/mm. All of the welded structural member samples in Example 1 exhibited plug rupture as shown in
The welding samples in Comparative Example 1 were subjected to the cross tensile test to find their breaking force F (kN). The number of samples in Comparative Example 1 was five.
When the nugget diameter was 6 mm, the breaking force of each welded structural member 1 was 4.6 kN, 4.20 kN, 4.50 kN, 4.59 kN, and 4.36 kN respectively. The average value of breaking force FAV was 4.45 kN, the range R of the difference between the maximum and the minimum values of breaking force was 0.40 kN, the standard deviation (σ) was 0.15 kN, and the ratio of average value of breaking force FAV to the diameter of the nugget (FAV/ND) was 0.74 kN/mm. As shown in
The welding samples in Comparative Example 2 were subjected to the cross tensile test to find their breaking force F (kN). The number of samples in Comparative Example 2 was five.
When the nugget diameter was 6 mm, the breaking force of each welded structural member was 7.00 kN, 6.79 kN, 7.46 kN, 6.96 kN, and 7.59 kN respectively. The average value of breaking force FAV was 7.16 kN, the range R of the difference between the maximum and the minimum values of breaking force was 0.80 kN, the standard deviation (σ) was 0.31 kN, and the ratio of average value of breaking force FAV to the diameter of the nugget (FAV/ND) was 1.21 kN/mm. As shown in
In Comparative Example 2, samples were welded by providing a cooling period between the second and the third energization by the low-frequency power in Comparative Example 1. The above results show that the breaking force F in Comparative Example 2 exhibited improved the breaking force F in the cross tensile test compared to Comparative Example 1. Regarding the breaking mode, the interfacial rupture, which occurred in Comparative Example 1, did not occur but the partial plug rupture occurred. However, the complete plug rupture did not occur unlike Example 1 and Comparative Example 3, which will be described later.
The welding samples in Comparative Example 3 were subjected to the cross tensile test to find their breaking fore F (kN). The number of samples in Comparative Example 3 was five.
When the nugget diameter was 6 mm, the breaking force of each welded structural member was 7.75 kN, 7.60 kN, 7.95 kN, 8.15 kN, and 8.11 kN respectively. The average value of breaking force FAV was 7.91 kN, the range R of the difference between the maximum and the minimum values of breaking force was 0.55 kN, the standard deviation (σ) was 0.21 kN, and the ratio of average value of breaking force FAV to the diameter of the nugget (FAV/ND) was 1.32 kN/mm. As shown in
(Formation of a Small-Diameter Nugget)
In actual spot welding, the diameter of the tip of electrodes 14 decreases due to deformation and wear. As a result, when the current of the same value is fed, the current density of the electrodes 14 gradually changes. Generally, the current density of electrodes 14 tends to decrease, hence the nugget diameter decreases, with the increase in the number of times of welding, namely the number of shots. As described above, the nugget diameter is determined by the current value of the low-frequency second energization. The spot welding was performed by decreasing the current value of the second energization so that the nugget diameter becomes smaller than 6 mm (5.4 mm, 4.9 mm, and 4.4 mm). Other conditions of the spot welding were the same as those in Example 1 and Comparative Examples 1 and 3, where the diameter of the electrodes 14 was 6 mm.
(Formation of a Small-Diameter Nugget in Example 1)
By setting the current value in the second energization to be 6.5 kA, 6.0 kA, and 5.5 kA, the nugget diameter was respectively made to be 5.4 mm, 4.9 mm, and 4.4 mm. The number of cycles in the second energization was 14 cycles. The number of samples of welded structural member 1 was five. These conditions are the same as those in Comparative Examples 1 and 3, which will be described later.
When the nugget diameter was 5.4 mm, the breaking force of each welded structural member 1 was 7.21 kN, 6.82 kN, 7.15 kN, 6.96 kN, and 6.26 kN respectively, the average value of breaking force FAV was 6.88 kN, the range R was 0.95 kN, the standard deviation (σ) was 0.34 kN, and FAV/ND was 1.27 kN/mm.
When the nugget diameter was 4.9 mm, the breaking force of each welded structural member 1 was 5.70 kN, 5.84 kN, 5.87 kN, 5.60 kN, an 5.68 kN respectively, the average value of breaking force FAV was 5.74 kN, the range R was 0.27 kN, the standard deviation (σ) was 0.10 kN, and FAV/ND was 1.17 kN/mm.
When the nugget diameter was 4.4 mm, the breaking force of each welded structural member 1 was 5.99 kN, 6.28 kN, 5.99 kN, 5.59 kN, and 5.55 kN respectively, the average value of breaking force FAV was 5.88 kN, the range R was 0.73 kN, the standard deviation (σ) was 0.27 kN, and FAV/ND was 1.34 kN/mm. Measurement values obtained by these cross tensile tests are summarized in Table 2 together with the case where the nugget diameter was 6 mm.
(Formation of a Small-Diameter Nugget in Comparative Example 1)
By setting the current value of the second energization to be the same as that in Example 1, welded structural members having respective nugget diameter of 5.4 mm, 4.9 mm, and 4.4 mm were produced. The number of welded structural member samples was five.
When the nugget diameter was 5.4 mm, the breaking force of each welded structural member was 3.03 kN, 3.03 kN, 2.89 kN, 3.22 kN, and 3.10 kN respectively, the average value of breaking force FAV was 3.05 kN, the range R was 0.33 kN, the standard deviation (σ) was 0.11 kN, and FAV/ND was 0.57 kN/mm. When the nugget diameter was 4.9 mm, the breaking force of each welded structural member was 2.90 kN, 3.36 kN, 3.44 kN, 3.12 kN, and 3.02 kN respectively, the average value of breaking force FAV was 3.17 kN, the range R was 0.54 kN, the standard deviation (σ) was 0.20 kN, and FAV/ND was 0.65 kN/mm. When the nugget diameter was 4.4 mm, the breaking force of each welded structural member was 2.61 kN, 2.50 kN, 2.23 kN, 2.16 kN, and 2.80 kN respectively, the average value of breaking force FAV was 2.46 kN, the range R was 0.64 kN, the standard deviation (σ) was 0.24 kN, and FAV/ND was 0.56 kN/mm. Measurement values obtained by these cross tensile tests are summarized in Table 3 together with the case where the nugget diameter was 6 mm.
(Formation of a Small-Diameter Nugget in Comparative Example 3)
By setting the current value of the second energization to be the same as that in Example 1, welded structural members having respective nugget diameter of 5.4 mm, 4.9 mm, and 4.4 mm were produced. The number of welded structural member samples was five.
When the nugget diameter was 5.4 mm, the breaking force of each welded structural member was 5.73 kN, 6.39 kN, 7.72 kN, 7.06 kN, and 6.50 kN respectively, the average value of breaking force FAV was 6.68 kN, the range R was 1.99 kN, the standard deviation (σ) was 0.67 kN, and FAV/ND was 1.24 kN/mm. When the nugget diameter was 4.9 mm, the breaking force of each welded structural member 1 was 6.03 kN, 6.62 kN, 6.64 kN, 5.66 kN, and 5.60 kN respectively, the average value of breaking force FAV was 6.11 kN, the range R was 1.04 kN, the standard deviation (σ) was 0.45 kN, and FAV/ND was 1.25 kN/mm. When the nugget diameter was 4.4 mm, the breaking force of each welded structural member 1 was 5.34 kN, 5.91 kN, 5.77 kN, 5.13 kN, and 5.16 kN respectively, the average value of breaking force FAV was 5.46 kN, the range R was 0.78 kN, the standard deviation (σ) was 0.32 kN, and FAV/ND was 1.24 kN/mm. Measurement values obtained by these cross tensile tests are summarized in Table 4 together with the case where the nugget diameter was 6 mm.
The results of the cross tensile test in Example and Comparative Examples to find the breaking force described above show that in welding of two 1.2 mm-thick steel plates, the breaking force of the welded part and breaking mode can be improved by providing a certain cooling period after low-frequency welding, and after the temperature of the whole welded part has decreased to Mf point or lower, allowing the heat of heat storage ring having been generated on the outer periphery of the welded part by high-frequency energization to flow into the welded part, thereby tempering the welded part in the quenched state.
The cooling of welded part depends largely on the heat removal into electrodes 14, and the cooling progresses from the center of the welded part toward the outer periphery. With the electrodes 14 having diameter of 6 mm, the cooling time of 0.7 sec. or longer was found to be necessary for the temperature of the entire welded part to decrease to the Mf point or lower, approximately 300° C.
Then, the spot welding was performed by overlapping three steel plates 2 used in Example 1.
Spot welding of three steel plates 2 was performed in the same manner as Example 1. Energization pattern is shown below.
Rise of a first current by low-frequency first energization: 1 cycle (0.02 sec.)
Low-frequency first energization: 9.0 kA, 1 cycle (0.02 sec.)
Low-frequency cooling: 1 cycle (0.02 sec.)
Low-frequency second energization: 6.5 kA, 14 cycles (0.28 sec.)
Cooling period: 60 cycles (1.2 sec.)
High-frequency energization: 29 kW, 0.6 sec.
Hold time: 1 cycle (0.02 sec.)
As Comparative Example 4 with respect to Example 2, the spot welding of three steel plates 2 was performed in the same manner as Comparative Example 1. The energization pattern is shown below.
Rise of a first current by first energization: 1 cycle (0.02 sec.)
First energization: 9 kA, 1 cycle (0.02 sec.)
Cooling: 1 cycle (0.02 sec.)
Second energization: 6.5 kA, 14 cycles (0.28 sec.)
Third energization: 3.3 kA, 5 cycles (0.1 sec.)
Hold time: 1 cycle (0.2 sec.)
As Comparative Example 5 with respect to Example 2, the spot welding of three steel plates 2 was performed in the same manner as Comparative Example 2. Welding was performed by energization in the energization pattern in Comparative Example 2 by the low-frequency power supply 16 only, and the welded steel plates were subjected to the heat treatment in the electric furnace at 300° C. for 30 minutes.
As shown in
As shown in
The hardness distribution of the spot-welded part 3 in Example 2 and that in Comparative Example 4 are compared. The hardness of Example 2 is found to be lower over the entire positions although there are angles such as those generated on the outermost side of the heat-affected zone in Comparative Example 4. The hardness at the center of the molten and solidified part 4 fell within a range approximately from 520 to 530 HV, which is higher than the hardness of the base material, 465 HV, by approximately 55 to 65 HV.
The hardness distributions of the spot-welded part 3 in Example 2 and that in Comparative Example 5 are compared. The hardness of Example 2 is found to be lower over the entire positions although there are angles such as those generated on the outermost side of the heat-affected zone in Comparative Example 5. The hardness at the center of the molten and solidified part 4 in Example 2 is found to be lower than that of Comparative Example 5 by approximately 10 to 20 HV.
(Observation of the Structure on the Cross Section at the Edge of Nugget)
The welding samples in Example 2 and Comparative Examples 4 and 5 were subjected to a cross tensile test to find their breaking force F (kN). The number of samples of welded structural member 1 in Example 2 was five. Assuming that the nugget diameter was 6 mm, the breaking force of welded structural members 1 in Example 2 was 8.07 kN, 8.54 kN, 8.75 kN, 8.86 kN, and 9.09 kN respectively, the average value of breaking force FAV was 8.66 kN, the range R of difference between the maximum and the minimum values of breaking force was 1.02 kN, standard deviation (σ) was 0.35 kN, and the ratio of average value of breaking force FAV to the diameter of the nugget (FAV/ND) was 1.42 kN/mm. Measurement values obtained by these cross tensile tests are summarized in Table 5.
The welded structural members in Comparative Example 4 were produced by the low-frequency welding, and the number of samples was five.
Assuming that the nugget diameter was 6 mm, the breaking force of welded structural members was 4.53 kN, 5.27 kN, 5.36 kN, 4.9 kN, and 4.99 kN respectively, the average value of breaking force FAV was 5.01 kN, the range R was 0.83 kN, the standard deviation (σ) was 0.29 kN, and FAV/ND was 0.82 kN/mm. The measurement values obtained by these cross tensile tests are summarized in Table 6.
The welded structural members in Comparative Example 5 were produced by performing conventional low-frequency welding in Comparative Example 4, and then performing heat treatment using the electric furnace at 300° C. for 30 minutes. The number of samples was five. When assumed nugget diameter was 6 mm, the breaking force of welded structural members were 8.99 kN, 8.50 kN, 8.58 kN, 9.53 kN, and 8.67 kN respectively, the average value of breaking force FAV was 8.85 kN, the range R was 1.03 kN, the standard deviation (σ) was 0.38 kN, and FAV/ND was 1.45 kN/mm. In Comparative Example 5, the plug rupture occurred to all of the welded structural members as in the case of Example 2. Measurement values obtained by these cross tensile tests are summarized in Table 7.
The results in Example 2 and Comparative Examples 4 and 5 are summarized as follows.
The present invention is not limited to the embodiment described above, and can be modified within the scope of claims of the present invention. It is not without saying that those modifications are included in the scope of the present invention. The cooling time in the embodiment described above can be designed as required so that the predetermined cross rupture strength can be obtained in accordance with the application time of the low-frequency power, and carbon composition and the shape of the steel plates 2.
Number | Date | Country | Kind |
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2013-135642 | Jun 2013 | JP | national |
Filing Document | Filing Date | Country | Kind |
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PCT/JP2014/067243 | 6/27/2014 | WO | 00 |