JPH04105721A - Press forming method for metallic sheet - Google Patents

Press forming method for metallic sheet

Info

Publication number
JPH04105721A
JPH04105721A JP2221500A JP22150090A JPH04105721A JP H04105721 A JPH04105721 A JP H04105721A JP 2221500 A JP2221500 A JP 2221500A JP 22150090 A JP22150090 A JP 22150090A JP H04105721 A JPH04105721 A JP H04105721A
Authority
JP
Japan
Prior art keywords
bead
blank
flange
plate
press forming
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP2221500A
Other languages
Japanese (ja)
Inventor
Jiro Iwatani
二郎 岩谷
Kenichi Watanabe
憲一 渡辺
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Kobe Steel Ltd
Original Assignee
Kobe Steel Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Kobe Steel Ltd filed Critical Kobe Steel Ltd
Priority to JP2221500A priority Critical patent/JPH04105721A/en
Publication of JPH04105721A publication Critical patent/JPH04105721A/en
Pending legal-status Critical Current

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  • Arc Welding In General (AREA)
  • Welding Or Cutting Using Electron Beams (AREA)
  • Shaping Metal By Deep-Drawing, Or The Like (AREA)
  • Laser Beam Processing (AREA)

Abstract

PURPOSE:To control the material flow with a simple means by radiating the high energy-beam preliminarily to the part where the blank material is pressed with the blank holder and the dies. CONSTITUTION:The melting bead 2 is formed by radiating the high energy beam 6 in the direction orthogonal to the flowing direction of the material followed with the shrink flange deforming or the flange deforming. The reason for the irradiation is that the welding bead 2 formed in this manner can exhibit the most effective resisting force against the shrink flange deforming or the stretch flange deforming. Accordingly, it is not required to use the drawing bead, to increase the pressure at the time of blank holding or to use the complicate blank shape, etc., and as the material control can be executed, so it is extremly effective for the ununiform flowing state of the material or the generation of wrinkles, etc.

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は金属板を金型を用いて所定の形状にプレス成形
する方法に関するものである。
DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to a method of press-molding a metal plate into a predetermined shape using a mold.

(従来の技術) 金属板を素材として、これをプレス成形して各種形状の
製品を得る場合、成形後のフランジ形状は、成形前の素
板の形状と異なることが知られている。これは、材料の
面内異方性にも起因するが、成形条件面からは、ダイス
型半径やコーナー半径の大きな部位や、成形高さが部分
的に高い部位では、材料のダイス内への流入が多くなり
、フランジ残存量が少な目となり、一方、特にそうでな
い部位ではフランジ残存量が多めとなるためである。
(Prior Art) It is known that when a metal plate is used as a raw material and press-molded to obtain products of various shapes, the shape of the flange after forming is different from the shape of the blank before forming. This is due to the in-plane anisotropy of the material, but from the perspective of the molding conditions, in areas with large die radii and corner radii, or areas where the molding height is partially high, the material may not enter the die. This is because the amount of inflow increases and the remaining amount of the flange becomes small, while the remaining amount of the flange becomes large especially in other parts.

また、上述の材料流入量の部分的な違いから、特に成形
高さが部分的に異なる成形品においては“しわ”が発生
したりする。
Further, due to the above-mentioned local differences in the amount of material inflow, "wrinkles" may occur, especially in molded products whose molding heights differ locally.

更に、成形後に成形品を金型から取り出すと、成形品が
金型の形状寸法と異なる形状に変形する、いわゆる弾性
回復減少による変形が生じて、成形品に形状不良が発生
することもよく知られている。
Furthermore, it is well known that when the molded product is removed from the mold after molding, the molded product deforms into a shape that differs from the shape and dimensions of the mold, resulting in deformation due to so-called reduced elastic recovery, resulting in shape defects in the molded product. It is being

この原因の一つとして、材料流入が容易なために成形品
に充分な引張り伸び歪を与えられないことが考えられる
One possible reason for this is that sufficient tensile elongation strain cannot be applied to the molded product because the material flows easily.

これらの不良現象を防止するために、従来、フランジが
流入し易い部位の金型に、絞リピートを設けて材料の流
入を制御し、材料が流入し易い部位とのバランスを取っ
たり、或いは予め材料が流入し易い部位の素板を太き目
にしておき、成形後に材料が流入しにくい部位とフラン
ジ残存量が同一になるようにすることが行われている。
In order to prevent these defective phenomena, conventionally, the flow of material is controlled by installing a throttling repeat in the part of the mold where the flange tends to flow, and the flow of material is balanced with the part where the material easily flows, or The base plate is made thicker in areas where material easily flows in, so that after molding, the remaining amount of the flange is the same as that in areas where material does not easily flow.

また、寸法精度の観点から、成形品に引張り伸び歪を与
える方法としては、前述の絞リピート形状に替え、固定
ビードとして材料の流入を防止したり、しわ押え時の圧
力を高くして材料の流入を防止又は規制したりする方法
が採られている。
In addition, from the perspective of dimensional accuracy, methods for applying tensile elongation strain to molded products include replacing the aforementioned drawing repeat shape with a fixed bead to prevent the material from flowing in, or increasing the pressure when pressing the wrinkles to strengthen the material. Measures are being taken to prevent or restrict the influx.

(発明が解決しようとする課題) しかしながら、上述のプレス成形時の材料流入制御に関
する従来法では以下の問題点が指摘されている。
(Problems to be Solved by the Invention) However, the following problems have been pointed out in the conventional method for controlling material inflow during press forming described above.

■前述の絞リピートにより材料の流入を制御する方法で
は、最適なビード通過抵抗力を発生するビード形状を得
るために、繰り返し金型修正を行う必要があり、このた
め多大なコストと時間を必要とする。また、絞リピート
部で金属板が非常に厳しい曲げ戻し変形を受けるため、
ビード通過後の材質劣化による割れの発生や、金型の摩
耗、型かじりの問題、メツキ材を用いた場合のメツキの
剥離の問題が生じる。
■The aforementioned method of controlling the inflow of material through repeated squeezing requires repeated mold modifications in order to obtain a bead shape that generates the optimal bead passage resistance force, which requires a large amount of cost and time. shall be. In addition, since the metal plate undergoes extremely severe bending deformation at the drawing repeat section,
Cracks occur due to material deterioration after passing through the bead, mold wear, mold galling problems, and plating peeling when plating materials are used.

■プレス成形終了時に、成形品のフランジ残存量を同一
にするために、素板の形状を材料流入量に応じて変更す
る方法では、多くの場合、複雑な素板形状を必要とする
ため、材料の歩留低下や、素板打ち抜き型のコスト上昇
の問題が生じる。
■The method of changing the shape of the blank plate according to the amount of material inflow in order to make the remaining amount of flange of the molded product the same at the end of press forming often requires a complicated blank shape. Problems arise such as a decrease in material yield and an increase in the cost of the die for blank punching.

本発明は、上記従来技術の問題点を解決するためになさ
れたものであって、金属板を金型を用いて所定形状の成
形品にプレス成形するに当り、簡易な手段によって材料
流入制御を可能にする方法を提供することを目的とする
ものである。
The present invention has been made in order to solve the above-mentioned problems of the prior art, and it is possible to control material inflow by simple means when press-forming a metal plate into a molded product of a predetermined shape using a mold. The purpose is to provide a method that makes it possible.

(課題を解決するための手段) 前記課題を解決するため、本発明者らは鋭意研究を重ね
た結果、成形前の素板のフランジ部(しわ押え板とダイ
スとによって押えられる部位)に、予め高エネルギービ
ームを照射することにより。
(Means for Solving the Problems) In order to solve the above problems, the present inventors have conducted intensive research and found that the flange portion (the portion pressed by the wrinkle presser plate and the die) of the raw plate before forming, By pre-irradiating with a high-energy beam.

溶接ビードを成形させ、その領域の硬度上昇による変形
抵抗の増加を利用して、成形中に材料の流入を制御する
方法を見い出したものである。
We have discovered a method to control the inflow of material during forming by forming a weld bead and taking advantage of the increased deformation resistance due to increased hardness in that area.

以下に本発明を更に詳細に説明する。The present invention will be explained in more detail below.

(作用) 素板のフランジ部かしわ押え板とダイスとによって押え
られるタイプのプレス成形で成形される金属板は、成形
中に材料流入方向に直角方向に縮みながら流入する縮み
フランジ変形、又は、直角方向に伸びながら流入する伸
びフランジ変形を伴いながら、流入していく場合が多い
(Function) A metal plate formed by a type of press forming in which the flange part of a blank plate is pressed by a presser plate and a die is subject to shrinkage flange deformation in which the material flows in while shrinking in a direction perpendicular to the material inflow direction during forming, or a right angle In many cases, the fluid flows in while being accompanied by stretch flange deformation in which the fluid flows in while stretching in the direction.

本発明は、このような縮みフランジ変形又は伸びフラン
ジ変形を伴いながら、ダイス穴内に流入するフランジ部
のうち、従来、絞リピートを用いて流入を抑制したり或
いは素板の形状を変更してフランジ残存量を調整してい
た領域に対し、高エネルギービームを照射するものであ
り、これにより、その領域の急熱急冷作用に起因する硬
度上昇による変形抵抗の増加を利用することによって、
材料流入制御を行うのである。
The present invention aims at reducing the flange portion of the flange that flows into the die hole with such shrinkage flange deformation or expansion flange deformation, by suppressing the inflow using conventional drawing repeats or by changing the shape of the blank plate. A high-energy beam is irradiated to the area where the residual amount was being adjusted, and by utilizing the increase in deformation resistance due to the increase in hardness caused by the rapid heating and cooling of that area,
It controls the inflow of materials.

具体的には、縮みフランジ変形又は伸びフランジ変形を
伴った材料流入方向に直角方向に溶融ビードを設ける。
Specifically, a molten bead is provided in a direction perpendicular to the material inflow direction with contraction flange deformation or stretch flange deformation.

ここで、溶融ビードの形成方法は材料流入方向に直角方
向とするのが好ましい。これは、そのような溶接ビード
は縮みフランジ変形又は伸びフランジ変形に対して最も
抵抗力を発揮することが可能となるためである。
Here, it is preferable that the molten bead is formed in a direction perpendicular to the material inflow direction. This is because such a weld bead can exhibit the greatest resistance to shrinkage flange deformation or stretch flange deformation.

更に、直角方向に溶融ビードを形成する態様としては、
例えば、素板が円形である場合には、円周方向の全部又
は一部に形成し、素板が矩形である場合には、コーナ一
部の近傍の直辺部に所定寸法で形成する。
Furthermore, as a mode of forming a molten bead in a right angle direction,
For example, if the blank is circular, it is formed on all or part of the circumference, and when the blank is rectangular, it is formed with a predetermined dimension on the right side near a part of the corner.

また、第1図に示すように、これら高エネルギービーム
■の照射による溶融ビード■は、必要に応じ任意の幅、
本数で良い。
Furthermore, as shown in Fig. 1, the molten bead (■) produced by irradiation with these high-energy beams (■) can be formed into any width or shape as needed.
The number is fine.

溶融ビード部の深さとしては、大別して、表面のみを溶
融する場合と、実質的に板厚に相当する深さに溶融する
場合があるが、溶融ビードによる変形抵抗を利用するこ
とを考えると、板厚に相当する深さに溶融することが最
も効果的であり、好ましい。後者(溶接ビード)の場合
、溶融ビード部の板厚増加は、フランジしわの発生防止
のため、ε、=5%以下とするのが望ましい。なお、ε
、は以下の式で定義される。
The depth of the molten bead can be roughly divided into cases where only the surface is melted and cases where it is melted to a depth substantially equivalent to the plate thickness, but considering that the deformation resistance by the molten bead is used. , melting to a depth corresponding to the plate thickness is most effective and preferred. In the case of the latter (welded bead), it is desirable that the increase in plate thickness at the molten bead portion be ε = 5% or less in order to prevent the occurrence of flange wrinkles. In addition, ε
, is defined by the following formula.

t’−t ε□= −X 10 Q (%) なお、本発明において、高エネルギービームを使用した
理由は、高エネルギーを局所に集中させることにより、
金属板母材への熱影響による熱歪みの増加を抑止できる
ためである。ここで、高エネルギービームとは、レーザ
ビーム、電子ビーム、プラズマビーム等の被照射体に熱
を付与するエネルギービームを云う。
t'-t ε□= -X 10 Q (%) In the present invention, the reason for using a high-energy beam is that by concentrating high energy locally,
This is because it is possible to suppress an increase in thermal strain due to thermal influence on the metal plate base material. Here, the high-energy beam refers to an energy beam that imparts heat to an irradiated object, such as a laser beam, electron beam, or plasma beam.

勿論、他のプレス成形条件は特に制限がない。Of course, other press molding conditions are not particularly limited.

また、本発明を適用する金属板としては、冷間及び熱間
圧延鋼板、メツキを施した表面処理鋼板などの鋼板のみ
ならず、チタン、アルミ、銅等の非鉄金属の板状のもの
も可能である。
In addition, the metal plates to which the present invention can be applied include not only steel plates such as cold- and hot-rolled steel plates and plated surface-treated steel plates, but also plate-shaped plates of non-ferrous metals such as titanium, aluminum, and copper. It is.

(実施例) 以下に本発明の実施例を示す。(Example) Examples of the present invention are shown below.

失亀貫よ 本例は、第2図に示すように円筒深絞り成形に適用した
例であり、第3図は成形前の素板のレーザー照射パター
ンを示したものである。
This example is applied to cylindrical deep drawing as shown in Fig. 2, and Fig. 3 shows the laser irradiation pattern of the raw plate before forming.

第2図及び第3図において、■は鋼板(供試材)、■は
この鋼板にレーザービームを照射することにより形成さ
れる溶融ビード、■はポンチ、■はダイス、■はしわ押
えを示す。
In Figures 2 and 3, ■ indicates a steel plate (sample material), ■ indicates a molten bead formed by irradiating this steel plate with a laser beam, ■ indicates a punch, ■ indicates a die, and ■ indicates a wrinkle presser. .

まず、供試材として、厚さ0.7■m、直径10Qmm
で引張強度30キロ級の冷延鋼板を準備した。
First, as a test material, the thickness is 0.7μm and the diameter is 10Qmm.
A cold-rolled steel plate with a tensile strength of 30 kg was prepared.

このような冷延鋼板の場合、r値は圧延方向に対し0°
、900方向で高く、45’方向で低くなる場合が多く
、これを円筒深絞り成形した場合、r値が低い方向が速
く材料流入してしまい、結果的にr値の高いO’、90
’方向が“耳″として残り、歩留を低下させることは良
く知られていることである。
In the case of such cold-rolled steel sheets, the r value is 0° with respect to the rolling direction.
, is often high in the 900 direction and low in the 45' direction, and when this is cylindrical deep drawing, the material flows in faster in the direction with a low r value, resulting in a high r value of O', 90
It is well known that the 'direction' remains as an 'ear' and reduces yield.

そこで、第3図に示すように、θ=45”方向のフラン
ジ部に円周方向にレーザービームを照射して溶融ビード
を第1図に示す要領にて形成した。
Therefore, as shown in FIG. 3, a laser beam was irradiated circumferentially on the flange portion in the θ=45'' direction to form a molten bead in the manner shown in FIG.

溶融ビードの長さは中心からの角度θで表わす。The length of the molten bead is expressed as the angle θ from the center.

ここで、円周方向にビードを形成した理由は、成形中の
フランジ部での縮みフランジ変形に対して最も効果的に
抵抗力を与えるためである。
Here, the reason why the beads are formed in the circumferential direction is to most effectively provide resistance against shrinkage flange deformation at the flange portion during molding.

このようにして、フランジ部にレーザービームの照射に
より溶融ビードを形成した素板と、従来のレーザービー
ム照射なし素板とを用いてプレス成形を行った。
In this way, press molding was performed using a blank plate whose flange portion had a molten bead formed by laser beam irradiation and a conventional blank plate that was not irradiated with a laser beam.

第4図は成形品においてθ=60’の場合の成形高さと
、成形中のフランジ部の最大外径と最小外径の差(ΔD
)との関係を示したものである。ここで、ΔDは耳”の
大きさを表わす指標であり、図中の0印のプロットはθ
=60°の場合(本発明例)、・印のプロットはレーザ
ーを照射しない場合(従来例)を表わす。
Figure 4 shows the molding height when θ = 60' and the difference between the maximum and minimum outer diameters of the flange during molding (ΔD
). Here, ΔD is an index representing the size of the ear, and the plot marked with 0 in the figure is θ
= 60° (example of the present invention), plots marked with * represent the case where no laser is irradiated (example of the prior art).

第4図より、比較例のレーザービーム照射しない材料は
、成形が進行すると共にΔDが増加し、耳が発生してい
るのに対し、本発明例のレーザービーム照射した材料は
、ΔDの増加が僅かであって“耳”の発生がないことが
わかる。これは、溶融ビードによる変形抵抗のため、4
5°方向の材料の流入が抑制され、成形が進行しても均
一に材料が流入していくためである。
From FIG. 4, it can be seen that in the material of the comparative example that was not irradiated with the laser beam, ΔD increased as molding progressed and ears were generated, whereas in the material that was irradiated with the laser beam of the inventive example, the ΔD increased. It can be seen that there is no occurrence of "ears", which are slight. This is due to the deformation resistance caused by the molten bead.
This is because the inflow of material in the 5° direction is suppressed, and even as the molding progresses, the material flows in uniformly.

第5図は、本発明例において溶融ビードの長さを表わす
θとΔDとの関係を成形高さ25mmの場合について示
したものである。
FIG. 5 shows the relationship between θ, which represents the length of the molten bead, and ΔD in the case of a molding height of 25 mm in an example of the present invention.

第5図より、ΔDはθ=50°〜70@の範囲で良好な
値を示していることがわかる。
From FIG. 5, it can be seen that ΔD shows a good value in the range of θ=50° to 70°.

失胤孤ス 本例は、プレス成形に際して、しわの問題の起こり易い
大曲面パネルに適用した例である。
This example is an example in which the present invention is applied to a large curved panel that is prone to wrinkles during press molding.

このような形状の素板をプレス成形する場合、コーナ一
部周辺では、コーナーR部より直辺部の方が流入し易い
ために、ボディしわと呼ばれるしわ■が発生する。第6
図は成形された大曲面パネルを示す斜視図であり、素板
には板厚Q、7+am、70 C)amX 700mm
の引張強度30キロ級の冷延鋼板を用いた。
When a blank plate having such a shape is press-molded, wrinkles (2) called body wrinkles occur around a part of the corner because it is easier to flow into the right side part than the corner R part. 6th
The figure is a perspective view showing a molded large curved panel, and the base plate has a board thickness of Q, 7+am, 70 C) am
A cold-rolled steel plate with a tensile strength of 30 kg was used.

これを抑制するために、第7図に示す位置■にレーザー
ビームを第1図に示す要領で照射し、溶融ビード■を形
成し、実施例1と同様にプレス成形を行った。
In order to suppress this, a laser beam was irradiated to the position (2) shown in FIG. 7 in the manner shown in FIG. 1 to form a molten bead (2), and press molding was performed in the same manner as in Example 1.

得られた大曲面パネルについて、コーナ一部に発生する
しわの高さ(H)を調べた。
The height (H) of wrinkles generated at some corners of the obtained large curved panel was examined.

第8図は上記の調査結果に基づき、形成された溶融ビー
ドの長さCQ/R)としわの高さ(H)の関係を示した
図であって、図中のプロット0、・。
FIG. 8 is a diagram showing the relationship between the length (CQ/R) of the formed molten bead and the wrinkle height (H) based on the above investigation results, and plots 0 and . in the diagram.

0印は、それぞれ溶融ビードを1本、2本、3本形成し
た場合の結果を示している。ここで、Q/Rで評価した
理由は、一般にコーナーRが小さくなる程しわが大きく
なるため、これを抑制するビードも長いものが必要とな
るためである。
The 0 mark indicates the results when one, two, and three molten beads were formed, respectively. Here, the reason why the Q/R was evaluated is that, in general, the smaller the corner R, the larger the wrinkles, so a long bead is required to suppress this.

第8図に示すように、これらの溶融ビードはしわの発生
に対して非常に効果的であることが明らかである。これ
は、溶融ビードの抵抗により、コーナ一部での材料流入
が抑制され、この部分での材料流入状態が改善されたた
めである。
As shown in Figure 8, it is clear that these fused beads are very effective against wrinkle formation. This is because the resistance of the molten bead suppressed the flow of material in a portion of the corner, and the state of material flow in this portion was improved.

(発明の効果) 以上詳述したように、本発明によれば、金属板のプレス
成形において、従来のように絞りビードを用いたり、し
わ押え時の圧力を高めたり、或いは複雑な素板形状を用
いる等々の必要なく、材料流入制御を行うことが可能で
あるので、材料の不均一な流入状態やしわの発生等に対
して極めて効果的である。しかも、素材である金属板の
種類、形状等々、材料特性面に制約されることな〈実施
可能であり、手段も簡易であるので、実用上の効果は顕
著である。
(Effects of the Invention) As described in detail above, according to the present invention, in press forming of a metal plate, it is possible to use a drawing bead as in the past, increase the pressure when pressing wrinkles, or to form a blank sheet with a complicated shape. Since it is possible to control the material inflow without the need to use a holder, etc., it is extremely effective against uneven material inflow conditions and the occurrence of wrinkles. In addition, it is possible to implement the method without being restricted by material properties such as the type and shape of the metal plate used as the raw material, and the means are simple, so the practical effects are significant.

【図面の簡単な説明】[Brief explanation of drawings]

第1図は本発明で利用する高エネルギービームの照射要
領と形成される溶融ビードを示す模式図、第2図は実施
例1の円筒深絞り成形方法の概念を説明する断面図、 第3図は実施例1のレーザービーム照射パターンを説明
する図、 第4図は実施例1におけるプレス成形中のフランジ部の
最大外径と最小外径の差(ΔD)と成形高さの関係を示
す図、 第5図は実施例1における溶融ビードの長さ(θ)とΔ
Dの関係を示す図、 第6図は実施例2で本発明を適用する大曲面パネルを示
す斜視図、 第7図は実施例2のレーザー照射パターンを説明する図
、 第8図は実施例2の溶融ビードの長さ(Q/R)としわ
高さ(H)の関係を示す図である。 ■・・・供試材、■・・・溶融ビード、■・・・ポンチ
、■・・・ダイス、■・・・しわ抑え、■・・・高エネ
ルギービーム、■・・・しわ。 第1図 特許出願人  株式会社神戸製鋼所 代理人弁理士 中  村   尚 第2図 第 図 第 図 へ刑1]τ(紙−) 第 図 シ勢&狐L・−ド−&J θ(°)
Fig. 1 is a schematic diagram showing the irradiation method of the high-energy beam used in the present invention and the molten bead formed, Fig. 2 is a cross-sectional view explaining the concept of the cylindrical deep drawing method of Example 1, Fig. 3 Figure 4 is a diagram explaining the laser beam irradiation pattern of Example 1, and Figure 4 is a diagram showing the relationship between the difference (ΔD) between the maximum and minimum outer diameters of the flange part during press forming in Example 1 and the molding height. , Figure 5 shows the length (θ) and Δ of the molten bead in Example 1.
FIG. 6 is a perspective view showing a large curved panel to which the present invention is applied in Example 2. FIG. 7 is a diagram explaining the laser irradiation pattern in Example 2. FIG. 8 is an example 2 is a diagram showing the relationship between the length (Q/R) and the wrinkle height (H) of the molten bead of No. 2. FIG. ■... Test material, ■... Molten bead, ■... Punch, ■... Dice, ■... Wrinkle suppression, ■... High energy beam, ■... Wrinkle. Figure 1 Patent Applicant Kobe Steel Co., Ltd. Patent Attorney Takashi Nakamura Figure 2 Figure Figure 1] τ (Paper-) Figure Sise & Fox L.-Do & J θ (°)

Claims (1)

【特許請求の範囲】[Claims] 金属板を金型を用いて所定形状の成形品とするプレス成
形方法において、素板がしわ押え板とダイスとによって
押えられる部位に、予め高エネルギービームを照射する
ことを特徴とするプレス成形時の材料流入制御方法。
In a press forming method in which a metal plate is molded into a predetermined shape using a mold, the press forming process is characterized in that a high-energy beam is irradiated in advance to the area where the blank plate is pressed by a wrinkle holding plate and a die. material inflow control method.
JP2221500A 1990-08-23 1990-08-23 Press forming method for metallic sheet Pending JPH04105721A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2221500A JPH04105721A (en) 1990-08-23 1990-08-23 Press forming method for metallic sheet

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2221500A JPH04105721A (en) 1990-08-23 1990-08-23 Press forming method for metallic sheet

Publications (1)

Publication Number Publication Date
JPH04105721A true JPH04105721A (en) 1992-04-07

Family

ID=16767685

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2221500A Pending JPH04105721A (en) 1990-08-23 1990-08-23 Press forming method for metallic sheet

Country Status (1)

Country Link
JP (1) JPH04105721A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0700735A2 (en) 1994-08-29 1996-03-13 Toyota Jidosha Kabushiki Kaisha Press working method including step of strengthening local portion of blank
EP1002594A2 (en) * 1998-11-19 2000-05-24 Schuler Pressen GmbH & Co. KG Method and device for forming a workpiece
JP2018051593A (en) * 2016-09-29 2018-04-05 本田技研工業株式会社 Press molding apparatus
WO2020121591A1 (en) * 2018-12-12 2020-06-18 Jfeスチール株式会社 Press forming method

Cited By (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0700735A2 (en) 1994-08-29 1996-03-13 Toyota Jidosha Kabushiki Kaisha Press working method including step of strengthening local portion of blank
EP0700735A3 (en) * 1994-08-29 1996-05-15 Toyota Motor Co Ltd Press working method including step of strengthening local portion of blank
US5735163A (en) * 1994-08-29 1998-04-07 Toyota Jidosha Kabushiki Kaisha Press working method including step of strengthening local portion of blank
EP1002594A2 (en) * 1998-11-19 2000-05-24 Schuler Pressen GmbH & Co. KG Method and device for forming a workpiece
EP1002594A3 (en) * 1998-11-19 2001-03-28 Schuler Pressen GmbH & Co. KG Method and device for forming a workpiece
US6775888B1 (en) 1998-11-19 2004-08-17 Schuler Pressen Gmbh & Co. Kg Forming system and process
JP2018051593A (en) * 2016-09-29 2018-04-05 本田技研工業株式会社 Press molding apparatus
WO2020121591A1 (en) * 2018-12-12 2020-06-18 Jfeスチール株式会社 Press forming method
JP2020093276A (en) * 2018-12-12 2020-06-18 Jfeスチール株式会社 Press molding method
CN113226584A (en) * 2018-12-12 2021-08-06 杰富意钢铁株式会社 Press forming method
CN113226584B (en) * 2018-12-12 2022-11-15 杰富意钢铁株式会社 Press forming method

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