JPH0819460B2 - Manufacturing method of metal material - Google Patents
Manufacturing method of metal materialInfo
- Publication number
- JPH0819460B2 JPH0819460B2 JP61315319A JP31531986A JPH0819460B2 JP H0819460 B2 JPH0819460 B2 JP H0819460B2 JP 61315319 A JP61315319 A JP 61315319A JP 31531986 A JP31531986 A JP 31531986A JP H0819460 B2 JPH0819460 B2 JP H0819460B2
- Authority
- JP
- Japan
- Prior art keywords
- metal material
- heating
- current value
- current
- temperature
- 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.)
- Expired - Lifetime
Links
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- Powder Metallurgy (AREA)
- Control Of Resistance Heating (AREA)
Description
【発明の詳細な説明】 〔発明の目的〕 (産業上の利用分野) 本発明は金属材を直接通電加熱法により加熱する金属
材の製造方法に関する。DETAILED DESCRIPTION OF THE INVENTION [Object of the Invention] (Field of Industrial Application) The present invention relates to a method for producing a metal material by heating the metal material by a direct current heating method.
(従来の技術) 高融点金属などの金属焼結体の加熱には直接通電加熱
法が用いられている。この直接通電加熱法(直接抵抗加
熱法ともいう。以下、通電加熱法と称する。)は、第3
図で示すように金属材1例えば高融点金属の焼結体の両
端部を夫々電極2,2と把持体3,3とで把持するとともに、
各電極2,2を交流電源Gに接続し、交流電源Gから電極
2,2を介して金属材1の両端部間に直接電流を流して金
属材1に生じる抵抗熱を利用して金属材1自身を加熱す
る方法である。(Prior Art) A direct electric heating method is used for heating a metal sintered body such as a refractory metal. This direct current heating method (also called direct resistance heating method, hereinafter referred to as current heating method) is the third method.
As shown in the figure, while holding both ends of the metal material 1, for example, a sintered body of a high melting point metal by the electrodes 2 and 2 and the gripping bodies 3 and 3, respectively,
Connect each electrode 2, 2 to AC power supply G,
This is a method in which a current is directly applied between both ends of the metal material 1 via 2 and 2 and the resistance heat generated in the metal material 1 is used to heat the metal material 1 itself.
しかして、この通電加熱方法においては金属材を均一
な温度分布で加熱することが要求される。特に厳しい温
度条件(許容温度条件のバラツキが少ないこと)を要求
される金属材に対しては、通電加熱時においては加熱時
間よりも加熱温度の均一性が厳しく要求されている。Therefore, in this electric heating method, it is required to heat the metal material with a uniform temperature distribution. For metal materials that are required to have particularly severe temperature conditions (there is little variation in allowable temperature conditions), the uniformity of the heating temperature is more severely required than the heating time during electric heating.
(発明が解決しようとする問題点) しかして、通電加熱法に於ける金属材の加熱温度と金
属材に流す電流との関係をみると、金属材のもつ抵抗率
と、金属材の断面寸法から金属材に流す電流のそれぞれ
の電流値での材料飽和温度が決定される。従って、加熱
目標温度に対応する標準電流値を設定した電流を流すこ
とにより金属材を所定の加熱目標温度に加熱できる。(Problems to be solved by the invention) Then, looking at the relationship between the heating temperature of the metal material in the electric heating method and the current flowing through the metal material, the resistivity of the metal material and the cross-sectional dimension of the metal material From this, the material saturation temperature at each current value of the current flowing through the metal material is determined. Therefore, the metal material can be heated to a predetermined heating target temperature by passing a current in which a standard current value corresponding to the heating target temperature is set.
そこで、従来通電加熱法において金属材の温度分布の
均一性を優先させる場合には、加熱目標温度に対応した
標準電流値の電流を加熱時間全体にわたって金属材に流
して加熱を行なっている。Therefore, when prioritizing the uniformity of the temperature distribution of the metal material in the conventional energization heating method, heating is performed by flowing a current having a standard current value corresponding to the heating target temperature to the metal material over the entire heating time.
しかし、この場合には次のような問題がある。すなわ
ち、第3図において金属材1の把持体3,3と電極2,2とで
把持された把持部A,Aの内側に隣接した部分B,Bの温度
が、金属材1の他の部分の温度に比して高くなり加熱目
標温度を越えることになる。これは次の理由によるもの
である。把持体3,3と電極2,2は冷却水を通して冷却する
水冷構造となっており、これにより金属材1の把持部A,
Aおよびその隣接部分B,Bが冷却される。しかし、金属材
1の部分B,Bは電極2,2と把持体3,3との接触による接触
抵抗のため冷却効果に勝って温度上昇する。この場合の
金属材1の温度分布は第4図の線図で示している。However, in this case, there are the following problems. That is, in FIG. 3, the temperature of the portions B, B adjacent to the inside of the gripping portions A, A gripped by the gripping bodies 3, 3 of the metal material 1 and the electrodes 2, 2 is different from that of the other portions of the metal material 1. The temperature will be higher than the target temperature and will exceed the heating target temperature. This is due to the following reasons. The grippers 3, 3 and the electrodes 2, 2 have a water-cooling structure in which cooling water is passed through to cool the grippers A,
A and its adjacent portions B and B are cooled. However, the temperature of the portions B, B of the metal material 1 exceeds the cooling effect due to the contact resistance due to the contact between the electrodes 2, 2 and the grippers 3, 3 and rises in temperature. The temperature distribution of the metal material 1 in this case is shown in the diagram of FIG.
これに対処するために、加熱目標温度に対応した標準
電流値より小さな電流値の電流を加熱時間全体にわたり
金属材に流して加熱目標温度まで加熱することが行なわ
れている。この場合には加熱時間が前者の場合に比して
長くなる。In order to deal with this, a current having a current value smaller than the standard current value corresponding to the heating target temperature is flown through the metal material for the entire heating time to heat to the heating target temperature. In this case, the heating time becomes longer than in the former case.
しかし、この場合には金属材1の部分B,Bの温度が中
央部と同様に加熱目標温度になるが、反面次のような問
題が生じる。第5図の金属材1における温度分布を示す
線図で明らかなように金属材1の把持部A,Aの温度が金
属材1の他の部分の温度より低くなり、加熱目標温度を
下回ることになる。これは金属材1の把持部A,Aにおけ
る冷却効果の影響が大きいという理由によるものであ
る。However, in this case, the temperatures of the portions B, B of the metal material 1 reach the heating target temperature as in the central portion, but the following problems occur. As is clear from the diagram showing the temperature distribution in the metal material 1 of FIG. 5, the temperature of the gripping portions A, A of the metal material 1 becomes lower than the temperature of the other parts of the metal material 1 and lower than the heating target temperature. become. This is because the influence of the cooling effect on the grips A, A of the metal material 1 is large.
本発明は前記事情に基づいてなされたもので、金属材
を均一な温度分布で通電加熱することができる金属材の
製造方法を提供することを目的とする。The present invention has been made in view of the above circumstances, and an object of the present invention is to provide a method for producing a metal material, which can electrically heat the metal material with a uniform temperature distribution.
(問題点を解決するための手段と作用) 前記目的を達成するために本発明の金属材の製造方法
は、金属材に直接電流を流してこの金属材に生じる抵抗
熱により金属材自身を加熱するに際して、前記金属材の
加熱目標温度に対応する電流値を標準電流値としたと
き、加熱開始時点から加熱終了時点に近い時点までの間
は、前記標準電流値よりも小さな電流値の電流を流すこ
とにより前記金属材を加熱し、前記加熱終了時点に近い
時点から加熱終了時点までの間は、前記標準電流値以上
の電流値の電流を流すことにより前記金属材を加熱する
ことを特徴とするものである。(Means and Actions for Solving Problems) In order to achieve the above-mentioned object, the method for producing a metal material according to the present invention is such that the metal material itself is heated by the resistance heat generated in the metal material by passing an electric current directly through the metal material. In doing so, when the current value corresponding to the heating target temperature of the metal material is the standard current value, from the heating start time to the time close to the heating end time, a current having a current value smaller than the standard current value is applied. The metal material is heated by flowing, and from the time point close to the heating end time point to the heating end time point, the metal material is heated by flowing a current having a current value equal to or higher than the standard current value. To do.
以下本発明について説明する。 The present invention will be described below.
この説明では、第3図で示すように金属材1として高
融点金属の焼結体を通電加熱する場合を例に取る。第1
図は金属材への通電状態を示す線図、第2図は金属材の
温度分布を示す線図である。In this description, as shown in FIG. 3, the case where a sintered body of a high melting point metal is electrically heated as the metal material 1 is taken as an example. First
The figure is a diagram showing the energized state of the metal material, and FIG. 2 is a diagram showing the temperature distribution of the metal material.
金属材1の通電加熱は、第3図で示すように交流電源
Gから電極2,2を介して金属材1に直接電流を流し、金
属材1に生じる抵抗熱により金属材1自身を加熱する。As shown in FIG. 3, the energization heating of the metal material 1 causes a current to flow directly from the AC power supply G to the metal material 1 via the electrodes 2 and 2, and the metal material 1 itself is heated by the resistance heat generated in the metal material 1. .
まず、第1図で示すように加熱開始時点S1から加熱終
了時点S3に近い時点S2までの間の時間すなわち加熱時間
の大部分は、加熱目標温度Tに対応した標準電流値Iよ
りも小さい電流値I1の電流(小電流)を金属材1に流
す。これにより金属材1は加熱目標温度Tよりも低い温
度T′に加熱される。すなわち、第2図の破線Xで示す
ように金属材1の中央部および把持部A,Aに隣接する部
分B,Bは揃って温度T′まで温度上昇し、これらを結ぶ
部分は温度分布が均一となる。但し、金属材1の把持部
A,Aは温度T′により低い温度までしか温度上昇しな
い。First, as shown in FIG. 1, the time from the heating start time S1 to the time S2 close to the heating end time S3, that is, most of the heating time, is a current smaller than the standard current value I corresponding to the heating target temperature T. A current of a value I1 (small current) is passed through the metal material 1. As a result, the metal material 1 is heated to a temperature T'which is lower than the heating target temperature T. That is, as shown by the broken line X in FIG. 2, the central portion of the metal material 1 and the portions B, B adjacent to the gripping portions A, A are uniformly heated to the temperature T ', and the portion connecting these portions has a temperature distribution. Be uniform. However, the grip of the metal material 1
The temperatures A and A rise only to a lower temperature due to the temperature T '.
金属材1の加熱時間が前記時点S2まで経過した後に前
記時点S2から加熱終了時点S3までの間の時間は、加熱目
標温度Tに対応した標準電流値Iより大きい電流値I2を
持つ電流(大電流)を金属材1に流す。これにより金属
材1は加熱目標温度Tに加熱される。すなわち、第2図
の実線Yで示すように金属材1の中央部および把持部A,
Aに隣接する部分B,Bが加熱目標温度Tまで温度上昇す
る。また、金属材1の把持部A,Aも加熱されて加熱目標
温度Tまで温度上昇する。なお、標準電流値Iより大き
い電流値I2を流す時間が短いので、金属材1の部分B,B
は加熱目標温度T以上に温度上昇しない。After the heating time of the metal material 1 elapses up to the time point S2, the time from the time point S2 to the heating end time point S3 is a current having a current value I2 larger than the standard current value I corresponding to the heating target temperature T (large Current) to the metal material 1. As a result, the metal material 1 is heated to the heating target temperature T. That is, as shown by the solid line Y in FIG.
The temperature of the portions B, B adjacent to A rises to the heating target temperature T. Further, the grips A, A of the metal material 1 are also heated and the temperature rises to the heating target temperature T. Since the time for which the current value I2 is larger than the standard current value I is short, the parts B, B of the metal material 1
Does not rise above the heating target temperature T.
このようにして金属材1は全体にわたり均一な温度分
布で加熱目標温度Tに通電加熱される。従って、金属材
1は通電加熱の後の加工例えば熱間圧延加工において厳
しい温度条件が要求される場合であっても良好に加工を
行なう事ができる。In this way, the metal material 1 is electrically heated to the heating target temperature T with a uniform temperature distribution throughout. Therefore, the metal material 1 can be satisfactorily processed even when severe temperature conditions are required in the processing after the electric heating, for example, hot rolling.
なお、前記時点S2から加熱終了時点S3までの間に流す
電流は標準電流値Iのものであってもよい。The current flowing from the time point S2 to the heating end time point S3 may have the standard current value I.
(実施例) 直径13mm、長さ700mmのタングステン焼結体を直接通
電加熱法により加熱した。加熱目標温度は1400℃、焼結
体に流す電流の標準電流値は2600Aである。(Example) A tungsten sintered body having a diameter of 13 mm and a length of 700 mm was heated by a direct current heating method. The heating target temperature is 1400 ° C, and the standard current value of the current flowing through the sintered body is 2600A.
本発明例として、電流値を2400A、3500Aの2段階に分
けて電流を焼結体に流した。この結果、焼結体の全体を
1400℃の均一な温度分布で加熱できた。As an example of the present invention, a current value was divided into two stages of 2400A and 3500A and a current was passed through the sintered body. As a result, the entire sintered body
It was possible to heat with a uniform temperature distribution of 1400 ° C.
従来例として、電流値2400Aの電流のみを焼結体に流
した。この結果焼結体の温度分布は、把持部A,Aが480
℃、他の部分が1400℃で、把持部の温度の低下を生じ
た。As a conventional example, only a current having a current value of 2400 A was passed through the sintered body. As a result, the temperature distribution of the sintered body is 480 for the grips A and A.
℃, 1400 ℃ in other parts, the temperature of the grip part decreased.
以上説明したように本発明の金属材の製造方法によれ
ば、小電流と大電流を組合わせた2段階の通電を行なう
直接通電加熱法により、金属材全体を均一な温度分布で
通電加熱することができ、加工において厳しい温度条件
を要求される金属材の通電加熱に最適である。As described above, according to the method for manufacturing a metal material of the present invention, the whole metal material is electrically heated with a uniform temperature distribution by the direct current heating method in which a small current and a large current are combined to perform two-step current application. It is suitable for electric heating of metal materials that require severe temperature conditions during processing.
第1図および第2図は本発明方法を示し、第1図は金属
材に対する通電状態を示す線図、第2図は金属材の加熱
温度分布を示す線図、第3図は直接通電加熱法を示す線
図、第4図および第5図は従来における金属材の加熱温
度分布を示す線図である。 1……焼結体、2……電極、3……把持体。FIGS. 1 and 2 show the method of the present invention, FIG. 1 is a diagram showing the energized state of a metal material, FIG. 2 is a diagram showing the heating temperature distribution of the metal material, and FIG. 4 and 5 are diagrams showing a heating temperature distribution of a conventional metal material. 1 ... Sintered body, 2 ... Electrode, 3 ... Gripping body.
Claims (2)
じる抵抗熱により金属材自身を加熱するに際して、前記
金属材の加熱目標温度に対応する電流値を標準電流値と
したとき、加熱開始時点から加熱終了時点に近い時点ま
での間は、前記標準電流値よりも小さな電流値の電流を
流すことにより前記金属材を加熱し、前記加熱終了時点
に近い時点から加熱終了時点までの間は、前記標準電流
値以上の電流値の電流を流すことにより前記金属材を加
熱することを特徴とする金属材の製造方法。1. When heating a metal material itself by resistance heat generated in the metal material by passing an electric current directly through the metal material, when the current value corresponding to the heating target temperature of the metal material is set to a standard current value, heating is performed. From the start time to the time close to the heating end time, the metal material is heated by passing a current having a current value smaller than the standard current value, and from the time close to the heating end time to the heating end time. Is a method for manufacturing a metal material, wherein the metal material is heated by passing a current having a current value equal to or higher than the standard current value.
までの間は、前記標準電流値を超える電流値の電流を流
すことを特徴とする特許請求の範囲第1項に記載の金属
材の製造方法。2. The metal material according to claim 1, wherein a current having a current value exceeding the standard current value is passed from a time point close to a heating end time point to a heating end time point. Production method.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61315319A JPH0819460B2 (en) | 1986-12-26 | 1986-12-26 | Manufacturing method of metal material |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61315319A JPH0819460B2 (en) | 1986-12-26 | 1986-12-26 | Manufacturing method of metal material |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS63166926A JPS63166926A (en) | 1988-07-11 |
| JPH0819460B2 true JPH0819460B2 (en) | 1996-02-28 |
Family
ID=18063970
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP61315319A Expired - Lifetime JPH0819460B2 (en) | 1986-12-26 | 1986-12-26 | Manufacturing method of metal material |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0819460B2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US8653399B2 (en) | 2008-01-29 | 2014-02-18 | Honda Motor Co., Ltd | Steel sheet heat treatment/stamp system and method |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5525713A (en) * | 1978-08-11 | 1980-02-23 | Doryokuro Kakunenryo | Rotary heat treatment apparatus |
| JPS5629352A (en) * | 1979-08-17 | 1981-03-24 | Nec Corp | Resin-sealed semiconductor device |
-
1986
- 1986-12-26 JP JP61315319A patent/JPH0819460B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS63166926A (en) | 1988-07-11 |
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