JPH0416259B2 - - Google Patents
Info
- Publication number
- JPH0416259B2 JPH0416259B2 JP10232584A JP10232584A JPH0416259B2 JP H0416259 B2 JPH0416259 B2 JP H0416259B2 JP 10232584 A JP10232584 A JP 10232584A JP 10232584 A JP10232584 A JP 10232584A JP H0416259 B2 JPH0416259 B2 JP H0416259B2
- Authority
- JP
- Japan
- Prior art keywords
- image
- casting
- melting
- detector
- brightness
- 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
Links
- 239000000463 material Substances 0.000 claims description 49
- 238000005266 casting Methods 0.000 claims description 47
- 238000009826 distribution Methods 0.000 claims description 37
- 238000010438 heat treatment Methods 0.000 claims description 32
- 238000002844 melting Methods 0.000 claims description 25
- 230000008018 melting Effects 0.000 claims description 25
- 238000000034 method Methods 0.000 claims description 25
- 238000005495 investment casting Methods 0.000 claims description 13
- 239000002184 metal Substances 0.000 claims description 8
- 229910052751 metal Inorganic materials 0.000 claims description 8
- 230000006698 induction Effects 0.000 claims description 4
- 238000003384 imaging method Methods 0.000 claims description 3
- 238000010586 diagram Methods 0.000 description 8
- 230000005855 radiation Effects 0.000 description 7
- 238000010309 melting process Methods 0.000 description 4
- 239000007789 gas Substances 0.000 description 3
- 238000013021 overheating Methods 0.000 description 3
- XKRFYHLGVUSROY-UHFFFAOYSA-N Argon Chemical compound [Ar] XKRFYHLGVUSROY-UHFFFAOYSA-N 0.000 description 2
- 239000000956 alloy Substances 0.000 description 2
- 239000011521 glass Substances 0.000 description 2
- 230000001788 irregular Effects 0.000 description 2
- 238000004519 manufacturing process Methods 0.000 description 2
- 239000000155 melt Substances 0.000 description 2
- 230000000007 visual effect Effects 0.000 description 2
- 238000012935 Averaging Methods 0.000 description 1
- 208000034693 Laceration Diseases 0.000 description 1
- 206010064127 Solar lentigo Diseases 0.000 description 1
- 229910045601 alloy Inorganic materials 0.000 description 1
- 229910052786 argon Inorganic materials 0.000 description 1
- 239000010425 asbestos Substances 0.000 description 1
- 238000009529 body temperature measurement Methods 0.000 description 1
- 150000001875 compounds Chemical class 0.000 description 1
- 230000006835 compression Effects 0.000 description 1
- 238000007906 compression Methods 0.000 description 1
- 238000010276 construction Methods 0.000 description 1
- 238000012937 correction Methods 0.000 description 1
- 239000013078 crystal Substances 0.000 description 1
- 230000007547 defect Effects 0.000 description 1
- 230000002950 deficient Effects 0.000 description 1
- 230000007274 generation of a signal involved in cell-cell signaling Effects 0.000 description 1
- 239000012535 impurity Substances 0.000 description 1
- 239000007788 liquid Substances 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 239000007769 metal material Substances 0.000 description 1
- 150000002739 metals Chemical class 0.000 description 1
- NJPPVKZQTLUDBO-UHFFFAOYSA-N novaluron Chemical class C1=C(Cl)C(OC(F)(F)C(OC(F)(F)F)F)=CC=C1NC(=O)NC(=O)C1=C(F)C=CC=C1F NJPPVKZQTLUDBO-UHFFFAOYSA-N 0.000 description 1
- 230000003287 optical effect Effects 0.000 description 1
- 238000012856 packing Methods 0.000 description 1
- 239000011819 refractory material Substances 0.000 description 1
- 229910052895 riebeckite Inorganic materials 0.000 description 1
- 230000035945 sensitivity Effects 0.000 description 1
- 238000001228 spectrum Methods 0.000 description 1
- 230000007704 transition Effects 0.000 description 1
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 description 1
Classifications
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B22—CASTING; POWDER METALLURGY
- B22D—CASTING OF METALS; CASTING OF OTHER SUBSTANCES BY THE SAME PROCESSES OR DEVICES
- B22D23/00—Casting processes not provided for in groups B22D1/00 - B22D21/00
- B22D23/06—Melting-down metal, e.g. metal particles, in the mould
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B22—CASTING; POWDER METALLURGY
- B22D—CASTING OF METALS; CASTING OF OTHER SUBSTANCES BY THE SAME PROCESSES OR DEVICES
- B22D46/00—Controlling, supervising, not restricted to casting covered by a single main group, e.g. for safety reasons
Landscapes
- Engineering & Computer Science (AREA)
- Mechanical Engineering (AREA)
Description
【発明の詳細な説明】
この発明は高周波誘導加熱や電気抵抗式加熱な
どの加熱手段によつて各種の合金を融解し歯科用
義歯・修復物または装飾品などの小型精密鋳造品
を製造する精密鋳造法およびその装置に関するも
のである。DETAILED DESCRIPTION OF THE INVENTION This invention is a precision method for manufacturing small precision cast products such as dental dentures, restorations, and decorative items by melting various alloys using heating means such as high-frequency induction heating and electric resistance heating. This article relates to a casting method and its equipment.
精密鋳造法を機能別に大別すると、(イ)鋳物材料
の加熱融解法、(ロ)溶湯の注湯タイミング(以下鋳
造タイミングと記す)判定法、(ハ)鋳造圧力を与え
る方法とになり、上記(イ)(ハ)は従来一般に安定して
余り問題がないが、(ロ)の方法においては可成り問
題があり、しかも鋳造工程の中でも製品の良否を
左右するもつとも重要な要素である。すなわち溶
湯の鋳込みに適正な温度(以下鋳造温度と記す)
は一般にその材料の融点より若干高い温度であ
り、これを越えオーバーヒートさせると結晶粒が
粗大化し、また結晶粒界に不純物が混入するなど
機械的性質を悪くするだけでなく、鋳造品に気泡
や肌荒など起し欠陥製品となる。また逆に適正温
度に満たないと融解不足となり、ナメラレ(鋳込
み不足)を生じ鋳造品の最大欠陥を生じる。従来
この鋳造温度および鋳造タイミングの適否を熟練
者が目視で判定するのが一般的であるが、融解中
僅かに変化する色調や形状の変化によつて適正な
タイミングをとらえることはきわめてむつかしく
高度の熟練を要する上に、その熟練者にてもその
判定を誤ることもあり、製品の歩留りが低く、高
価な材料を使用する歯科用においてはその損失は
大きい。そこでこの目視法の歩留りを向上させる
ため従来からいろいろ試みられている方法の一つ
は放射温度計を用いて融解金属の温度を測定する
方法とか、上記鋳造温度を目標値とし、これと放
射温度計の検出値とを比較し、その偏差に応じて
加熱源を自動制御する方法とかである。しかしな
がら上記放射温度計は材料が融解する際放射する
赤外線の量によつて材料の表面温度を測定するの
で、各種の材料の温度に対する放射率を決定する
ことが面倒であるだけでなく、融解室のぞき窓の
ガラスの曇りによつて測定誤差が生じるし、また
鋳造材が少ないばあい放射温度計の受熱板全面に
像が結ばず、正しい測温ができないなどの問題が
あり、実用上正確な測温が困難で、したがつて鋳
造タイミングが狂うという欠点がある。つぎに別
の方法として融解時間を制御して鋳造タイミング
を管理する方法がある。しかしながらこの方法で
は常に融解強さいいかえると加熱エネルギーの時
間当りの出力を一定にする必要があり、さらに鋳
造量やるつぼ内での材料位置などもすべて一定に
しなければならない。しかもこの方法は融解過程
を無視しているので応用範囲が限られるという欠
点がある。 Precision casting methods can be roughly classified by function: (a) a method of heating and melting the casting material, (b) a method of determining the timing of pouring molten metal (hereinafter referred to as casting timing), and (c) a method of applying casting pressure. Methods (a) and (c) above are conventionally generally stable and have no problems, but method (b) has quite a few problems, and is also an important element in the casting process that influences the quality of the product. In other words, the appropriate temperature for casting molten metal (hereinafter referred to as casting temperature)
is generally a temperature slightly higher than the melting point of the material, and overheating beyond this will not only cause the crystal grains to coarsen and impurities to enter the grain boundaries, worsening mechanical properties, but also cause bubbles and bubbles in the cast product. This results in defective products such as rough skin. On the other hand, if the temperature is lower than the appropriate temperature, there will be insufficient melting, resulting in name lare (insufficient pouring) and the largest defect in the cast product. Conventionally, it is common for an expert to visually judge whether or not the casting temperature and casting timing are appropriate, but it is extremely difficult to determine the appropriate timing due to slight changes in color tone and shape during melting, and requires a high level of skill. In addition to requiring skill, even those skilled in the art may make mistakes in judgment, which is a great loss in dental applications where product yields are low and expensive materials are used. Therefore, one of the methods that have been tried in the past to improve the yield of this visual method is to measure the temperature of molten metal using a radiation thermometer, or to set the above casting temperature as a target value, and to set this as the target value and to combine this with radiation temperature. This method compares the detected value with the meter and automatically controls the heating source according to the deviation. However, since the above-mentioned radiation thermometer measures the surface temperature of the material by the amount of infrared rays emitted when the material melts, it is not only troublesome to determine the emissivity of various materials at different temperatures, but also the melting chamber Clouding of the glass in the viewing window causes measurement errors, and if there is little casting material, the image will not be focused on the entire surface of the radiation thermometer's heat receiving plate, making it impossible to measure temperature accurately. It has the disadvantage that temperature measurement is difficult and therefore the casting timing is out of order. Another method is to control melting time to manage casting timing. However, in this method, it is necessary to always maintain a constant melting strength, or in other words, a constant output of heating energy per hour, and furthermore, everything such as the casting amount and the position of the material within the crucible must also be constant. Moreover, this method ignores the melting process, so it has the disadvantage that its range of applications is limited.
以上述べたとおり鋳造タイミングの適正化が実
用的に困難である現況において筆者らが考案し、
去る昭和59年4月25日出願した特許願「精密鋳造
装置」は測温を一切行わずに鋳造タイミングを正
確にとらえようとするものである。すなわち金属
材料は融解時に必ず形状変化を伴ない、またその
表面にスポツト(黒点)や表皮の破れなどが生ず
るという冶金学上の定理にもとづき、近年発達し
たCCDイメージ・センサを用い、上記形状変化
をその輪郭画像信号として検出し、鋳造タイミン
グを適正に決定するように構成されており、精密
鋳造における現在の問題点や欠点をほぼ解消する
ものである。しかしながら上記装置はつぎのばあ
いに限り、適正な鋳造タイミングを決定しえない
という欠点がある。すなわち鋳物材料が円柱状で
これを同心円状のるつぼ内に収容するばあい、上
記材料の外径がるつぼ内径に近似していると、
CCDが撮像する輪郭像の変化を材料の融解時に
見出すことができないことである。 As mentioned above, the authors devised this method in the current situation where it is practically difficult to optimize the casting timing.
The patent application for ``Precision Casting Apparatus'' filed on April 25, 1980 is intended to accurately determine casting timing without measuring temperature at all. In other words, based on the metallurgical theorem that metallic materials always undergo shape changes when melted, and that spots (sunspots) and skin tears occur on their surfaces, we use recently developed CCD image sensors to detect the above shape changes. The present invention is configured to detect the contour image signal as a contour image signal and appropriately determine the casting timing, which almost eliminates the current problems and drawbacks in precision casting. However, the above device has the disadvantage that it cannot determine the proper casting timing only in the following cases. In other words, when the casting material is cylindrical and is housed in a concentric crucible, if the outer diameter of the material approximates the inner diameter of the crucible,
The problem is that no change in the contour image captured by the CCD can be detected when the material melts.
この発明は上記の現況に鑑みてなされたもの
で、筆者らの先に出願した「精密鋳造装置」の欠
点を解消し、鋳物材料の形状の如何にかかわら
ず、最適の鋳造タイミングを確認し、注湯するよ
うにしたものである。すなわちるつぼ内の鋳物材
料を加熱するばあい、現在用いられている如何な
る加熱手段によつても材料全体を一様に加熱する
ことはできず、したがつて材料の加熱が進行する
に伴ない材料自体に温度分布が生じ、そのそれぞ
れの部分から発せられる輝度をCCDイメージ・
センサによつて検出することによつて上記加熱進
行中の材料の温度分布が時々刻々輝度分布像とし
て表示器に映像され、その輝度分布像の頂部が直
線を形成した時点を基準として鋳造最適タイミン
グを決定し、鋳型に注湯することによつて良質の
鋳造品を高い歩留りで鋳造しうる方法と、この方
法による構成簡単にして高能率の小型低廉な装置
とを提供しようとするものである。 This invention was made in view of the above-mentioned current situation, and it eliminates the drawbacks of the "precision casting device" that the authors previously applied for, and confirms the optimal casting timing regardless of the shape of the casting material. It was designed to be poured with hot water. In other words, when heating a casting material in a crucible, it is not possible to uniformly heat the entire material using any heating means currently in use, and therefore, as the material heats up, the material A temperature distribution occurs within itself, and the brightness emitted from each part is measured using a CCD image.
By detecting it with a sensor, the temperature distribution of the material being heated is displayed moment by moment as a brightness distribution image on the display, and the optimal casting timing is determined based on the point when the top of the brightness distribution image forms a straight line. The present invention aims to provide a method for casting high-quality cast products with a high yield by determining the molten metal and pouring it into a mold, and a compact, inexpensive device with a simple construction and high efficiency using this method. .
以下図面を用いてこの発明の精密鋳造法を用い
た鋳造装置の実施例を説明する。第1図は実施例
としての高周波溶解加圧精密鋳造装置の外観斜視
図であり、装置1は筆者らが考案し既に公開され
ている特開昭58−74263号公報「高周波溶解加圧
鋳造機」に示した加熱室(第2図にて示す)2の
底面外表面部3と、上下可動筐体からなる下室部
5とを外部に露出し、その他の機構部分を上部・
下部器筐6,7でもつて包被した装置を一部改造
したものである。すなわち上部器筐6前面の操作
盤8に設けてあつた加熱室のぞき窓(第2図に示
す9)を外部から観察できる観察窓を廃し、この
発明の要部の一つである映像表示器10を設けた
ことである。したがつて操作盤8上の手動操作ボ
タン群11およびそれらと連動する表示灯群12
は上記装置のままであり、手動操作の順序なども
同じであるが、ただ術者が上記観察窓から加熱室
内の融解状況を目視せずに操作盤上の映像表示器
10の映像すなわちるつぼ内材料の輝度分布像に
よつて鋳造タイミングを決めるようにしたのであ
る。第2図に移つて、上記上部器筐6内の加熱室
2と凸状鋳型14と、この鋳型14を加熱室底面
外表面部3に圧接している鋳型受台15とを断面
図にて説明し、併せてるつぼ17内の鋳物材料M
の融解状況を上記表示器10に映像するこの発明
の要部の構成を説明する。凸状鋳型14は上部突
出部にるつぼ17と、ロストワツクス法にて造形
した精密鋳型空洞部18および湯道19とを1体
に成型し、上記るつぼ17は耐火筒状体20の内
部すなわち加熱室2に収容され、かつ凸状鋳型下
部基部21は鋳型受台15上にアスベストリング
22を介して支承されている。この受台15は第
1図で示した下室部5の中心軸上で空気圧シリン
ダピストン23または図示しない圧縮ばねによつ
て下方から所定の圧力にて押上げられ、上記基部
21肩部をアスベストパツキング24を介して上
記加熱室底面外表面部3に圧接されている。耐火
筒状体20の周囲には高周波誘導加熱コイル25
が巻回してあり、さらに加熱室2の上端部を密封
する透明耐火材にてなるのぞき窓9を設けるとと
もに、加熱室2内を減圧する排気管27およびた
とえば約5Kg/cm2Gの圧力のアルゴンガス導入管
28を設けている。以上の構成は従来装置のもの
であり、この発明の要部はるつぼ17内の鋳物材
料Mの輝度分布を映像として表示せしめる構成で
ある。上記ののぞき窓9のたとえば上部所定の位
置にたとえば倍率10倍の集射レンズ30と、フイ
ルター31とを設ける。集射レンズ30は単一凸
レンズに限らず複合レンズでもよい。このように
して材料Mの加熱が進行し、その放射する放射光
Lはレンズ30の結像位置に設置した1次元
CCDイメージ・センサ32の感光部33に入射
される。この感光部33はたとえば幅約30μm、
長さ約30mmの間に約2600個の感光画素を1列に配
列し、ここで光電変換・蓄積された信号電荷を
CCD内のアナログシフトレジスタで転送し、時
系列的なアナログ電圧信号D1を出力する。この
信号D1は材料Mのたとえば中心線上の輝度分布
を示し、これが映像信号発生回路34によつて輝
度分布映像信号D2に変換され、映像表示器10
に入力される。映像表示器10は横軸を上記材料
Mの中心線とし、縦軸にその中心線上の各位置に
おける単位面積当りの明るさすなわち輝度の分布
像I・Bを平面状に映像する。この輝度分布像は
いうまでもなく材料Mの加熱の進行に伴なつて
時々刻々に変化する。これを第3,第4図で説明
する。図はこの説明の実施例装置によつて鋳物材
料を融解したときの実際の輝度分布像の変化を示
すもので、それぞれの図Aは目視にて得た材料の
形状を図Bの分布図との対象のため付記したもの
であり、表示器10の映像ではない。図Bの横軸
Pはるつぼ内材料MのたとえばX方向(図A参
照)の位置(るつぼ内壁1端からの距離(mm))
を示し、dはるつぼ17の内径に対応し、タテ軸
Bは材料の輝度(ead/m2)を示す。ただし、つ
ぎにのべるように〜の分布像I・Bは時系列
的に順次映像されるもので、これをまとめて示し
たのが図Bである。第3図Bにおいて加熱開始後
60secにて分布はとなり、そのときの形状は図
Aののように外周部の輝度が内部のそれに比し
高い。(高輝度部を斜線で示す)つぎに数sec後に
のように高輝度の部分が増すと、分布がのよ
うに相似状に上昇する。さらに加熱が進行し、
のときには外形が円形に変化するが中央部の輝度
は未だ低い。加熱時間が70secに達するとよう
に中央にスポツト状に低輝度の部分を残すだけと
なり、分布像も平坦に近づく。そして72secにて
全面が同一輝度になると、分布像ものように凹
凸のない直線を形成する。この時点が材料Mが鋳
造温度に達したことを示すものであるから、鋳造
タイミングの適正値はこの材料のばあい72+2=
74secである。このように分布像の頂部が直線化
した時点を基準として材料によつてそれぞれ決定
する。ただし、この時点を超える遅延時間が永い
と分布像に再び凹凸が発生し、前述したオーバー
ヒートとなる。つぎに第4図A,Bに移る。この
ばあいは、合金材が図Aに示すようにシヨツト状
であるので、融解途中に分布線に多くの山が不規
則に発生し、形状ものように不定形である
が、完全融解寸前にも形状ものようにるつぼ内
径の円形となつたことを分布像にて認められ
る。さらに加熱が進行すれば第3図のばあいと同
様、分布像の頂部が直線を形成する。この時点が
材料の温度が鋳造温度に達したことを示すもので
あり、鋳造タイミングはこの時点を基準として決
めることによつて、融解不足は絶無となり、遅延
時間を任意に設定すればオーバヒートのない最適
の鋳造タイミングを確立することができる。な
お、上記CCDイメージ・センサは波長400nmか
ら1000nmにわたりすぐれた感度を有しており、
上記加熱室のぞき窓9のガラスが融解中に発生す
る金属蒸気やガスによつて曇つても材料Mから放
射される赤外線域のいずれかのスペクトルがそれ
を透過して輝度分布を的確に撮像するため、上記
鋳造タイミングが狂うことはない。 Embodiments of a casting apparatus using the precision casting method of the present invention will be described below with reference to the drawings. Fig. 1 is an external perspective view of a high-frequency melting and pressure precision casting machine as an example. The bottom outer surface part 3 of the heating chamber (shown in Figure 2) 2 shown in Figure 2 and the lower chamber part 5 consisting of a vertically movable casing are exposed to the outside, and other mechanical parts are exposed to the outside.
This is a partially modified device in which the lower housings 6 and 7 are also enclosed. In other words, the observation window for observing the heating chamber viewing window (9 shown in FIG. 2) from the outside, which was provided on the operation panel 8 on the front side of the upper case 6, has been eliminated, and an image display, which is one of the main parts of the present invention, has been implemented. 10 was established. Therefore, the manual operation button group 11 on the operation panel 8 and the indicator light group 12 interlocked with them
The device is still the same as described above, and the order of manual operations is the same, but the operator does not have to visually observe the melting situation inside the heating chamber through the observation window, but instead displays the image on the video display 10 on the operation panel, that is, the inside of the crucible. The casting timing was decided based on the brightness distribution image of the material. Turning to FIG. 2, a sectional view shows the heating chamber 2 and the convex mold 14 in the upper housing 6, and the mold holder 15 that presses the mold 14 against the bottom outer surface 3 of the heating chamber. Explain and also describe the casting material M in the crucible 17.
The configuration of the main part of the present invention, which images the melting state of the liquid on the display 10, will be explained. The convex mold 14 has a crucible 17 in its upper protrusion, a precision mold cavity 18 formed by the lost wax method, and a runner 19, which are molded into one body. 2, and the convex mold lower base 21 is supported on the mold holder 15 via an asbestos ring 22. This pedestal 15 is pushed up from below with a predetermined pressure by a pneumatic cylinder piston 23 or a compression spring (not shown) on the central axis of the lower chamber 5 shown in FIG. It is pressed into contact with the bottom outer surface portion 3 of the heating chamber via a packing 24. A high frequency induction heating coil 25 is installed around the fireproof cylindrical body 20.
is wound around the heating chamber 2, and is further provided with a viewing window 9 made of a transparent refractory material to seal the upper end of the heating chamber 2, an exhaust pipe 27 for reducing the pressure inside the heating chamber 2 , and a An argon gas introduction pipe 28 is provided. The above configuration is that of a conventional device, and the essential part of the present invention is a configuration for displaying the luminance distribution of the casting material M in the crucible 17 as an image. For example, a condenser lens 30 with a magnification of 10 times and a filter 31 are provided at a predetermined position, for example, above the above-mentioned viewing window 9. The condenser lens 30 is not limited to a single convex lens, but may be a compound lens. In this way, the heating of the material M progresses, and the emitted radiation L is emitted from a one-dimensional lens placed at the imaging position of the lens 30.
The light is incident on the photosensitive section 33 of the CCD image sensor 32. This photosensitive section 33 has a width of about 30 μm, for example.
Approximately 2,600 photosensitive pixels are arranged in a row within a length of approximately 30 mm, and the signal charges that are photoelectrically converted and accumulated are converted here.
It is transferred using an analog shift register within the CCD and outputs a time-series analog voltage signal D1 . This signal D 1 indicates the luminance distribution on the center line of the material M, and this is converted into a luminance distribution video signal D 2 by the video signal generation circuit 34, and the video display 10
is input. The image display 10 has a horizontal axis as the center line of the material M, and a vertical axis as a planar image of brightness per unit area, that is, luminance distribution images I and B at each position on the center line. Needless to say, this brightness distribution image changes from moment to moment as the heating of the material M progresses. This will be explained with reference to FIGS. 3 and 4. The figures show changes in the actual brightness distribution image when a casting material is melted using the apparatus described in this example. Each figure A shows the shape of the material obtained by visual observation, and the distribution diagram in figure B shows the change in the actual luminance distribution image. This is an additional note because it is intended for use in the following, and is not an image on the display 10. The horizontal axis P in Figure B is the position (distance (mm) from one end of the crucible inner wall) of the material M in the crucible in the X direction (see Figure A), for example.
, d corresponds to the inner diameter of the crucible 17, and the vertical axis B indicates the brightness (ead/m 2 ) of the material. However, as described below, the distribution images I and B of ~ are sequentially imaged in time series, and Figure B shows them all together. After starting heating in Figure 3B
At 60 seconds, the distribution becomes as shown in Figure A, where the brightness at the outer periphery is higher than that at the inside. (High-brightness areas are indicated by diagonal lines) When the high-brightness areas increase several seconds later, the distribution rises in a similar manner as shown below. Heating progresses further,
When , the outer shape changes to a circular shape, but the brightness at the center is still low. When the heating time reaches 70 seconds, only a spot-like low-intensity part remains in the center, and the distribution image becomes almost flat. When the entire surface becomes the same brightness at 72 seconds, a straight line with no unevenness is formed like a distribution image. Since this point indicates that the material M has reached the casting temperature, the appropriate value for the casting timing is 72+2=
It is 74 seconds. The point at which the top of the distribution image becomes straight in this way is determined depending on the material. However, if the delay time beyond this point is long, unevenness will occur again in the distribution image, resulting in the above-mentioned overheating. Next, move to FIG. 4A and B. In this case, since the alloy material has a shot shape as shown in Figure A, many irregular peaks occur on the distribution line during melting, and the shape is irregular, but it is on the verge of complete melting. It can be seen in the distribution image that the crucible had a circular inner diameter, just like the shape. As the heating progresses further, the top of the distribution image forms a straight line, as in the case of FIG. This point indicates that the temperature of the material has reached the casting temperature. By determining the casting timing based on this point, there will be no insufficient melting, and by setting the delay time arbitrarily, there will be no overheating. Optimal casting timing can be established. The above CCD image sensor has excellent sensitivity over wavelengths from 400nm to 1000nm.
Even if the glass of the heating chamber viewing window 9 becomes cloudy due to metal vapor or gas generated during melting, any spectrum of the infrared range emitted from the material M will pass through it, and the brightness distribution will be accurately imaged. Therefore, the above-mentioned casting timing will not be disrupted.
つぎに第5図によつて自己走査型画像検出器3
2を2次元検出器40にした一つの実施例装置を
説明する。第5図Aは材料Mをたとえば上記第3
図で示した六角形インゴツトとし、これを2次元
CCDイメージ・センサ40にて撮像するばあい、
2次元センサ40は通常水平(X軸)方向と垂直
(Y軸)方向の自己走査回路を備えているが、こ
れの垂直方向走査回路を出力平均化回路41に置
換えた状態を示している。このことによつてY方
向のたとえばY1、Y2………Ynの出力のうちある
一定のレベル以上の輝度信号を平均化して輝度信
号Dx1として出力し、同じくY11〜Yn1の出力の
うち同じく一定レベル以上のものを平均化し、
Dx2として出力する。このようにしてDxnまでの
変化は図Bにすように第3図のBのと同じく材
料MのX軸上の輝度分布像として表示器に映像し
うるものである。この2次元センサ40は1次元
センサ32に比し、高価になるが第4図にて説明
したシヨツト状などの不定形の材料の融解過程に
おいては材料とセンサとの方向を合わせる必要が
なく、作業能率が良い。ただし、完全融解の時点
すなわち分布像頂部が直線を形成する頃には特に
1次元センサとの差異はない。 Next, according to FIG. 5, the self-scanning image detector 3
One example device in which 2 is a two-dimensional detector 40 will be described. Figure 5A shows material M, for example,
The hexagonal ingot shown in the figure is taken as a two-dimensional ingot.
When capturing an image with the CCD image sensor 40,
The two-dimensional sensor 40 normally includes self-scanning circuits in the horizontal (X-axis) direction and the vertical (Y-axis) direction, but this figure shows a state in which the vertical scanning circuit is replaced with an output averaging circuit 41. By this, among the outputs of, for example, Y 1 , Y 2 , Yn in the Y direction, the luminance signals above a certain level are averaged and output as the luminance signal Dx 1 , and the outputs of Y 11 to Yn 1 are also averaged. Among them, those above a certain level are averaged,
Output as Dx 2 . In this way, the change up to Dxn can be imaged on the display as a luminance distribution image on the X-axis of the material M, as shown in FIG. 3B, as shown in FIG. Although this two-dimensional sensor 40 is more expensive than the one-dimensional sensor 32, it is not necessary to align the direction of the material and the sensor during the melting process of irregularly shaped materials such as the shot shape explained in FIG. Good work efficiency. However, at the time of complete melting, that is, when the top of the distribution image forms a straight line, there is no particular difference from the one-dimensional sensor.
以上がこの発明の実施例であるが、この発明は
図示や説明に限定されるものでないことはいうま
でもない。たとえばこの発明は高周波溶解加圧鋳
造に限らず、電気抵抗式や発熱体るつぼ加熱式な
どるつぼ内材料の融解状況がCCDイメージ・セ
ンサにて撮像しうる方法ならびに装置であればど
のようなものにも適用できる。またCCDイメー
ジ・センサ32の取付位置は材料の放射光軸上に
限らず、反射鏡などを用いて任意の位置に取付け
られる。映像表示器は通常デイスプレイ用CRT
とするが、オシロ管またはその他の表示器にても
よく、また必ずしも鋳造装置の操作盤に組込まな
くてもよい。また2次元CCDによる方法は、上
記に限らずいろいろ考えられるものである。 Although the embodiments of the present invention have been described above, it goes without saying that the present invention is not limited to the illustrations and descriptions. For example, this invention is not limited to high-frequency melting and pressure casting, but can be applied to any method or device that can image the melting state of the material in the crucible using a CCD image sensor, such as an electric resistance type or a heating element crucible heating type. can also be applied. Further, the mounting position of the CCD image sensor 32 is not limited to the radiation optical axis of the material, but may be mounted at any arbitrary position using a reflecting mirror or the like. The video display is usually a CRT for display.
However, it may be an oscilloscope or other display, and it does not necessarily have to be incorporated into the operation panel of the casting machine. Furthermore, the method using the two-dimensional CCD is not limited to the above method, and there are various other methods that can be considered.
この発明は以上のように構成されているので従
来の精密鋳造における大きい懸案であつた最適の
鋳造タイミングの決め手となり、鋳造品の歩留り
を飛躍的に向上させるとともに筆者らが先に出願
した発明の装置の欠点を解消したものである。す
なわち高価にして校正や補正を要し、しかも正確
な測温が困難である放射温度計の代りに小形低廉
にして特に融解室のガスや金属蒸気などの影響が
少なく、材料の融解状況をその輝度分布像によつ
て正確に撮像するCCDと、上記分布像を表示す
る映像表示器とによつて鋳物材料の種類ごとの最
適鋳造タイミングが容易かつ正確にとらえること
ができ、高品質の鋳造品が能率良く製造できる精
密鋳造方法ならびに簡単な構造にして小形低廉な
便宜な装置を提供しえたものである。 Since this invention is constructed as described above, it becomes the decisive factor in determining the optimal casting timing, which was a major concern in conventional precision casting, dramatically improves the yield of cast products, and improves the invention previously filed by the authors. This eliminates the drawbacks of the device. In other words, instead of using a radiation thermometer that is expensive, requires calibration and correction, and is difficult to measure temperature accurately, it is small and inexpensive, and is less affected by gases and metal vapors in the melting chamber, and can be used to measure the melting state of the material. The optimal casting timing for each type of casting material can be easily and accurately determined using a CCD that accurately captures a luminance distribution image and a video display that displays the distribution image, resulting in high-quality castings. The present invention has provided a precision casting method that allows for efficient production of metals, as well as a convenient device that has a simple structure, is compact, and is inexpensive.
第1図はこの発明の実施例としての高周波溶解
加圧精密鋳造装置の外観斜視図、第2図は上記装
置の融解室の断面および輝度分布映像部のブロツ
ク図、第3図Aは上記装置によるインゴツト材の
融解過程の形状ならびに輝度変移図、図Bは同じ
く上記インゴツト材の表示器画面での輝度分布像
の変移図、第4図Aは上記装置によるシヨツト材
の融解過程の形状ならびに輝度変移図、図Bは同
じく上記シヨツト材の表示器画面での輝度分布像
の変移図、第5図Aはこの発明の別の実施例とし
て2次元自己走査形画像検出器の使用法を説明す
る原理図、図Bは上記図Aによる輝度分布図であ
る。
2……融解室、8……鋳造操作盤、10……映
像表示器、11……手動操作ボタン群、12……
鋳造工程表示ランプ群、14……鋳型、M……鋳
物材料、17……るつぼ、18……精密鋳型空洞
部、19……湯道、25……加熱手段としての高
周波誘導コイル、30……集射レンズ、32,4
0……自己走査型画像検出器(32は1次元、4
0は2次元検出器)、D1……輝度信号、D2……輝
度分布映像信号、I・B……輝度分布像。
FIG. 1 is an external perspective view of a high-frequency melting and pressure precision casting apparatus as an embodiment of the present invention, FIG. 2 is a cross-sectional view of the melting chamber and a block diagram of the brightness distribution imaging section of the above-mentioned apparatus, and FIG. 3A is a block diagram of the above-mentioned apparatus. Fig. 4A shows the shape and brightness change of the ingot material in the melting process using the above device, Figure B is a change diagram of the brightness distribution image of the ingot material on the display screen, and Figure 4A shows the shape and brightness of the shot material in the melting process using the above device. Figure B is a transition diagram of the luminance distribution image of the above-mentioned shot material on the display screen, and Figure 5A is a diagram illustrating the use of a two-dimensional self-scanning image detector as another embodiment of the present invention. The principle diagram, Figure B, is a brightness distribution diagram based on Figure A above. 2... Melting chamber, 8... Casting operation panel, 10... Video display, 11... Manual operation button group, 12...
Casting process display lamp group, 14... Mold, M... Casting material, 17... Crucible, 18... Precision mold cavity, 19... Runway, 25... High frequency induction coil as heating means, 30... Condenser lens, 32,4
0... Self-scanning image detector (32 is one-dimensional, 4
0 is a two-dimensional detector), D1 ...Brightness signal, D2 ...Brightness distribution video signal, I/B...Brightness distribution image.
Claims (1)
段によつて融解し、その融解進行状態をレンズを
介して自己走査形画像検出器によつて輝度信号と
して検出し、前記材料の輝度分布を表示器に映像
せしめ、この分布像の頂部が直線を形成したと
き、これを基準として鋳型に注湯する鋳込みタイ
ミングを決定することを特徴とする精密鋳造方
法。 2 るつぼ内の鋳物材料を融解する加熱手段と、
前記材料の放射光を結像する集射レンズと、前記
レンズの結像位置に設け、入射光像を輝度信号に
変換し出力する自己走査型画像検出器と、前記検
出器の出力信号を、輝度分布像として映像する映
像表示器とを設けたことを特徴とする精密鋳造装
置。 3 加熱手段が高周波誘導加熱装置である特許請
求の範囲第2項記載の精密鋳造装置。 4 自己走査形画像検出器が1次元検出器である
特許請求の範囲第2項または第3項記載の精密鋳
造装置。 5 自己走査形画像検出器が2次元検出器である
特許請求の範囲第2項または第3項記載の精密鋳
造装置。[Scope of Claims] 1. A small amount of casting material contained in a crucible is melted by heating means, and the progress of melting is detected as a brightness signal by a self-scanning image detector through a lens, and the A precision casting method characterized in that the brightness distribution of the material is displayed on a display, and when the top of this distribution image forms a straight line, the timing of pouring the metal into the mold is determined based on this as a reference. 2. heating means for melting the casting material in the crucible;
a condensing lens that forms an image of the emitted light of the material; a self-scanning image detector that is provided at the imaging position of the lens and converts the incident light image into a brightness signal and outputs the image; and an output signal of the detector; A precision casting device characterized by being equipped with a video display device that displays an image as a luminance distribution image. 3. The precision casting apparatus according to claim 2, wherein the heating means is a high frequency induction heating device. 4. The precision casting apparatus according to claim 2 or 3, wherein the self-scanning image detector is a one-dimensional detector. 5. The precision casting apparatus according to claim 2 or 3, wherein the self-scanning image detector is a two-dimensional detector.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10232584A JPS60244458A (en) | 1984-05-21 | 1984-05-21 | Method and device for precision casting |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10232584A JPS60244458A (en) | 1984-05-21 | 1984-05-21 | Method and device for precision casting |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS60244458A JPS60244458A (en) | 1985-12-04 |
| JPH0416259B2 true JPH0416259B2 (en) | 1992-03-23 |
Family
ID=14324395
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP10232584A Granted JPS60244458A (en) | 1984-05-21 | 1984-05-21 | Method and device for precision casting |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS60244458A (en) |
-
1984
- 1984-05-21 JP JP10232584A patent/JPS60244458A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS60244458A (en) | 1985-12-04 |
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