JPH0325262B2 - - Google Patents

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Publication number
JPH0325262B2
JPH0325262B2 JP21417487A JP21417487A JPH0325262B2 JP H0325262 B2 JPH0325262 B2 JP H0325262B2 JP 21417487 A JP21417487 A JP 21417487A JP 21417487 A JP21417487 A JP 21417487A JP H0325262 B2 JPH0325262 B2 JP H0325262B2
Authority
JP
Japan
Prior art keywords
vibrator
mold
frequency
vibrators
vibration
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
Application number
JP21417487A
Other languages
Japanese (ja)
Other versions
JPS6462256A (en
Inventor
Masaji Uehara
Haruo Kitamura
Kenzo Sawada
Tetsuo Nakamura
Katsuhiko Yui
Juichi Kato
Ryuichi Hiratsuka
Daijiro Mizukoshi
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.)
Nippon Steel Corp
Original Assignee
Nippon Steel Corp
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 Nippon Steel Corp filed Critical Nippon Steel Corp
Priority to JP62214174A priority Critical patent/JPS6462256A/en
Priority to EP88113989A priority patent/EP0305930B1/en
Priority to ES198888113989T priority patent/ES2034073T3/en
Priority to CA000575784A priority patent/CA1316325C/en
Priority to DE8888113989T priority patent/DE3873451T2/en
Priority to AU21623/88A priority patent/AU603251B2/en
Priority to US07/237,740 priority patent/US4867226A/en
Priority to KR1019880010986A priority patent/KR920004972B1/en
Publication of JPS6462256A publication Critical patent/JPS6462256A/en
Publication of JPH0325262B2 publication Critical patent/JPH0325262B2/ja
Granted legal-status Critical Current

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  • Continuous Casting (AREA)

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は、金属の連続鋳造において、鋳型を超
音波で加振する方法に関する。
DETAILED DESCRIPTION OF THE INVENTION [Industrial Application Field] The present invention relates to a method of exciting a mold with ultrasonic waves in continuous metal casting.

[従来の技術] 金属の連続鋳造において、溶湯のメニスカス近
傍の鋳型内壁を振動させるために、多数の超音波
振動子(本明細書では超音波振動子を振動子と略
記する)を鋳型に配設する技術については、例え
ば特開昭62−57742号等にも記載の如く公知であ
る。第1図は振動子1〜12を配設した連続鋳造
用鋳型のメニスカス近傍の横断面の例を示す図で
ある。鋳型13の内壁は振動子1〜12による加
振によつて振動せしめるが、例えば鋳型内壁面と
溶湯14との焼付きやステイツキングを防止する
ためには、鋳型内壁は、メニスカス近傍部の全て
の壁面部が常に望ましい振動に保たれている事が
必要である。振動子1〜12の各々は、振動特性
が同じものが通常用いられるが、従来の方法では
振動子1〜12の周波数が同じであつたために、
例えば第2図で振動子Aから発信された超音波と
振動子Bから発信された超音波が干渉して、両超
音波の位相が同じ場合AP1=BP1の距離にある鋳
型内壁面のP1点は振幅が倍増し激しく振動する
が、AP2−BP2=λ/2(但しλ=超音波の波長)
のP2点では振動子A及びBからの超音波は干渉
されて振幅が常に極めて小さくなるため焼付やス
テイツキング等が発生することとなる。
[Prior Art] In continuous metal casting, a large number of ultrasonic transducers (ultrasonic transducers are abbreviated as transducers in this specification) are arranged in a mold in order to vibrate the inner wall of the mold near the meniscus of molten metal. The technology to provide this is well known, as described in, for example, Japanese Patent Laid-Open No. 62-57742. FIG. 1 is a diagram showing an example of a cross section near the meniscus of a continuous casting mold in which vibrators 1 to 12 are arranged. The inner wall of the mold 13 is vibrated by the vibrations of the vibrators 1 to 12. For example, in order to prevent the inner wall surface of the mold from seizing or states-king between the inner wall surface of the mold and the molten metal 14, the inner wall of the mold must be vibrated in all areas near the meniscus. It is necessary that the wall surface of the machine is always maintained at the desired vibration level. Generally, each of the vibrators 1 to 12 has the same vibration characteristics, but in the conventional method, since the frequencies of the vibrators 1 to 12 were the same,
For example, in Fig. 2, if the ultrasonic waves emitted from transducer A and the ultrasonic waves emitted from transducer B interfere and the phases of both ultrasonic waves are the same, the inner wall of the mold at a distance of AP 1 = BP 1 . At point P, the amplitude doubles and it vibrates violently, but AP 2 - BP 2 = λ/2 (where λ = wavelength of the ultrasonic wave)
At point P2 , the ultrasonic waves from the transducers A and B are interfered with and the amplitude is always extremely small, resulting in seizure, statesking, etc.

[発明が解決しようとする問題点] 本発明は、振動特性が等しい多数の振動子を配
設した連続鋳造用鋳型においても、各振動子から
発信される超音波の干渉を調整して、鋳型内壁の
メニスカス近傍の全ての壁面部に、望ましい振動
を常に与えるための加振方法を目的としている。
[Problems to be Solved by the Invention] Even in a continuous casting mold in which a large number of oscillators with the same vibration characteristics are arranged, the present invention adjusts the interference of ultrasonic waves emitted from each oscillator, and improves the mold quality. The objective is to provide a vibration method that constantly applies desired vibrations to all wall surfaces near the meniscus of the inner wall.

[問題点を解決するための手段] 本発明は (1)振動特性が等しい振動子を複数個配設した連
続鋳造用鋳型において、各振動子の加振周波数の
差を2KHz以内の範囲に保ち、且つ隣り合う振動
子の加振周波数を変えて加振する事を特徴とす
る、連続鋳造用超音波振動モールドの加振方法で
あり、(2)隣り合う振動子の加振周波数を変えて加
振する方法が、加振周波数が最大となる振動子
(基準振動子)に対して、基準振動子の片側ある
いは両側に配設した他の各振動子の加振周波数
を、基準振動子から遠ざかるに従い順次小さくな
るように設定した方法である、前記(1)に記載の、
連続鋳造用超音波モールドの加振方法である。
[Means for Solving the Problems] The present invention has the following features: (1) In a continuous casting mold in which a plurality of vibrators having the same vibration characteristics are arranged, the difference in the excitation frequency of each vibrator is maintained within a range of 2 KHz. , and is a method of exciting an ultrasonic vibration mold for continuous casting, which is characterized by changing the excitation frequency of adjacent vibrators and excitation, and (2) changing the excitation frequency of adjacent vibrators. The method of excitation is to change the excitation frequency of each other vibrator placed on one side or both sides of the reference vibrator from the reference vibrator to the vibrator with the maximum excitation frequency (reference vibrator). The method described in (1) above is a method in which the distance is set to gradually decrease as the distance increases.
This is a method of excitation of an ultrasonic mold for continuous casting.

[作用及び実施例] 本発明は振動特性が等しい振動子を複数個配設
した連続鋳造用鋳型に関する。超音波振動鋳型に
は第1図に例示した如く、多数の例えば電歪型振
動子が配設されるが、各振動子は振動特性が等し
い方が互換性もきゝ設備コストも低減出来るし又
シユミレーシヨン等による鋳型振動パターンの設
計も容易となる。
[Operations and Examples] The present invention relates to a mold for continuous casting in which a plurality of vibrators having the same vibration characteristics are arranged. As illustrated in Fig. 1, an ultrasonic vibration mold is equipped with a large number of, for example, electrostrictive vibrators, but it is better for each vibrator to have the same vibration characteristics for better compatibility and to reduce equipment costs. Furthermore, it becomes easy to design the mold vibration pattern by simulation or the like.

本発明では、各振動子は、加振周波数が異る超
音波を発信する。第3図は1個の振動子の、周波
数−振幅特性の例を示す図である。各々の振動子
の周波数は周波数設定器により変更設定が出来る
が、最大の振幅が得られる周波数f0に対して、
(f0−1)KHz未満あるいは(fo+1)KHz超に
周波数を設定すると、第3図にみられる如くその
振動子の発する超音波の振幅は急激に小となり、
又その結果各振動子の発する超音波の合成振幅も
顕著に低下することとなる。各振動子の振幅は従
つて最大振幅A1からはA1×70%の範囲に保つこ
とが望ましく、この振幅を得るための周波数の調
整範囲は第3図から(fo−1)KHz〜(fo+1)
KHzの2KHzの範囲となる。本発明では各振動子
はこの(fo−1)KHz〜(fo+1)KHzの間で各
振動子の周波数を違えて設定するため、各振動子
の周波数の差は2KHz以内となる。
In the present invention, each vibrator emits ultrasonic waves with different excitation frequencies. FIG. 3 is a diagram showing an example of frequency-amplitude characteristics of one vibrator. The frequency of each vibrator can be changed using a frequency setting device, but for the frequency f 0 that gives the maximum amplitude,
When the frequency is set below (f 0 −1) KHz or above (fo+1) KHz, the amplitude of the ultrasonic wave emitted by the transducer suddenly decreases, as shown in Figure 3.
As a result, the combined amplitude of the ultrasonic waves emitted by each vibrator also decreases significantly. Therefore, it is desirable to keep the amplitude of each vibrator in the range of A 1 × 70% from the maximum amplitude A 1 , and the frequency adjustment range to obtain this amplitude is from (fo-1) KHz to ( fo+1)
KHz to 2KHz range. In the present invention, each vibrator is set to have a different frequency between (fo-1) KHz and (fo+1) KHz, so the difference in frequency between the vibrators is within 2 KHz.

本発明では隣り合う振動子の加振周波数を変え
て加振する。例えば第2図で振動子Aから発信さ
れる超音波の周波数と振動子Bから発信される超
音波の周波数が同じであると、前述の如くP1
では干渉によつて振幅が常に重畳され倍増する。
第4図イはこの状態を図示したもので、点線は
P1点での振動子Aから発信された超音波を、鎖
線は振動子Bからの超音波を、実線は両者を合成
した振動を示す図である。又P2点では前述の如
く、Aからの振動とBからの振動が相互に打ち消
し合い常に小さな振幅の合成した振動となる。第
4図ロはこの状態を図示したものである。
In the present invention, adjacent vibrators are vibrated by changing their excitation frequencies. For example, in Figure 2, if the frequency of the ultrasonic waves emitted from transducer A is the same as the frequency of the ultrasonic waves emitted from transducer B, the amplitudes will always be superimposed at point P1 due to interference, as described above. Double.
Figure 4 A illustrates this state, and the dotted line is
The figure shows the ultrasonic wave emitted from the transducer A at point P1 , the chain line shows the ultrasonic wave from the transducer B, and the solid line shows the vibration that is a combination of both. Also, at point P2 , as mentioned above, the vibrations from A and the vibrations from B cancel each other out, resulting in a composite vibration with a constant small amplitude. FIG. 4B illustrates this state.

例えば振動子Aの周波数を大きくすると、Aか
らの超音波とBからの超音波は刻々に相対的位相
が変化するため、P1点で常に振動が重なり合う
事はない。第4図ハ,ニはこの状態を示す。又
P2点でも同様に常には振動が打ち消されること
がなく、P1点と同様の振幅の合成した振動が得
られることゝなる。以上振動子が2ヶの場合の例
を説明したが、例えば第5図イの如く、周波数が
同じmヶの振動子を配設した時の合成振幅は下式
A0でしめされる。
For example, when the frequency of transducer A is increased, the relative phase of the ultrasonic waves from A and B changes moment by moment, so the vibrations do not always overlap at point P1 . Figures 4(c) and 4(d) show this state. or
Similarly, at the P2 point, the vibrations are not always canceled out, and a combined vibration with the same amplitude as the P1 point is obtained. Above we have explained an example in which there are two oscillators, but for example, when m oscillators with the same frequency are arranged as shown in Figure 5A, the combined amplitude is calculated by the following formula.
It is indicated by A 0 .

Ao=ΣAncos{ω(t −|ln−x|/ν)e-an(|ln-x|) ……(1) An:各振動子同一パワー時位置の違いによる
振幅係数、ω:2πf(但しf:加振周波数Hz)、
t:加振経過時間(sec)、ln:No1振動子と各振
動子間距離、x:No1振動子位置を原点とした振
動位置、ν:モールドの音波伝搬速度、an:各
振動子の振幅が他部へ伝搬してゆくときの減数係
数。
Ao=ΣAncos {ω(t −|ln−x|/ν)e -an( | ln−x | ) ...(1) An: Amplitude coefficient due to difference in position when each vibrator has the same power, ω: 2πf( However, f: excitation frequency Hz),
t: Vibration elapsed time (sec), ln: Distance between the No. 1 transducer and each transducer, x: Vibration position with the No. 1 transducer position as the origin, ν: Sound wave propagation speed of the mold, an: Amplitude of each transducer The reduction coefficient when propagating to other parts.

この合成振幅は、鋳型の位置χに関して第5図
ロの如く表され、部分的に合成振幅が常に低い領
域が発生する事を示している。
This composite amplitude is expressed as shown in FIG. 5B with respect to the position χ of the mold, indicating that a region where the composite amplitude is always low is generated in some parts.

しかしこの場合も、隣接する振動子の周波数を
変える事により、第5図ハの如く鋳型内面各位置
での振幅分布は平坦化され、振動しない部分をな
くすることが出来る。
However, in this case as well, by changing the frequencies of the adjacent vibrators, the amplitude distribution at each position on the inner surface of the mold can be flattened, as shown in FIG.

尚本発明で振動子相互の間の周波数の差は、前
述の如く最大は2KHzとするが、最小は0.01KHzで
あり、これ以下では効果が小さい。
In the present invention, the maximum frequency difference between the vibrators is 2 KHz as described above, but the minimum is 0.01 KHz, and below this, the effect is small.

又本発明で、隣り合う振動子の加振周波数を変
えて加振するに際し、加振周波数が最大となる振
動子(基準振動子)に対して、基準振動子の片側
あるいは両側に配設した他の各振動子の加振周波
数を、基準振動子から遠ざかるに従い順次小なる
ように設定すると、うなり波の振幅分布が、経過
時間と共に方向性をもつて進むため、鋳型のどの
位置にも周期的に均一で好ましい振幅分布を付与
できることとなる。
In addition, in the present invention, when excitation is performed by changing the excitation frequency of adjacent vibrators, the vibrator (reference vibrator) with the maximum excitation frequency is placed on one side or both sides of the reference vibrator. If the excitation frequency of each of the other oscillators is set to gradually decrease as it moves away from the reference oscillator, the amplitude distribution of the beat wave will progress directionally with elapsed time, so there will be no periodicity at any position on the mold. Therefore, it is possible to provide a uniform and preferable amplitude distribution.

第6図は各振動子の周波数のモデルを示す図で
ある。例えば第1図の3,4,5,6の各振動子
の周波数を無秩序に変えて設定した例を第6図イ
に示した。第6図ロは振動子3を基準振動子と
し、4,5,6の振動子の加振周波数を、基準振
動子3から遠ざかるに従い順次小なるように設定
した例で、第6図ハは振動子4を基準振動子と
し、地の振動子の加振周波数を同様に順次小なる
ように設定した例で、第6図ニは振動子5を基準
振動子とした同様の例、第6図ホは振動子6を基
準振動子とした同様の例である。第6図イではう
なり波の振幅分布が一方向に進行しないために、
方向性をもつて進行するロ,ハ,ニ,ホの場合に
比べて効果は小さい。
FIG. 6 is a diagram showing a model of the frequency of each vibrator. For example, FIG. 6A shows an example in which the frequencies of each of the vibrators 3, 4, 5, and 6 in FIG. 1 are randomly changed and set. Figure 6(b) is an example in which the oscillator 3 is used as the reference oscillator, and the excitation frequencies of the 4th, 5th, and 6th oscillators are set to become smaller as they move away from the reference oscillator 3. This is an example in which the vibrator 4 is used as a reference vibrator and the excitation frequency of the earth vibrator is similarly set to decrease sequentially. Figure E shows a similar example in which the vibrator 6 is used as a reference vibrator. In Figure 6 A, since the amplitude distribution of the beat wave does not proceed in one direction,
The effect is smaller than in the case of B, C, D, and E, which progress in a direction.

[発明の効果] 本発明は、同じ特性の振動子を多数個使用する
方法であるために加振制御が容易であり設備コス
トも少なくてすむ。本発明により超音波振動モー
ルドで常に振動の小さい部分がなくなり、且つ超
音波振動モールドの各部分の振動が均一化され且
つ振幅が増大する。従つて溶湯とモールド内壁の
焼付等が解消され、ブレークアウト事故等が防止
できるし又鋳片表面の品質が向上するため疵取り
や表面手入が簡易化されあるいは不必要となり、
歩留りや能率が大幅に向上する。
[Effects of the Invention] Since the present invention is a method of using a large number of vibrators with the same characteristics, vibration control is easy and equipment costs can be reduced. According to the present invention, there is always no part of the ultrasonic vibrating mold where the vibration is small, and the vibration of each part of the ultrasonic vibrating mold is made uniform and the amplitude is increased. Therefore, seizure of the molten metal and the inner wall of the mold is eliminated, breakout accidents can be prevented, and the quality of the slab surface is improved, making scratch removal and surface maintenance easier or unnecessary.
Yield and efficiency are greatly improved.

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

第1図は多数の振動子を配設した連続鋳造用振
動モールドの横断面の例を示す図、第2図は2個
の振動子から発信された超音波のモールド内壁面
での干渉を示す図、第3図は個々の振動子の周波
数と振幅の関係を示す図、第4図は第2図での合
成した振動の例を示す図、第5図はm個の振動子
による合成した振幅を示す図、第6図は多数の振
動子を配設したモールドで、各振動子の設定周波
数のモデルの例を示す図、である。
Figure 1 is a diagram showing an example of a cross section of a vibrating mold for continuous casting in which a large number of vibrators are arranged, and Figure 2 is a diagram showing the interference of ultrasonic waves emitted from two vibrators on the inner wall surface of the mold. Figure 3 is a diagram showing the relationship between frequency and amplitude of individual oscillators, Figure 4 is a diagram showing an example of the combined vibration in Figure 2, and Figure 5 is a diagram showing the relationship between the frequency and amplitude of each vibrator. FIG. 6 is a diagram showing the amplitude, and is a diagram showing an example of a model of the set frequency of each vibrator in a mold in which a large number of vibrators are arranged.

Claims (1)

【特許請求の範囲】 1 振動特性が等しい振動子を複数個配設した連
続鋳造用鋳型において、各振動子の加振周波数の
差を2KHz以内の範囲で、隣り合う振動子の加振
周波数を変えて加振する事を特徴とする、連続鋳
造用超音波振動モールドの加振方法。 2 隣り合う振動子の加振周波数を変えて加振す
る方法が、加振周波数が最大となる振動子(基準
振動子)に対して、基準振動子の片側あるいは両
側に配設した他の各振動子の加振周波数を、基準
振動子から遠ざかるに従い順次小さくなるように
設定した方法である、特許請求の範囲第1項に記
載の、連続鋳造用超音波振動モールドの加振方
法。
[Scope of Claims] 1. In a continuous casting mold in which a plurality of vibrators with the same vibration characteristics are arranged, the excitation frequency of adjacent vibrators is set within a range of 2 KHz or less between the excitation frequencies of each vibrator. A method of exciting an ultrasonic vibration mold for continuous casting, which is characterized by changing the vibration. 2 The method of excitation by changing the excitation frequency of adjacent vibrators is to apply vibrations to the vibrator (reference vibrator) with the maximum excitation frequency, and to vibrate other vibrators placed on one or both sides of the reference vibrator. 2. A method for exciting an ultrasonic vibration mold for continuous casting according to claim 1, wherein the vibration frequency of the vibrator is set to gradually decrease as the distance from the reference vibrator increases.
JP62214174A 1987-08-29 1987-08-29 Method for exciting ultrasonic oscillation mold for continuous casting Granted JPS6462256A (en)

Priority Applications (8)

Application Number Priority Date Filing Date Title
JP62214174A JPS6462256A (en) 1987-08-29 1987-08-29 Method for exciting ultrasonic oscillation mold for continuous casting
EP88113989A EP0305930B1 (en) 1987-08-29 1988-08-26 Method of oscillating continuous casting mold at high frequencies and mold oscillated by such method
ES198888113989T ES2034073T3 (en) 1987-08-29 1988-08-26 METHOD TO ROCK A MOLD FOR CONTINUOUS CASTING AT HIGH FREQUENCIES AND MOLD MADE TO ROCK BY SUCH A METHOD.
CA000575784A CA1316325C (en) 1987-08-29 1988-08-26 Method of oscillating continuous casting mold at high frequencies and mold oscillated by such method
DE8888113989T DE3873451T2 (en) 1987-08-29 1988-08-26 CONTINUOUS CHOCOLATE AND METHOD FOR THEIR HIGH FREQUENCY OSCILLATION.
AU21623/88A AU603251B2 (en) 1987-08-29 1988-08-29 Method of oscillating continuous casting mold at high frequencies and mold oscillated by such method
US07/237,740 US4867226A (en) 1987-08-29 1988-08-29 Method of oscillating continuous casting mold at high frequencies and mold oscillated by such method
KR1019880010986A KR920004972B1 (en) 1987-08-29 1988-08-29 Method of oscilating continuous casting mold at high frequencies and mold oscillated by such method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62214174A JPS6462256A (en) 1987-08-29 1987-08-29 Method for exciting ultrasonic oscillation mold for continuous casting

Publications (2)

Publication Number Publication Date
JPS6462256A JPS6462256A (en) 1989-03-08
JPH0325262B2 true JPH0325262B2 (en) 1991-04-05

Family

ID=16651460

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62214174A Granted JPS6462256A (en) 1987-08-29 1987-08-29 Method for exciting ultrasonic oscillation mold for continuous casting

Country Status (1)

Country Link
JP (1) JPS6462256A (en)

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CN104057040B (en) * 2014-06-23 2016-03-16 安徽工业大学 A kind of pinion steel horizontal casting applies the devices and methods therefor of ultrasonic wave vibration

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