JPH0325263B2 - - Google Patents

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Publication number
JPH0325263B2
JPH0325263B2 JP21417587A JP21417587A JPH0325263B2 JP H0325263 B2 JPH0325263 B2 JP H0325263B2 JP 21417587 A JP21417587 A JP 21417587A JP 21417587 A JP21417587 A JP 21417587A JP H0325263 B2 JPH0325263 B2 JP H0325263B2
Authority
JP
Japan
Prior art keywords
frequency
vibrator
mold
excitation
setting
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
JP21417587A
Other languages
Japanese (ja)
Other versions
JPS6462257A (en
Inventor
Katsuhiko Yui
Juichi Kato
Daijiro Mizukoshi
Tetsuo Nakamura
Masaji Uehara
Kenzo Sawada
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 JP62214175A priority Critical patent/JPS6462257A/en
Priority to DE8888113989T priority patent/DE3873451T2/en
Priority to ES198888113989T priority patent/ES2034073T3/en
Priority to CA000575784A priority patent/CA1316325C/en
Priority to EP88113989A priority patent/EP0305930B1/en
Priority to KR1019880010986A priority patent/KR920004972B1/en
Priority to AU21623/88A priority patent/AU603251B2/en
Priority to US07/237,740 priority patent/US4867226A/en
Publication of JPS6462257A publication Critical patent/JPS6462257A/en
Publication of JPH0325263B2 publication Critical patent/JPH0325263B2/ja
Granted legal-status Critical Current

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Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は高周波振動をモールドに付与しながら
金属を連続鋳造する際に用いる連続鋳造用高周波
振動モールド(以下振動モールドと略記する)の
加振方法に関する。
[Detailed Description of the Invention] [Industrial Application Field] The present invention is directed to excitation of a high-frequency vibration mold for continuous casting (hereinafter abbreviated as vibration mold) used when continuously casting metal while applying high-frequency vibration to the mold. Regarding the method.

特願昭60−197617号は、複数個の振動子を配設
した振動モールドの加振方法で、相隣り合う振動
子の加振周波数差をうなり発生限界周波数差以上
として、鋳型壁を高周波加振する方法である。し
かしこの方法では各振動子の加振周波数を大きく
相違させるために、振動子の管理が厄介である。
Japanese Patent Application No. 197617 describes a method of excitation of a vibrating mold equipped with multiple vibrators, in which the mold wall is subjected to high-frequency excitation with the excitation frequency difference between adjacent vibrators being equal to or higher than the beat generation limit frequency difference. This is a method of shaking. However, in this method, the excitation frequency of each vibrator is greatly different, making management of the vibrators difficult.

第10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。1個の振動子の加振周波数
は、周波数設定器を制御して変更する事は出来
る。しかし最大の振幅が得られる周波数がfoであ
る振動氏の周波数を(fo−1)KHz未満にしたり
あるいは(fo+1)KHz超にすると、第10図に
みられる如くその振幅は急激に小さくなる。
FIG. 10 is a diagram showing an example of frequency-amplitude characteristics of one vibrator. The excitation frequency of one vibrator can be changed by controlling the frequency setter. However, if the frequency of the vibration at which the maximum amplitude is obtained is fo, it becomes less than (fo-1) KHz or more than (fo+1) KHz, the amplitude decreases rapidly as shown in FIG.

特願昭60−197617号の方法では各振動子の加振
周波数を大きく相違させるが、各振動子を同じ加
振特性の振動子に統一するとこの方法では第10
図の如く一部の振動子の振幅を小さくして加振す
ることとなるために好ましくなく、又加振特性の
異なる複数種類の振動子を振動モールドに配設す
ると、制御や管理が厄介となる。
In the method of Japanese Patent Application No. 60-197617, the excitation frequency of each vibrator is greatly different, but if all the vibrators are unified to vibrators with the same excitation characteristics, this method
As shown in the figure, it is undesirable because some of the vibrators must be excited with a small amplitude, and if multiple types of vibrators with different excitation characteristics are arranged in a vibrating mold, control and management becomes difficult. Become.

[発明が解決しようとする問題点] 振動モールドに配置する複数の振動子は、性能
の等しい振動子である事が制御や管理上望まし
い。しかし例えば、加振周波数や振幅を同じに設
定した複数の振動子で振動モールドを加振する
と、合成振動は定常波となり、この定常波で振動
モールドを加振することとなる。この定常波は進
行しないために、定常波の節に相当する位置の振
動モールドの壁面では振幅が極めて小さくなり、
このために節に相応する位置でフラツクス(振動
モールド内壁面と溶湯との潤滑剤)が円滑に流入
せず、振動モールドの内壁面と溶湯との焼付きが
発生することとなる。
[Problems to be Solved by the Invention] For control and management purposes, it is desirable that the plurality of vibrators placed in the vibrating mold have the same performance. However, for example, when a vibrating mold is vibrated with a plurality of vibrators having the same excitation frequency and amplitude, the resulting vibration becomes a standing wave, and the vibrating mold is vibrated with this standing wave. Since this standing wave does not travel, the amplitude becomes extremely small on the wall of the vibrating mold at the position corresponding to the node of the standing wave.
For this reason, flux (a lubricant between the inner wall surface of the vibrating mold and the molten metal) does not flow smoothly at positions corresponding to the nodes, and seizure between the inner wall surface of the vibrating mold and the molten metal occurs.

各振動子の加振周波数は、第10図に示す如
く、(fo−1)KHz〜(fo+1)KHzの間に設定
すると、各振動子の振幅は大きく保たれるために
望ましい。各振動子の周波数を(fo−1)KHz〜
(fo+1)KHzの間でそれぞれ相違させて振動モ
ールドを加振すると定常波は軽減されるが、しか
し加振周波数の差が小さいために、特別の工夫を
行なわないと矢張り進行しない合成振動が形成さ
れて、振動モールドの内壁面で、大きな振幅で加
振される部分と常に小さな振幅で加振される部分
が発生し、この小さな振幅で加振される部分で、
振動モールドと溶湯との焼付きが発生することゝ
なる。
As shown in FIG. 10, it is preferable to set the excitation frequency of each vibrator between (fo-1) KHz and (fo+1) KHz because the amplitude of each vibrator can be kept large. Set the frequency of each vibrator to (fo−1)KHz~
(fo + 1) KHz When the vibrating mold is excited at different frequencies, the standing waves are reduced, but because the difference in the excitation frequencies is small, a composite vibration is formed that will not progress rapidly unless special measures are taken. As a result, on the inner wall surface of the vibrating mold, there are parts that are vibrated with a large amplitude and parts that are always vibrated with a small amplitude, and in these parts that are vibrated with a small amplitude,
Seizure between the vibrating mold and the molten metal will occur.

本発明は、同じ加振特性の複数の振動子を配置
した振動モールドにおいて、各振動子の加振周波
数を、(fo−1)KHz〜(fo+1)KHzの間に設
定して振動モールドを加振するに際して、振動モ
ールドに局所的に振幅の常に小さい箇所を発生さ
せる事なく、振動モールドの全部分を万遍なく大
きな振幅で加振する、振動モールドの加振方法を
目的としている。
In a vibrating mold in which a plurality of vibrators having the same excitation characteristics are arranged, the present invention applies the vibrating mold by setting the excitation frequency of each vibrator between (fo-1) KHz and (fo+1) KHz. To provide a vibrating method for a vibrating mold that vibrates all parts of the vibrating mold uniformly and with a large amplitude without causing localized parts of the vibrating mold where the amplitude is always small when vibrating.

[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
設した振動モールドにおいて、各振動子の加振周
波数を2KHz以内の範囲内で、隣り合う振動子の
加振周波数が異なるように設定すると共に、各振
動子の加振周波数を、時間経過と共に断続的ある
いは連続的にそれぞれ変えて加振させる事を特徴
とする、振動モールドの加振方法である。
[Means for Solving the Problems] The present invention provides (1) In a vibrating mold in which a plurality of vibrators having the same vibration characteristics are arranged, the excitation frequency of each vibrator is set within a range of 2 KHz, and adjacent vibrations are A vibrating mold excitation method characterized by setting the excitation frequency of each vibrator to be different, and changing the excitation frequency of each vibrator intermittently or continuously over time. be.

以下本発明の(1)を第1図によつて具体的に説明
する。第1図は振動モールドの横断面の例を示す
図で、a〜lは振動特性が等しい振動子で鋳型1
の内壁を加振する。以下振動子a〜dについて説
明する。
Hereinafter, (1) of the present invention will be specifically explained with reference to FIG. Figure 1 is a diagram showing an example of a cross section of a vibrating mold.
vibrates the inner wall of the The vibrators a to d will be explained below.

加振中の特定の時期T1における各振動子とそ
の振動数を、 a:νa、b:νb、c:νc、d:νd とすると、本発明で各振動子の周波数設定器を制
御して、νa〜νdを下記の如く設定する。
Assuming that each vibrator and its frequency at a specific time T1 during excitation are a: νa, b: νb, c: νc, and d: νd, the frequency setter of each vibrator is controlled by the present invention. Then, νa to νd are set as follows.

νmax−νmin<2KHz ……(1) 但し、νmax:νa〜νdのうち周波数が最大の振
動子の周波数、νmit:νa〜νaのうち周波数が最
小の振動子の周波数。更に本発明では νa≠νb、νb≠νc、νc≠νd ……(2) となる如く、νa〜νdは設定してある。
νmax−νmin<2KHz...(1) However, νmax: The frequency of the oscillator with the maximum frequency among νa to νd, νmit: The frequency of the oscillator with the minimum frequency among νa to νa. Further, in the present invention, νa to νd are set so that νa≠νb, νb≠νc, νc≠νd (2).

T1からt秒後の時期T2において各振動子の加
振周波数を変更して a:νa′、b:νb′、c:νc′、d:νd′ とする。尚νa′〜νd′も、(1)式及び(2)式をそれぞれ
満足するように設定する。
At time T2 , which is t seconds after T1, the excitation frequency of each vibrator is changed to a: νa', b: νb', c: νc', and d: νd'. Note that νa′ to νd′ are also set so as to satisfy equations (1) and (2), respectively.

T2を更にt秒後には、各振動子を加振周波数
を a:νa″、b:νb″、c:νc″、d:νd″とする
が、νa″、νb″、νc″、νd″前記と同様に(1)式及
び(2)
式をそれぞれ満足するように設定する。尚この
際、νa=νa″、νb=νb″、νc=νc″、νd=νd″
とし
てもよい。
After t seconds after T 2 , the excitation frequencies of each vibrator are set to a: νa'', b: νb'', c: νc'', d: νd'', and νa'', νb'', νc'', νd ``Similar to the above, equations (1) and (2)
Set each expression so that it is satisfied. In this case, νa=νa″, νb=νb″, νc=νc″, νd=νd″
You can also use it as

以下、同様に時間経過と共に断続的あるいは連
続的に各振動子の加振周波数を変更して振動モー
ルドを加振する。
Thereafter, similarly, the vibration mold is vibrated by changing the excitation frequency of each vibrator intermittently or continuously as time passes.

以上振動子a〜dについて説明したがe〜lに
ついても同様に行なう。又 本発明の(2)は隣り合う振動子の加振周波数が異
なるように設定する方法が、特定の振動子(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な
設定(設定)、又は該基準振動子の片側あるい
は両側に配設した他の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大となるような
設定(設定)であり、各振動子の加振周波数を
時間経過と共に断続的あるいは連続的にそれぞれ
変えて加振させる方法が、時間経過と共に設定
から設定へ、次には設定から設定へ断続的
にあるいは連続的に変えて加振させる方法であ
る、前記(1)に記載の、連続鋳造用高周波振動モー
ルドの加振方法である。
The above description has been made for the vibrators a to d, but the same applies to the vibrators e to l. In addition, (2) of the present invention is a method of setting the excitation frequencies of adjacent vibrators to be different, such as by arranging them on one side or both sides of the reference vibrator with respect to a specific vibrator (reference vibrator). The excitation frequency of each vibrator is set to become smaller as it moves away from the reference vibrator, or the excitation frequency of other vibrators placed on one or both sides of the reference vibrator is set as the reference vibrator. It is a setting (setting) that gradually increases as it moves away from the vibrator, and the method of excitation by changing the excitation frequency of each vibrator intermittently or continuously over time is to change the setting from the setting as time passes. Next, there is a method of excitation of a high-frequency vibration mold for continuous casting as described in (1) above, which is a method of excitation while changing settings intermittently or continuously.

本発明の(2)を第1図について説明する。基準振
動子はa〜dの任意の振動子でよい。例えば振動
子aを基準振動子にすると、特定の時期T1にお
ける各振動子の周波数は設定であり、前記の(1)
式は 0<νa−νd<2KHz ……(1′) (1′)式となり、又(2)式は νa>νb>νc>νd ……(2′) (2′)式となる。
(2) of the present invention will be explained with reference to FIG. The reference vibrator may be any vibrator from a to d. For example, if oscillator a is used as the reference oscillator, the frequency of each oscillator at a specific time T1 is a setting, and the above (1)
The equation becomes 0<νa−νd<2KHz...(1') (1') equation, and equation (2) becomes νa>νb>νc>νd...(2') (2') equation.

T1からt秒後の時期T2においては、各振動子
の加振周波数を下記の(1)″式及び(2)″式式
を満足するような設定に変更する。
At time T2 , which is t seconds after T1 , the excitation frequency of each vibrator is changed to a setting that satisfies the following expressions (1)'' and (2)''.

0<ν′d−ν′a<2KHz ……(1″) ν′a<ν′b<ν′c<ν′d ……(2″) T2から更にt秒後の各振動子の加振周波数
νa″、νb″、νc″、νd″は νa:νa″、νb:νb″、νc:νc″、νd:νd″と
する。
従つて、νa″、νb″、νc″、νd″についても(1)′
式及
び(2′)式が成立する。
0<ν′d−ν′a<2KHz……(1″) ν′a<ν′b<ν′c<ν′d……(2″) Each oscillator after t seconds after T 2 The excitation frequencies νa″, νb″, νc″, and νd″ are νa: νa″, νb: νb″, νc: νc″, and νd: νd″.
Therefore, for νa″, νb″, νc″, and νd″, (1)′
Equations and (2') hold true.

以下同様に時間経過と共に断続的あるいは連続
的に、設定から設定へ、更に設定から設定
へ、繰返して振動モールドを加振する。
Thereafter, the vibrating mold is similarly vibrated intermittently or continuously as time passes, from setting to setting, and then from setting to setting.

[作用及び実施例] 第2図は、第1図のa,b,c,dの各振動子
が下記の加振周波数で振動モールドの1を加振し
た際の、モールド1の振動状況を示す図である。
[Operations and Examples] Figure 2 shows the vibration status of mold 1 when each of the vibrators a, b, c, and d in Figure 1 vibrates mold 1 at the following excitation frequencies. FIG.

a:νaKHz、b:(νa−1)KHz、c:νaKHz、
d:(νa−1)KHz 第2図のイは加振開始後0〜t秒の間の、ロは
t〜2t秒の間の、ハは2t〜3t秒の間の、ニは3t〜
4t秒の間の、ホは4t〜5t秒の間の振動状況であ
る。図中点線は、各時間内での最大振幅の範囲で
ある。第2図に見られる如く、各振動子の振動は
重なり合つて、点線で示した波束を形成する。こ
の波束は時間経過と共にイ→ロ→ハ→ニと変化し
て、ホに至り一周期が完了する。以後は時間の経
過と共にイ〜ホを繰り返す。第3図は第2図のイ
〜ホを同一の図に重ね書きした際の図の外周を示
す図で、一周期の間での振動モールドの各位置に
おける最大振幅を示す図である。第3図で、例え
ば振動モールドのP1の位置は一周期の間に大き
な振幅で加振されるために常に振幅が大きく好ま
しいが、Q1の位置は常に小さい振幅でしか加振
されないこととなる。従つてQ1の位置では、振
動モールドと溶湯の焼付きが発生し易くなる。
a: νaKHz, b: (νa-1)KHz, c: νaKHz,
d: (νa-1) KHz In Figure 2, A is between 0 and t seconds after the start of vibration, B is between t and 2t seconds, C is between 2t and 3t seconds, and D is between 3t and 3t seconds.
During 4t seconds, Ho is the vibration situation between 4t and 5t seconds. The dotted line in the figure is the range of maximum amplitude within each time period. As seen in FIG. 2, the vibrations of each vibrator overlap to form a wave packet shown by a dotted line. This wave packet changes from A to B to C to D as time passes, and reaches E, completing one cycle. After that, repeat I-ho as time passes. FIG. 3 is a diagram showing the outer periphery of the diagram when I to E of FIG. 2 are superimposed on the same diagram, and is a diagram showing the maximum amplitude at each position of the vibrating mold during one cycle. In Figure 3, for example, position P 1 of the vibrating mold is always vibrated with a large amplitude during one cycle, so it is always desirable to have a large amplitude, but position Q 1 is always vibrated with only a small amplitude. Become. Therefore, at the position Q1 , seizing of the vibrating mold and the molten metal is likely to occur.

第4図は、a:νaKHz、b:(νa+1)KHz、
c:νaKHz、d:(νa+1)KHzに設定した際の、
一周期の間でのモールドの各位置における最大振
幅を示す図である。
Figure 4 shows a: νaKHz, b: (νa+1)KHz,
When set to c: νaKHz, d: (νa+1)KHz,
It is a figure which shows the maximum amplitude in each position of a mold during one period.

各振動子の加振周波数を変えると、振動モール
ドで振幅の大きな位置は例えば第4図のP2とな
り又振幅の小さな位置は例えばQ2となる。第5
図は第3図と第4図を同一の重ね書きしてその外
周を示す図である。即ち各振動子の周波数を第3
図で説明した如くにt1秒間設定し、次に第4図で
説明した如くに変更してt2秒間設定すると、t1
t2秒間に振動モールドに加えられる最大の振幅は
第5図に示した如く、振動モールドの各位置で均
一化され、常に小さな振幅で加振される位置は消
滅する。
When the excitation frequency of each vibrator is changed, the position of a large amplitude in the vibrating mold becomes, for example, P 2 in FIG. 4, and the position of a small amplitude becomes, for example, Q 2 . Fifth
The figure is a diagram showing the outer periphery of FIG. 3 and FIG. 4 by overwriting them in the same manner. In other words, the frequency of each vibrator is
If we set t for 1 second as explained in the figure, then change it as explained in figure 4 and set t for 2 seconds, t 1 +
As shown in FIG. 5, the maximum amplitude applied to the vibrating mold during t 2 seconds is made uniform at each position of the vibrating mold, and the positions that are always vibrated with a small amplitude disappear.

以上の如く、各振動子の加振周波数を加振の途
中で変更すると振動モールドに局所的に振幅の常
に小さい箇所は発生しなくなる。
As described above, if the excitation frequency of each vibrator is changed during excitation, there will be no localized areas in the vibrating mold where the amplitude is always small.

第6図は本発明(2)の例で、設定を基準振動子
をaとして、a:νaKHz、b:(νa−0.3)KHz、
c:(νa−0.6)KHz、d:(νa−0.9)KHzに設定
した際の、一周期の間のモールドの各位置におけ
る最大振幅を示す図である。この設定での波束
は、振動子aから振動子dへ向かう群速度をもつ
たうなり波となるために、一周期の間のモールド
の各位置での最大振幅は第3図よりも均等化され
る。各振動子の加振周波数をt2秒間第6図の如く
設定した後で、設定に変更する。この際各振動
子の加振周波数は、a:νaKHz、b:(νa+0.3)
KHz、c:(νa+0.6)KHz、d:(νa+0.9)KHz とする。設定でt4秒間保持するがこの際のモー
ルド各位置における最大振幅の分布は第7図とな
る。
FIG. 6 shows an example of the present invention (2), where the reference oscillator is a, a: νaKHz, b: (νa−0.3)KHz,
It is a figure showing the maximum amplitude at each position of the mold during one cycle when setting c: (va-0.6) KHz and d: (va-0.9) KHz. In this setting, the wave packet becomes a beat wave with a group velocity traveling from oscillator a to oscillator d, so the maximum amplitude at each position of the mold during one period is more equalized than in Fig. 3. Ru. After setting the excitation frequency of each vibrator for t 2 seconds as shown in Fig. 6, change the setting. At this time, the excitation frequency of each vibrator is a: νaKHz, b: (νa + 0.3)
KHz, c: (νa + 0.6) KHz, d: (νa + 0.9) KHz. The setting is held for t 4 seconds, and the distribution of the maximum amplitude at each position of the mold at this time is shown in Figure 7.

第8図は、第6図と第7図を同一の図に重ね書
きしてその外周を示す図である。即ちt3+t4秒間
に振動モールドの各位置に加えられる最大の振幅
を示す。第8図は第5図よりも一層均一化された
振動分布を示すこととなる。
FIG. 8 is a diagram showing the outer periphery of FIG. 6 and FIG. 7 overlaid on the same diagram. That is, it shows the maximum amplitude applied to each position of the vibrating mold during t 3 +t 4 seconds. FIG. 8 shows a more uniform vibration distribution than FIG. 5.

第9図は、基準振動子を他の振動子とした場合
の例を示す図で、イ図は振動子bを、ロ図は振動
子cを、ハ図は振動子dを基準振動子とした例
で、実線は設定で点線は設定である。
Fig. 9 is a diagram showing an example in which the reference oscillator is used as another oscillator. In this example, the solid line is the setting and the dotted line is the setting.

[発明の効果] 本発明により、複数の振動子を配置した振動モ
ールドにおいて、各振動子の周波数を大幅に相違
させないために全ての振動子を振動特性が等しい
同じタイプの振動子とする事ができ、振動子制御
や管理が容易となる。又本発明により振動モール
ドに局所的に振幅が常に小さい箇所が発生する事
はなく、振動モールドの全部分が万遍なく大きな
振幅で加振される。従つてフラツクスの流入も円
滑で鋳片の鋳肌も優れ、又焼付き等も発生しない
ため鋳造事故も防止できる。
[Effects of the Invention] According to the present invention, in a vibrating mold in which a plurality of vibrators are arranged, all the vibrators can be made of the same type of vibrator with the same vibration characteristics in order to prevent the frequency of each vibrator from greatly differing. This makes it easier to control and manage the transducer. Furthermore, according to the present invention, there are no localized areas in the vibrating mold where the amplitude is always small, and all parts of the vibrating mold are uniformly vibrated with a large amplitude. Therefore, the flow of flux is smooth, the casting surface of the slab is excellent, and since seizure etc. do not occur, casting accidents can be prevented.

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

第1図は振動モールドの横断面を示す図、第2
図は各時期での振動モールド各部の最大振幅を示
す図、第3図は第2図の加振パターンでの振動モ
ールドの各位置での最大振幅を示す図、第4図は
他の加振パターンでの振動モールドの各位置の最
大振幅を示す図、第5図は第3図の加振パターン
と第4図の加振パターンに断続的に変更し組合せ
た際の振動モールドの各位置での最大振幅を示す
図、第6図は本発明(2)の設定における振動モー
ルドの各位置の最大振幅を示す図、第7図は設定
における振動モールドの各位置の最大振幅を示
す図、第8図は設定と設定に断続的に変更し
組合せた際の振動モールドの各位置での最大振幅
を示す図、第9図は基準振動子を変更した際の各
振動子の加振周波数の例を示す図、第10図は1
個の振動子の周波数−振幅特性を示す図、であ
る。
Figure 1 is a diagram showing a cross section of the vibration mold, Figure 2 is a diagram showing a cross section of the vibration mold.
The figure shows the maximum amplitude of each part of the vibrating mold at each period, Figure 3 shows the maximum amplitude at each position of the vibrating mold in the excitation pattern of Figure 2, and Figure 4 shows other excitation patterns. A diagram showing the maximum amplitude at each position of the vibrating mold in the pattern, Figure 5 shows the maximum amplitude at each position of the vibrating mold when the excitation pattern in Figure 3 and the excitation pattern in Figure 4 are intermittently changed and combined. 6 is a diagram showing the maximum amplitude of each position of the vibrating mold in the setting of the present invention (2). FIG. 7 is a diagram showing the maximum amplitude of each position of the vibrating mold in the setting. Figure 8 is a diagram showing the maximum amplitude at each position of the vibration mold when the settings are changed and combined intermittently, and Figure 9 is an example of the excitation frequency of each vibrator when the reference vibrator is changed. Figure 10 shows 1
FIG. 3 is a diagram showing frequency-amplitude characteristics of individual vibrators.

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
続鋳造用高周波振動モールドにおいて、各振動子
の加振周波数を2KHz以内の範囲内で、隣り合う
振動子の加振周波数が異なるように設定すると共
に、各振動子の加振周波数を時間経過と共に断続
的あるいは連続的にそれぞれ変えて加振させる事
を特徴とする、連続鋳造用高周波振動モールドの
加振方法。 2 隣り合う振動子の加振周波数が異なるように
設定する方法が、特定の振動子(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な設定(設定
)、又は該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大となるような設定(設
定)であり、各振動子の加振周波数を時間経過
と共に断続的あるいは連続的にそれぞれ変えて加
振させる方法が、時間経過と共に設定から設定
へ、次には設定から設定へ断続的にあるい
は連続的に変えて加振させる方法である、特許請
求の範囲第1項に記載の、連続鋳造用高周波振動
モールドの加振方法。
[Claims] 1. In a high-frequency vibration mold for continuous casting in which a plurality of vibrators with the same vibration characteristics are arranged, the excitation frequency of each vibrator is within a range of 2 KHz, and the excitation frequency of adjacent vibrators is A method for exciting a high-frequency vibrating mold for continuous casting, characterized in that the vibration frequency of each vibrator is set to be different, and the vibration frequency of each vibrator is changed intermittently or continuously over time. 2 The method of setting the excitation frequency of adjacent vibrators to be different is to set the excitation frequency of other vibrators placed on one side or both sides of the reference vibrator for a specific vibrator (reference vibrator). is set so that it becomes smaller as it moves away from the reference transducer, or the excitation frequency of each other transducer placed on one side or both sides of the reference transducer is set to gradually increase as it moves away from the reference transducer. The method of excitation by changing the excitation frequency of each vibrator intermittently or continuously over time is to change it from setting to setting over time, and then from setting to setting. A method of exciting a high-frequency vibration mold for continuous casting according to claim 1, which is a method of exciting a high-frequency vibration mold for continuous casting, which is a method of exciting a high-frequency vibration mold by changing settings intermittently or continuously.
JP62214175A 1987-08-29 1987-08-29 Method for controlling oscillation of high-frequency oscillation mold for continuous casting of metal Granted JPS6462257A (en)

Priority Applications (8)

Application Number Priority Date Filing Date Title
JP62214175A JPS6462257A (en) 1987-08-29 1987-08-29 Method for controlling oscillation of high-frequency oscillation mold for continuous casting of metal
DE8888113989T DE3873451T2 (en) 1987-08-29 1988-08-26 CONTINUOUS CHOCOLATE AND METHOD FOR THEIR HIGH FREQUENCY OSCILLATION.
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
EP88113989A EP0305930B1 (en) 1987-08-29 1988-08-26 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
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

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62214175A JPS6462257A (en) 1987-08-29 1987-08-29 Method for controlling oscillation of high-frequency oscillation mold for continuous casting of metal

Publications (2)

Publication Number Publication Date
JPS6462257A JPS6462257A (en) 1989-03-08
JPH0325263B2 true JPH0325263B2 (en) 1991-04-05

Family

ID=16651479

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62214175A Granted JPS6462257A (en) 1987-08-29 1987-08-29 Method for controlling oscillation of high-frequency oscillation mold for continuous casting of metal

Country Status (1)

Country Link
JP (1) JPS6462257A (en)

Also Published As

Publication number Publication date
JPS6462257A (en) 1989-03-08

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